Absstract of: CN122693874A
本发明公开了一种光量子相位漂移预测性控制方法、系统及介质,本发明的方法包括:由漂移趋势预测模型基于历史相位漂移数据预测未来前瞻时间窗口内的相位漂移轨迹;根据预测结果与预设阈值的比较,针对将超标的目标通道输出决策信号;分级补偿执行单元响应决策信号执行幅度受控的相位补偿,使目标通道相位返回容错阈值内,且不中断计算任务;采集补偿后的实际相位残留量,并与预测值比较产生反馈信号;利用反馈信号在线更新漂移趋势预测模型。本发明保障了对大规模通道的高效实时控制,显著提升了光量子计算机的运行效率和长期稳定性。
Absstract of: CN122696182A
本发明公开了一种基于QAOA量子线路解决分子相似性问题的方法及相关装置,包括:将待比较的两个药物分子分别表示为带属性的药物分子拓扑图结构,其中,药物分子拓扑图结构的节点用于表示药物分子的原子,药物分子拓扑图结构的边用于表示药物分子的化学键,属性包括药物分子的节点属性和键属性;基于药物分子拓扑图结构中的节点属性匹配关系,生成所有允许的节点配对作为新节点,以及根据双摄理论约束和键类型冲突关系在新节点之间生成边连接,以构建冲突图;本申请通过构建冲突图,将求解药物分子的相似性问题转化成求解冲突图的最大加权独立集问题,旨在高效解决分子相似性求解过程中的计算性困难等问题。
Absstract of: CN122691727A
本发明公开了一种基于量子芯片的量子计算任务调度方法及相关装置,属于量子计算技术领域,方法包括:获取用户提交的量子计算任务;获取每个量子计算任务对应的量子比特数量、量子线路深度、量子线路的每个量子比特执行的逻辑门数量作为调度参数;确定量子芯片的量子比特的空间性能参数、时间性能参数为调度依据;根据调度参数和所述调度依据从量子芯片上调度量子计算任务的量子比特;本申请通过引入量子比特数量、量子线路深度、量子线路比特执行的逻辑门数量作为执行线路调度的参考依据,旨在更有效地利用有限的量子计算资源,减少资源浪费,提升整体量子计算效率,以及量子计算任务结果的准确性。
Absstract of: CN122693876A
本发明涉及量子控制和非厄米物理领域,为解决非厄米系统在奇异点附近因强带间绝热耦合和复相位因子竞争导致的非绝热跃迁问题,克服传统绝热捷径技术在非厄米系统中失效的挑战,提出一种非厄米系统中避免非绝热跃迁的操控方法,包括:获取系统哈密顿量并设定一条参考路径;分析参考路径下的动力学,计算绝热基和绝热基下的哈密顿量中的非对角耦合项;通过设计调控参数对角化有效哈密顿量用于抵消非绝热耦合效应;将调控参数与参考路径结合,构造非厄米捷径;驱动系统沿所述非厄米捷径演化,获得目标态。本发明通过主动构造非厄米捷径路径,实现了非厄米系统的高保真、快速且鲁棒的态传输,有效抑制非厄米奇异点附近的非绝热跃迁。
Absstract of: CN122693875A
本发明提供了一种超导量子比特的多路复用控制系统,属于量子领域,该多路复用控制系统包括:第一微波源,用于输出控制信号;第二微波源,用于输出偏置信号;寻址选择机构;M个可调超导滤波器与寻址选择机构的M个输出部以及M个超导量子比特一一对应的连接;传输机构与M个可调超导滤波器连接;寻址选择机构适用于将控制信号路由至与任一超导量子比特连接的可调超导滤波器,传输机构将偏置信号路由至可调超导滤波器,偏置信号用于将可调超导滤波器的滤波频率配置为与超导量子比特的工作频率相匹配,以对控制信号滤波,滤波后的控制信号用以操控超导量子比特,本发明的多路复用控制系统使超导量子处理器的具有可扩展性。
Absstract of: CN122699557A
本申请公开了一种约瑟夫森结的制备方法、量子比特和超导量子芯片,属于量子芯片制备技术领域。约瑟夫森结的制备方法,包括:刻蚀衬底表面的复合层,复合层包括在衬底表面依次沉积形成的第一超导层、势垒层和第二超导层,其中被刻蚀后的第一超导层形成底电极;去除结区区域以外的势垒层和第二超导层;沉积形成与底电极在结区处相交、并与第二超导层完全接触的顶电极。通过上述方式,本发明能够精准的制备约瑟夫森结,使得约瑟夫森结的电极和势垒层的尺寸和成分稳定。
Absstract of: CN122696179A
一种基于波函数文件的分子描述符自动提取解析与机器学习数据集构建方法,涉及计算化学数据处理与材料信息技术领域。包括:1)递归扫描分子文件夹,识别量子化学计算文件,建立分子数据对象;2)根据文件格式特征自动识别量化计算程序类型,并提取计算参数与结果等信息;3)按照预设优先级自动选择不同波函数文件,并调用Multiwfn进行静默批处理;4)自动提取30余种电子结构描述符,并与分子基础信息、目标标签和文件来源进行统一存储、匹配、合并和格式规整,输出可直接用于机器学习的标准化数据集。本发明能够实现不同来源量子化学计算结果的自动识别、解析以及机器学习数据集自动构建,提高大规模分子电子结构数据处理效率,降低人工整理误差。
Absstract of: US20250079034A1
Example embodiments provide quantum computers, laser light delivery systems for quantum computers, and methods for delivering laser light from lasers of quantum computers to atomic object confinement apparatuses of quantum computers. In an example embodiment, a quantum computer comprises an atomic object confinement apparatus, a laser, a cylindrical guide positioned such that a first end of the cylindrical guide is adjacent the laser and a second end of the cylindrical guide is adjacent the atomic object confinement apparatus, and an optical fiber cable helically wrapped around the cylindrical guide and spanning from the first end to the second end. The optical fiber cable is configured to deliver laser light generated by the laser to the atomic object confinement apparatus. A pitch of the helically wrapped optical fiber cable is selected to provide a desired effective bend radius of the optical fiber cable to strip higher-order modes of the laser light.
