| 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 | Superconducting, fast rise-time voltage source | US102076 | 1979-12-10 | US4370568A | 1983-01-25 | Robert M. Lumley |
| A pulse generator comprises a toroid (11) of a superconducting material such as Niobium on a glass or ceramic substrate (12). A cryogenic source such as liquid helium cools the toroid to within a few degrees of absolute zero and a perpetually circulatory current is set up in the toroid. A laser beam is fired at the toroid to cause localized heating and the resultant current drop due to the material resistance causes an output pulse to be induced in an adjacent current winding (14). | ||||||
| 62 | APPARATUS AND METHOD FOR DETERMINING MOLECULAR STRUCTURE | PCT/US2013/052772 | 2013-07-30 | WO2014022426A1 | 2014-02-06 | KONG, Wei; BECKMAN, Joseph; VOINOV, Valery, G.; FREUND, William, M. |
Certain disclosed embodiments concern a method and an apparatus for determining molecular structure. One embodiment comprises producing sample ions from a sample, cooling molecules of the sample ions by either embedding sample ions in superfluid droplets, such as superfluidic helium droplets, or subjecting sample ions in a cooled ion trap, to a selected temperature approaching absolute zero. Plural cooled sample ions confined in a diffraction zone are oriented using a laser, and a diffraction image is produced from oriented sample ions using an electron beam. Molecular structure is determined using collected images. Embodiments of an apparatus for determining molecular structure also are disclosed. The apparatus operation, data accumulation and processing are controlled by software. The software can directly calculate electron density maps without using heavy atom derivatives or multi- wavelength anomalous dispersion phasing methods. |
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| 63 | CATALYST-REACTIVE IONIC TOOTHBRUSH | PCT/KR2011002509 | 2011-04-11 | WO2011129559A4 | 2012-04-12 | YOON SEUNG-YONG |
| The present invention relates to a catalyst-reactive ionic toothbrush, and more particularly, to a catalyst ionic toothbrush capable of effectively improving the sanitary conditions of teeth and mouth by means of a redox reaction by exciting conduction electrons when heat, light, or DC current is applied to impurity semiconductors obtained from metal oxides which protrude from one side of a toothbrush handle and inserted into a communication hole of a brushing part. The present invention provides a catalytic ionic toothbrush including impurity semiconductors having a plurality of band gaps comprising different materials which can be responsive to a number of various conditions such as absolute zero temperature, finite temperature, outdoor temperature, indoor temperature, body temperature, in-mouth temperature, infrared light, visible light, ultraviolet rays, and DC power. | ||||||
| 64 | ZWEISEITIGER REFLEKTOR UND ZWEISEITIGES ZIELOBJEKT | PCT/EP2006/009046 | 2006-09-18 | WO2007036309A1 | 2007-04-05 | WIEBKING, Mirko; SCHORR, Christian; HINDERLING, Jürg |
Ein zweiseitiger Reflektor (l',l'') zur Reflexion eines beugungsbegrenzten optischen Strahlenbündels ist erfindungsgemäss so ausgebildet, dass ein flächiges erstes und zweites Reflexionselement, wie beispielsweise eine Reflexfolie und ein Katzenaugen-Reflektor (3) , bezüglich einer Referenzachse (RA) des Reflektors derart angeordnet sind, dass sich aus der gezielten Wahl der Eigenschaften des ersten bzw. zweiten Reflexionselements sowie der Anordnung derselben bezüglich der Referenzachse (RA) für eine Distanzmessung eine absolute Additionskonstante von Null ergibt. Die Distanzmessung entspricht also im Wesentlichen einer Distanzmessung auf eine natürliche Oberfläche. Damit kann die Distanzmessung ohne Zusatzkorrektur direkt auf die Referenzachse (RA) bezogen werden. |
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| 65 | DESIGN AND FABRICATION OF SYNTHETIC SUPERCONDUCTORS | PCT/US1989003063 | 1989-07-17 | WO1990001218A1 | 1990-02-08 | ARTHUR D. LITTLE, INC.; RONA, Mehmet |
