| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 61 | Method of polarizing ions, and sources of polarized ions, notably protons and deuterons, obtained therefrom | US29699363 | 1963-07-23 | US3286162A | 1966-11-15 | ANATOLE ABRAGAM; RENE BEURTEY; ANDRE PAPINCAU; JACQUES THIRION; MICHEL WINTER JACQUES |
| 62 | APPARATUS FOR GENERATING FOCUSED ELECTROMAGNETIC RADIATION | US15489160 | 2017-04-17 | US20170323697A1 | 2017-11-09 | Arzhang Ardavan; Houshang Ardavan |
| An apparatus for generating electromagnetic radiation comprises a polarizable or magnetizable medium. A polarization or magnetisation current can be generated, in a controlled manner, whose distribution pattern has an accelerated motion, so that non-spherically decaying and intense spherically decaying components of electromagnetic radiation can be generated. The coordinated motion of aggregates of charged particles can give rise to extended electric charges and currents. The charged distribution patterns can propagate with a phase speed exceeding the speed of light in vacuo and that, once created, such propagating charged patterns act as sources of electromagnetic fields in precisely the same way as any other moving sources of these fields. That the distribution patterns of these sources travel faster than light is not, of course, in any way incompatible with the requirements of special relativity. The superluminally moving charged pattern is created by the coordinated motion of aggregates of subluminally moving particles. | ||||||
| 63 | Illumination optical unit for microlithography | US13370829 | 2012-02-10 | US09235137B2 | 2016-01-12 | Damian Fiolka; Ralf Stuetzle |
| An illumination optical unit includes a collector mirror which produces a polarization distribution that is applied to the first faceted optical element during the operation of the illumination optical unit. There are at least two first facet elements to which radiation having a differing polarization is applied. The first faceted optical element has at least one first state in which the normal vectors of the reflective surfaces of the first facet elements are selected so that a first predetermined polarization distribution results at the location of the object field during the operation of the illumination optical unit. | ||||||
| 64 | Versatile spin-polarized electron source | US14185651 | 2014-02-20 | US09142634B2 | 2015-09-22 | Chris Jozwiak; Cheol-Hwan Park; Kenneth Gotlieb; Steven G Louie; Zahid Hussain; Alessandra Lanzara |
| One or more embodiments relate generally to the field of photoelectron spin and, more specifically, to a method and system for creating a controllable spin-polarized electron source. One preferred embodiment of the invention generally comprises: method for creating a controllable spin-polarized electron source comprising the following steps: providing one or more materials, the one or more materials having at least one surface and a material layer adjacent to said surface, wherein said surface comprises highly spin-polarized surface electrons, wherein the direction and spin of the surface electrons are locked together; providing at least one incident light capable of stimulating photoemission of said surface electrons; wherein the photon polarization of said incident light is tunable; and inducing photoemission of the surface electron states. | ||||||
| 65 | VERSATILE SPIN-POLARIZED ELECTRON SOURCE | US14185651 | 2014-02-20 | US20150235799A1 | 2015-08-20 | Chris Jozwiak; Cheol Hwan Park; Kenneth Gotlieb; Steven Gwon Sheng Louie; Zahid Hussain; Alessandra Lanzara |
| One or more embodiments relate generally to the field of photoelectron spin and, more specifically, to a method and system for creating a controllable spin-polarized electron source. One preferred embodiment of the invention generally comprises: method for creating a controllable spin-polarized electron source comprising the following steps: providing one or more materials, the one or more materials having at least one surface and a material layer adjacent to said surface, wherein said surface comprises highly spin-polarized surface electrons, wherein the direction and spin of the surface electrons are locked together; providing at least one incident light capable of stimulating photoemission of said surface electrons; wherein the photon polarization of said incident light is tunable; and inducing photoemission of the surface electron states. | ||||||
| 66 | POLARIZED ULTRAVIOLET LIGHT SPLITTING ELEMENT | US14424915 | 2013-08-29 | US20150219918A1 | 2015-08-06 | Tae Su Kim; Jae Jin Kim; Jong Byung Lee; Jeong Ho Park; Jin Mi Jung; Bu Gon Shin |
| The present application relates to a polarized ultraviolet light splitting element and to the use thereof. The present application may provide a polarized ultraviolet light splitting element which exhibits excellent splitting efficiency within a wide range of the ultraviolet light region and which has excellent durability. The element can be used, for example, in a photoalignment process of a liquid crystal alignment film. | ||||||
| 67 | EUV LIGHT SOURCE FOR GENERATING A USABLE OUTPUT BEAM FOR A PROJECTION EXPOSURE APPARATUS | US14636413 | 2015-03-03 | US20150173163A1 | 2015-06-18 | Ingo Saenger; Manfred Maul; Christoph Hennerkes; Johannes Ruoff; Daniel Kraehmer |
| An EUV light source serves for generating a usable output beam of EUV illumination light for a projection exposure apparatus for projection lithography. The light source has an EUV generation device which generates an EUV raw output beam. The latter is circularly polarized. For the purposes of setting the polarization of the usable output beam and in respect of the polarization direction, a polarization setting device has a linearly polarizing effect on the raw output beam. This results in an EUV light source, which provides an improved output beam for a resolution-optimized illumination. | ||||||