Absstract of: US2022014277A1
0001 A photon source module includes a plurality of photon sources, wherein each photon source is configured to non-deterministically generate one or more non-entangled or entangled photons in response to receiving a trigger signal. When two or more photon sources simultaneously generate photons in response to a trigger signal, one photon of a first photon pair is directed to a photon processing system and one photon of a second photon pair is directed to a photon analyzer. During repetitive operation, the photon analyzer analyzes photons from each of the plurality of photon sources to determine characteristics of each photon source and can use that information to direct the highest quality photons to the photon processing system.
Absstract of: WO2025162852A1
Disclosed is a Josephson junction traveling-wave parametric circuit (100) comprising unit cells (1101) which are coupled in series to form a transmission line between an input port (PIN) and an output port (POUT)- Each unit cell comprises a series Josephson junction (Ji) and a dispersive ground-shunt admittance (112i), particularly comprising a capacitive element (Ci) and an inductive element (Li) adding dispersion, configured to cause suppression of one or more sideband frequency components. The circuit may be a Josephson traveling- wave parametric amplifier (JTWPA), particularly for amplifying a readout signal of a quantum bit.
Absstract of: DE102025107736A1
Die Erfindung betrifft eine Vorrichtung (1) zur charakteristischen Analyse von Lichtfeldern, aufweisendeine erste Lichtquelle (2) zum Erzeugen eines optischen Referenzsignals (A),eine zweite Lichtquelle (4) zum Erzeugen eines optischen Testsignal (B),eine Verzögerungsstrecke (3) zum Erzeugen eines relativen Phasenverschubs zwischen dem optischen Referenzsignal (A) und dem optischen Testsignal (B),einen der ersten Lichtquelle (2) und der zweiten Lichtquelle (4) nachgeschalteten ersten polarisierenden Strahlteiler (5),eine dem ersten polarisierenden Strahlteiler (5) nachgeschaltete Halbwellenplatte (6) zum Drehen der Polarisation des optischen Referenzsignals (A) und des optischen Testsignals (B),einen der Halbwellenplatte (6) nachgeschalteten zweiten polarisierenden Strahlteiler (7) zum Aufteilen des kombinierten optischen Signals (A, B),ein Detektor (8) zum Erfassen der an dem Detektor (8) interferierenden optischen Teilsignale (T1, T2),einen dem Detektor (8) nachgeschalteten Filter (9) zum Herausfiltern des Referenzsignals (A) aus dem interferierten Signal (A, B),eine dem Filter (9) nachgeschaltete Auswerteeinheit (10) zum Auswerten des Messignals (C),eine Photodiode (11), die derart angeordnet ist, dass ein Teil des optischen Referenzsignals (A) auf die Photodiode (11) zum Aktivieren der Auswerteeinheit (10) geleitet wird.Auf diese Weise wird eine Vorrichtung für eine Quantentomographie in Echtzeit und mit verringerter Komplexität bereitgestellt.
