专利汇可以提供Electromagnetic alignment and scanning apparatus专利检索,专利查询,专利分析的服务。并且An apparatus capable of high accuracy position and motion control utilizes one or more linear commutated motors to move a guideless stage in one long linear direction and small yaw rotation in a plane. A carrier/follower holding a single voice coil motor (VCM) is controlled to approximately follow the stage in the direction of the long linear motion. The VCM provides an electromagnetic force to move the stage for small displacements in the plane in a linear direction perpendicular to the direction of the long linear motion to ensure proper alignment. One element of the linear commutated motors is mounted on a freely suspended drive assembly frame which is moved by a reaction force to maintain the center of gravity of the apparatus. Where one linear motor is utilized, yaw correction can be achieved utilizing two VCMs.,下面是Electromagnetic alignment and scanning apparatus专利的具体信息内容。
What is claimed is:1. An exposure apparatus that transfers a pattern of a mask onto an object comprising:a mask stage that is movable while holding said mask;a first drive device connected to said mask stage to move said mask stage in a first direction;a balancing portion having a moving member that moves responsive to the movement of said mask stage in a direction opposite to the direction of movement of said mask stage; anda projection system that exposes said pattern onto said object, wherein at least a portion of said projection system is disposed below said mask and said balancing portion.2. An exposure apparatus according to claim 1, wherein said first drive device has a first portion connected to said mask stage and a second portion connected to said moving member.3. An exposure apparatus according to claim 2, wherein said first portion and said second portion are not in contact with each other.4. An exposure apparatus according to claim 2, wherein said first portion comprises a coil and said second portion comprises a magnet.5. An exposure apparatus according to claim 2, wherein the movements of said mask stage and of said moving member cooperatively follow the law of conservation of momentum.6. An exposure apparatus according to claim 1, wherein said first drive device comprises a linear motor.7. An exposure apparatus according to claim 1, further comprising a base structure that movably supports said mask stage.8. An exposure apparatus according to claim 7, wherein said moving member is movably supported by said base stricture.9. An exposure apparatus according to claim 7, wherein said mask stage is movable over a surface of said base structure via a bearing.10. An exposure apparatus according to claim 9, wherein said bearing is a non-contact bearing that opposes said mask stage to said base structure without contact therebetween.11. An exposure apparatus according to claim 1, further comprising a position detector that detects a position of said mask stage.12. An exposure apparatus according to claim 11, wherein said position detector comprises a reflective surface located on said mask stage.13. An exposure apparatus according to claim 12, wherein said reflective surface is a corner-cube mirror.14. An exposure apparatus according to claim 11, wherein said position detector detects a position of said mask stage with regard to a scanning direction during the movement of said mask stage.15. An exposure apparatus according to claim 11, wherein said position detector detects a position of said mask stage with regard to a direction that is different from a scanning direction during the movement of said mask stage.16. An exposure apparatus according to claim 11, further comprising a control system that corrects yaw rotation of said mask stage based on a detection result of said position detector.17. An exposure apparatus according to claim 16, wherein said control system is connected to said first drive device.18. An exposure apparatus according to claim 1, further comprising a second drive device that moves said mask stage in a second direction that is different from said first direction.19. An exposure apparatus according to claim 1, wherein said projection system projects the pattern optically.20. An exposure apparatus according to claim 1, wherein said moving member moves so that a center of gravity of said exposure apparatus does not shift substantially.21. An exposure apparatus according to claim 1, wherein said exposure apparatus is a scanning exposure apparatus that moves the mask and the object in a scanning manner.22. An exposure apparatus according to claim 1, wherein said balancing portion operates without a drive source.23. An exposure apparatus according to claim 1, further comprising:an object stage that holds said object; andan object stage drive device that moves said object stage, said object stage drive device comprising a planar motor.24. An object on which a pattern has been exposed utilizing the exposure apparatus of claim 1.25. An exposure apparatus that transfers a pattern of a mask onto an object comprising:movable mask holding means for movably holding said mask;first means for moving said mask holding means in a first direction;balancing means for moving responsive to the movement of said mask holding means in a direction opposite to the direction of movement of said mask holding means; andexposing means for exposing said pattern onto said object, wherein at least a portion of said exposing means is disposed below said mask and said balancing means.26. A method of making an exposure apparatus that transfers a pattern of a mask onto an object, the method comprising the steps of:providing a mask stage that is movable while holding said mask;providing a first drive device that is connected to said mask stage to move said mask stage in a first direction;providing a balancing portion having a moving member that moves responsive to the movement of said mask stage in a direction opposite to the direction of movement of said mask stage; andproviding a projection system that exposes said pattern onto said object, wherein at least a portion of said projection system is disposed below said mask and said balancing portion.27. A method according to claim 26, wherein said first drive device has a first portion connected to said mask stage and a second portion connected to said moving member.28. A method according to claim 27, wherein said first portion and said second portion do not contact each other.29. A method according to claim 27, wherein said first portion comprises a coil and said second portion comprises a magnet.30. A method according to claim 26, wherein the movements of said mask stage and of said moving member cooperatively follow the law of conservation of momentum.31. A method according to claim 26, wherein said first drive device comprises a linear motor.32. A method according to claim 26, wherein a base structure movably supports said mask stage.33. A method according to claim 32, wherein said moving member is movably supported by said base structure.34. A method according to claim 32, wherein said mask stage is movable over a surface of said base structure via a bearing.35. A method according to claim 34, wherein said bearing is a non-contact bearing that opposes said mask stage to said base structure without contact between said mask stage and said base structure.36. A method according to claim 26, further comprising providing a position detector that detects a position of said mask stage.37. A method according to claim 36, wherein said position detector comprises a reflective surface located on said mask stage.38. A method according to claim 37, wherein said reflective surface is a corner-cube mirror.39. A method according to claim 36, wherein said position detector detects a position of said mask stage with regard to a scanning direction during the movement of said mask stage.40. A method according to claim 36, wherein said position detector detects a position of said mask stage with regard to a direction that is different from a scanning direction during the movement of said mask stage.41. A method according to claim 36, further comprising providing a control system that adjusts yaw rotation of said mask stage based on a detection result of said position detector.42. A method according to claim 41, wherein said control system is connected to said first drive device.43. A method according to claim 26, further comprising providing a second drive device that moves said mask stage in a second direction that is different from said first direction.44. A method according to claim 26, wherein said projection system projects the pattern optically.45. A method according to claim 26, wherein said moving member moves so that a center of gravity of said exposure apparatus does not shift substantially.46. A method according to claim 26, wherein said exposure apparatus is a scanning exposure apparatus that moves the mask and the object during exposure.47. A method according to claim 26, wherein said balancing poriton operates without a drive source.48. method according to claim 26, further comprising:providing an object stage that holds said object; andproviding an object stage drive device that moves said object stage, said object stage drive device comprising a planar motor.49. An object on which a pattern has been exposed utilizing the exposure apparatus made by the method of claim 26.50. An exposure method for forming a pattern of a mask onto an object utilizing an exposure apparatus, the method comprising the steps of:moving a mask stage, which holds said mask, in a first direction;moving a balancing portion in a direction opposite to the direction of movement of said mask stage responsive to the movement of said mask stage; andexposing said pattern onto said object with a projection system, at least a portion of said projection system disposed below said mask and said balancing portion.51. A method according to claim 50, wherein said mask stage is moved by a first drive device having a first portion connected to said mask stage and a second portion connected to said balancing portion.52. A method according to claim 51, wherein said first portion and said second portion do not contact each other.53. A method according to claim 51, wherein said first portion comprises a coil and said second portion comprises a magnet.54. A method according to claim 51, wherein said first drive device comprises a linear motor.55. A method according to claim 50, wherein the movements of said mask stage and of said balancing portion cooperatively follow the law of conservation of momentum.56. A method according to claim 50, further comprising movably supporting said mask stage on a base structure.57. A method according to claim 56, wherein said balancing portion is movably supported by said base structure.58. A method according to claim 56, wherein said mask stage is movable over a surface of said base structure via a bearing.59. A method according to claim 58, wherein said bearing is a non-contact bearing that opposes said mask stage to said base structure without contact between said mask stage and said base structure.60. A method according to claim 50, further comprising detecting a position of said mask stage with a position detector.61. A method according to claim 60, wherein said position detector comprises a reflective surface located on said mask stage.62. A method according to claim 61, wherein said reflective surface is a corner-cube mirror.63. A method according to claim 60, wherein said position detector detects a position of said mask stage with regard to a scanning direction during the movement of said mask stage.64. A method according to claim 60, wherein said position detector detects a position of said mask stage with regard to a direction that is different from a scanning direction during the movement of said mask stage.65. A method according to claim 60, further comprising adjusting yaw rotation of said mask stage based on a detection result of said position detector.66. A method according to claim 50, further comprising moving said mask stage in a second direction that is different from said first direction.67. A method according to claim 50, wherein said projection system projects the pattern optically.68. A method according to claim 50, wherein said balancing portion moves so that a center of gravity of said exposure apparatus does not shift substantially.69. A method according to claim 50, wherein said exposure apparatus is a scanning exposure apparatus that moves said mask and said object during exposure.70. A method according to claim 50, wherein said balancing portion operates without a drive source.71. A method according to claim 50, further comprising:holding said object with an object stage; andmoving said object stage with an object stage drive device that includes a planar motor.
CROSS-REFERENCE TO RELATED APPLICATIONS
This is a Continuation-in-Part of application Ser. No. 08/698,827 filed Aug. 16, 1996, abandoned, which in turn is a Divisional of Application Ser. No. 09/260,544, filed Mar. 2, 1999, which is a Continuation of application Ser. No. 08/266,999 filed Jun. 27, 1994, abandoned.
BACKGROUND OF THE INVENTION
1. Field of Invention
The present invention relates to a movable stage apparatus capable of precise movement, and particularly relates to a stage apparatus movable in one linear direction capable of high accuracy positioning and high speed movement, which can be especially favorably utilized in a microlithographic system. This invention also relates to an exposure apparatus that is used for the transfer of a mask pattern onto a photosensitive substrate during a lithographic process to manufacture, for example, a semiconductor element, a liquid crystal display element, a thin film magnetic head, or the like.
2. Description of Related Art
When a semiconductor element or the like is manufactured, a projection exposure apparatus is used that transfers an image of a pattern of a reticle, used as a mask, onto each shooting area on a wafer (or a glass plate or the like) on which a resist is coated, used as a substrate, through a projection optical system. Conventionally, as a projection exposure apparatus, a step-and-repeat type (batch exposure type) projection exposure apparatus (stepper) has been widely used. However, a scanning exposure type projection exposure apparatus (a scanning type exposure apparatus), such as a step-and-scan type, which performs an exposure as a reticle and a wafer are synchronously scanned with respect to a projection optical system, has attracted attention.
In a conventional exposure apparatus, a reticle stage, which supports and carries the reticle, which is the original pattern, and the wafer to which the pattern is to be transferred, and the driving part of the wafer stage are fixed to a structural body that supports a projection optical system. The vicinity of the center of gravity of the projection optical system is also fixed to the structural body. Additionally, in order to position a wafer stage with high accuracy, the position of the wafer stage is measured by a laser interferometer, and a moving mirror for the laser interferometer is fixed to the wafer stage.
Furthermore, in order to carry a wafer to a wafer holder on the wafer stage, a wafer carrier arm that takes out a wafer from a wafer cassette and carries it to the wafer holder, and a wafer carrier arm that carries the wafer from the wafer holder to the wafer cassette, are independently provided. When the wafer is carried in, the wafer that has been carried by the wafer carrier arm is temporarily fixed to and supported by a special support member that can be freely raised and lowered and that is provided on the wafer holder. Thereafter, the carrier arm is withdrawn, the support member is lowered, and the wafer is disposed on the wafer holder. After this, the wafer is vacuum absorbed to the top of the wafer holder. When the wafer is carried out from the exposure device, the opposite operation is performed.
As described above, in the conventional exposure apparatus, the driving part of the wafer stage or the like and the projection optical system are fixed to the same structural body. Thus, the vibration generated by the driving reaction of the stage is transmitted to the structural body, and the vibration is also transmitted to the projection optical system. Furthermore, all the mechanical structures were mechanically resonate to a vibration of a predetermined frequency, so there are disadvantages such that deformation of the structural body and the resonance phenomenon occurred, and position shifting of a transfer pattern image and deterioration of contrast occurred when this type of vibration is transmitted to the structural body.
Furthermore, because the wafer stage moves over a long distance from the carrier arm for carrying in and out of the wafer to the exposure position, it is necessary to provide an extremely long moving mirror for the laser interferometer. Because of this, the weight of the wafer stage becomes relatively heavy and the driving reaction becomes large because a heavy motor with a large driving force is needed. Furthermore, in order to improve throughput, when the moving speed and acceleration of the stage needs to be increased, the driving reaction becomes even larger. In addition, as the weight and acceleration of the stage increase, the heating amount of the motor increases, and there is a disadvantage such that measurement stability or the like of the laser interferometer deteriorates.