| Synthetic superconductors adapted for superconduction at temperatures substantially above those temperatures near absolute zero where conventional superconduction has been observed. The superconductors comprise alternating and spaced conducting and lesser conducting strata in a relationship which induces superconductivity as a result of the interplay between the conducting and lesser conducting strata. The type, nature and dielectric spacing of the conducting and lesser conducting strata produce charge carrier pairing or grouping in the lesser conducting strata by electrostatic forces. The grouped charge carriers provide the superconducting characteristic to the superconductors. The strata may be produced by layered deposition or plating. | ||||||
| 66 | APPARATUS AND METHOD FOR GRANULATING A MATERIAL | PCT/ZA1999/000112 | 1999-10-28 | WO00024518A1 | 2000-05-04 | |
| An apparatus for processing material comprises a cyclone chamber, an impeller suction fan for creating a cyclone within the chamber, feed means for introducing material into the chamber batchwise and means for collecting the processed material, the impeller and/or the inlet to the chamber being adapted to reduce the temperature of water in the chamber to a temperature approaching absolute zero, under which conditions of temperature and vacuum the material to be processed is subjected to forces which result in the disassociation of bonding within the material, the chamber being further adapted to contain any explosions or implosions which may occur and to ensure any recombination of hydrogen and oxygen to form water before the outlet. | ||||||
| 67 | DESIGN AND FABRICATION OF SYNTHETIC SUPERCONDUCTORS | PCT/US1993008167 | 1993-08-30 | WO1995001870A1 | 1995-01-19 | ARTHUR D. LITTLE, INC.; RONA, Mehmet |
| Synthetic superconductors adapated for superconduction at temperatures substantially above those near absolute zero where conventional superconduction has been observed. The superconductors comprise alternating and spaced conducting (20, 22) and lesser conducting (24) strata in a relationship which induces superconductivity as a result of the interplay between the conducting (20, 22) and lesser conducting (24) strata. The type, nature and dielectric spacing (26, 28) of the conducting (20, 22) and the lesser conducting (24) strata produce charge carrier pairing or grouping in the lesser conducting (24) strata by electrostatic forces. The grouped charge carriers provide the superconducting characteristic to the superconductors. The strata (20, 22, 24, 26, 28) may be produced by layered deposition or plating. | ||||||
| 68 | 粒化材料的設備 | TW088119406 | 1999-11-06 | TW445175B | 2001-07-11 | 道格拉斯佛比斯 |
| 一種用來處理材料的設備，其包含一個漩渦室、一個用來在漩渦室內生成一漩渦的動葉輪吸入風扇、一個用來逐批導引材料進入該漩渦室的饋給機構，以及一個用來收集該完成處理材料的機構，該動葉輪及/或通達該漩渦室入口係用於降低在漩渦室內之水溫至一趨近絕對零度的溫度;在此溫度與真空的條件下，欲進行處理的材料係受到可使材料內之鍵結分解的力量所影響，且該漩渦室更可用以承受任何可能發生之爆炸或內爆裂，確定在出口之前氫或氧組合成水的任何重組。 | ||||||
| 69 | 気体吸蔵材 | JP2014033413 | 2014-02-24 | JP2015157255A | 2015-09-03 | 林 秀光; 向江 友佑 |
| 【課題】従来より優れた気体の取り出し可能量を有する気体吸蔵材を提供する。 【解決手段】少なくとも1種の金属元素を含む金属クラスターと、前記金属クラスターを架橋し、1つ以上の芳香環を含む1つ以上の多座配位子と、を有する金属有機構造体と、前記金属元素と異なる金属元素であって、前記金属有機構造体に担持される添加金属元素と、を有し、前記添加金属元素が担持された金属有機構造体は、気体吸着量に応じて小細孔構造と大細孔構造との間で構造変化するものであり、絶対零度における前記小細孔構造のエネルギーと前記大細孔構造のエネルギーとの差が−50kL/mol以上〜0kJ/mol未満である気体吸蔵材。 【選択図】なし |
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| 70 | Amplifier circuit | JP19845789 | 1989-07-31 | JPH0362709A | 1991-03-18 | AOKI HIDEHIKO |
