181 |
CHARGED PARTICLE RADIATION THERAPY |
US12618297 |
2009-11-13 |
US20100230617A1 |
2010-09-16 |
KENNETH GALL |
Among other things, an accelerator is mounted on a gantry to enable the accelerator to move through a range of positions around a patient on a patient support. The accelerator is configured to produce a proton or ion beam having an energy level sufficient to reach any arbitrary target in the patient from positions within the range. The proton or ion beam passes essentially directly from the accelerator to the patient. In some examples, the synchrocyclotron has a superconducting electromagnetic structure that generates a field strength of at least 6 Tesla, produces a beam of particles having an energy level of at least 150 MeV, has a volume no larger than 4.5 cubic meters, and has a weight less than 30 Tons. |
182 |
Methods and Systems for Treating Cancer Using External Beam Radiation |
US12572265 |
2009-10-01 |
US20100102244A1 |
2010-04-29 |
George Zdasiuk; James Clayton; Josh Star-Lack; David Humber; Gary Virshup; Michael C. Green |
A radiation system employs magnetic field to move particle beams and radiation sources. The radiation system includes a source operable to produce a particle beam, a scanning magnet operable to scan the particle beam, and a target configured to be impinged by at least a portion of the scanned particle beam to produce radiation. |
183 |
FAST ELECTROMAGNET DEVICE |
US12518704 |
2007-07-04 |
US20100060206A1 |
2010-03-11 |
Toshiyuki Oki; Takahisa Itahashi; Yoshitaka Kuno |
A fast electromagnet device (140) receives a high voltage from a pulse power supply through a coaxial cable and excites an electromagnet at high speed, so as to bend a charged particle beam. The fast electromagnet device (140) includes a kicker magnet (150) and an auxiliary circuit (160). The kicker magnet (150) is equivalent to a circuit element of a lumped constant circuit, is formed with a space penetrating in the traveling direction of the charged particle beams, instantaneously generates a magnetic field in the penetrated space with a high voltage applied, and bends the charged particle beams passing through the penetrated space. The auxiliary circuit (160) constitutes a matching circuit in combination with the kicker magnet (150), so that the input impedance of the matching circuit and the characteristic impedance of the coaxial cable connected to the input terminal of the matching circuit are matched. |
184 |
MAGNETIC FIELD CONTROL METHOD AND APPARATUS USED IN CONJUNCTION WITH A CHARGED PARTICLE CANCER THERAPY SYSTEM |
US12545815 |
2009-08-22 |
US20090309520A1 |
2009-12-17 |
Vladimir Balakin |
The invention comprises a charged particle beam acceleration, extraction, and/or targeting method and apparatus used in conjunction with charged particle beam radiation therapy of cancerous tumors. Novel design features of a synchrotron are described. Particularly, turning magnets, edge focusing magnets, concentrating magnetic field magnets, winding and control coils, flat surface incident magnetic field surfaces, and extraction elements are described that minimize the overall size of the synchrotron, provide a tightly controlled proton beam, directly reduce the size of required magnetic fields, directly reduces required operating power, and allow continual acceleration of protons in a synchrotron even during a process of extracting protons from the synchrotron. |
185 |
Coil Magnets With Constant or Variable Phase Shifts |
US12470328 |
2009-05-21 |
US20090289753A1 |
2009-11-26 |
Rainer Meinke |
A wiring assembly having a conductor positioned about an axis in a helical-like configuration to provide a repetitive pattern which rotates around the axis. In one embodiment, when a current passes through the conductor, a magnetic field having an orientation orthogonal to the axis changes direction as a function of position along the axis. |
186 |
PARTICLE BEAM THERAPY SYSTEM |
US12427011 |
2009-04-21 |
US20090289194A1 |
2009-11-26 |
Kazuyoshi SAITO |
A particle beam therapy system that is capable of irradiating a target area with an irradiation beam suitable for a particle beam therapy using a spot scanning method includes a synchrotron, a beam transport system and an irradiation device. The beam transport system is provided with a beam interrupting device adapted to block supply of a charged particle beam to the irradiation device. The beam interrupting device has a beam shielding magnet, an exciting power supply for the beam shielding magnet and a beam dump. The beam transport system has a bending magnet. The beam shielding magnet is provided on an inlet side of the bending magnet. The beam dump is provided on an outlet side of the bending magnet. A controller controls the exciting power supply to control the timing of an operation of the beam shielding magnet. |