Furthermore, in the case of carrying the wafer into and out of the exposure apparatus, the wafer is temporarily fixed and supported on the top of a special support member, so carrying in and out of the wafer consumes time. This causes deterioration of throughput. Additionally, as one example, because giving and receiving of the wafer is performed between the carrier arms, the probability of the wafer being contaminated is high, and the probability of having an operation error when the wafer was given and received is high. Furthermore, the number of carrier arms is a major point governing the size of the carrier unit, so the carrier path becomes long when giving and receiving of the wafer is performed between the carrier arms on the carrier path. Additionally, a floor area (foot print) that is needed for the exposure apparatus also becomes large.
In wafer steppers, the alignment of an exposure field to the reticle being imaged affects the success of the circuit of that field. In a scanning exposure system, the reticle and wafer are moved simultaneously and scanned across one another during the exposure sequence.
To attain high accuracy, the stage should be isolated from mechanical disturbances. This is achieved by employing electromagnetic forces to position and move the stage. It should also have high control bandwidth, which requires that the stage be a light structure with no moving parts. Furthermore, the stage should be free from excessive heat generation which might cause interferometer interference or mechanical changes that compromise alignment accuracy.
Commutatorless electromagnetic alignment apparatus such as the ones disclosed in U.S. Pat. Nos. 4,506,204, 4,506,205 and 4,507,597 are not feasible because they require the manufacture of large magnet and coil assemblies that are not commercially available. The weight of the stage and the heat generated also render these designs inappropriate for high accuracy applications.
An improvement over these commutatorless apparatus was disclosed in U.S. Pat. No. 4,592,858, which employs a conventional XY mechanically guided sub-stage to provide the large displacement motion in a plane, thereby eliminating the need for large magnet and coil assemblies. The electromagnetic means mounted on the sub-stage isolates the stage from mechanical disturbances. Nevertheless, the combined weight of the sub-stage and stage still results in low control bandwidth, and the heat generated by the electromagnetic elements supporting the stage is still substantial.
Even though the current apparatus using commutated electromagnetic means is a significant improvement over prior commutatorless apparatus, the problems of low control bandwidth and interferometer interference persist. In such an apparatus, a sub-stage is moved magnetically in one linear direction and the commutated electromagnetic means mounted on the sub-stage in turn moves the stage in the normal direction. The sub-stage is heavy because it carries the magnet tracks to move the stage. Moreover, heat dissipation on the stage compromises interferometer accuracy.
It is also well known to move a movable member (stage) in one long linear direction (e.g. more than 10 cm) by using two of the linear motors in parallel where coil and magnet are combined. In this case, the stage is guided by some sort of a linear guiding member and driven in one linear direction by a linear motor installed parallel to the guiding member. When driving the stage only to the extent of extremely small stroke, the guideless structure based on the combination of several electromagnetic actuators, as disclosed in the prior art mentioned before, can be adopted. However, in order to move the guideless stage by a long distance in one linear direction, a specially structured electromagnetic actuator as in the prior art becomes necessary, causing the size of the apparatus to become larger, and as a result, generating a problem of consuming more electricity.
SUMMARY OF THE INVENTION
It is an object of the present invention to make it possible for a guideless stage to move with a long linear motion using electromagnetic force, and to provide a light weight apparatus in which low inertia and high response are achieved.
It is another object of the present invention to provide a guideless stage apparatus using commercially available regular linear motors as electromagnetic actuators for one linear direction motion.
It is another object of the present invention to provide a guideless stage apparatus capable of active and precise position control for small displacements without any contact in the direction orthogonal to the long linear motion direction.
It is another object of the present invention to provide a completely non-contact stage apparatus by providing a movable member (stage body) that moves in one linear direction and a second movable member that moves sequentially in the same direction, constantly keeping a certain space therebetween, and providing the electromagnetic force (action and reaction forces) in the direction orthogonal to the linear direction between this second movable member and the stage body.
It is another object of the present invention to provide a non-contact stage apparatus capable of preventing the positioning and running accuracy from deteriorating by changing tension of various cables and tubes to be connected to the non-contact stage body that moves as it supports an object.
It is another object of the present invention to provide a non-contact apparatus that is short in its height, by arranging the first movable member and the second movable member in parallel, which move in the opposite linear direction to one another.
It is another object of the present invention to provide an apparatus that is structured so as not to change the location of the center of gravity of the entire apparatus even when the non-contact stage body moves in one linear direction.
Another object of this invention is to provide an exposure apparatus that can perform an exposure with high accuracy by reducing the effects of vibration on a projection optical system or the like that occurs when the wafer stage or the like is driven.
Another object of this invention is to provide an exposure apparatus that suppresses the amount of heat generated by the driving part of the wafer stage, to perform positioning of the driving part of the wafer stage with high accuracy, and to maintain the measurement stability of a position measurement device or the like.
Another object of this invention is to provide an exposure apparatus with high throughput that can carry a wafer to an exposure apparatus without temporarily fixing the wafer, and without giving and receiving of the wafer between wafer carrier arms.
In order to achieve the above and other objects, embodiments of the present invention may be constructed as follows.
An apparatus that is capable of high accuracy position and motion control utilizes linear commutated motors to move a guideless stage in one long linear direction and to create small yaw rotation in a plane. A carrier/follower holding a single voice coil motor (VCM) is controlled to approximately follow the stage in the direction of the long linear motion. The VCM provides an electromagnetic force to move the stage for small displacements in the plane in a linear direction perpendicular to the direction of the long linear motion to ensure proper alignment. This follower design eliminates the problem of cable drag for the stage since the cables connected to the stage follow the stage via the carrier/follower. Cables connecting the carrier/follower to external devices will have a certain amount of drag, but the stage is free from such disturbances because the VCM on the carrier/follower acts as a buffer by preventing the transmission of mechanical disturbances to the stage.
According to one aspect of the invention, the linear commutated motors are located on opposite sides of the stage and are mounted on a driving frame. Each linear commutated motor includes a coil member and a magnetic member, one of which is mounted on one of the opposed sides of the stage, and the other of which is mounted on the driving frame. Both motors drive in the same direction. By driving the motors slightly different amounts, small yaw rotation of the stage is produced.
In accordance with another aspect of the present invention, a moving counter-weight is provided to preserve the location of the center of gravity of the stage system during any stage motion by using the conservation of momentum principle. In an embodiment of the present invention, the drive frame carrying one member of each of the linear motors is suspended above the base structure, and when the drive assembly applies an action force to the stage to move the stage in one direction over the base structure, the driving frame moves in the opposite direction in response to the reaction force to substantially maintain the center of gravity of the apparatus. This apparatus essentially eliminates any reaction forces between the stage system and the base structure on which the stage system is mounted, thereby facilitating high acceleration while minimizing vibrational effects on the system.
By restricting the stage motion to the three specified degrees of freedom, the apparatus is simple. By using electromagnetic components that are commercially available, the apparatus design is easily adaptable to changes in the size of the stage. This high accuracy positioning apparatus is ideally suited for use as a reticle scanner in a scanning exposure system by providing smooth and precise scanning motion in one linear direction and ensuring accurate alignment by controlling small displacement motion perpendicular to the scanning direction and small yaw rotation in the scanning plane.
An exposure apparatus according to another aspect of this invention includes a projection optical system support member that supports a projection optical system, so that the projection optical system rotates within a specified area, taking a reference point as a center. Therefore, even if vibration from a substrate stage and a mask stage is transmitted to the projection optical system, the position relationship between the object plane (mask) and the image plane (substrate) is not shifted. Thus, it is possible to prevent position shifting of the pattern to be transferred, and highly accurate exposure can be performed.
Furthermore, a mask stage that moves a mask, a structural body that supports this mask stage and the projection optical system, and a substrate stage that moves a substrate are provided. The projection optical system support part (the structural body) has at least three flexible support members extending from the structural body, and the extending lines of each support member cross at the reference point. In this case, even if vibration is transmitted to the projection optical system, the projection optical system is minutely rotated taking the reference point as a center. Therefore, it is possible to prevent position shifting of the pattern to be transferred to the substrate. Furthermore, the support members are flexible, so the minute vibration can be reduced and the deterioration of contrast of a pattern to be formed can be prevented.
An exposure apparatus according to another aspect of this invention controls the mask base so that the mask base moves at a specified speed in a direction opposite to the moving direction of the mask stage. This reduces the effects to the structural body of the driving reaction of the mask stage. Additionally, the excitation of mechanical resonance is controlled, and the vibration transmitted to the structural body and the projection optical system can be reduced. Therefore, exposure with a high accuracy can be performed.
In an exposure apparatus according to another aspect of this invention, by having an elastic member at both ends of a guide axis, when the substrate table performs constant velocity reciprocation on the guide axis, the kinetic energy of the substrate table is converted to potential energy and is stored in the elastic members. Therefore, the energy to be consumed when the substrate table is reciprocated at constant velocity is mainly only the energy to be consumed in the viscosity resistance of the substrate table with respect to air. The only heat generated is the heat from when the elastic members are deformed. Therefore, it is possible to control the heating amount of the driving part when the substrate table moves at constant velocity.
Furthermore, when the elastic member has first magnetic members disposed at both ends of the guide axis and second magnetic members disposed corresponding to the first magnetic members, by the attraction of the first and second magnetic members, when the substrate table is still-positioned at an end of the guide axis, it is possible to reduce the thrust of the driving part of the substrate table required to oppose the resistance of the elastic member. Thus, the heating amount of the driving part can be controlled when the substrate table is still-positioned.
In an exposure apparatus according to another aspect of this invention, by controlling the length of the support legs that can be freely extended and retracted in the support direction, the tilt angle of the substrate table and its position in the height direction can be controlled, and highly accurate exposure can be performed as the surface of the substrate is aligned within the image plane.
Furthermore, when the mask and the substrate are synchronously and moved during exposure, the tilt angle of the scanning surface of the substrate stage of the structural body in the scanning direction, the tilt angle in the non-scanning direction, and the height are detected. When the support legs that can be freely extended and retracted are controlled based upon the detection result, highly accurate scanning exposure can be performed as the surface of the substrate is aligned within the image plane.
Furthermore, when the rotation angle of the substrate stage about the optical axis of the projection optical system and the position shifting amount are detected, and the position of the mask stage or the substrate stage is controlled based upon this detection result, the positioning between the surface of the substrate and the image plane can be performed with high accuracy.
In an exposure apparatus according to another aspect of this invention, a visco-elastic body exists between the support member and the structural body, so it is possible to reduce the vibration from the floor on which the exposure device is disposed. Therefore, exposure can be performed with high accuracy.
In an exposure apparatus according to another aspect of this invention, at least one groove is provided in the substrate table, and a substrate can be disposed on the substrate table without the substrate carrier arms contacting the substrate table. That is, there is an advantage such that the substrate can be carried into and out from the exposure device, without temporarily fixing and supporting the substrate on the substrate table, and throughput can be improved.
Furthermore, when the substrate carrier mechanism has at least two substrate carrier arms and substrate storage case support members, the substrate carrier arms can be freely moved in the three directions such as a rotational direction about the optical axis of the projection optical system, the horizontal direction, and the vertical direction, and the substrate storage case support member can be freely moved in the vertical direction, there are advantages such that the substrate stage can be moved below the substrate carrying-out arms or the substrate carrying-in arms, the substrate can be carried to the exposure device without transferring the substrate between the substrate carrier arms, and the probability of problems occurring during the carrying and the probability of foreign objects attaching to the wafer can be reduced.
Other aspects and features and advantages of the present invention will become more apparent upon a review of the following specification taken in conjunction with the accompanying drawings wherein similar characters of reference indicate similar elements in each of the several views.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1
is a schematic perspective view of an apparatus in accordance with an embodiment of the present invention.
FIG. 2
is a top plan view of the apparatus shown in FIG.
1
.
FIG. 3
is an end elevational view of the structure shown in
FIG. 2
taken along line
3
—
3
′ in the direction of the arrows.
FIG. 4A
is an enlarged perspective, partially exploded view showing the carrier/follower structure of FIG.
1
and exploded from the positioning guide.
FIG. 4B
is an enlarged horizontal sectional view of a portion of the structure shown in
FIG. 5
taken along line
4
B in the direction of the arrow.
FIG. 4C
is an enlarged elevational sectional view of a portion of the structure shown in
FIG. 2
taken along line
4
C in the direction of the arrow but with the voice coil motor removed.
FIG. 5
is an elevational sectional view of a portion of the structure shown in
FIG. 2
taken along line
5
—
5
′ in the direction of the arrows.
FIG. 6
is a block diagram schematically illustrating the sensing and control systems for controlling the position of the stage.
FIG. 7
is a plan view, similar to
FIG. 2
, illustrating a preferred embodiment of the present invention.
FIG. 8
is an elevational sectional view of the structure shown in
FIG. 7
taken along line
8
—
8
′ in the direction of the arrows.