| 68 | Apparatus for producing nuclear spin-polarized noble gas, nuclear magnetic resonance spectrometer, and nuclear magnetic resonance imager | US11984869 | 2007-11-23 | US07710114B2 | 2010-05-04 | Mineyuki Hattori; Takashi Hiraga; Noritaka Yamamoto |
| An apparatus for producing a nuclear spin-polarized noble gas by spin-polarizing a noble gas in the presence of an optical pumping catalyst under application of magnetic field and laser light, including a cell having a thin reaction chamber, a gas introduction conduit connected in fluid communication with the reaction chamber for feeding the noble gas, a gas discharge conduit connected in fluid communication with the reaction chamber, a first gate valve having an outlet port connected to the gas introduction conduit and an inlet port adapted to be in fluid communication with a noble gas introduction line, a second gate valve having an inlet port connected to the gas discharge conduit and an outlet port, and a capillary tube removably connected to the outlet port of the second valve for recovering a nuclear spin-polarized noble gas produced in the reaction chamber. The apparatus may be directly connected to NMR or MRI. | ||||||
| 69 | Neutron Polarization Apparatus | US11992848 | 2006-11-01 | US20100032554A1 | 2010-02-11 | Hirohiko Shimizu; Jun-ichi Suzuki; Takayuki Oku |
| A neutron polarization apparatus is provided that provides a neutron beam polarized by an interaction between a spin of a neutron in an incident neutron beam and a magnetic field. The apparatus includes a quadrupole magnet (2) disposed around a passage of a neutron beam, a tubular neutron absorber (3) provided in the quadrupole magnet (2) along am axial direction of the neutron beam, and a solenoid coil (4) disposed at an exit of the quadrupole magnet (2), adiabatically coupling the quadrupole magnetic field produced by the quadrupole magnet (2) and applying a bipolar magnetic field. The neutron polarization apparatus can polarize a neutron with a high polarization unavailable in the prior art. | ||||||
| 70 | Polarized neutron guide | US11449374 | 2006-06-08 | US07560687B2 | 2009-07-14 | Sang Jin Cho; Chang Hee Lee; Hark Rho Kim; Young Jin Kim |
| A polarized neutron guide for separating neutrons into polarized neutrons while minimizing loss of the neutrons is provided. The polarized neutron guide includes a body, the first space and the second space, and a neutron separation space. The body includes super mirrors coated with a neutron-reflective thin film and the first and second spaces are formed by the first plate inside the body. The neutron separation space is formed by the second plate disposed at the entry of the first space and the third plate disposed at the entry of the second space. Spin-up polarized neutrons and spin-down polarized neutrons are simultaneously separated and transferred in the first and second spaces, respectively. Therefore, with minimum loss of the neutrons, the spin-up polarized neutrons and the spin-down polarized neutrons are effectively separated and collected. | ||||||
| 71 | Spin Isolation Apparatus, Spin Asymmetric Material Producing Method, Current Source, and Signal Processing Method | US12087152 | 2006-12-27 | US20090107895A1 | 2009-04-30 | Takashi Suzuki |
| A spin isolation apparatus comprising a particle source for emitting particles having spins, a receiving section for receiving the particles emitted by the particle source, a magnet for separating the particles into first particles having positive spins and second particles having negative spins, and a trajectory restricting section for isolating the first and the second particles received by the receiving section through restricting trajectories of the first particles and/or the second particles is provided. By applying this apparatus, particles having spins whose every sign is either one of the two signs can be mass-produced. | ||||||
| 72 | Polarized neutron guide | US11449374 | 2006-06-08 | US20070076837A1 | 2007-04-05 | Sang Cho; Chang Lee; Hark Kim; Young Kim |
| A polarized neutron guide for separating neutrons into polarized neutrons while minimizing loss of the neutrons is provided. The polarized neutron guide includes a body, the first space and the second space, and a neutron separation space. The body includes super mirrors coated with a neutron-reflective thin film and the first and second spaces are formed by the first plate inside the body. The neutron separation space is formed by the second plate disposed at the entry of the first space and the third plate disposed at the entry of the second space. Spin-up polarized neutrons and spin-down polarized neutrons are simultaneously separated and transferred in the first and second spaces, respectively. Therefore, with minimum loss of the neutrons, the spin-up polarized neutrons and the spin-down polarized neutrons are effectively separated and collected. | ||||||
| 73 | Method of converting transverse electrical modes and a helically outlined aperture antenna for implementing the method | US803079 | 1991-12-06 | US5266962A | 1993-11-30 | Arnold Mobius; Manfred Thumm |
