Non-Arbel Arbitrary Sub-Control System

Abstract

The invention discloses a non-Arbel arbitrary sub-control system. The time division multiplexing module is configured to analyze the received control instruction, determine a first target radio frequency superconducting quantum interference device and a first control signal corresponding to the first target radio frequency superconducting quantum interference device, and send the first control signal to the first target interference device switch. Then, the first target interference device switch is configured to couple the first electrical parameter pulse signal to the first target radio frequency superconducting quantum interference device according to the first state switching instruction. And then, the first target radio frequency superconducting quantum interference device is configured to generate a target magnetic field according to the received first electrical parameter pulse signal, so that the superconducting vortex array layer forms a target vortex array matched with the topological structure of the radio frequency superconducting quantum interference device under the action of the target magnetic field, and each vortex in the target vortex array is used for constraining one non-Arbel arbitrary sub-. In this way, any non-Arbel sub-array can be formed as required.

Description

Technical Field

[0001] This application relates to the field of quantum computing technology, and more specifically, to a non-Abelian anyon control system and a non-Abelian anyon control method. Background Technology

[0002] Topologically protected qubits (qubits) are constructed based on non-Abelian anyons and can meet the fault-tolerance requirements of quantum computing through their intrinsic noise immunity, thus providing a physical carrier for the practical application of quantum computing. In related technologies, the preparation and weaving of non-Abelian anyons are often achieved through local probe manipulation. However, because the probe volume is larger than the non-Abelian anyon manipulation unit, the spatial resolution is insufficient, resulting in poor overall manipulation efficiency of non-Abelian anyons. Summary of the Invention

[0003] This application provides a non-Abelian anyon control system and a non-Abelian anyon control method.

[0004] This application provides a non-Abelian anyon control system, which includes a time-division multiplexing module, an interferometer switch, a radio frequency superconducting quantum interference device (RFQFID), and a superconducting vortex array layer, wherein the interferometer switch and the RFQFID correspond one-to-one. The time-division multiplexing module is configured to parse the received control command, determine the first target radio frequency superconducting quantum interference device (RF-SQFID) and a first control signal corresponding to the first target RF-SQFID, and send the first control signal to the first target interference device switch. The RF-SQFID includes the first target RF-SQFID, the first target interference device switch corresponds to the first target RF-SQFID, and the first control signal includes a first state switching command and a first electrical parameter pulse signal. The first target interferometer switch is configured to couple the first electrical parameter pulse signal to the first target radio frequency superconducting quantum interference device according to the first state switching instruction; The first target radio frequency superconducting quantum interference device is configured to generate a target magnetic field based on a received first electrical parameter pulse signal, so that the superconducting vortex array layer forms a target vortex array under the action of the target magnetic field that matches the topology of the radio frequency superconducting quantum interference device, wherein each vortex in the target vortex array is used to bind one of the non-Abelian anyons.

[0005] Thus, the non-Abelian anyon control system includes a time-division multiplexing module, an interferometer switch, a radio-frequency superconducting quantum interference device (RF-SQFID), and a superconducting vortex array layer, with a one-to-one correspondence between the interferometer switch and the RF-SQFID. The time-division multiplexing module is configured to parse received control commands, determine a first target RF-SQFID and a corresponding first control signal, and send the first control signal to the first target interferometer switch. The RF-SQFID includes the first target RF-SQFID, and the first target interferometer switch corresponds to it. The first control signal includes a first state switching command and a first electrical parameter pulse signal. Next, the first target interferometer switch is configured to couple the first electrical parameter pulse signal to the first target RF-SQFID according to the first state switching command. Then, the first target radio frequency superconducting quantum interference device (RF-SQFID) is configured to generate a target magnetic field based on the received first electrical parameter pulse signal. This causes the superconducting vortex array layer to form a target vortex array under the influence of the target magnetic field, matching the topology of the RF-SQFID. Each vortex in the target vortex array is used to bind a non-Abelian anyon. Thus, by precisely controlling the magnetic field parameters generated by the RF-SQFID and the topology of the RF-SQFID, periodic or aperiodic arrays of non-Abelian anyons can be formed as needed, meeting the requirements of different topological quantum computing scenarios. Furthermore, the one-to-one correspondence between the interferometer switch and the RF-SQFID, combined with the precise control of the target magnetic field by the electrical parameter pulse signal, avoids signal crosstalk and ensures the stability of the vortex array, thereby achieving stable binding of non-Abelian anyons.