FIGS. 9 and 10
are simplified schematic views similar to
FIGS. 7 and 8
and illustrating still another embodiment of the present invention.
FIG. 11
is a perspective view showing a schematic structure of a projection exposure apparatus according to an embodiment of this invention.
FIG. 12
is a cross-sectional view taken through a part showing a method of supporting the projection optical system of FIG.
11
.
FIG. 13A
is a plan view showing the wafer stage of FIG.
11
.
FIG. 13B
is a cross-sectional view of
FIG. 13A
along line B—B.
FIG. 13C
is a front view omitting part of FIG.
13
A.
FIG. 13D
is across-sectional view of
FIG. 13A
along line D—D.
FIG. 14
is a block diagram showing a structure of a controller that controls a wafer table and a carrier.
FIGS. 15A-C
are schematic diagrams that accompany an operation explanation of a guide shaft and a guide member of the wafer table of
FIGS. 13A-C
.
FIG. 16A
is a diagram showing the speed of the wafer table when the moving speed of the wafer table is shifted to a constant speed on a guide axis without an elastic body.
FIG. 16B
is a diagram showing thrust of linear motors.
FIG. 17A
is a diagram showing a speed curve of a wafer table that is calculated assuming the case where an ideal wafer table without vibration is accelerated to a constant speed on a guide axis with springs.
FIG. 17B
is a diagram showing thrust of linear motors which is calculated assuming the case where a wafer table with vibration is controlled taking the speed curve of
FIG. 17A
as a speed governing value.
FIG. 18A
is a diagram showing the speed when a wafer table is accelerated to a constant speed using a guide axis with springs, taking the speed curve of
FIG. 17A
as a speed governing value.
FIG. 18B
is a diagram showing thrust of a wafer table at that time and the thrust generated by linear motors.
FIG. 19A
is a diagram showing a speed curve when a wafer table is accelerated to a constant speed when a guide axis with springs in which a spring constant is the optimum value is used.
FIG. 19B
is a diagram showing thrust of the wafer table.
FIG. 20
is a diagram showing the resistance of the springs at the ends of a guide axis with springs.
FIGS. 21A-C
are schematic diagrams that accompany the explanation of the operation of the guide member and the guide shaft when a magnetic member is further provided.
FIG. 22A
is a diagram showing speed that is calculated assuming the case where an ideal wafer table without vibration is accelerated to a constant speed on a guide axis provided with springs, steel plates, and magnets.
FIG. 22B
is a diagram showing thrust of linear motors calculated assuming the case where a wafer table with vibration is controlled taking the speed curve of
FIG. 22A
as a speed governing value.
FIG. 23A
is a diagram showing the speed curve when a wafer table on a guide axis with steel plates and magnets is accelerated to a constant speed, taking the speed curve of
FIG. 22A
as a speed governing value.
FIG. 23B
is a diagram showing thrust of the wafer table at that time, and the thrust of linear motors.
FIG. 24
is a diagram showing the resultant force between the resistance of the spring and the attraction between the magnet and the steel plate at an end of the guide axis to which the steel plate and the magnet are fixed.
FIG. 25A
is a schematic diagram showing a support leg that supports a wafer table, and the vicinity thereof, by enlargement.
FIG. 25B
is a side view of FIG.
25
A.
FIG. 26
is a block diagram showing a structure of a controller that controls a reticle stage, a wafer stage, and a wafer base.
FIGS. 27A-B
are diagrams explaining the operation of the wafer stage when a wafer is carried into or out from an exposure device.
FIGS. 28A-B
are diagrams explaining the operation of a wafer carrier arm when an already-exposed wafer is carried out from an exposure device.
FIGS. 29A-B
are diagrams explaining the operation of a wafer carrier arm when a non-exposed wafer is carried into an exposure device.
DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS
While the present invention has applicability generally to electromagnetic alignment system, the preferred embodiments involve a scanning apparatus for a reticle stage as illustrated in
FIGS. 1-6
.
Referring now to the drawings, the positioning apparatus
10
of the present invention includes a base structure
12
above which a reticle stage
14
is suspended and moved as desired, a reticle stage position tracking laser interferometer system
15
, a position sensor
13
and a position control system
16
operating from a CPU
16
′ (see FIG.
6
).
An elongate positioning guide
17
is mounted on the base
12
, and support brackets
18
(two brackets in the illustrated embodiment) are movably supported on the guide
17
such as by air bearings
20
. The support brackets
18
are connected to a driving assembly
22
in the form of a magnetic track assembly or driving frame for driving the reticle stage
14
in the X direction and small yaw rotation. The driving frame includes a pair of parallel spaced apart magnetic track arms
24
and
26
which are connected together to form an open rectangle by cross arms
28
and
30
. In the preferred embodiment, the driving frame
22
is movably supported on the base structure
12
such as by air bearings
32
so that the frame is free to move on the base structure in a direction aligned with the longitudinal axis of the guide
17
, the principal direction in which the scanning motion of the reticle stage is desired. As used herein “one direction” or a “first direction” applies to movement of the frame
22
or the reticle stage
14
either forward or backward in the X direction along a line aligned with the longitudinal axis of the guide
17
.
Referring now to
FIGS. 1 and 3
to explain further in detail, the elongate guiding member
17
in the X direction has front and rear guiding surfaces
17
A and
17
B, which are almost perpendicular to the surface
12
A of the base structure
12
. The front guiding surface
17
A is against the rectangular driving frame
22
and guides the air bearing
20
which is fixed to the inner side of the support bracket
18
. A support bracket
18
is mounted on each end of the upper surface of the arm
24
, which is parallel to the guiding member
17
of the driving frame
22
. Furthermore, each support bracket
18
is formed in a hook shape so as to straddle the guiding member
17
in the Y direction, and with the free end against the rear guiding surface
177
B of the rear side of the guiding member
17
. The air bearing
20
′ is fixed inside the free end of the support brackets
18
and against the rear guiding surface
17
B. Therefore, each of the support brackets
18
is constrained in its displacement in the Y direction by the guiding member
17
and air bearings
20
and
20
′ and is able to move only in the X direction.
Now according to the first embodiment of the present invention, the air bearings
32
, which are fixed to the bottom surfaces of the four rectangular parts of the driving frame
22
, make an air layer leaving a constant (several &mgr;m) between the pad surface and the surface
12
A of the base structure
12
. The driving frame is buoyed up from the surface
12
A and supported perpendicularly (in the Z direction) by the air layer. It will be explained in detail later, but in
FIG. 1
, the carrier/follower
60
shown positioned above the upper part of the elongate arm
24
is positioned laterally in the Y direction by air bearings
66
A and
66
B supported by a bracket
62
against opposite surfaces
17
A and
17
B of guiding member
17
and vertically in the Z direction by air bearings
66
above the surface
12
A of the base structure
12
. Thus, the carrier/follower
60
is positioned so as not to contact any part of the driving frame
22
. Accordingly, the driving frame
22
moves only in one linear X direction, guided above the base surface
12
A and laterally by the guiding member
17
.
Referring now to both FIG.
1
and
FIG. 2
, the structure of the reticle stage
14
and the driving frame
22
will be explained. The reticle stage
14
includes a main body
42
on which the reticle
44
is positioned above an opening
46
. The reticle body
42
includes a pair of opposed sides
42
A and
42
b
and is positioned or suspended above the base structure
12
such as by air bearings
48
. A plurality of interferometer mirrors
50
are provided on the main body
42
of the reticle stage
14
for operation with the laser interferometer position sensing system
15
(see
FIG. 6
) for determining the exact position of the reticle stage which is fed to the position control system
16
in order to direct the appropriate drive signals for moving the reticle stage
14
as desired.
Primary movement of the reticle stage
14
is accomplished with first electromagnetic drive assembly or means in the form of separate drive assemblies
52
A and
52
B (
FIG. 2
) on each of the opposed sides
42
A and
42
B, respectively. The drive assemblies
52
A and
52
B include drive coils
54
A and
54
B fixedly mounted on the reticle stage
14
at the sides
42
A and
42
B, respectively, for cooperating with magnet tracks
56
A and
56
B on the magnet track arms
24
and
26
, respectively, of the drive frame
22
. While in the preferred embodiment of the invention the magnet coils are mounted on the reticle stage and the magnets are mounted on the drive frame
22
, the positions of these elements of the electromagnetic drive assembly
52
could be reversed.
Here, the structure of the reticle stage
14
will be explained further in detail. As shown in
FIG. 1
, the stage body
42
is installed so that it is free to move in the Y direction in the rectangular space inside the driving frame
22
. The air bearing
48
fixed under each of the four corners of the stage body
42
makes an extremely small air gap between the pad surface and the base surface
12
A, and buoys up and supports the entire stage
14
from the surface
12
A. These air bearings
48
should preferably be pre-loaded types with a recess for vacuum attraction to the surface
12
A.
As shown in
FIG. 2
, a rectangular opening
46
in the center of the stage body
42
is provided so that the projected image of the pattern formed on the reticle
44
can pass therethrough. In order for the projected image via the rectangular opening
46
to pass through the projection optical system PL (see
FIG. 5
) which is installed below the rectangular opening, there is another opening
12
B provided at the center part of the base structure
12
. The reticle
44
is loaded on the top surface of the stage body by clamping members
42
C, which are protrusively placed at four points around the rectangular opening
46
, and clamped by vacuum pressure.
The interferometer mirror
50
Y, which is fixed near the side
42
B of the stage body
42
near the arm
26
, has a vertical elongate reflecting surface in the X direction which length is somewhat longer than the movable stroke of the stage
14
in the X direction, and the laser beam LBY from the Y-axis interferometer is incident perpendicularly on the reflecting surface. In
FIG. 2
, the laser beam LBY is bent at a right angle by the mirror
12
D, which is fixed on the side of the base structure
12
.
Referring now to
FIG. 3
as a partial cross-sectional drawing of the view along line
3
—
3
′ in
FIG. 2
, the laser beam LBY which is incident on the reflecting surface of the interferometer mirror
50
Y is placed so as to be on the same plane as the bottom surface (the surface where the pattern is formed) of the reticle
44
which is mounted on the clamping member
42
C. Furthermore, in
FIG. 3
, the air bearing
20
on the end side of the support brackets
18
against the guiding surface
17
B of the guiding member
17
is also shown.
Referring once again to
FIGS. 1 and 2
, the laser beam LBX1 from the X1-axis interferometer is incident and reflected on the interferometer mirror
50
X1, and the laser beam LBX2 from the X2-axis interferometer is incident and reflected on the interferometer mirror
50
X2. These two mirrors
50
X1 and
50
X2 are structured as corner tube type mirrors, and even when the stage
14
is in yaw rotation, they always maintain the incident axis and reflecting axis of the laser beams parallel within the XY plane. Furthermore, the block
12
C in
FIG. 2
is an optical block, such as a prism, to orient the laser beams LBX1 and LBX2 to each of the mirrors
50
X1 and
50
X2, and is fixed to a part of the base structure
12
. The corresponding block for the laser beam LBY is not shown.
In
FIG. 2
, the distance BL in the Y direction between each of the center lines of the two laser beams LBX1 and LBX2 is the length of the base line used to calculate the amount of yaw rotation. Accordingly, the value of the difference between the measured value &Dgr;X1 in the X direction of the X1-axis interferometer and the measured value &Dgr;X2 in the X direction of the X2-axis interferometer divided by the base line length BL is the approximate amount of yaw rotation in an extremely small range. Also, half the value of the sum of &Dgr;X1 and &Dgr;X2 represents the X coordinate position of the entire stage
14
. These calculations are performed by a high speed digital processor in the position control system
16
shown in FIG.
6
.
Furthermore, the center lines of each of the laser beams LBX1 and LBX2 are set on the same surface where the pattern is formed on the reticle
44
. The extension of the line GX, which is shown in FIG.
2
and divides in half the space between each of the center lines of laser beams LBX1 and LBX2, and the extension of the laser beam LBY intersect within the same surface where the pattern is formed. Additionally, the optical axis AX (see
FIGS. 1 and 5
) also crosses at this intersection as shown in FIG.
1
. In
FIG. 1
, a slit shaped illumination field ILS which includes the optical axis AX is shown over the reticle
44
, and the pattern image of the reticle
44
is scanned and exposed onto the photosensitive substrate via the projection optical system PL.
Furthermore, there are two rectangular blocks
90
A and
90
B fixed on the side
42
A of the stage body
42
in
FIGS. 1 and 2
. These blocks
90
A and
90
B are to receive the driving force in the Y direction from the second electromagnetic actuator
70
which is mounted on the carrier/follower
60
. Details will be explained below.
The driving coils
54
A and
54
B which are fixed on the both sides of the stage body
42
are formed flat parallel to the XY plane, and pass through the magnetic flux space in the slot which extends in the X direction of the magnetic tracks
56
A and
56
B without any contact. The assembly of the driving coil
54
and the magnetic track
56
used in the present embodiment is a commercially easily accessible linear motor for general purposes, and it could be either with or without a commutator.