| PURPOSE: To make the temperature coefficient of an output voltage zero and to eliminate an output voltage fluctuation due to a temperature change by selecting the sum of voltages caused in a voltage path comprising a PN junction formed between a reference level point and an output terminal and a resistor in which a voltage proportional to a thermal voltage VT is generated to be a multiple of number of PN junctions having an Si energy band gap voltage at the absolute zero degree. CONSTITUTION: The sum of voltages VR 4+VF(Q 4)+VBE(Q 3) in a voltage path of V cc → R 4 → Q 4 → base of Q 3 → emitter of Q 3 → OUT in terms of the absolute sum is selected to be twice an Si (silicon) band gap voltage Vgo in an amplifier circuit in which a voltage path comprising two PN junctions of a diode Q 4 and a base-emitter of a transistor(TR) Q 3 and a resistor R 4 with a voltage proportional to a thermal voltage VT generated therein is formed between an output terminal OUT and a line of power supply VCC. Moreover, the similar effect is obtained by using a Darlington emitter follower circuit comprising the TR Q 3 in place of the diode Q 4. COPYRIGHT: (C)1991,JPO&Japio | ||||||
| 71 | Refrigerant-free refrigerating machine and functional thermal binding body | JP2007246525 | 2007-09-25 | JP2009074774A | 2009-04-09 | YAYAMA HIDEKI |
| <P>PROBLEM TO BE SOLVED: To provide a refrigerant-free refrigerating machine and a functional thermal binding body capable of reaching a very low temperature in a short time by a simple operation, having high operation efficiency and cooling efficiency at low costs, having a simple structure, and being easily maintained. <P>SOLUTION: In the refrigerant-free refrigerating machine and the functional thermal binding body, a columnar first graphite bar 41 made of graphite having heat conductivity rapidly reduced in proportion to power of a temperature toward absolute zero, is disposed between a 40K plate 13 and a 4K plate 14, heat is conducted between the 40K plate 13 and the 4K plate 14 until the first graphite bar 41 reaches a first temperature equilibrium point when a temperature is lowered to 4K, and the 40K plate 13 and the 4K plate 14 are kept in a state of almost thermally separated from each other at the first temperature equilibrium point or less. <P>COPYRIGHT: (C)2009,JPO&INPIT | ||||||
| 72 | Soft magnetic thin film | JP21873785 | 1985-10-01 | JPS6278805A | 1987-04-11 | HAYASHI KAZUHIKO; HAYAKAWA MASATOSHI; OCHIAI YOSHITAKA; MATSUDA HIDEKI; ISHIKAWA OSAMU; IWASAKI HIROSHI; ASO KOICHI |
| PURPOSE: To make the saturated magnetic flux density of the titled soft magnetic thin film higher than that of the Sendust alloy without changing soft magnetic characteristics and the like by a method wherein Fe, Co, Ga and Si are selected as the constituent elements of the soft magnetic thin film, and the compositional ratio of said elements is set within the prescribed range. CONSTITUTION: In order to increase the density of saturated magnetic flux, the composition of the titled soft magnetic thin film is set as Fe xCo yGa aSi b (the compositional ratio of x, y, a and b is indicated by atomic %) taking into consideration of the fact that the point of intersection of the line of magnetostriction λ s=0 with the line of crystal magnetic anisotropy K=0 is to be set closer to the side of Fe high density, and that the rate of reduction of magnetic moment in absolute zero and the addition of Co improves the density of saturated magnetic flux, the corrosion resistance and the abrasion resistance of the soft magnetic thin film. In this compositional ratio, when the adding quantity of Co is too much, the density of saturated magnetic flux and soft magnetic characteristics are deteriorated in inverse proportion to the corrosion resistance and the abrasion resistance. Therefore, the compositional ratio of the material used is set as follows: 65≤x+y≤85.0≤y≤20.1≤a≤35.1≤b≤35, x+y+a+b=100. COPYRIGHT: (C)1987,JPO&Japio | ||||||
| 73 | Sample atmosphere regulator for x-ray apparatus | JP33402894 | 1994-12-16 | JPH08170948A | 1996-07-02 | SAWANO NARITAMI |