Absstract of: US20260260774A1
Aspects of the present disclosure may include methods and systems for trapping an ion chain along a first axis, the ion chain including a plurality of trapped ions, applying a magnetic field, to the ion chain, along a second axis perpendicular to the first axis, applying a first beam, to the ion chain, at a first angle relative to the first axis, the first beam including two or more first polarization components, and applying a second beam, to the ion chain, at a second angle relative to the first axis, the second beam including two or more second polarization components, the first angle and the second angle being non-parallel to the first axis or the second axis.
Absstract of: WO2026180455A1
The invention relates to a quantum system (1) comprising a set (N) of identical quantum subsystems of which a majority, referred to as guide quantum subsystems (G), are in a first stable quantum state (|5S1/2, F=2, mF=1) and at least one quantum subsystem, referred to as emitter quantum subsystem (E), is in a second stable quantum state (|5S1/2, F=2, mF=2), characterized in that it comprises an excitation system (11, 12) capable of causing only the one or more emitter quantum subsystems to transition from the second stable state to a state referred to as emission state (|5P3/2, F=3, mF=3) in which these one or more emitter quantum subsystems emit a photon in order to return to the second stable state, the one or more photons emitted by the one or more emitter quantum subsystems in the emission state being capable of coupling the guide quantum subsystems in the first stable state with a state referred to as guide state (|5P3/2, F=3, mF=2) such that these coupled guide quantum subsystems form a medium having a refractive index (neff), at the frequency of the one or more photons emitted by the one or more emitter quantum subsystems in the emission state, greater than the refractive index of the surrounding medium.
Absstract of: US20260260144A1
Examples of the present disclosure are directed to a method for operating a quantum computing system (QCS) to load classical data. The method includes configuring a quantum circuit to implement a target classical function that is defined over a string of input bits. The target classical function is decomposed into a set of parity sub-functions. A set of quantum registers of the QCS is initialized with a superposition of input states corresponding to the string of input bits. A sequence of Quantum Read-Only Memory (QROM) operations is executed on the set of quantum registers to generate a set of outputs. Each QROM operation of the sequence of QROM operations encodes a separate parity sub-function of the set of parity sub-functions. Each output of the set of outputs is routed to a separate output register of a set of output registers of the QCS.
Absstract of: US20260260152A1
A computer-readable recording medium stores therein a program for causing a computer to execute a process, the process including: calculating energy of a molecule based on energy of each of multiple fragments obtained by dividing a structure of the molecule by a molecule dividing method, the calculating including: estimating, for each of the multiple fragments, a candidate value from which noise has been removed, based on multiple candidate values that are calculated by a variational quantum eigenvalue solver, each of the multiple candidate values being calculated for each of a multiple parameters of a first variational quantum circuit representing a Hamiltonian of the each of the multiple fragments, the each of the multiple candidate values being a potential solution of the parameter; and calculating, for each of the multiple fragments, an energy thereof based on the candidate value from which noise has been removed and estimated for each of the multiple parameters.
Absstract of: US20260260142A1
A method may include generating directed graphs, each of the directed graphs representing a quantum circuit. The method may also include evaluating each of the directed graphs according to operation of the quantum circuit represented by each of the directed graphs. The method may include selecting one of the directed graphs based on the evaluations. The method may further include transforming the selected directed graph to generate a second directed graph.
Absstract of: US20260260776A1
0000 The invention relates to neutral atom quantum computers having a zoned architecture that includes a storage zone and an interaction zone as part of an array of atoms that form the quantum register in an optical lattice. A schedule optimizer determines an optimized atom schedule for moving atoms between the storage zone and the interaction zone using optical tweezers generated by an optical trap generator responsive to the optimized atom schedule. The schedule optimizer may be implemented according to several variations of algorithms that include an annealing solver and a mathematical optimization engine. The schedule optimizer receives an objective function that includes selectable factors that correlate to minimizing the logical error rate for a set of operational tasks, various hardware constraints such as zone geometries and circuit schedules.
Absstract of: WO2026180934A1
In a method for implementing a Clifford gate on a quantum hardware system, a symplectic matrix representation of the Clifford gate is determined that factorizes as a product comprising at least five matrices alternating between matrices corresponding to X-diagonal Clifford operators and matrices corresponding to Z-diagonal Clifford operators. The Clifford gate is synthesized into a sequence of quantum gates, based on the symplectic matrix representation of the Clifford gate. The method comprises causing the quantum hardware system to implement the sequence of quantum gates.
