子分类：
| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 21 | Elektronenstrahl-Vorrichtung | EP93101880.8 | 1993-02-06 | EP0563543A1 | 1993-10-06 | Mathews, Hans-Günter,Dr.; Schminke, Wolfram, Dr. |
Bei einer Elektronenstrahl-Vorrichtung mit einer Kathode (1), in welcher ein sich entlang einer Strahlachse (5) ausbreitender Hochleistungs-Elektronenstrahl erzeugt wird, einer in Richtung der Strahlachse (5) hinter der Kathode (1) angeordneten Anode (3), und einem in Richtung der Strahlachse (5) hinter der Anode (3) angeordneten Kollektor (4) zur Abbremsung der Elektronen des Elektronenstrahls, wird der Kollektor (4) aus mehreren in Richtung der Strahlachse (5) hintereinander angeordneten Kollektorstufen (6) aufgebaut, die sich jeweils auf einem stufenweise abgesenkten Potential befinden. Für die Speisung ist eine Hochspannungs-Gleichstromversorgung (13) vorgesehen, die aus einer Mehrzahl von gleichartigen Schaltstufen (S1,..,S6) besteht, die jeweils als schaltbare Mittelspannungsquellen ausgebildet und mit ihren Ausgängen in Serie geschaltet sind. Die abgestuften Potentiale der Kollektorstufen (6) werden durch entsprechende Abgriffe zwischen den Schaltstufen (S1,..,S6) der Hochspannungs-Gleichstromversorgung (13) bereitgestellt. |
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| 22 | Electrostatic ion accelerator | EP87307575.8 | 1987-08-27 | EP0300105A3 | 1989-08-09 | Shefer, Ruth; Klinkowstein,Robert Edward |
A high current (0.2 to at least 2 milliamperes), low-energy (2.2 to 4 MV) ion beam is generated and is utilized to produce clinically significant quantities of medical isotopes useful in applications such as positron emission tomography. For a preferred embodiment, a tandem accelerator is utilized. Negative ions (202) generated by a high current negative-ion source (200) are accelerated by an electrostatic accelerator in which the necessary high voltage is produced by a solid state power supply. The accelerated ions then enter a stripping cell (212) which removes electrons from the ions, converting them into positive ions. The positive ions (218) are then accelerated to a target which is preferably at ground potential. For a preferred embodiment, the solid state power supply utilized to develop the required voltages is a cascade rectifier power supply (206) which is coaxial with the accelerator between the ion source (200) and the stripper (212), and is designed to have a voltage gradient which substantially matches the maximum voltage gradient of the accelerator. |
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| 23 | 車載アンテナ装置 | JP2015085550 | 2015-12-18 | JPWO2017046972A1 | 2018-07-12 | 水野 浩年; 後藤 正幸; 横田 勇介 |
| 電子機器等から放射される電磁ノイズを抑制して、ノイズに起因するラジオ、テレビ等の受信障害を防止可能な車載アンテナ装置を提供する 取付手段を介して車体に固定されるアンテナベース2と、これに被せられるアンテナケースと、アンテナベース2とアンテナケースとで囲まれた内部空間に設けられるアンテナエレメント5及び電子機器としてのカメラモジュール10とを備え、カメラモジュール10の回路基板50を囲むようにカメラモジュール筐体40でシールドしている。 |
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| 24 | High-current DC proton accelerator | JP2011523098 | 2009-08-11 | JP5472944B2 | 2014-04-16 | クレランド，マーシャル，アール．; ギャロウェー，リチャード，エー．; デサント，レオナルド; ヨンゲン，イヴ |
| 25 | Electrostatic ion accelerator | JP24774987 | 1987-09-30 | JPS6435898A | 1989-02-06 | ROBAATO EDOWAADO KURINKOSUTAIN; RUSU SHIIFUAA |
| PURPOSE: To provide an ion accelerator capable of outputting a current higher than a general low-energy accelerator by generating isotopes for medical use for positron emission tomographic X-ray radiograph by an ion beam of about 0.2mA and 1MV. CONSTITUTION: An accelerating column 208 is housed within a pressurizing chamber 222, a vacuum pump connected to T-shaped tube fittings 201, 220 provided on both end parts of the pressurizing chamber 222 is sued to produce high vacuum inside the column 208, and an ion beam of 0.2mA accelerated at 1MV is emitted from a power source 200 to a target set to a ground potential through the fitting 201, the column 208 and the fitting 220. On the inlet side of the column 208, the beam passing in the inner part is made into a low-energy negative ion beam by a cascade rectifier circuit 206 enclosing the column 208, and the beam is changed into a positive ion beam 218 by a stripping cell 212 which is enclosed by a high-voltage terminal 210. On the outlet side, it is accelerated by use of an accelerator column 216 and emitted toward the target. A high-pressure insulating gas 204 such as SF6 is sealed in the pressurizing chamber 222. | ||||||
| 26 | JPS6236360B2 - | JP50025579 | 1979-12-26 | JPS6236360B2 | 1987-08-06 | DOMITORIEFU SUTANISURAFU PYOOT; RAJIN GENNADEII IWANOITSUCHI |
| 27 | JPS56501818A - | JP50025580 | 1979-12-26 | JPS56501818A | 1981-12-10 | |
| 28 | JPS5613108B2 - | JP10424177 | 1977-09-01 | JPS5613108B2 | 1981-03-26 | |
| 29 | JPS55500307A - | JP50025579 | 1979-12-26 | JPS55500307A | 1980-05-29 | |
| 30 | CONNECTOR HOUSING APPARATUS AND INTER-CONNECTOR CONNECTING SYSTEM | US15052073 | 2016-02-24 | US20160248204A1 | 2016-08-25 | Toru SASAKI; Shuuji KAMENO; Junji BABA |