187 |
CIRCULAR ACCELERATOR |
US12277861 |
2008-11-25 |
US20090256501A1 |
2009-10-15 |
Hirofumi TANAKA; Takashi Hifumi; Katsuhisa Yoshida; Kazuo Yamamoto; Yoichi Kuroda |
In a circular accelerator, a magnetic pole edge portion of a bending electromagnet into and from which a charged particle beam enters and exits is provided with endpacks. A first protrusion is provided at that part of each end pack which is radially outside the equilibrium orbit of a center energy beam, while a second protrusion is provided at that part of each end pack which is radially inside the equilibrium orbit of the center energy beam. The shapes of the first and second protrusions are set so that the betatron oscillation numbers of beams of different acceleration energies may be held constant or become linear to the energies. In case of emitting the charged particle beam out of the circular accelerator, the change of a tune attributed to the change of the beam orbit can be statically corrected, the tune is linearly changed, and an adjustment of the emission of the beam becomes easy. |
188 |
Permanent magnet for particle beam accelerator and magnetic field generator |
US10524314 |
2004-02-20 |
US07570142B2 |
2009-08-04 |
Ken Makita; Eiji Sugiyama; Masaaki Aoiki; Kaichi Murakami; Tadamichi Kawakubo; Eiji Nakamura |
A permanent magnet for a particle accelerator and a magnetic field generator, in which Nd—Fe—B based magnets are used but are not demagnetized so easily even when exposed to a radiation, are provided. A permanent magnet for a particle accelerator is used in an environment in which the magnet is exposed to a radiation at an absorbed dose of at least 3,000 Gy. The magnet includes R (which is at least one of the rare-earth elements), B, TM (which is at least one transition element and includes Fe) and inevitably contained impurity elements. The magnet is a sintered magnet that has been magnetized to a permeance coefficient of 0.5 or more and that has a coercivity HcJ of 1.6 MA/m or more. |
189 |
Conductor Assembly Formed About A Curved Axis |
US12133613 |
2008-06-05 |
US20090174517A1 |
2009-07-09 |
Rainer Meinke |
A conductor assembly of the type which, when conducting current, generates a magnetic field or in which, in the presence of a changing magnetic field, a voltage is induced. In the assembly a first layer, tubular in shape, is formed about an axis. The axis includes a curved portion along which a conductor may be positioned to define a first conductor path. The first layer also includes a curved portion having a shape that includes a curve extending along the curved portion of the axis. A first conductor is arranged about the curved portion of the first layer in a first helical configuration including a curved segment, helical in shape and formed about the curved portion of the axis. The configuration is capable of sustaining a magnetic field having multipole components oriented in directions transverse to the axis. |
190 |
Conductor Assembly Having An Axial Field In Combination With High Quality Main Transverse Field |
US12133760 |
2008-06-05 |
US20090085710A1 |
2009-04-02 |
Rainer Meinke |
A conductor assembly of the type which, when conducting current, generates a magnetic field or in which, in the presence of a changing magnetic field, a voltage is induced. In one series of embodiments a plurality of coil rows comprise conductor in a helical wiring pattern formed about an axis. One of the coil rows is positioned a radial distance R from the axis. For each of the coil rows the helical pattern comprises conductor loops each exhibiting a tilt in the same direction with respect to a plane transverse to the axis, the assembly capable of generating an axial field component and a transverse field component. |
191 |
Undulator |
US10597352 |
2005-01-18 |
US20080231215A1 |
2008-09-25 |
Hideo Kitamura; Toru Hara; Takashi Tanaka; Tsutomu Kohda; Yutaka Matsuura |