Absstract of: US20260260145A1
0000 Techniques are described for controlling qubits using baseband pulse sequences. Many, or even all, qubits in a system can be controlled by baseband pulse sequences that are synchronized to a clock signal shared by the qubits. The baseband pulse control techniques allow many qubits to be driven with the same parameterized baseband pulse sequence applied based on a common clock signal, with parameters of the baseband pulse sequence selected based on the desired operation. This approach greatly simplifies the electronics needed to drive a collection of qubits, as there is no need for picosecond timing, nor the complexities that arise from varied gate durations.
Absstract of: US20260260711A1
0000 A non-transitory computer-readable recording medium stores therein a program that causes a computer to execute a process including dividing a molecule into a plurality of fragments, calculating, for each of the fragments, a first eigenvalue for each of bath orbitals included in the fragments, calculating a second value for each of the bath orbitals based on the first eigenvalue, sorting the second values in a descending order and deriving a cumulative distribution function of the second values, determining the number of the bath orbitals for which a cumulative probability of the cumulative distribution function is greater than a predetermined threshold value, selecting the bath orbitals corresponding to the second values from a largest one among the second values sorted in the descending order, in the number equal to the determined number of the bath orbitals, and calculating an energy of the molecule using the selected bath orbitals.
Absstract of: US20260260199A1
0000 The present disclosure provides a method of facilitating automated regulatory compliance determination. Further, the method may include receiving, using a communication device, a compliance input data from a regulatory data source. Further, the method may include receiving, using the communication device, an operational input data from an enterprise system. Further, the method may include determining, using a processing device, a compliance status data by processing the compliance input data and the operational input data using a quantum-inspired neural network. Further, the method may include generating, using the processing device, a compliance output data based on the compliance status data. Further, the method may include storing, using a storage device, the compliance output data. Further, the method may include transmitting, using the communication device, the compliance output data to a client system.
Absstract of: WO2026180792A1
A quantum error correction method and quantum computing system are disclosed. The quantum computing system receives syndrome data and sets defect states of nodes in a decoding hypergraph according to defects identified in the syndrome data. The quantum computing system determines a plurality of decoding windows associated with logical observable subsets of a logical observable and independently decodes the decoding windows to determine partial corrections. The partial corrections are then combined by the quantum computing system to determine an aggregate correction for an error state of quantum devices in the quantum computing system.
Absstract of: WO2026182926A1
An optical beam delivery system is provided. The optical beam delivery system includes one or more micro-optical benches (MOBs). Each MOB of the one or more MOBs includes a substrate, and a plurality of signal manipulation elements. Each signal manipulation element of the plurality of signal manipulation elements is disposed on or in the substrate. The plurality of signal manipulation elements are configured to provide an array of optical beams directly to an array of target locations. For example, the optical beams propagate through free space from the signal manipulation elements to the respective target locations without interacting with any additional optical elements, in various embodiments.
Absstract of: WO2026178585A1
A quantum computing system is described, comprising a quantum processor comprising multiple qubits, the quantum processor being configured to implement one or more operations on the multiple qubits; and an energy storage system configured to store energy in a quantum state, wherein the energy storage system is coupled to the multiple qubits and configured to supply the multiple qubits with energy from the quantum state to perform the one or more operations. A method for operating a quantum processor is also described, the method comprising initialising an energy storage system into a quantum state; and performing one or more operations on multiple qubits of the quantum processor by supplying the multiple qubits with energy from the quantum state.
Nº publicación: WO2026182682A1 03/09/2026
Applicant:
NANYANG TECHNOLOGICAL UNIV [SG]
NANYANG TECHNOLOGICAL UNIVERSITY
Absstract of: WO2026182682A1
Various embodiments may relate to an optical circuit. The optical circuit may include an inline detection portion including a waveguide and a super conducting nanowire. The optical circuit may also include an input optical circuit portion optically coupled to a first end of the waveguide of the inline detection portion. The optical circuit may further include an output optical circuit portion optically coupled to a second end of the waveguide of the inline detection portion. The optical circuit may be configured such that a light traveling through the waveguide of the inline detection portion from the input optical circuit portion is partially absorbed by the superconducting nanowire of the inline detection portion, with an unabsorbed portion of the light traveling to the output circuit portion, the output circuit portion configured to manipulate the unabsorbed portion of the light.