Here, considering the actual design, the moving stroke of the reticle stage
14
is mostly determined by the size of the reticle
44
(the amount of movement required at the time of scanning for exposure and the amount of movement required at the time of removal of the reticle from the illumination optical system to change the reticle). In the case of the present embodiment, when a 6-inch reticle is used, the moving stroke is about 30 cm.
As mentioned before, the driving frame
22
and the stage
14
are independently buoyed up and supported on the base surface
12
A, and at the same time, magnetic action and reaction forces are applied to one another in the X direction only by the linear motor
52
. Because of that, the law of the conservation of momentum is seen between the driving frame
22
and the stage
14
.
Now, suppose the weight of the entire reticle stage
14
is about one fifth of the entire weight of the frame
22
which includes the support brackets
18
. Then, the forward movement of 30 cm of the stage
14
in the X direction makes the driving frame
22
move by 6 cm backwards in the X direction. This means that the location of the center of gravity of the apparatus on the base structure
12
is essentially fixed in the X direction. In the Y direction, there is no movement of any heavy object. Therefore, the change in the location of the center of gravity in the Y direction is also relatively fixed.
The stage
14
can be moved in the X direction as described above, but the moving coils (
54
A,
54
B) and the stators (
56
A,
56
B) of the linear motors
52
will interfere with each other (collide) in the Y direction without an X direction actuator. Therefore, the carrier/follower
60
and the second electromagnetic actuator
70
are provided to control the stage
14
in the Y direction. Their structures will be explained with reference to
FIGS. 1
,
2
,
3
and
5
.
As shown in
FIG. 1
, the carrier/follower
60
is movably installed in the Y direction via the hook-like support bracket
62
which straddles over the guiding member
17
. Furthermore as evident from
FIG. 2
, the carrier/follower
60
is placed above the arm
24
, so as to maintain a certain space between the stage
14
(the body
42
) and the arm
24
, respectively. One end
60
E of the carrier/follower
60
, is substantially protruding inward (toward the stage body
42
) over the arm
24
. Inside this end part
60
E is fixed a driving coil
68
(
FIGS. 4A and 6
) (having the same shape as the coil
54
) which enters a slot space of the magnetic track
56
A.
Furthermore, the bracket
62
supported by air bearing
66
A (see
FIGS. 2
,
3
,
4
A and
5
) against the guiding surface
17
A of the guiding member
17
is fixed in the space between the guiding member
17
of the carrier/follower
60
and the arm
24
. The air bearing
66
that buoys up and supports the carrier/follower
60
on the base surface
12
A is also shown in FIG.
3
.
The air bearing
66
B against the guiding surface
17
B of the guiding member
17
is also fixed to the free end of support bracket
62
on the other side of the hook from air bearing
66
A with guiding member
17
therebetween.
Now, as evident from
FIG. 5
, the carrier/follower
60
is arranged so as to keep certain spaces with respect to both the magnetic track
56
A and the stage body
42
in the Y and Z directions, respectively. Shown in
FIG. 5
are the projection optical system PL and column rod CB to support the base structure
12
above the projection optical system PL. Such an arrangement is typical for a projection aligner, and unnecessary shift of the center of gravity of the structures above the base structure
12
would cause a lateral shift (mechanical distortion) between the column rod CB and the projection optical system PL, and thus result in a deflection of the image on the photosensitive substrate at the time of exposure. Hence, the merit of the device as in the present embodiment where the motion of the stage
14
does not shift the center of gravity above the base structure
12
is substantial.
Furthermore referring now to
FIG. 4A
, the structure of the carrier/follower
60
will be explained. In
FIG. 4A
, the carrier/follower
60
is disassembled into two parts,
60
A and
60
B, for the sake of facilitating one's understanding. As evident from
FIG. 4A
, the driving coil
68
that moves the carrier/follower
60
itself in the X direction is fixed at the lower part of the end
60
E of the carrier/follower
60
. Furthermore, the air bearing
66
C is placed against the base structure
12
A on the bottom surface of the end
60
E and helps to buoy up the carrier/follower
60
.
Hence the carrier/follower
60
is supported in the Z direction with three points—the two air bearings
66
and one air bearing
66
C—and is constrained in the Y direction for movement in the X direction by air bearings
66
A and
66
B. What is important in this structure is that the second electromagnetic actuator
70
is arranged back to back with the support bracket
62
so that when the actuator generates the driving force in the Y direction, reaction forces in the Y direction between the stage
14
and the carrier/follower
60
actively act upon the air bearings
66
A and
66
B which are fixed inside the support bracket
62
. In other words, arranging the actuator
70
and the air bearings
66
A,
66
B on the line parallel to the Y-axis in the XY plane helps prevent the generation of unwanted stress, which might deform the carrier/follower
60
mechanically when the actuator
70
is in operation. Conversely, it means that it is possible to reduce the weight of the carrier/follower
60
.
As evident from
FIGS. 2
,
4
A and
4
C described above, the magnetic track
56
A in the arm
24
of the driving frame
22
provides magnetic flux for the driving coil
54
A on the stage body
42
side, and concurrently provides magnetic flux for the driving coil
68
for the carrier/follower
60
. As for the air bearings
66
A,
66
B and
66
C, a vacuum pre-loaded type is preferable, since the carrier/follower
60
is light. Besides the vacuum pre-loaded type, a magnetic pre-loaded type is also acceptable.
Next with reference to
FIGS. 3
,
4
B and
5
, the second actuator mounted on the carrier/follower
60
will be explained. A second electromagnetic drive assembly in the form of a voice coil motor
70
is made up of a voice coil
74
attached to the main body
42
of the reticle stage
14
and a magnet
72
attached to the carrier/follower
60
to move the stage
14
for small displacements in the Y direction in the plane of travel of the stage
14
orthogonal to the X direction long linear motion produced by the driving assembly
22
. The positions of the coil
74
and magnet
72
could be reversed. A schematic structure of the voice coil motor (VCM)
70
is as shown in
FIGS. 3 and 5
, and the detailed structure is shown in FIG.
4
B.
FIG. 4B
is a cross-sectional view of the VCM
70
sectioned at the horizontal plane shown with an arrow
4
B in FIG.
5
. In
FIG. 4B
, the magnets
72
of the VCM
70
are fixed onto the carrier/follower
60
side. The coil of the VCM
70
comprises the coil body
74
A and its supporting part
74
B. The supporting part
74
B is fixed to a connecting plate
92
(a plate vertical to the XY plane) which is rigidly laid across the two rectangular blocks
90
A and
90
B. A center line KX of the VCM
70
shows the direction of the driving force of the coil
74
, and when an electric current flows through the coil body
74
A, the coil
74
displaces into either positive or negative movement in the Y direction in accordance with the direction of the current, and generates a force corresponding to the amount of the current. Normally, in a commonly used VCM, a ring-like damper or bellows are provided between the coil and magnet so as to keep the gap between the coil and magnet, but according to the present embodiment, that gap is kept by a follow-up motion of the carrier/follower
60
, and therefore, such supporting elements as a damper or bellows are not necessary.
In the present embodiment, capacitance gap sensors
13
A and
13
B are provided as a positioning sensor
13
(see
FIG. 6
) as shown in FIG.
4
B. In
FIG. 4B
, electrodes for capacitance sensors are placed so as to detect the change in the gap in the X direction between the side surface of the rectangular blocks
90
A and
90
B facing each other in the X direction and the side surface of a case
70
′ of the VCM
70
. Such a positioning sensor
13
can be placed anywhere as far as it can detect the gap change in the Y direction between the carrier/follower
60
and the stage
14
(or the body
42
). Furthermore, the type of the sensor can be any of a non-contact type such as, for example, photoelectric, inductive, ultrasonic, or air-micro system.
The case
70
′ in
FIG. 4B
is formed with the carrier/follower
60
in one, and placed (spatially) so as not to contact any member on the reticle stage
14
side. As for the gap between the case
70
′ and the rectangular blocks
90
A and
90
B in the X direction (scanning direction), when the gap on the sensor
13
A side becomes wider, the gap on the sensor
133
B side becomes smaller. Therefore, if the difference between the measured gap value by the sensor
13
A and the measured gap value by the sensor
13
B is obtained by either digital operation or analog operation, and a direct servo (feedback) control system which controls the driving current of the driving coil
68
for the carrier/follower
60
is designed using a servo driving circuit which makes the gap difference zero, then the carrier/follower
60
will automatically perform a follow-up movement in the X direction always keeping a certain space to the stage body
42
. Alternatively, it is also possible to design an indirect servo control system which controls an electric current flow to the driving coil
68
, with the operation of position control system
16
in
FIG. 6
using the measured gap value obtained only from one of the sensors and the X coordinate position of the stage
14
measured from the X axis interferometer, without using the two gap sensors
13
A and
13
B differentially.
In the VCM
70
as described in
FIG. 4B
, the gap between the coil body
74
A and the magnet
72
in the X direction (non-energizing direction) is in actuality about 2-3 mm. Therefore, a follow-up accuracy of the carrier/follower
60
with respect to the stage body
42
would be acceptable at around ±0.5-1 mm. This accuracy depends on how much of the yaw rotation of the stage body is allowed, and also depends on the length of the line in the KX direction (energizing direction) of the coil body
74
A of the VCM
70
. Furthermore, the degree of the accuracy for this can be substantially lower than the precise positioning accuracy for the stage body
42
using an interferometer (e.g., ±0.03 &mgr;m supposing the resolution of the interferometer is 0.01 &mgr;m). This means that the servo system for a follower can be designed fairly simply, and the amount of cost to install the follower control system would be small. Furthermore, the line KX in
FIG. 4B
is set so as to go through the center of gravity of the entire stage
14
on the XY plane, and each of centers of the pair of the air bearings
66
A and
66
B provided inside the support brackets
62
shown in
FIG. 4
is also positioned on the line KX in the XY plane.
FIG. 4C
is a cross-sectional drawing of the part which includes the guiding member
17
, the carrier/follower
60
, and the magnetic track
56
A sectioned from the direction of the arrow
4
C in FIG.
2
. The arm
24
storing the magnetic track
56
A is buoyed up and supported on the base surface
12
A by the air bearing
32
, and the carrier/follower
60
is buoyed up and supported on the base surface
12
A by the air bearing
66
. At this time, the height of the air bearing
48
at the bottom surface of the stage body
42
(see
FIGS. 3
or
5
) and the height of the air bearing
32
are determined so as to place the driving coil
54
A on the stage body
42
side keeping a 2-3 mm gap in the Z direction in the slot space of the magnetic track
56
A.
Each of the spaces between the carrier/follower
60
and the arm
24
in the Z and Y directions hardly changes because they are both guided by the common guiding member
17
and the base surface
12
A. Furthermore, even if there is a difference in the height in the Z direction between the part on the base surface
12
A where the air bearing
32
at the bottom surface of the driving frame
22
(arm
24
) is guided and the part on the base surface
12
A where the air bearing
48
at the bottom surface of the stage body is guided, as long as the difference is precisely constant within the moving stroke, the gap in the Z direction between the magnetic track
56
A and the driving coil
54
A is also maintained constant.
Furthermore, since the driving coil
68
for the carrier/follower
60
is originally fixed to the carrier/follower
60
, it is arranged, maintaining a certain gap of 2-3 mm above and below in the slot space of the magnetic track
56
A. The driving coil
68
hardly shifts in the Y direction with respect to the magnetic track
56
A.
Cables
82
(see
FIG. 2
) are provided for directing the signals to the drive coils
54
A and
54
B on stage
14
, the voice coil motor coil
74
and the carrier/follower drive coil
68
, and these cables
82
are mounted on the carrier/follower
60
and guide
17
thereby eliminating drag on the reticle stage
14
. The voice coil motor
70
acts as a buffer by preventing transmission of external mechanical disturbances to the stage
14
.
Therefore, referring now to
FIGS. 2 and 4A
, the cable issues will be described further in detail. As shown in
FIG. 2
, a connector
80
which connects wires of the electric system and tubes of the air pressure and the vacuum system (hereafter called “cables”) is mounted on the base structure
12
on one end of the guiding member
17
. The connector
80
connects a cable
81
from the external control system (including the control system of the air pressure and the vacuum systems besides the electric system control system shown in
FIG. 6
) to a flexible cable
82
. The cable
82
is further connected to the end part
60
E of the carrier/follower
60
, and electric system wires and the air pressure and the vacuum system tubes necessary for the stage body
42
are distributed as the cable
83
.
As mentioned before, the VCM
70
works to cancel a cable's drag or an influence by tension, but sometimes its influence appears as a moment in an unexpected direction between the carrier/follower
60
and the stage body
42
. In other words, the tension of the cable
82
gives the carrier/follower
60
a force to rotate the guiding surface of the guiding member
17
or the base surface
12
A, and the tension of the cable
83
gives a force to the carrier/follower
60
and the stage body to rotate relatively.