| PURPOSE: To simplify and miniaturize a mechanism for adjusting the position of a sample while preventing the positional fluctuations of the sample placed in a specific atmosphere in a sample atmosphere regulator used in an X-ray apparatus. CONSTITUTION: A sample atmosphere regulator is used in an X-ray apparatus detecting X-rays diffracting a sample 4 by an X-ray counter and holds the atmosphere around the sample 4 to a desired state, for example, extremely low temp. near to absolute zero. This regulator is formed by connecting two units, that is, a casing unit 15 and a sample support unit 16. A cooling medium supply system regulating the temp. regulation chamber RT housing the sample 4 to extremley low temp. and a vacuum exhaust system are provided on the side of the casing unit 15 and an X-Y table 41 moving the sample 4 in order to regulate the position thereof and lift mechanisms 37, 38 are provided on the side of the sample support unit 16. COPYRIGHT: (C)1996,JPO | ||||||
| 74 | Absolute type encoder | JP6274389 | 1989-03-15 | JPH02242117A | 1990-09-26 | CHIKAOKA TAKASHI |
| PURPOSE: To enable detection of an absolute angle beyond 360° with high resolutions by storing an absolute angle within 360° mechanically with an angle of rotation and a plurality of revolutions of a code plate as axial position thereof. CONSTITUTION: On a code plate 31, codes 32 made up of a number of transmission type slits storing absolute angles within 360° are arranged being aligned circumferentially. A plurality revolutions of a rotating shaft 14 are stored mechanically as axial current position of the code plate 31. When a power source is closed, a fine angle detector 41 determines the absolute value within one rotation of the code plate 31 instantaneously and a coarse angle detector 51 determines an absolute angle of (n) rotation × 360° from absolute zero° of the shaft 14 from the current position of the code plate 31. Then, an angle detection means 61 adds outputs of the detectors 41 and 51 to the results. This enables mechanical detection of the absolute angle beyond 360° with high resolutions. COPYRIGHT: (C)1990,JPO&Japio | ||||||
| 75 | Heater control device for oxygen concentration sensor | JP2034284 | 1984-02-06 | JPS60164241A | 1985-08-27 | KURAOKA HIROAKI |
| PURPOSE:To prevent the overheating of a heater and to prevent the wire breakdown of the heater, by controlling power to the heater with the temperature of the heater for oxygen concentration sensor being computed. CONSTITUTION:The resistance value of a heater (a) that is enclosed in an oxygen concentration sensor (b), which detects the oxygen concentration in exhaust gas, the number of rotation of an internal combustion engine, and exhaust gas temperature are detected by respective detecting means M1-M3. When the exhaust gas and the heater reach a thermal equilibrium, the initial resistance value of the heater at the absolute zero degree is computed from the exhaust gas temperature, the resistance of the heater and the temperature coefficient of the heater, which is memorized beforehand. The temperature of the heater is computed from the resistance value of the heater, the initial resistance value of the heater and the temperature coefficient. Based on the heater temperature, power supply to the heater is controlled by an operation control means M4. | ||||||
| 76 | Superconductive resistance element | JP13327383 | 1983-07-21 | JPS6025283A | 1985-02-08 | MIHASHI TAKASHI; YASUE KUNIO |
| PURPOSE:To realize a desired resistance value by a superconductive metal without using a special material, and to obtain the titled element having high reliability and a small occupying area by forming a conductor pattern consisting of the superconductive metal on an insulative substrate and crossing the pattern through an insulating film in thickness through which a tunnel effect can be ignored. CONSTITUTION:A first thin-film pattern 2 consisting of a superconductive metal such as Nb is formed on a substrate 1. An insulative silicon oxide film 3 in thickness such as 100nm is shaped on the thin-film pattern 2, and a contact hole 4 is bored to the predetermined section of the oxide film 3. A second thin-film pattern 5 composed of a superconductive metal such as Nb is formed on the oxide film 3. The thin-film pattern 5 is formed so as to coat the contact hole 4 and cross with the thin-film pattern 2. An element formed in this manner is cooled up to a temperature close to absolute zero and used, and the thin-film patterns 2, 5 function as resistance elements. | ||||||