An undulator comprises a first magnetic circuit (11) for forming a periodic magnetic field, a first support body (21) for supporting the first magnetic circuit (11), a second magnetic circuit (12) arranged opposite to the first magnetic circuit (11), for forming a periodic magnetic field, a second support body (22) for supporting the second magnetic circuit (12), a space (13) formed between the oppositely arranged first magnetic circuit (11) and the second magnetic circuit (12), for passing an electron beam, a vacuum chamber (1) for vacuum-sealing the first magnetic circuit (11) and the second magnetic circuit (12), and a refrigerant passing tube (30) for cooling a permanent magnet (m) constituting the first magnetic circuit (11) and the second magnetic circuit (12) below the room temperature. |
192 |
Particle beam irradiation apparatus, treatment planning unit, and particle beam irradiation method |
US11646298 |
2006-12-28 |
US07425717B2 |
2008-09-16 |
Koji Matsuda; Takahide Nakayama |
A particle beam irradiation apparatus includes a synchrotron, two scanning electromagnets, an beam delivery apparatus for outputting an ion beam extracted from the synchrotron, and an accelerator and transport system controller, and a scanning controller. These controllers stop the output of the ion beam from the beam delivery apparatus; in a state where the output of the ion beam is stopped, change the irradiation position of the ion beam by controlling the scanning electromagnets; and after this change, control the scanning electromagnets to start the output of the ion beam from the beam delivery apparatus and to perform irradiations of the ion beam to at least one irradiation position a plurality of times based on treatment planning information. |
193 |
Charged Particle Beam Irradiator and Rotary Gantry |
US11792940 |
2005-10-31 |
US20080006776A1 |
2008-01-10 |
Takuji Furukawa; Kouji Noda |
A charged particle beam 2 which enters a final bending electromagnet 7 after traveling through quadrupole electromagnets 4, 5, 6 travels through the final bending electromagnet 7 in an arc shape path by increasing or decreasing a bending magnetic field generated in the final bending electromagnet 7, with a pre-determined period for example and is scanned in an X-direction. The charged particle beam 2 scanned in the X-direction is scanned in a Y-direction while traveling through a Y-direction Wobbler electromagnet 8. Consequently, the charged particle beam 2 is scanned in the X-direction and the Y-direction, and the target 9 is irradiated with the charged particle beam 2 so that a round field is drawn, for example. |
194 |
Ion beam delivery equipment and an ion beam delivery method |
US11714219 |
2007-03-06 |
US20070158592A1 |
2007-07-12 |
Kazuo Hiramoto; Hiroshi Akiyama; Masaki Yanagisawa; Hisataka Fujimaki; Alfred Smith; Wayne Newhauser |
The invention is intended to increase the number of patients treatable using one wheel having a thickness varied in the rotating direction to change energy of an ion beam passing the wheel. Ion beam delivery equipment for irradiating an ion beam to a patient for treatment comprises a beam generator for producing and accelerating the ion beam, an beam delivery nozzle including a range modulation wheel which has a predetermined thickness distribution in the rotating direction and is rotated on a travel passage of the ion beam generated from the beam generator to control a range of the ion beam, and an irradiation controller for controlling the beam producing and accelerating operation of the beam generator in accordance with the phase of rotation of the range modulation wheel. |
195 |
Undulator and method of operation thereof |
US11363427 |
2006-02-27 |
US07129807B2 |
2006-10-31 |
Robert Rossmanith; Uwe Schindler |
In an undulator for the generation of synchrotron radiation from a particle beam introduced into the undulator, two partial undulators are provided each comprising a conductor of superconductive material which, when a current is conducted therethrough, generates an undulator field that extends perpendicularly to the current flow, and the superconductive conductors are arranged in the individual partial undulators such that the undulator fields generated are not parallel, whereby, by controlling the energization of the two partial undulators, the polarization direction of the synchrotron radiation can be adjusted without mechanical movements. |
196 |
Particle beam irradiation apparatus, treatment planning unit, and particle beam irradiation method |
US10842463 |
2004-05-11 |
US07102144B2 |
2006-09-05 |
Koji Matsuda; Takahide Nakayama |
