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 |
|---|---|---|---|---|---|---|
| 121 | QUANTUM COMPUTER AND QUANTUM COMPUTING METHOD | US15211112 | 2016-07-15 | US20160321558A1 | 2016-11-03 | Satoshi NAKAMURA; Kouichi ICHIMURA; Hayato GOTO; Mamiko KUJIRAOKA |
| According to an embodiment, a quantum computer includes physical systems Xi, a physical system Yj and a light source unit. The physical systems Xi and the physical system Yj are provided in a cavity. Each physical system Xi includes states |0>i, |1>i, |2>i and |e>i, the states |0>i and |1>i being used for a qubit, a |2>i-|e>i transition being resonant with a cavity mode of the cavity. The physical system Yj includes states |2>′j and |e>′j, a |2>′j-|e>′j transition being resonant with the cavity mode. The light source unit applies laser beams to the cavity to manipulate states of two of physical systems Xi, the laser beams including a laser beam for collecting population in the state |2>′j in the |2>′j-|e>′j transition. | ||||||
| 122 | STATE-CHANGEABLE DEVICE | US14914030 | 2014-08-14 | US20160225449A1 | 2016-08-04 | Emanuel Loertscher |
| A state-changeable device includes a first and a second particle arranged in proximity to each other; and a coupling material between the first and the second particle; wherein the first and the second particle are adapted to provide a charge carrier distribution such that surface plasmon polaritons (SPP) occur; the coupling material is adapted to exhibit a variable conductivity in response to a trigger signal thereby changing an electro-optical coupling between the first and the second particle; and the first and the second particle are arranged in proximity to each other such that a first SPP configuration corresponds to a first electro-optical coupling between the first and the second particle and a second SPP configuration corresponds to a second electro-optical coupling between the first and the second particle. | ||||||
| 123 | DELAYED OPTICAL LOGIC GATES FOR BOOLEAN ALGEBRA | US14729840 | 2015-06-03 | US20150346581A1 | 2015-12-03 | Byoung Seung HAM |
| A system, method, and apparatus for delayed optical logic gates based on slow light and enhanced nondegenerate four-wave mixing processes, where a single or multiple delayed optical routers are utilized for dark resonance interactions in which two-color lasers interact with a three-level nonlinear optical medium comprised of two ground states and one excited state through the nondegenerate four-wave mixing processes. The delayed optical logic mechanism is based on combination of single or multiple dark resonance-induced two-photon coherence conversion via slow light phenomenon. The two-photon coherence induced on the ground states is optically detected via nondegenerate four-wave mixing processes. The nondegenerate four-wave mixing generation is enhanced owing to dark resonance or electromagnetically induced transparency. The delayed optical logic gates have potential to keep up ultra-high-bandwidth optical information processing using relatively slow electronic processing devices. | ||||||
| 124 | Solid state nano-based optical logic gate | US13608062 | 2012-09-10 | US09128306B2 | 2015-09-08 | Talal Ghannam |
| A logic gate is disclosed having a photonic or polaritonic band gap medium and a plurality of nano particles, atoms or artificial atoms are disposed in the band gap medium. Two coupled electromagnetic pulses are propagated within the medium and produce two output pulses. The output pulses are detected or sensed and a third external electronic field controls the relative velocities of the two output pulses. A method for producing a time delay of an electromagnetic pulse is also disclosed. | ||||||
| 125 | OPTICAL LOGIC GATES AND METHOD FOR GENERATING LOGIC SIGNALS USING DNA BASED NANOSTRUCTURE | US14185419 | 2014-02-20 | US20150131134A1 | 2015-05-14 | Chulki KIM; Jae Hun KIM; Byeong Ho PARK; Seok LEE; Seong Chan JUN; Taikjin LEE |
| An optical logic gate includes: a DNA based nanostructure including DNA and metal nanoparticles coupled to the DNA, the DNA based nanostructure being configured to rotate a polarization plane of an incident light; a polarizer to which light passing through the DNA based nanostructure is incident, the polarizer being configured to extract a component in a direction of a predetermined reference axis from light whose polarization plane is rotated by the DNA based nanostructure; and a detection unit to which light passing through the polarizer is incident, the detection unit being configured to generate a logic signal based on a result obtained by comparing the intensity of the component in the reference axis direction extracted by the polarizer with a predetermined threshold value. | ||||||