One of these moments, the constituent which shifts the carrier/follower
60
, is not problematic, but the one which shifts the stage body in X, Y, or &thgr; direction (yaw rotation direction) could affect the alignment or overlay accuracy. As for the X and &thgr; directions, shifts can be corrected by a consecutive drive by the two linear motors (
54
A,
56
A,
54
B,
56
B), and as for in the Y direction, the shift can be corrected by the VCM
70
. In the present embodiment, since the weight of the entire stage
14
can be reduced substantially, the response of the motion of the stage
14
by VCM
70
in the Y direction and the response by the linear motor in X and &thgr; directions will be extremely high in cooperation with the completely non-contact guideless structure. Furthermore, even when a micro vibration (micron order) is generated in the carrier/follower
60
and it is transferred to the stage
14
via the cable
83
, the vibration (from several Hz to tens of Hz) can be sufficiently canceled by the above mentioned high response.
Now,
FIG. 4A
shows how each of the cables is distributed at the carrier/follower
60
. Each of the driving signals to the driving coils
54
A,
54
B for the stage body
42
and the driving coil
74
of the VCM
70
and the detection signal from the position sensor
13
(the gap sensors
13
A,
13
B) go through the electric system wire
82
A from the connector
80
. The pressure gas and the vacuum to each of the air bearings
48
and
66
go through the pneumatic system tube
82
B from the connector
80
. On the other hand, the driving signal to the driving coils
54
A and
54
B goes through the electric system wire
83
A which is connected to the stage body
42
, and the pressurized gas for the air bearing
48
and the vacuum for the clamping member
42
C go through the pneumatic system hoses
83
B.
Furthermore, it is preferable to have a separate line for the pneumatic system for the air bearings
20
,
20
′ and
32
of the driving frame
22
, independent of the one shown in FIG.
2
. Also, as shown in
FIG. 4A
, in case the tension or vibration of the cable
83
cannot be prevented, it is advisable to arrange the cable
83
so as to limit the moment by the tension or vibration the stage body
42
receives only to the Y direction as much as possible. In that case, the moment can be canceled only by the VCM
70
with the highest response.
Referring now to
FIGS. 1
,
2
and
6
, the positioning of the reticle stage
14
is accomplished first knowing its existing position utilizing the laser interferometer system
15
. Drive signals are sent to the reticle stage drive coils
54
A and
54
B for driving the stage
14
in the X direction. A difference in the resulting drive to the opposite sides
42
A and
42
B of the reticle stage
14
will produce small yaw rotation of the reticle stage
14
. An appropriate drive signal to the voice coil
72
of voice coil motor
70
produces small displacements of the reticle stage
14
in the Y direction. As the position of the reticle stage
14
changes, a drive signal is sent to the carrier/follower coil
68
causing the carrier/follower
60
to follow the reticle stage
14
. Resulting reaction forces to the applied drive forces will move the magnetic track assembly or drive frame
22
in a direction opposite to the movement of the reticle stage
14
to substantially maintain the center of gravity of the apparatus. It will be appreciated that the counter-weight or reaction movement of the magnetic track assembly
22
need not be included in the apparatus in which case the magnetic track assembly
22
could be fixedly mounted on the base
12
.
As described above, in order to control the stage system according to the present embodiment, a control system as shown in
FIG. 6
is installed. This control system in
FIG. 6
will be further explained in detail here. X1 driving coil and X2 driving coil composed as the driving coils
54
A and
54
B of two linear motors respectively, and Y driving coil composed as the driving coil
72
of the VCM
70
are placed in the reticle stage
14
, and the driving coil
68
is placed in the carrier/follower
60
. Each of these driving coils is driven in response to the driving signals SX1, SX2, SY1 and S&Dgr;X, respectively, from the position control system
16
. The laser interferometer system
15
which measures the coordinates position of the stage
14
comprises the Y axis interferometer which sends/receives the beam LBY, the X1 axis interferometer which sends/receives the beam LBX1, and the X2 axis interferometer which sends/receives the beam LBX2, and they send position information for each of the directions of the axes, IFY, IFX1, IFX2 to the position control system
16
. The position control system
16
sends two driving signals SX1 and SX2 to the driving coils
54
A and
54
B so that the difference between the position information IFX1 and IFX2 in the X direction will become a preset value, or in other words, the yaw rotation of the reticle stage
14
is maintained at the specified amount. Thus, the yaw rotation (in &thgr; direction) positioning by the beams LBX1 and LBX2, X1 axis and X2 axis interferometers, the position control system
16
, and the driving signals SX1 and SX2 is constantly being conducted, once the reticle
44
is aligned on the stage body
42
, needless to mention the time of the exposure.
Furthermore, the control system
16
, which obtained the current coordinate position of the stage
14
in the X direction from the average of the sum of position information IFX1 and IFX2 in the X direction, sends the driving signals SX1, SX2 to the driving coils
54
A and
54
B, respectively, based on the various commands from the Host CPU
16
′ and the information CD for the parameters. Especially when scanning exposure is in motion, it is necessary to move the stage
14
straight in the X direction while correcting the yaw rotation, and the control system
16
controls the two driving coils
54
A and
54
B to give the same or slightly different forces as needed.
Furthermore, the position information IFY from the Y axis interferometer is also sent to the control system
16
, and the control system
16
sends an optimum driving signal S&Dgr;X to the driving coil
68
of the carrier/follower
60
. At that time, the control system
16
receives the detection signal S
pd
from the position sensor
13
which measures the space between the reticle stage
14
and the carrier/follower
60
in the X direction, and sends a necessary signal S&Dgr;X to make the signal S
pd
into the preset value as mentioned before. The follow-up accuracy for the carrier/follower
60
is not so strict that the detection signal S
pd
of the control system
16
does not have to be evaluated strictly either. For example, when controlling the motion by reading the position information IFY, IFX1, IFX2 every 1 millisecond from each of the interferometers, the high speed processor in the control system
16
samples the current of the detection signal S
pd
each time, determines whether the value is large or small compared to the reference value (acknowledge the direction), and if the deviation surpasses a certain point, the signal S&Dgr;X in proportion to the deviation can be sent to the driving coil
68
. Furthermore as mentioned before, it is also acceptable to install a control system
95
which directly servo controls the driving coil
68
, and directly controls the follow-up motion of the carrier/follower
60
without going through the position control system
16
.
Since the moving stage system as shown has no attachment to constrain it in the X direction, small influences may cause the system to drift toward the positive or negative X direction. This would cause certain parts to collide after this imbalance became excessive. The influences include cable forces, imprecise leveling of the base reference surface
12
A or friction between components. One simple method is to use weak bumpers (not shown) to prevent excessive travel of the drive assembly
22
. Another simple method is to turn off the air to one or more of the air bearings (
32
,
20
) used to guide the drive assembly
22
when the drive assembly reaches close to the end of the stroke. The air bearing(s) can be turned on when the drive begins to move back in the opposite direction.
More precise methods require monitoring the position of the drive assembly by a measuring device (not shown) and applying a driving force to restore and maintain the correct position. The accuracy of the measuring device need not be precise, but on the order of 0.1 to 1.0 mm. The driving force can be obtained by using another linear motor (not shown) attached to the drive assembly
22
, or another motor that is coupled to the drive assembly.
Finally, the one or more air bearings (
66
,
66
A,
66
B) of the carrier/follower
60
can be turned off to act as a brake during idle periods of the stage
42
. If the coil
68
of the carrier/follower
60
is energized with the carrier/follower
60
in the braked condition, the drive assembly will be driven and accelerated. Thus, the position control system
16
monitors the location of the drive assembly
22
. When the drive assembly drifts out of position, the drive assembly is repositioned with sufficient accuracy by intermittently using the coil
68
of the carrier/follower
60
.
In the first embodiment of the present invention, the driving frame
22
which functions as a counter weight is installed in order to prevent the center of gravity of the entire system from shifting, and was made to move in the opposite direction from the stage body
42
. However, when the structures in
FIGS. 1-5
are applied to a system where the shift of the center of gravity is not a major problem, it is also acceptable to fix the driving frame
22
on the base structure
12
together. In that case, except for the problem regarding the center of gravity, some of the effects and function can be applied without making any changes.
This invention provides a stage which can be used for high accuracy position and motion control in three degrees of freedom in one plane: (1) long linear motion; (2) short linear motion perpendicular to the long linear motion; and (3) small yaw rotation. The stage is isolated from mechanical disturbances of surrounding structures by utilizing electromagnetic forces as the stage driver. By further using a structure for this guideless stage, a high control bandwidth is attained. These two factors contribute to achieve the smooth and accurate operation of the stage.
Bearing in mind the description of the embodiment illustrated in
FIGS. 1-6
, one preferred embodiment of the present invention is illustrated in
FIGS. 7 and 8
, wherein the last two digits of the numbered elements are similar to the corresponding two digit numbered elements in
FIGS. 1-5
.
In
FIGS. 7 and 8
, differing from the previous first embodiment, the driving frame which functions as a counter weight is removed, and each of the magnet tracks
156
A and
156
B of the two linear motors is rigidly mounted onto the base structure
112
. The stage body
147
which moves straight in the X direction is placed between the two magnetic tracks
156
A and
156
B. As shown in
FIG. 8
, an opening
112
B is formed in the base structure
112
, and the stage body
142
is arranged so as to straddle the opening
112
B in the Y direction. There are four pre-loaded air bearings
148
fixed on the bottom surface at both ends of the stage body
142
in the Y direction, and they buoy up and support the stage body
142
against the base surface
112
A.
Furthermore, according to the present embodiment, the reticle
144
is clamped and supported on a reticle chuck plate
143
which is separately placed on the stage body
142
. The straight mirror
150
Y for the Y axis laser interferometer and two corner mirrors
150
X1,
150
X2 for the X axis laser interferometer are mounted on the reticle chuck plate
143
. The driving coils
154
A and
154
B are horizontally fixed at both ends of the stage body
142
in the Y direction with respect to the magnetic tracks
156
A and
156
B, and due to the control subsystem previously described, make the stage body
142
run straight in the X direction and yaw only to an extremely small amount.
As evident from
FIG. 8
, the magnetic track
156
B of the right side of the linear motor and the magnetic track
156
A of the left side of the linear motor are arranged so as to have a difference in level in the Z direction between them. In other words, the bottom surface of both ends in the direction of the long axis of the magnetic track
156
on the left side is, as shown in
FIG. 7
, elevated by a certain amount with a block member
155
against the base surface
112
A. The carrier/follower
160
where the VCM
170
is fixed is arranged in the space below the elevated magnetic track
156
A.
The carrier/follower
160
is buoyed up and supported by the pre-loaded air bearings
166
(at 2 points) on the base surface
112
A′ of the base structure
112
which is one level lower. Furthermore, two pre-loaded air bearings
164
against the vertical guiding surface
117
A of the straight guiding member
117
, which is mounted onto the base structure
112
, are fixed on the side surface of the carrier/follower
160
. This carrier/follower
160
is different from the one in
FIG. 4A
according to the previous embodiment, and the driving coil
168
(
FIG. 7
) for the carrier/follower
160
is fixed horizontally to the part which extends vertically from the bottom of the carrier/follower
160
, and positioned in the magnetic flux slot of the magnetic track
156
A without any contact. The carrier/follower
160
is arranged so as not to contact any part of the magnetic track
156
A within the range of the moving stroke, and has the VCM
170
which positions the stage body
142
precisely in the Y direction.
Furthermore, in
FIG. 7
, the air bearing
166
which buoys up and supports the carrier/follower
160
is provided under the VCM
170
. The follow-up motion to the stage body
142
of the carrier/follower
160
is also done based on the detection signal from the position sensor
13
as in the previous embodiment.
In the second embodiment structured as above, there is an inconvenience where the center of gravity of the entire system shifts in accordance with the shift of the stage body
142
in the X direction, since there is substantially no member which functions as a counter weight. It is, however, possible to position the stage body
142
precisely in the Y direction with non-contact electromagnetic force by the VCM
170
by way of following the stage body
142
without any contact using the carrier/follower
160
. Furthermore, since the two linear motors are arranged with a difference in the level in the Z direction between them, there is a merit where the sum of the vectors of the force moment generated by each of the linear motors can be minimized at the center of gravity of the entire reticle stage because the force moment of each of the linear motors substantially cancels with the other.
Furthermore, since an elongated axis of action (the line KX in
FIG. 4B
) of the VCM
170
is arranged so as to pass through the center of gravity of the entire structure of the stage not only on the XY plane but also in the Z direction, it is more difficult for the driving force of the VCM
170
to give unnecessary moment to the stage body
142
. Furthermore, since the method of connecting the cables
82
,
83
via the carrier/follower
160
can be applied in the same manner as in the first embodiment, the problem regarding the cables in the completely non-contact guideless stage is also improved.