| 77 | Semiconductor device and data generation method | US13439289 | 2012-04-04 | US09360381B2 | 2016-06-07 | Naoya Arisaka; Takayasu Ito; Masashi Horiguchi |
| A semiconductor device with improved temperature detection accuracy includes a coefficient calculation circuitry which calculates a plurality of N-th order coefficients, where N is an integer equal to or greater than one, of a correction function as an N-th order approximation of a characteristic function which relates temperature data measured by the temperature sensor and the actual temperature. The coefficient calculation circuitry uses N+1 pieces of the temperature data including a theoretical value at absolute zero in the characteristic function and N measured values of the temperature data measured by the temperature sensor unit at N points of temperature. A corrected temperatures are output using the correction function with the calculated coefficients and measured temperature values. | ||||||
| 78 | Spindle nut holder for a spindle gear for driving levers | US09669166 | 2000-09-25 | US06612208B1 | 2003-09-02 | Juergen Stephan |
| Spindle nut holder for a spindle gear which drives a lever and functions under extreme conditions such as in a vacuum, under radiation exposure, and at a temperature close to absolute zero. The spindle nut holder includes a spindle nut and strip-shaped links each having an elongated, narrow cross section. One end of each link is connected to the spindle nut and the other end is connected to a frame. A pair of links are arranged on opposite sides of the spindle nut holder and each is oriented perpendicular to the spindle axis and the cross-section provides longer sides and shorter sides, the longer sides being parallel to the spindle axis. The cross-section of another link provides longer sides and shorter sides and is arranged relative to the pair of links such that the longer sides of this link are perpendicular to the longer sides of the pair of links. | ||||||
| 79 | Low noise cryogenic dielectric resonator oscillator | US116810 | 1987-11-05 | US4757278A | 1988-07-12 | G. John Dick |
| A microwave oscillator is provided which can operate at a temperature of many degrees above absolute zero while providing very low phase noise that has heretofore generally required temperatures within a few degrees K. The oscillator includes a ring-shaped resonator element of ruby (sapphire plus chromium) or iron sapphire crystal, lying adjacent to a resonator element of sapphire, so the regenerator element lies directly in the magnetic field of the resonator element. The resonator element is substantially devoid of contact with electrically conductive material. Microwave energy of a pump frequency (e.g. 31GHz) is applied to the regenerator element, while signal energy (e.g. 10GHz) is outputted from the resonator element. | ||||||
| 80 | Apparatus for producing electrical energy | US719978 | 1976-09-02 | US4237391A | 1980-12-02 | Paul E. Schur; Andrew I. Abolafia |
| An electrical generator comprises a stationary permanent magnet for establishing a magnetic field, one or more sensing coils responsive to the magnetic field, and a diamagnetic blocking element movable between the magnet and the sensing coils for periodically interrupting the magnetic field to produce electrical energy in the coils. A preferred embodiment includes a pair of semi-circular coils arranged side-by-side in the magnetic field and a rotatable blocking disc interposed between the magnet and the coils. The disc includes a semi-circular portion of superconductive material rendered impermeable to the magnetic field at temeperatures near absolute zero and a semi-circular portion of magnetically inert material to alternately block and pass the magnetic field to the coils upon rotation of the disc.This is a continuation, of application Ser. No. 566,090, filed Apr. 8, 1975 now abandoned. | ||||||
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