| 126 | OPTICAL DEVICES, SYSTEMS AND METHODS | US14388261 | 2013-03-12 | US20150049377A1 | 2015-02-19 | Nikolay Ivanovich Zheludev; Kevin Francis MacDonald; Jianfa Zhang; David John Richardson |
| First and second coherent light beams of the same wavelength are propagated in opposite directions to interact on a sub-wavelength thickness metallic metamaterial layer which is structured with a periodicity such that there is a resonance matched to the wavelength of the coherent beams. The first beam is then able to modulate the intensity of the second beam by modulating the phase and/or intensity of the first beam. The interference of the counter- propagating beams can eliminate or substantially reduce Joule loss of light energy in the metamaterial layer or, on the contrary, can lead to a near total absorption of light, depending on the mutual phase and/or intensity of the interacting beams. A modulation is thus provided without using a non-linear effect. | ||||||
| 127 | Reservoir Computing Using Passive Optical Systems | US14324459 | 2014-07-07 | US20150009548A1 | 2015-01-08 | Peter BIENSTMAN; Joni DAMBRE; Kristof VANDOORNE |
| A method comprising providing an input signal to at least one input node of a computing reservoir by temporally encoding the input signal by modulating the at least one photonic wave as function of the input signal is described. The method further comprises propagating the at least one photonic wave via passive guided or unguided propagation between discrete nodes of the computing reservoir, in which each discrete node is adapted for passively relaying the at least one photonic wave over the passive interconnections connected thereto. The method also comprises obtaining a plurality of readout signals, in which each readout signal is determined by a non-linear relation to the at least one photonic wave in at least one readout node of the computing reservoir, and combining this plurality of readout signals into an output signal by taking into account a plurality of training parameters. | ||||||
| 128 | Organic electroluminescence device and testing method thereof | US13375688 | 2009-12-30 | US08836337B2 | 2014-09-16 | Yong Qiu; Zhaoji Peng; Xinyi Zhong; Jian Sun |
| An organic electroluminescence device is provided, which comprises: a lighting region, a wiring region, a bonding region and a wiring extending region (300), the lighting region comprises an anode, an organic functional layer, a cathode; the wiring region comprises wirings connecting the anode and cathode with a driving chip or a circuit board; the bonding region is a region in which the wirings connect with the driving chip or the circuit board; the ends of the wirings locate in the wiring extending region, the wirings in the wiring extending region are parallel with the wirings in the wiring region or form an angle with the wirings in the wiring region. A method for testing the organic electroluminescence device is also provided. With improving the wiring arrangement of the organic electroluminescence device, it is easier and more accurate to press bond a conductive adhesive tape and the wirings, and, the row wirings and the column wirings are protected from being shorted during screen testing. | ||||||
| 129 | Devices and methods for optical signal control | US12401779 | 2009-03-11 | US08792159B2 | 2014-07-29 | Zeev Zalevsky; Arkady Rudnitsky |
| A device for use in optical signal control is presented. The device comprises an amplification waveguide, including a pumpable medium, and a reference and a control inputs and an output selectively allowing transmission of light respectively into and out of said amplification waveguide. The reference input, the amplification waveguide and the output define together a transmission scheme for reference light through the pumpable medium. The control input and the amplification waveguide define a depletion scheme for the pumpable medium and control light. The device thus allows for controlling an output signal, formed by the transmission of the reference light, by controllable depletion of the pumpable medium. | ||||||
| 130 | Morphable Identity, Networkable Photonic Quantum Logic Gate System & Method | US13735823 | 2013-01-07 | US20140192390A1 | 2014-07-10 | Daniel S. Klotzer |
| Systems and methods of performing logical operations with photonic quantum logic gates. The logic gates utilize photon states, usually orthogonal linearly polarized states, to selectively enact self-interference operations whose outputs can be altered by inducing phase shifts in one or more portions of the section of the logic gate where the photon states undergo self-interference. The polarization direction switchings are differentially enacted and/or not enacted, in groupings of switches, to perform various logic operations. Additionally, networked logic gates with interrelated self-interference section phase shifts and output states are described that provide additional capabilities. | ||||||