| A connector housing apparatus includes a main body section that has a plurality of connectors confronting a plurality of external connectors of an external housing and a moving guide section that guides movement of the main body section toward the external housing. The moving guide section has a latching section that latches the moving guide section on the external housing. The main body section is connected to the moving guide section so as to be movable in a fitting direction of the plurality of connectors. The latching section latches the moving guide section on a position at which the plurality of connectors are fitted to the plurality of external connectors. The main body section moves along the moving guide section in the fitting direction of the plurality of connectors, and thereby the plurality of connectors are fitted to the plurality of external connectors. | ||||||
| 31 | High-current dc proton accelerator | US13408069 | 2012-02-29 | US08508158B2 | 2013-08-13 | Marshall R. Cleland; Richard A. Galloway; Leonard DeSanto; Yves Jongen |
| A dc accelerator system able to accelerate high currents of proton beams at high energies is provided. The accelerator system includes a dc high-voltage, high-current power supply, an evacuated ion accelerating tube, a proton ion source, a dipole analyzing magnet and a vacuum pump located in the high-voltage terminal. The high-current, high-energy dc proton beam can be directed to a number of targets depending on the applications such as boron neutron capture therapy BNCT applications, NRA applications, and silicon cleaving. | ||||||
| 32 | Method and apparatus for accelerating charged particles | US10800583 | 2004-03-15 | US07015661B2 | 2006-03-21 | Sergey A. Korenev |
| A method and apparatus for accelerating charged particles. The charged particles accelerate as they travel through electric fields produced by a plurality of accelerating elements having first and second electrode plates. A magnetic field produced by a pair of magnets causes the charged particles to travel in a generally circular orbit. | ||||||
| 33 | Nuclear decay laser and method | US09303480 | 1999-04-30 | US06331774B1 | 2001-12-18 | Henry J. Stern |
| A nuclear decay laser that produces a stream of nuclear decay particles and/or photons of electromagnetic radiation. The stream of nuclear decay particles and/or photons is produced by subjecting radioactive materials to an external magnetic field which causes the radioactive nuclei to align with and precess around the external magnetic field vector. The precessing radioactive nuclei are then subjected to Radio Frequency (RF) pulses tuned to the Larmor frequency of the precessing nuclei which causes the nuclei to flip out of the plane of the external magnetic field vector into the X-Y plane. A refocusing RF pulse is then applied to the radioactive material which brings all of the magnetic moments of the flipped radioactive nuclei into phase. This can also be achieved with MRI gradient echo technology. When the initial RF pulse is discontinued, the flipped radioactive nuclei undergo T1 or spin-lattice relaxation which occurs when the radioactive nuclei relax back into phase with the external magnetic field vector during the process of T1 relaxation. The radioactive nuclei undergo accelerated coordinated decay with emission of a laser type pulse of electromagnetic radiation or particles according to the decay scheme of the radioactive nucleus. Alternatively, a ray of energy and/or particles is released when radioactive nuclei capable of undergoing fission experience a coordinated, accelerated fission reaction achieved when the refocusing RF pulse or gradient echo brings the radioactive nuclei into a coherent phase. The release of energy and/or particles can be focused and used in medical treatment and imaging, industrial and military applications, and for the production of energy. In addition, these methods of accelerating nuclear decay can be used to treat unwanted radioactive materials to background radiation levels providing for a way of disposing of unwanted nuclear waste. | ||||||
| 34 | Electrostatic ion accelerator | US643855 | 1991-01-18 | USRE34575E | 1994-04-05 | Robert E. Klinkowstein; Ruth Shefer |
| A high current (0.2 to at least 2 milliamperes), low-energy (2.2 to 4 MV) ion beam is generated and is utilized to produce clinically significant quantities of medical isotopes useful in applications such as positron emission tomography. For a preferred embodiment, a tandem accelerator is utilized. Negative ions generated by a high current negative-ion source are accelerated by an electrostatic accelerator in which the necessary high voltage is produced by a solid state power supply. The accelerated ions then enter a stripping cell which removes electrons from the ions, converting them into positive ions. The positive ions are then accelerated to a target which is preferably at ground potential. For a preferred embodiment, the solid state power supply utilized to develop the required voltages is a cascade rectifier power supply which is coaxial with the accelerator between the ion source and the stripper, and is designed to have a voltage gradient which substantially matches the maximum voltage gradient of the accelerator. | ||||||