The same guideless principle can be employed in another embodiment. For example, in schematic
FIGS. 9 and 10
, the stage
242
, supported on a bases
212
, is driven in the long X direction by a single moving coil
254
moving within a single magnetic track
256
. The magnetic track is rigidly attached to the base
212
. The center of the coil is located close to the center of gravity of the stage
242
. To move the stage in the Y direction, a pair of VCMs (
274
A,
274
B,
272
A,
272
B) are energized to provide an acceleration force in the Y direction. To control yaw, the coils
274
A and
274
B are energized differentially under control of the electronics subsystem. The VCM magnets (
272
A,
272
B) are attached to a carrier/follower stage
260
. The carrier/follower stage
260
is guided and driven like the first embodiment previously described. This alternative embodiment can be utilized for a wafer stage. Where it is utilized for a reticle stage the reticle can be positioned to one side of the coil
254
and track
256
, and if desired to maintain the center of gravity of the stage
242
passing through the coil
254
and track
256
, a compensating opening in the stage
242
can be provided on the opposite side of the coil
254
and track
256
from the reticle.
Merits gained from each of the embodiments can be roughly listed as follows. To preserve accuracy, the carrier/follower design eliminates the problem of cable drag for the stage since the cables connected to the stage follow the stage via the carrier/follower. Cables connecting the carrier/follower to external devices will have a certain amount of drag, but the stage is free from such disturbances since there is no direct connection to the carrier/follower which acts as a buffer by denying the transmission of mechanical disturbances to the stage.
Furthermore, the counter-weight design preserves the location of the center of gravity of the stage system during any stage motion in the long stroke direction by using the conservation of momentum principle. This apparatus essentially eliminates any reaction forces between the stage system and the base structure on which the stage system is mounted, thereby facilitating high acceleration while minimizing vibrational effects on the system.
In addition, because the stage is designed for limited motion in the three degrees of freedom as described, the stage is substantially simpler than those which are designed for full range motions in all three degrees of freedom. Moreover, unlike a commutatorless apparatus, the instant invention uses electromagnetic components that are commercially available. Because this invention does not require custom-made electromagnetic components which become increasingly difficult to manufacture as the size and stroke of the stage increases, this invention is easily adaptable to changes in the size or stroke of the stage.
The embodiment with the single linear motor eliminates the second linear motor and achieves yaw correction using two VCMs.
The following explains another embodiment of this invention with reference to
FIGS. 11-29B
. In this example, the invention is applied to a step-and-scan type projection exposure apparatus.
FIG. 11
shows a projection apparatus of this example. In this figure, during exposure, exposure light such as i rays of a mercury lamp, excimer laser light or the like such as KrF, ArF, F
2
, or the like from an illumination optical system (not depicted) illuminates an illumination area of a pattern face of a reticle
301
. Furthermore, a pattern image within the illumination area of the reticle
301
is projected and exposed on the top of the wafer
303
on which photoresist is coated, at a predetermined projection magnification &bgr; (&bgr; is normally {fraction (1/4, 1/5)}, or the like) through a projection optical system
302
. Hereafter, an explanation is given with the Z-axis defined as being parallel to an optical axis AX of the projection optical system
302
in a non-vibrating state, and with the X-axis and Y-axis defining a perpendicular coordinate system within a plane perpendicular to the optical axis AX.
First, the reticle
301
is held on the reticle stage
304
, and when the reticle stage
304
continuously moves in the X direction (scanning direction) by a linear motor method on the reticle base
309
, a micro-adjustment of the position of the reticle
301
is performed within the XY plane. The two-dimensional position of the reticle stage
304
(reticle
301
) is measured by moving mirrors
343
X and
343
Y and laser interferometers
318
X and
318
Y on the reticle stage
304
. This measured value is supplied to a main controller
350
comprising a computer that controls an operation of the device as a whole. The main controller
350
controls the position and the moving speed of the reticle stage
4
through the reticle stage controller
352
, based upon the measured value.
Meanwhile, a wafer
303
is held on top of a wafer stage
305
by vacuum absorption, and the wafer stage
305
is disposed on a wafer base
307
via three support legs
331
A-
331
C, which can freely extend and retract within a specified range in the Z direction. The extending or retracting amount of the support legs
331
A-
331
C is controlled by a support leg controller
363
(see FIG.
26
). By making the extending or retracting amount of the support legs
331
A-
331
C the same, the position of the Z direction of the wafer
303
(focus position) is controlled. Controlling of the tilt angle (leveling) of the surface of the wafer
303
can be performed by controlling the extending or retracting amount of the support legs
331
A-
331
C independently.
The wafer stage
305
can continuously move on the wafer base
307
in the X and Y directions by, for example, a linear motor method. Additionally, stepping can also be performed by the continuous movement. Furthermore, in order to perform coordinate measurement of the wafer
303
(wafer stage
305
), an X-axis moving mirror
344
X (see
FIG. 13
) with a reflecting surface that is substantially perpendicular to the X-axis and a Y-axis moving mirror
344
Y (see
FIG. 13
) with a reflecting surface that is substantially perpendicular to the Y-axis are fixed to a side surface of the wafer stage
305
. Corresponding to these moving mirrors, an X-axis reference mirror
314
and a Y-axis reference mirror
313
are fixed to a side surface of the projection optical system
302
.
During scanning exposure, the reticle stage
304
is moved at constant velocity in the X-axis direction and, in synchronization with this movement, the wafer stage
305
on which the wafer
303
is disposed is moved in the opposite direction at a speed that is reduced by the projection magnification &bgr; of the moving speed of the reticle stage
304
, and scanning exposure is performed. After completion of the scanning exposure, the wafer stage
305
step-moves in the scanning direction or in the Y-axis direction that is perpendicular to the scanning direction. The reticle stage
304
and the wafer stage
305
are moved in sychronization in a direction opposite to the previous direction, and scanning exposure is performed. Hereafter, a pattern image of the reticle
301
is transferred to all the shooting areas on the wafer
303
by the same operation.
Next, the reticle stage and the reticle base of the exposure apparatus of this example are explained. The reticle stage
304
is a guideless stage which is disclosed in Japanese Laid-Open Patent Publication No. 8-63231 (corresponding to parent application no. 08/698,827) and can be driven in rotational directions about the optical axis AX of the projection optical system
302
and about the X- and the Y-axes. Furthermore, a pair of linear motors that drive the reticle stage
304
using a coil, which are fixed to a side surface of the reticle stage
304
, and a pair of motor magnets
311
A and
311
B, which are fixed to the top of the reticle base
309
are provided, and the reticle base
309
is supported through a fluid bearing (not depicted) such as an air bearing with respect to a top surface
310
of a structural body
306
. Ends of coil units
312
A and
312
B disposed on the top of the structural body
306
are inserted from ends of the motor magnets
311
A and
311
B, and by the pair of linear motors structured by the motor magnets
311
A and
311
B and the coil units
312
A and
312
B, the reticle base
309
is positioned in the X-axis direction with respect to the structural body
306
. Furthermore, the structural body
306
is supported on the floor by vibration control pads
349
through four legs
306
a
, decreasing the vibration from the floor.
When the reticle stage
304
moves during the scanning exposure, when the driving reaction added by the motor magnets
311
A and
311
B is received, the reticle base
309
moves, so as to maintain a momentum in the direction opposite to the moving direction of the reticle stage
304
, by the linear motor that has the coil units
312
A and
312
B. For example, if the masses of the reticle stage
304
and the reticle base
309
are 20 kg and 1000 kg, respectively, and the reticle base
309
thus has a mass 50 times that of the reticle stage
304
, if the reticle stage
304
moves by approximately 300 mm during scanning, the reticle base
309
moves in the direction opposite to the moving direction of the reticle stage
304
by approximately 6 mm. By moving the reticle stage
304
and the reticle base
309
, so as to maintain the momentum, transmission of the driving reaction to the structural body
306
of the reticle stage
304
can be prevented, and occurrence of vibration, which is a cause of disturbance during the positioning of the reticle stage
304
, can be prevented. Furthermore, the displacement amount of the reticle base
309
is constantly measured by a linear encoder (not depicted), and a current signal is formed when the reticle stage
304
is driven, based upon this measured value.
Furthermore, in the projection exposure apparatus of this example, there is no movement of the center of the gravity of the system above the reticle base
309
, so there is no fluctuation of the load to the structural body
306
that supports the reticle base
309
, and the position of the reference mirrors
313
and
314
used for the measurement of the relative position between the reticle stage
304
and the projection optical system
302
does not fluctuate. Furthermore, when the reticle base
309
is displaced a specified amount or more, if it mechanically interferes with other members, it is acceptable to constantly maintain the reticle base
309
at a substantially constant position while controlling the coil units
312
A and
312
B, which are electromagnetic driving parts disposed between the reticle base
309
and the structural body
306
, and decreasing the vibration transmitted to the structural body
306
. By doing this, it is possible to prevent the reticle base
309
from interfering with other members.
Next, a method of supporting the projection optical system of the exposure apparatus of this example is explained.
FIG. 12
shows the projection optical system
302
of the exposure apparatus of this example. In this figure, the point at which the object plane
315
and the image surface
316
are internally divided at the reduction projection magnification ratio &bgr; (=a/b) on the optical axis AX is defined as a reference point
317
of the projection optical system
302
. This reference point
317
is defined as a center, and even if the projection optical system
302
is minutely rotated about an arbitrary axis within a plane that is orthogonal to the optical axis AX, the position relationship between the object plane
315
and the image surface
316
does not change. The centers of the reference mirrors
313
and
314
are set on a plane perpendicular to the optical axis AX which pass through this reference point
317
, and a laser beam is irradiated to these centers. Accordingly, when the projection optical system
302
is slid by a disturbance vibration, the reference point
317
also moves. Furthermore, the relative displacement between the reticle stage
304
and the wafer stage
305
and the crossing point (reference mirrors
313
and
314
) of the plane perpendicular to the optical axis AX of the projection optical system
302
and the external surface of the lens barrel surrounding the projection optical system
302
are constantly measured by the laser interferometers
318
X and
318
Y. By controlling the reticle stage
304
and the wafer stage
305
so as to match the measured value with a desired value, it is possible to prevent position shifting of a pattern to be formed on the wafer
302
.
Furthermore, the bottom part of the projection optical system
302
passes through an opening of a support plate
306
b
which is disposed between the legs
306
a
, and is spaced from the opening by a gap. Additionally, the support part of the projection optical system
302
is formed by three flexible rods
319
A-
319
C extending from the structural body
306
. The extended lines of the respective rods
319
A-
319
C cross at one point, which coincides with the reference point
317
. Accordingly, even if the projection optical system
302
is slid by receiving a disturbance vibration, the projection optical system
302
is minutely rotated using the center of the reference point
317
as a center of rotation, so the position in the X and Y directions of the reference mirrors
313
and
314
hardly changes. Furthermore, because the rods
319
A-
319
C are flexibly structured, high frequency vibrations dissipate, and hardly any deterioration of the contrast occurs during transfer of the pattern.
Next, the wafer stage of the exposure apparatus of this example is explained.
As shown in
FIG. 11
, the wafer stage
305
is positioned on top of the wafer base
307
, and the wafer base
307
is supported by an elevator driving part
308
that can displace several hundred &mgr;m in the vertical direction. Between the wafer base
307
and the elevator driving part
308
, a visco-elastic body (not depicted) is provided, and vibration from the floor can be decreased. In addition, on the wafer base
307
, five speed sensors (two of the five speed sensors,
336
A and
336
B, are shown in
FIG. 26
) are provided, and the movement of the wafer stage
305
can be measured. It is also acceptable to use acceleration sensors instead of speed sensors.
FIGS. 13A-13D
show the wafer stage
305
of the exposure apparatus of this example by enlargement.
FIG. 13A
is a plan view of the wafer table
320
.
FIG. 13B
is a cross-sectional view of
FIG. 13A
along line B—B.
FIG. 13C
is a front view (however, a carrier
321
is not depicted) of FIG.
13
A.
FIG. 13D
is a cross-sectional view of
FIG. 13A
along line D—D. First, in
FIG. 13D
, the wafer stage
305
has a wafer table
320
on which a wafer
303
is disposed and a carrier
321
that carries a driving/guiding part of the wafer table
320
. The carrier
321
is movable on the wafer base
307
and can be driven in the X and Y directions by a pulse motor type of planar motor (for example, a Sawyer motor). In this example, when the carrier
321
is driven, a pulse motor (not depicted) is used to supply pulses according to the distance to a desired position by the open loop method. Because the pulses to a desired position is output to a motor controller, it is not necessary to provide a new position measurement device for the carrier
321
. Furthermore, it is also acceptable to use an ultrasonic wave motor as a flat motor.
Meanwhile, as shown in
FIG. 13A
, on the top surface of the wafer table
320
, a plurality of parallel shallow grooves
339
are disposed to vacuum absorb the wafer
303
. Many holes in the shallow grooves
339
are in communication with a vacuum pump, which is not depicted. Furthermore, deep grooves
338
to receive the wafer carrier arms, described later, are disposed in spaces between four shallow grooves
339
without interfering with the shallow grooves
339
. When a wafer
303
is fixed on the wafer table
320
, the wafer carrier arm used as the carrier of the wafer
303
can be taken in and out without interfering with the wafer table
320
.