| 131 | INTEGRATED OPTICS LOGIC GATE FOR POLARIZATION-ENCODED QUANTUM QUBITS AND A METHOD FOR THE PRODUCTION AND USE THEREOF | US14115622 | 2012-05-03 | US20140126030A1 | 2014-05-08 | Andrea Crespi; Paolo Mataloni; Roberta Ramponi; Linda Sansoni; Fabio Sciarrino; Giuseppe Vallone; Roberto Osellame |
| A quantum logic gate for qubits, suitable for receiving as inputs at least two polarization-encoded qubits, includes at least one partially polarizing beam splitter (PPBS), the beam splitter comprising a first waveguide and a second waveguide which are constructed in integrated optics, the first and second waveguides having a refractive index contrast of between 0.1% and 6% and a birefringence of between 10−6 and 6*10−5. | ||||||
| 132 | Device interface apparatus and test apparatus | US13196866 | 2011-08-02 | US08699018B2 | 2014-04-15 | Hideo Hara; Shin Masuda |
| It is an object of the present invention to test a device under test including an optical interface. Provided is a device interface apparatus on which is loaded a device under test including an optical interface. The device interface apparatus comprises a device loading section on which the device under test is loaded; an optical connector that is to be connected to the optical interface of the device under test; and an optical connector moving section that moves the optical connector toward the optical interface of the device under test loaded on the device loading section, to optically connect the optical connector and the optical interface. | ||||||
| 133 | Optical XOR gate | US12973470 | 2010-12-20 | US08582931B1 | 2013-11-12 | G. Allen Vawter |
| An optical XOR gate is formed as a photonic integrated circuit (PIC) from two sets of optical waveguide devices on a substrate, with each set of the optical waveguide devices including an electroabsorption modulator electrically connected in series with a waveguide photodetector. The optical XOR gate utilizes two digital optical inputs to generate an XOR function digital optical output. The optical XOR gate can be formed from III-V compound semiconductor layers which are epitaxially deposited on a III-V compound semiconductor substrate, and operates at a wavelength in the range of 0.8-2.0 μm. | ||||||
| 134 | Optical component having a waveguide array heterostructure | US13120661 | 2009-09-25 | US08488927B2 | 2013-07-16 | Jean-Marie Moison; Christophe Minot |
| The invention relates to an optical component including an array of coupled waveguides, wherein said waveguide array includes: a first area made of parallel waveguides coupled according to a first coupling coefficient; a second area adjacent to the first area and made of parallel waveguides coupled according to a second coupling coefficient lower than the first coupling coefficient; a third area adjacent to the second area and made of parallel waveguides coupled according to a third coupling coefficient higher than the second coupling coefficient; a fourth area adjacent to the third area and made of parallel waveguides coupled according to a fourth coupling coefficient lower than the third coupling coefficient; and a fifth area adjacent to the fourth area and made of parallel waveguides coupled according to a fifth coupling coefficient higher than the fourth coupling coefficient. | ||||||
| 135 | Optological Gates | US13209604 | 2011-10-13 | US20130094070A1 | 2013-04-18 | Shahin Mojtabaee Tabatabaee |
| In this invention truth logic is defined as that “Light existence=TRUE” and “NO light or Dark=FALSE”. And through the optical principles (: “Fraunhofer” single slit & “Young” double slits light diffraction pattern), I have designed logical function gates (AND, OR, XOR & NOT), using the optical equipments and a coherent light beam (Laser beam), with no interference of any electronic circuits or devices. This design would lead us to make Optological Gates which run at the light speed, so we would have logical function gates with very high speed. | ||||||
| 136 | All-optical reconfigurable cascadable logic with linear preprocessing by lightwave interference and post-processing by nonlinear phase erasure | US12476822 | 2009-06-02 | US08345335B2 | 2013-01-01 | Moshe Nazarathy; Amir Nevet |