| 35 | Portable radiography system using a relativistic electron beam | US99850 | 1987-09-22 | US4924485A | 1990-05-08 | Robert F. Hoeberling |
| A portable radiographic generator is provided with an explosive magnetic flux compression generator producing the high voltage necessary to generate a relativistic electron beam. The relativistic electron beam is provided with target materials which generates the desired radiographic pulse. The magnetic flux compression generator may require at least two conventional explosively driven generators in series to obtain a desired output voltage of at least 1 MV. The cathode and anode configuration of the diode are selected to provide a switching action wherein a high impedance load is presented to the magnetic flux compression generator when the high voltage is being generated, and thereafter switching to a low impedance load to generate the relativistic electron beam. Magnetic flux compression generators can be explosively driven and provided in a relatively compact, portable form for use with the relativistic x-ray equipment. | ||||||
| 36 | Particle accelerator employing transient space charge potentials | US160384 | 1988-02-25 | US4899084A | 1990-02-06 | Richard F. Post |
| The invention provides an accelerator for ions and charged particles. The plasma is generated and confined in a magnetic mirror field. The electrons of the plasma are heated to high temperatures. A series of local coils are placed along the axis of the magnetic mirror field. As an ion or particle beam is directed along the axis in sequence the coils are rapidly pulsed creating a space charge to accelerate and focus the beam of ions or charged particles. | ||||||
| 37 | Electrostatic ion accelerator | US72883 | 1987-07-20 | US4812775A | 1989-03-14 | Robert E. Klinkowstein; Ruth Shefer |
| A high current (0.2 to at least 2 milliamperes), low-energy (2.2 to 4 MV) ion beam is generated and is utilized to produce clinically significant quantities of medical isotopes useful in applications such as positron emission tomography. For a preferred embodiment, a tandem accelerator is utilized. Negative ions generated by a high current negative-ion source are accelerated by an electrostatic accelerator in which the necessary high voltage is produced by a solid state power supply. The accelerated ions then enter a stripping cell which removes electrons from the ions, converting them into positive ions. The positive ions are then accelerated to a target which is preferably at ground potential. For a preferred embodiment, the solid state power supply utilized to develop the required voltages is a cascade rectifier power supply which is coaxial with the accelerator between the ion source and the stripper, and is designed to have a voltage gradient which substantially matches the maximum voltage gradient of the accelerator. | ||||||
| 38 | Energy-stable accelerator with needle-like source and focused particle beam | US379736 | 1982-05-19 | US4555666A | 1985-11-26 | Frederick W. Martin |
| A high voltage particle accelerator and an energy analyzer fed back to the accelerator, in which the beam of extremely small diameter from a particle source of the field-emission or field-ionization type and the energy analyzer function to produce precisely defined high voltages; use of such an accelerator and focusing lenses to produce a microbeam with reduced chromatic aberration; and production of a microbeam by use of such an accelerator and focusing lenses of the achromatic quadrupole type, further compensated for aperture aberration. | ||||||
| 39 | Area beam electron accelerator having plural discrete cathodes | US725334 | 1976-09-21 | US4079328A | 1978-03-14 | Marshall Robert Cleland; Kennard Harold Morganstern; Peter Ronald Hanley |
| An area beam of electrons capable of delivering large doses of electron irradiation at small dose rates and having a predetermined distribution pattern is provided by an electron accelerator comprising plural discrete cathodes positioned as required to achieve the desired pattern. An individual emission control is provided for the filament of each cathode. In a preferred embodiment plural cathodes are movably mounted in a row extending transversely of the transport path of material to be irradiated, a plurality of such rows being positioned along the direction of transport. | ||||||
| 40 | Linear particle accelerator with coast through shield | US3761828D | 1970-12-10 | US3761828A | 1973-09-25 | POLLARD J |
| Charged particles injected into an energy beam, are accelerated by electric fields established in gaps between tubular electrodes through which the particles pass. Alternate gaps between the electrodes are enclosed by tubular shields through which the particles coast between the accelerating fields. The electrodes are charged by d.c. sources of opposite polarity.
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