A particle beam irradiation apparatus includes a synchrotron, two scanning electromagnets, an beam delivery apparatus for outputting an ion beam extracted from the synchrotron, and an accelerator and transport system controller, and a scanning controller. These controllers stop the output of the ion beam from the beam delivery apparatus; in a state where the output of the ion beam is stopped, change the irradiation position of the ion beam by controlling the scanning electromagnets; and after this change, control the scanning electromagnets to start the output of the ion beam from the beam delivery apparatus and to perform irradiations of the ion beam to at least one irradiation position a plurality of times based on treatment planning information. |
197 |
Particle therapy system |
US11185717 |
2005-07-21 |
US07060997B2 |
2006-06-13 |
Tetsuro Norimine; Masumi Umezawa; Kazuo Hiramoto |
A particle therapy system is provided which can simply and quickly correct a beam orbit. In a particle therapy system provided with an irradiation facility comprising a first beam transport system for receiving a beam and transporting the beam to the patient side, and an irradiation nozzle for forming an irradiation field of the beam, the particle therapy system comprises first beam position monitors for detecting a position upstream of the irradiation nozzle at which the beam passes, second beam position monitors for detecting a position downstream of the irradiation nozzle at which the charged-particle beam passes, and first and second steering magnets. Correction bending amounts for causing the beam to be coincident with a predetermined orbit after the correction are determined in accordance with detected results from the first and second beam position monitors, and first and second steering magnets are excited under control so that the determined correction bending amounts are obtained. |
198 |
Charged particle buncher |
US10641189 |
2003-08-14 |
US07045792B2 |
2006-05-16 |
Victor Carl Parr; Stephen Paul Thompson; Mark Duncan Mills |
A charged particle buncher with a series of spaced apart electrodes 1 arranged to generate a shaped electric field, the series comprising a first electrode 1a, a last electrode 1b and one or more intermediate electrodes, wherein the shaped electric field is generated substantially without free charges being transferred onto or away from the intermediate electrode or electrodes. The first and last electrodes may be connected to means for transferring charged on to or off the electrode. The first, intermediate and last electrodes may be connected in serried with capacitors. |
199 |
Concentric tilted double-helix dipoles and higher-order multipole magnets |
US10067487 |
2002-02-05 |
US06921042B1 |
2005-07-26 |
Carl L. Goodzeit; Rainer B. Meinke; Millicent Ball |
Concentric tilted double-helix magnets, which embody a simplified design and construction method for production of magnets with very pure field content, are disclosed. The disclosed embodiment of the concentric tilted double-helix dipole magnet has the field quality required for use in accelerator beam steering applications, i.e., higher-order multipoles are reduced to a negligibly small level. Magnets with higher multipole fields can be obtained by using a simple modification of the coil winding procedure. The double-helix coil design is well-suited for winding with superconducting cable or cable-in-conduit conductors and thus is useful for applications that require fields in excess of 2 T. The coil configuration has significant advantages over conventional racetrack coils for accelerators, electrical machinery, and magneto-hydrodynamic thrusting devices. |
200 |
Apparatus for pre-acceleration of ion beams used in a heavy ion beam application system |
US11037572 |
2005-01-18 |
US20050134204A1 |
2005-06-23 |
Alexander Bechthold; Ulrich Ratzinger; Alwin Schempp; Bernhard Schlitt |
The present invention relates to an apparatus for pre-acceleration of ions and optimized matching of beam parameters used in a heavy ion application comprising a radio frequency quadruple accelerator (RFQ) having two mini-vane pairs supported by a plurality of alternating stems accelerating the ions from about 8 keV/u to about 400 keV/u and an intertank matching section for matching the parameters of the ion beam coming from the radio frequency quadruple accelerator (RFQ) to the parameters required by a subsequent drift tube linear accelerator (DTL). |