Furthermore, as shown in
FIG. 13B
, a guide shaft
322
B is disposed in the scanning direction (X direction) via a support member
322
C on the carrier
321
. A guide member
322
A is fixed to the bottom surface of the wafer table
320
, with the guide shaft
322
B passing therethrough. The wafer table
320
is restricted by a noncontact guide (for example, a fluid bearing or a magnetic bearing) comprising the guide member
322
A, which guides the wafer table
320
on the carrier
321
in the X direction, and the guide shaft
322
B. Furthermore, in
FIG. 13D
, a pair of linear motors
323
A,
324
A, and
323
B,
324
B are structured by coils
323
A and
323
B fixed to the carrier
321
and magnets
324
A and
324
B fixed to the bottom surface of the wafer table
320
. The wafer table
320
is driven in the Y direction and the rotational direction by the linear motors
323
A,
324
A, and
323
B,
324
B, which serve as non-contact electromagnetic driving parts. The displacement of the wafer table
320
with respect to the carrier
321
is measured by a linear encoder (not depicted), which serves as a non-contact position measurement device. Furthermore, the guide shaft
322
B is structured so as to be rotatable about the guide axis by a rotation member
322
D. Additionally, when the linear motors
323
A,
324
A and
323
B,
324
B generate a driving force in the same direction, the wafer table
320
moves in the guide axis direction (X direction). Conversely, when the linear motors
323
A,
324
A, and
323
B,
324
B generate a driving force in different directions, respectively, the wafer table
320
is rotated about the center of gravity.
The center of the thrust of the linear motors
323
A,
324
A, and
323
B,
324
B and the center of the guide member
322
A are disposed so that they can be positioned in a plane parallel to the top surface of the wafer base
307
, and includes the center of gravity of the wafer table
320
. Therefore, unnecessary inclination of the wafer table does not occur at the time of acceleration of the wafer table
320
. Furthermore, the size of the guide shaft
22
B and the linear motors
323
A,
324
A, and
323
B,
324
B, only needs to be long enough for the movement of the wafer during the scanning exposure. Therefore, the size can be small so as to store the carrier
321
below the wafer table
320
, and the wafer can be moved at high speed with high accuracy.
Furthermore, because the positioning accuracy needed for receiving the wafer
303
is approximately several &mgr;m, measurement by a laser interferometer is not particularly needed in the area that receives the wafer
303
, and the resolution of the pulse motor and/or the resolution of the position measurement device of the carrier
321
is sufficient. Therefore, the moving mirrors
344
X and
344
Y which are provided for the wafer table
320
of
FIG. 13
for the laser interferometers
318
X and
318
Y do not necessarily have to cover the entire moving area of the wafer table
320
. Only the length of the area in which precise positioning in nm units is needed, that is, the length of the diameter of the wafer
303
, is needed.
The moving mirrors
344
X and
344
Y for the laser interferometer
318
are disposed on side surfaces of the wafer table
320
of this example, and the rotational angle about the Z-axis and the position of the wafer table
320
are measured. Side surfaces of the wafer table
320
are used as moving mirrors
344
X and
344
Y for the laser interferometers
318
X and
318
Y, so the wafer table
320
is of a size that substantially circumscribes the wafer
303
, and it is extremely small and light, compared to a conventional wafer table. Furthermore, when the wafer table
320
is structured so as to dispose a rib structure in the bottom surface with a thickness of approximately 3 mm by using a silicon carbide, the weight of the wafer table
320
is approximately 5 kg.
FIG. 14
is a block diagram showing a structure of a controller that controls both the wafer table
320
and the carrier
321
. In
FIG. 14
, the main controller
350
supplies desired positions of the carrier
321
and the wafer table
320
, respectively, to subtractors
354
and
357
within the wafer stage controller
325
. Furthermore, the relative displacement amount of the wafer table
320
with respect to the carrier
321
is detected by a hypothetical subtractor
356
and a displacement sensor (linear encoder)
360
. A table controller
355
drives the wafer table
320
, based upon the output of the subtractor
354
and the displacement sensor
360
, and the carrier controller
358
drives the carrier
321
based upon the output of the subtractor
357
. The subtractor
354
outputs a value corresponding to the measured value of the laser interferometers
318
X and
318
Y subtracted from the desired value, and the subtractor
357
outputs a value that corresponds to the measured value of a hypothetical linear encoder
359
for the carrier
321
subtracted from the desired value.
When the laser interferometers
318
X and
318
Y (see
FIG. 11
) are not used while the mode switch
326
is OFF, that is, in the case of the approximate positioning, based upon the signal from the displacement sensor
360
that serves as a linear encoder, the wafer stage controller
325
controls the linear motors
323
A,
324
A and
323
B,
324
B of
FIGS. 13A-13D
so as to constantly position the wafer table
320
at the middle point of the moving range with respect to the carrier
321
. Furthermore, when the driving part of the carrier
321
has an encoder
359
, the carrier controller
358
moves the carrier
321
to a desired position with reference to the encoder
359
. When an encoder is not especially provided, such as in the case of a pulse motor in this example, pulses to a desired position are output to the motor controller and the carrier
321
is controlled. Therefore, regardless of the existence of an encoder, the wafer table
320
is controlled so as to be moved while following the movement of carrier
321
.
When the mode switch
326
of
FIG. 14
is in the ON state and the wafer table
320
moves based upon the measured value of the laser interferometers
318
X and
318
Y, that is, in the case of precise positioning, based upon the output of the subtractor
354
, which references the measured value of the laser interferometers
318
X and
318
Y, the table controller
355
causes the linear motors
323
A,
324
A and
323
B,
324
B to generate thrust with respect to the wafer table
320
, and causes the wafer table
320
to move. Furthermore, the carrier
321
is controlled just like in the approximate positioning.
When the wafer table
320
moves at constant velocity while using the laser interferometers
318
X and
318
Y, that is, at the time of scanning exposure, the table controller
355
causes the linear motors
323
A,
324
A and
323
B,
324
B to generate thrust and move the wafer table
320
while referring to the output of the subtractor
354
, which has subtracted the measured value of the laser interferometers
318
X and
318
Y. At this time, the carrier
321
maintains a still state, and only the wafer table
320
moves at a constant velocity. Therefore, it is only the light weight wafer table
320
that generates the driving reaction with respect to the wafer base
307
during the scanning exposure, so the disturbance reaction to be generated becomes extremely small, and scanning exposure can be performed at high speed with high accuracy.
Next, the guide member
322
A and the guide shaft
322
B of the wafer table
320
of the exposure apparatus of this example are explained.
FIG. 15A-C
show the guide member
322
A and the guide shaft
322
B of
FIGS. 13A-D
by enlargement. In this figure, springs
327
A and
327
B are provided as elastic bodies at both ends of the guide shaft
322
B. When the wafer table
320
reciprocates with respect to the carrier
321
, first, as shown in
FIG. 15A
, kinetic energy of the wafer table
320
is converted to potential energy via the guide member
322
A and is stored in the spring
327
A. Next, as shown in
FIG. 15B
, the potential energy that has been stored in the spring
327
A is again converted to kinetic energy of the wafer table
320
, and the wafer stage controller
325
of
FIG. 11
controls the wafer table
320
using the kinetic energy so that it moves the wafer table
320
at the speed of −V. Furthermore, as shown in
FIG. 15C
, when the support member
322
A contacts the spring
327
B, an opposing force of +F occurs in the spring
327
B and the kinetic energy of the wafer table
320
is again converted to potential energy and is saved in the spring
327
B. Therefore, mechanical energy to be consumed in the case of reciprocation of the wafer table
320
is mainly only the heat from the viscosity resistance of the wafer table
320
with respect to the air, and from when the elastic bodies are deformed. Thus, the heating amount of the linear motors
323
A,
324
A, and
323
B,
324
B becomes extremely small.
FIG. 16A
shows a speed curve of the wafer table
320
when the moving speed of the wafer table
320
is shifted to a constant speed (0.5 m/s) and is moved on the guide shaft
322
B, which is hypothetically defined as a guide axis without an elastic body. In
FIG. 16A
, the horizontal axis shows time t (s), and the vertical axis shows the moving speed V (m/s) of the wafer table
320
. Furthermore,
FIG. 16B
shows the thrust of the linear motors
323
A,
324
A and
323
B,
324
B at that time. In
FIG. 16B
, the horizontal axis is time t (s), and the vertical axis is a thrust F(N) of the linear motors. Furthermore, the mass of the wafer table
320
which is used is 5 kg.
FIG. 17A
corresponds to FIG.
16
A and shows a speed curve of the wafer table
320
calculated assuming the case where an ideal wafer table
320
without vibration is accelerated to a certain speed on the guide axis provided with a specified spring.
FIG. 17B
shows a thrust F(N) of the linear motors
323
A,
324
A and
323
B,
324
B, which is calculated assuming the case where a wafer table
320
that resonates is controlled with the speed curve of
FIG. 17A
as the speed governing value. When
FIGS. 16A-B
are compared with
FIGS. 17A-B
, the ratio of the heating amount of the linear motors
323
A,
324
A, and
323
B,
324
B is 1:0.94, which is substantially the same.
FIG. 18A
shows a speed curve when the speed curve of
FIG. 17A
is the speed governing value, the guide shaft
322
B provided with the springs
327
A and
327
B of
FIG. 15
is used, and the wafer table
320
is accelerated to a constant speed.
FIG. 18B
shows the thrust of the wafer table
320
and thrust generated by the linear motors
323
A,
324
A and
323
B,
324
B. In
FIG. 18B
, the horizontal axis is time t (s), and the vertical axis is thrust F(N). The curve A in a solid line is the thrust added to the wafer table
320
, and the curve B in the single-dot chain line shows the thrust of the linear motors
323
A and
323
B. The spring constant of the springs
327
A and
327
B is 1,000 N/m, and this is 40% of an ideal spring constant (2,500 N/m). By using the springs
327
A and
327
B, the heating amount of the linear motors
323
A,
324
A and
323
B,
324
B can be reduced to approximately 35% of the heating amount of the case when an elastic body is not used.
FIG. 19A
shows a speed curve when the wafer table
320
is accelerated to a constant speed using a guide shaft
322
B with springs
327
A and
327
B with the optimum spring constant value of 2,500 N/m.
FIG. 19B
shows the thrust F of the wafer table
320
at that time. The heating amount of the linear motors
323
A,
324
A and
323
B,
324
B can be reduced to 1% or less of the case when an elastic body is not used. Thus, by having the springs
327
A and
327
B at both ends of the guide shaft
322
B, the heating amount of the linear motors
323
A,
324
A and
323
B,
324
B can be reduced when the wafer table
320
constantly moves.
However, in the case of the still-positioning of the wafer table
320
at the end of the guide shaft
322
B, the linear motors
323
A,
324
A and
323
B,
324
B need to generate a thrust that can be balanced with the resistance of the springs
327
A and
327
B, which causes the heating amount of the linear motors
323
A,
324
A and
323
B,
324
B to increase.
FIG. 20
shows the resistance of the springs
327
A and
327
B at the end of the guide shaft
322
B provided with the springs
327
A and
327
B. In
FIG. 20
, the horizontal axis shows distance D(m) from the end of the guide shaft
322
B, and the vertical axis shows the resistance F
p
(N) of the springs
327
A and
327
B. In order to still-position the wafer table
320
at the end of the guide shaft
322
B, the linear motors
323
A,
324
A and
323
B,
324
B need to generate a thrust (50 N) that is large enough to balance the resistance of the springs
327
A and
327
B. Otherwise, the heating amount increases. Therefore, in this case, a magnetic member is fixed to the end of the guide shaft
322
B. Preferably, the heating amount is reduced when the wafer table
320
is still-positioned by using the attractive force of the magnet member.
FIGS. 21A-C
show the guide member
322
A and the guide shaft
322
B to which the magnetic member is fixed, corresponding to
FIGS. 15A-C
. In
FIGS. 21A-C
, steel plates
329
are fixed to both ends of the guide member
322
A, and magnets
330
are fixed at both ends of the guide shaft
322
B. As shown in
FIGS. 21A-C
, when the wafer table
320
is still-positioned at the end of the guide shaft
322
B via the guide member
322
A, by using the attraction of the steel plate
329
and the magnet
330
, the thrust of the linear motors
323
A,
324
A and
323
B,
324
B needed against the resistance of the springs
327
A and
327
B can be reduced and the heating amount can be controlled. Furthermore, in the case of moving the wafer table
320
at a constant velocity, as shown in
FIG. 21B
, by using the resistance of the springs
327
A and
327
B, the heating amount of the linear motors
323
A,
324
A, and
323
B,
324
B is reduced. In this case, the heating amount of the linear motors can be reduced to approximately ⅙ of the case when a spring or the like is not used on the guide shaft
322
B. Additionally, when there is no limitation to the thrust of the linear motors, the potential energy at both ends of the guide shaft
322
B can be set at 0. Furthermore, the setting relationship between the steel plates
329
and the magnets
330
can be reversed, and it is acceptable to dispose anything that generates attractive force opposing the resistance of the elastic member of the springs
327
A and
327
B or the like at the ends of the guide shaft
322
B.