| There is provided a new architecture for all-optical logic architecture. In this architecture the gate is partitioned into a linear front-end followed by a nonlinear back-end. The logic calculation is practically performed within the linear stage, easing the requirements placed on the non-linear part and thus reducing the gate complexity. The new structures provide flexibility and improved performance for the all-optical logic. The proposed scheme may be integrated optics/electronics. An important additional attribute of our all-optical logic family is reconfigurability, i.e. the ability of the hardware architecture or devices to rapidly alter the functionalities of its components and the interconnection between them as needed. | ||||||
| 137 | Passive all optical polarization switch and logic devices utilizing the same | US12359945 | 2009-01-26 | US08331002B2 | 2012-12-11 | Yasser A. Zaghloul; Arm Zaghloul |
| A passive all optical polarization switch and apparatus and methods for implementing logical operations using the switch is provided. The switch converts a first polarized beam having a polarization angle equals to or nearly equals to ±45 degrees into a beam equal to or nearly equal to the vertical component of the first polarized beam. The switch converts a second polarized beam having a polarization angle equals to or nearly equals to ±45 degrees into a beam equal to or nearly equal to the horizontal component of the second polarized beam. The switch combines the vertical component of the first polarized beam and the horizontal component of the second polarized beam to produce an output polarized beam. The switch is used to implement all optical polarization logic gates. | ||||||
| 138 | All optical and hybrid reflection switch at a semiconductor/glass interface due to laser beam intersection | US12925566 | 2010-10-25 | US08330960B2 | 2012-12-11 | Bruno Ullrich; Artur Erlacher |
| The present invention includes a method of changing intensity of a reflected beam which may be expressed as a method of changing the amount of reflected light from a beam of light, the method comprising: (a) providing a substrate bearing a film of a reflective material; (b) directing a first beam of light at a reflecting point upon the reflective material so as to create a reflecting beam therefrom; (c) directing a second beam of light at the reflecting point upon the reflective material so as to alter the amount of light in the reflecting beam, and (d) detecting the change in the amount of light in the reflecting beam. The invention also includes an apparatus for changing the amount of reflected light from a beam of light and measuring that change, as well as related apparatus for a pulsed optical signal. | ||||||
| 139 | Optical logic devices having polarization-based logic level representation and method of designing the same | US13195619 | 2011-08-01 | US08325404B2 | 2012-12-04 | Yasser A. Zaghloul; Abdel Rahman M Zaghloul |
| Logical operations are implemented using polarization-based logic level representation. An input polarized beam is split into a first beam and a second beam. The first beam is polarized at a first relative polarization angle and the second beam is polarized at a second relative polarization angle. The ratio of the amplitudes of two perpendicular polarization components of the input polarized beam is one or nearly one and the difference between the first relative polarization angle and the second relative polarization angle is 180 degrees or nearly 180 degrees. The relative polarization angle of the input polarized beam equals or nearly equals either the first relative polarization angle or the second relative polarization angle. | ||||||
| 140 | Delayed optical logic gates for boolean algebra | US13014344 | 2011-01-26 | US08259377B2 | 2012-09-04 | Byoung-Seung Ham |
| A system, method, and apparatus for delayed optical logic gates based on slow light and enhanced nondegenerate four-wave mixing processes, where a single or multiple delayed optical routers are utilized for dark resonance interactions in which two-color lasers interact with a three-level nonlinear optical medium comprised of two ground states and one excited state through the nondegenerate four-wave mixing processes. The delayed optical logic mechanism is based on combination of single or multiple dark resonance-induced two-photon coherence conversion via slow light phenomenon. The two-photon coherence induced on the ground states is optically detected via nondegenerate four-wave mixing processes. The nondegenerate four-wave mixing generation is enhanced owing to dark resonance or electromagnetically induced transparency. The delayed optical logic gates have potential to keep up ultra-high-bandwidth optical information processing using relatively slow electronic processing devices. | ||||||
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