| A mode converter for converting transverse electric modes into hybrid modes of type EH.sub.mn and including a circular waveguide provided with corrugations extending in a circumferential (azimuth) direction that become deeper toward its end and are continued in a subsequent helically outlined aperture antenna with constant depth. The emitted radiation is circularly polarized and, by the use of suitable reflectors for the emitted radiation, may be cause to be linearly polarized. The emitted radiation no longer has any sidelobes in the far field and its characteristic has a Gaussian profile over the azimuth angle. | ||||||
| 74 | Composite light source unit and scanning device | US408005 | 1989-09-15 | US5083023A | 1992-01-21 | Ichirou Miyagawa |
| A composite light source unit including a plurality of semiconductor lasers disposed in a housing, a plurality of collimator optical systems for converting the laser beams to parallel laser beams, respectively, and a combining optical system for combining all the laser beams except one as a group of laser beams having close, parallel optical axes, respectively, extending in a direction different from the direction of said one laser beam, whereby said one laser beam and the group of laser beams are emitted from the housing in different directions. Alternatively, the combining optical system combines the laser beams as a group of laser beams having close, parallel optical axes, respectively, and emits the group of laser beams out of the housing, one of the laser beams emitted out of the housing having a different optical property than that of the other laser beams. Said one laser beam can easily be separated from the other laser beams, and will be used as a synchronizing beam in a scanning device. | ||||||
| 75 | Wave mode converter | US863235 | 1977-12-22 | US4175830A | 1979-11-27 | Georges R. P. Marie |
| Mode converter for electromagnetic, light or infrared waves. This mode converter converts particle non-confining modes to particle confining modes. In a confining mode wave beam the phase of the wave with respect to time at a point of the beam having a given azimuth with respect to the beam axis is proportional to this azimuth. Two types of mode converter are disclosed. In the first type, the wave passes through a block of transparent isotropic material the thickness of which is proportional to the azimuth around the beam axis. In the second type, the converter is formed with triangular or sectoral plates of birefringent material and in each plate the slow and fast axes are given an adequate orientation. | ||||||
| 76 | Dielectic refrigerator using orientable defect dipoles | US755890 | 1976-12-30 | US4136525A | 1979-01-30 | James A. Van Vechten |
| This disclosure describes a dielectric refrigerator using orientable defect dipoles and operating between a high temperature, T.sub.h reservoir illustratively supplied by a Stirling cycle refrigerator (8.degree. K .ltoreq. T.sub.h .ltoreq. 20.degree. K) and a low temperature, T.sub.1, load, illustratively the liquid He cooling fluid for Josephson junction or other superconducting devices (2.degree. K .ltoreq. T.sub.1 .ltoreq. 6.degree. K).Exemplary practice of this invention provides cooling from the limit of a refrigerator based on the Stirling thermodynamic cycle (20 to 8.degree. K) to operating temperatures of common and useful superconductive devices (3 to 6.degree. K). Orientable electric dipoles of defects in electrically insulating materials, e.g., crystals, are utilized to provide cooling in the range from (8-20 K) to (2-6.degree. K). The following are particular considerations concerning the practice of this invention: use of LiF, MgO and BeO as host crystals; use of OH and/or NH.sub.2 as defects in LiF, and use of HF, HCl, HBr and/or NH as defects in MgO or BeO; mechanical or electromechanical means to make and break thermal contact between dielectric crystal and load and between load and reservoir; and use of thermal rectifiers to obviate the need for thermal switches in order to transfer heat from the load to the refrigerator material and thence to the reservoir. | ||||||
| 77 | Source of spin polarized electrons | US581837 | 1975-06-03 | US3968376A | 1976-07-06 | Daniel Thornton Pierce; Felix Andrea Meier; Hans-Christoph Siegmann |
| The invention concerns a method of producing intense beams of polarized free electrons in which a semiconductor with a spin orbit split valence band and negative electron affinity is used as a photocathode and irradiated with circularly polarized light. | ||||||
| 78 | Collection of ions in a plasma by magnetic field acceleration with selective polarization | US428661 | 1973-12-27 | US3959649A | 1976-05-25 | Harold K. Forsen |
| Method and apparatus for generating and accelerating ions in a vapor by use of relatively polarized laser radiation and a magnetic field. As applied to uranium isotope enrichment, a flowing uranium vapor has particles of the U.sub.235 isotope type selectively ionized by laser radiation and the ionized flow is subjected to a transverse gradient in a magnetic field. The magnetic field gradient induces an acceleration on the ionized particles of U.sub.235 which deflects them from their normal flow path toward a collecting structure. High magnetic field and corresponding high ion accelerations are achieved without loss in ionization selectivity by maintaining a polarization between the applied laser radiation and magnetic field which minimizes Zeeman splitting of the uranium energy states. | ||||||
| 79 | Process for producing negative hydrogen ions | US3424905D | 1966-04-25 | US3424905A | 1969-01-28 | DONNALLY BAILEY L |
| 80 | Process for producing negative hydrogen ions from protons | US3424904D | 1965-05-03 | US3424904A | 1969-01-28 | DONNALLY BAILEY L |
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