FIG. 22A
shows a speed curve that is calculated assuming the case where an ideal wafer table
320
without vibration is accelerated to a constant speed on a guide shaft
322
B provided with springs, steel plates, and magnets. In
FIG. 22A
, the horizontal axis is time t(s), and the vertical axis is moving speed V(m/s) of the wafer table
320
.
FIG. 22B
shows a thrust of the linear motors
323
A,
324
A and
323
B,
324
B calculated assuming the case where the wafer table
320
that resonates is controlled with the speed curve of
FIG. 22A
as the speed governing value. In
FIG. 22B
, the horizontal axis is time t(s), and the vertical axis is thrust F(N) of the linear motors.
FIG. 23A
shows a speed curve when the speed curve of
FIG. 22A
is the speed governing value and the wafer table
320
is accelerated to a constant speed on the guide axis
322
provided with the steel plates
329
and the magnets
330
.
FIG. 23B
shows the thrust F (curve A in solid line) that is added to the wafer table
320
at that time, and the thrust F (curve B in single-dot chain line) of the linear motors
323
A,
324
A and
323
B,
324
B. The spring constant of the springs
327
A and
327
B is 2,000 N/m, which is the optimum spring constant. The heating amount of the linear motors
323
A,
324
A and
323
B,
324
B in this case is 1% or less of the case when springs, magnets, and steel plates are not used. Furthermore, compared to the case where a magnet or the like is not provided, the thrust required at the start of moving is small and the wafer table
320
is gradually accelerated, so there is an advantage such that the mechanical resonance of the wafer table
320
can be eased.
FIG. 24
shows the resultant force F
p
(N) between the resistance of the springs
327
A and
327
B and the attraction between the magnet
330
and the steel plate
329
at an end of the guide shaft
322
B to which the steel plate
329
and the magnet
330
are fixed according to FIG.
20
. In
FIG. 24
, the horizontal axis is distance D(m) from the end of the guide shaft
322
B. As the magnet
330
is fixed to the end of the guide shaft
322
B, and the steel plate
329
is fixed to the guide member
322
A, the thrust of the linear motors
323
A,
324
A and
323
B,
324
B required for the still-positioning of the wafer table
320
at the end of the guide shaft
322
B can be reduced and the heating amount can be controlled.
Next, the structure of the support legs
331
A-
331
C that support the wafer table
320
with respect to the wafer base
307
of the exposure apparatus of this example is explained.
FIG. 25A
is an enlarged view showing the support leg
331
A and the like of the wafer table
320
.
FIG. 25B
is a side view. In the support leg
331
A, between slot
331
Aa and a lower slot
331
Ab is a displacement part
334
. A fluid bearing
332
A is attached to the bottom of the displacement part
334
through a spherical bearing
335
so that it can be rotated. In the same manner, as shown in
FIG. 13
, fluid bearings
332
B and
332
C are fixed to the other support legs
331
B and
331
C. The fluid bearing
332
A is disposed on the wafer base
307
of
FIG. 13
by a hydrostatic pressure fluid bearing method. Additionally, as shown by the support leg
331
B of
FIG. 13C
, piezoactuators
333
are fixed to the support legs
331
A-
331
C, and the piezoactuators
333
are fixed to the wafer table
320
via fixing members
353
.
Referring to
FIGS. 25A-B
, a displacement enlargement mechanism that can be extended and retracted in the direction of support is structured by the piezoactuator
333
and the displacement part
334
. The fluid bearing
332
A has a magnet or a vacuum absorption part for applying pressure. In general, because the displacement by the piezoactuator is only approximately 60 &mgr;m, a displacement enlargement mechanism is needed. The displacement enlargement mechanism of this example uses a parallel motion link. When the extending/retracting part of the piezoactuator
333
presses an input point A of the slot
331
Aa of the support leg
331
A, the input point A is linearly displaced in the horizontal direction by a minute displacement area. Then, point B of the link mechanism part of the displacement part
334
of the displacement enlargement mechanism is rotated about center point C, and point D is displaced in a vertical direction as a result thereof. In the displacement part
334
of the displacement enlargement mechanism of this example, the slope of the link is 26.6°, the displacement enlargement percentage becomes double, and it can be displaced to a maximum of 120 &mgr;m. Furthermore, by adjusting the displacement of the displacement part
334
of the support legs
331
A-
331
C, correction of the tilt angle (leveling) of the wafer table
320
and the correction of the position in the vertical direction (focus adjustment) with respect to the wafer base
307
are performed.
Furthermore, even if the support legs
331
A-
331
C are displaced 120 &mgr;m, which is the maximum displacement amount, if focus adjustment and leveling cannot be appropriately performed, the front surface positioning of the wafer
303
is premeasured before the exposure starts, and the elevator driving part
308
of
FIG. 11
is driven and the wafer base
307
is positioned so that the position of the surface of the wafer
303
can be placed at a specified position (the image plane of the projection optical system
302
). After that, focus adjustment and leveling are performed by adjusting the support legs
331
A-
331
C.
FIG. 26
is a block diagram showing a structure of a controller that controls the reticle stage
304
and the wafer stage
305
. In
FIG. 26
, the main controller
350
supplies the desired value of the displacement amount to a desired position in the X and Y directions of the wafer table
320
of the wafer stage
305
and the Z direction of the support legs
331
A-
331
C to the subtractors
361
and
362
, respectively. Based upon the value corresponding to a value that is multiplied by −¼ of the measured value, from the desired position in the subtractor
361
of the laser interferometers
318
X and
318
Y in the converter
365
, the wafer stage controller
325
drives the wafer stage
305
. The subtractor
362
adds a value obtained by integrating the speed in the Z direction of the wafer base
307
, which is measured by the speed sensor
336
B, to the desired value, and further supplies a value obtained by subtracting a defocus amount of the wafer stage
305
, which is measured by an autofocus sensor, not depicted, to a support leg controller
363
. The support leg controller
363
controls the extending or retracting amount of the support legs
331
A-
331
C, which support the wafer stage
305
based upon the supplied value, and focus adjustment and leveling can be performed. Furthermore, the reticle stage controller
352
controls the reticle stage
304
, based upon the detection result of the vibration component (yawing) of the projection optical system
302
in the rotational direction about the optical axis and the displacement of the wafer base
307
in the direction perpendicular to the scanning direction detected by the speed sensor
336
A, and on the value corresponding to the measured value of the laser interferometers
318
X and
318
Y subtracted from the output of the converter
365
using the subtractor
366
. Thus, the effects of vibration of the wafer base
307
in the horizontal direction can be reduced. Furthermore, the vibration of the wafer base
307
in the Z direction can be reduced by a visco-elastic body
364
.
Next, the wafer carrier mechanism of the exposure apparatus of this example is explained. In
FIG. 11
, in front of the wafer base
307
, a carrier base
345
is disposed via a vibration control table
351
. A wafer carrier mechanism such as wafer carrier arms
340
A and
340
B and the wafer cassette
348
and/or the like are disposed on the carrier base
345
.
FIG. 27A
is a plan view showing part of the wafer carrier mechanism of the exposure apparatus of this example.
FIG. 27B
is a side view. First, the wafer stage
305
on which is disposed a wafer
303
A to which exposure has been completed moves from the exposure completion position A to the wafer carrier position B, and the wafer
303
A moves to the position P
1
. At this time, three fingers of the wafer carrier arms
340
A are inserted into spaces which are surrounded by the wafer
303
A and the deep grooves
338
of the wafer table
320
, and do not contact the wafer table
320
. The wafer carrier arm
340
A is attached on the support part
367
A via an actuator
369
A that can be extended and retracted in the Z direction and that can be rotated, and the support part
367
A moves on the carrier base
345
by a driving part
368
A. A support part
367
B, an actuator
369
B, and a driving part (not depicted) are provided on another wafer carrier arm
340
B as well. When the wafer stage
305
is still, the wafer table
320
releases the fixation of the wafer
303
A by vacuum absorption, and the wafer carrier arm
340
A vacuum-absorbs the wafer
303
A and is raised by the actuator
369
A. Furthermore, a wafer
303
A to which exposure has been completed is collected to the wafer cassette
348
shown in
FIGS. 28A-B
.
When the wafer carrier arm
340
A raises, the wafer stage
305
simultaneously moves at high speed to below the wafer carrier arm
340
B (wafer carry-in position C) which holds a non-exposed wafer
303
B. When the wafer table
320
of the wafer stage stops, the wafer carrier arm
340
B is lowered by the actuator
369
B, and the non-exposed wafer
303
B is disposed on the wafer table
320
and is vacuum-absorbed. At this time, because the wafer carrier arm
340
B is also inserted into the deep grooves
338
, it does not contact the wafer table
320
. After this, the wafer stage
305
moves at high speed from the wafer carrier-in position C to the exposure start position D, the wafer
303
B moves to the position P
2
, and exposure begins. At the same time, the wafer carrier arm
340
B takes a new wafer out from the wafer cassette
348
of
FIGS. 28A-B
and waits.
When superposition exposure is performed, the rotational angle of the wafer of the exposure object is measured in advance and the wafer table
320
is rotated during the positioning so as to cancel the angle of the wafer stage
305
at the wafer carrier position C. By doing this, when the wafer table
320
is facing in the scanning direction, a pattern that is formed in a shooting area that is already arrayed in a grid state on the wafer and a pattern image of the reticle
301
can be in a specified positional relationship.
FIG. 28A
is a plan view showing the vicinity of the wafer cassette
348
when a wafer is carried out.
FIG. 28B
is a side view of FIG.
28
A. The wafer carrier arms
340
A and
340
B can be freely driven in three directions such as a rotational direction about the Z-axis, a scanning direction (X direction), and a vertical direction (Z direction). A wafer cassette support member
347
that supports the wafer cassette
348
on the carrier base
345
can be freely driven in the vertical direction. When an already-exposed wafer
303
A is collected to the wafer cassette
348
, first, the wafer carrier arm
340
A that holds the wafer
303
A is revolved by the actuator
369
A. At the moment the wafer
303
A goes through the position P
4
and reaches the front surface of the wafer cassette
348
, the support member
367
A of the wafer carrier arm
340
A linearly moves to the position P
3
in the X-axis direction and the wafer carrier arm
340
A is revolved at the same time so that the wafer
303
A linearly moves in the Y-axis direction. Next, when the wafer
303
A reaches a predetermined position within the wafer cassette
348
, vacuum absorption by the wafer carrier arm
340
A is released, and the wafer cassette support member
347
raises and lifts up the wafer
303
A. Then, the wafer carrier arm
340
A performs an opposite operation compared to the previous process and withdraws.
FIG. 29A
is a plan view showing the vicinity of the wafer cassette
348
when the wafer is carried in.
FIG. 29B
is a side view of FIG.
29
A. When the wafer is carried out from the wafer cassette
348
, first the wafer carrier arm
340
B moves below the non-exposed wafer
303
B. When the wafer carrier arm
340
B stops, the wafer cassette support member
347
lowers, and the wafer
303
B is disposed on the wafer carrier arm
340
B. Then, after the wafer carrier arm
340
B vacuum-absorbs the wafer
303
B, the support member
367
B of the wafer carrier arm
340
B linearly moves in the X-axis direction, the wafer carrier arm
340
B is revolved by the actuator
369
B and takes the wafer
303
B out from the wafer cassette
348
. It then waits until the wafer stage
305
arrives. Furthermore, the wafer carrier arm
340
B can linearly move parallel to the front surface of the device, so it is also possible to structure the device in-line with surrounding devices such as a coater or a developer.
Thus, as the wafer stage
305
of
FIG. 27
moves to the position of carrying out the wafer or the position of carrying in the wafer, it is not necessary to temporarily fix and support the wafer as in a conventional exposure apparatus, and there is no need for receiving and giving the wafer between wafer carrier arms. Therefore, the probability of foreign objects attaching to the wafer and the probability of carrier error can be reduced. Furthermore, a larger mass wafer can be carried and a larger size of wafer can be developed, compared to when the wafer is carried to the exposure position by wafer carrier arms, because the effects of vibration of the wafer carrier arms are not easily received due to the mass of the wafer.
While the present invention has been described with reference to preferred embodiments thereof, it is to be understood that the invention is not limited to the disclosed embodiments or constructions. To the contrary, the invention is intended to cover various modifications and equivalent arrangements. In addition, while the various elements of the disclosed invention are shown in various combinations and configurations, which are exemplary, other combinations and configurations, including more, less or only a single element, are also within the spirit and scope of the invention.
标题 | 发布/更新时间 | 阅读量 |
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