[0006] In some implementations, the time-division multiplexing module is configured to: The control command is parsed to determine the addressing signal; Based on the pre-configured addressing signal-RF superconducting quantum interference device (RFQUMP) mapping relationship, the first target RFQUMP is determined according to the addressing signal. The control command is parsed to determine the first state switching command and the first electrical parameter pulse signal, wherein the first electrical parameter pulse signal includes a polarity parameter and an amplitude parameter, the polarity parameter is used to determine the polarity of the target magnetic field, and the amplitude parameter is used to control the strength of the target magnetic field.

[0007] Thus, the control command is parsed to determine the addressing signal. Next, based on the pre-configured addressing signal-RF superconducting quantum interference device (RFQFID) mapping relationship, the first target RFQFID is determined according to the addressing signal. Then, the control command is parsed again to determine the first state switching command and the first electrical parameter pulse signal. The first electrical parameter pulse signal includes a polarity parameter and an amplitude parameter; the polarity parameter is used to determine the polarity of the target magnetic field, and the amplitude parameter is used to control the strength of the target magnetic field. In this way, through the addressing signal-RFQFID mapping relationship, it can be ensured that the control signal is accurately delivered to the target RFQFID, avoiding signal crosstalk and malfunctions.

[0008] In some embodiments, the first target radio frequency superconducting quantum interference device (RFQU) includes multiple RFQUs, the first control signal further includes timing parameters, and the time division multiplexing module is configured to: Based on the pre-configured addressing signal-RF superconducting quantum interference device mapping relationship, the control command is parsed to determine multiple addressing signals; Based on the addressing signal-RF superconducting quantum interference device (RFQUMP) mapping relationship, the first target RFQUMP is determined according to multiple addressing signals. Based on the timing parameters, the first state switching command and the first electrical parameter pulse signal are sent to the first target interferometer switch.

[0009] In this way, the control commands are parsed to determine multiple addressing signals. Then, based on the addressing signal-RF superconducting quantum interference device (QFID) mapping relationship, the first target QFID is determined according to the multiple addressing signals. Finally, based on timing parameters, the first state switching command and the first electrical parameter pulse signal are sent to the first target interferometer switch. In this way, by using timing parameters, the state switching and magnetic field generation of multiple QFIDs can be highly coordinated, preventing magnetic field distribution disorder caused by asynchronous signal transmission, thus enabling parallel operation.

[0010] In some embodiments, the polarity parameter includes a positive polarity parameter and a negative polarity parameter, wherein if the polarity parameter is the positive polarity parameter, the first target radio frequency superconducting quantum interference device outputs a first magnetic pole magnetic field; if the polarity parameter is the negative polarity parameter, the first target radio frequency superconducting quantum interference device outputs a second magnetic pole magnetic field.

[0011] Thus, the polarity parameters include positive and negative polarity parameters. If the polarity parameter is positive, the first target RF superconducting quantum interference device (RFQUANDV) outputs a first magnetic pole field; if the polarity parameter is negative, the first target RFQUANDV outputs a second magnetic pole field. This ensures that the magnetic field polarity of each first target RFQUANDV can be accurately predicted and controlled, avoiding disordered vortex directions caused by magnetic pole chaos, thereby ensuring the topological integrity of the target vortex array.

[0012] In some embodiments, the radio frequency superconducting quantum interference device consists of a single Josephson junction and a superconducting loop.

[0013] Thus, the radio frequency superconducting quantum interference device consists of a single Josephson junction and a superconducting loop. This single Josephson junction avoids interference from multiple junctions, allowing for more precise current regulation and ensuring that the polarity and strength of the target magnetic field perfectly match the control commands, thereby guaranteeing the orderliness of the target vortex array.

[0014] In some embodiments, the radio frequency superconducting quantum interference device (RFQU) is in the shape of a ring, and the target magnetic field output by the ring-shaped RFQU is rotationally symmetrically distributed, with the magnetic field strength of the target magnetic field gradually decreasing outward along the axis of the ring.

[0015] Thus, the radio frequency (RF) superconducting quantum interference device (QFID) is circular in shape, and the target magnetic field output by the circular QFID is rotationally symmetrically distributed, with the magnetic field strength gradually decreasing outward along the axis of the ring. This rotational symmetry ensures precise alignment between the vortex center and the interferometer axis, preventing vortex offset or distortion, and ensuring that the topology of the target vortex array matches the topology of the RF QFID, thereby improving the accuracy of vortex excitation. Furthermore, the gradual decrease in magnetic field strength outward along the ring axis confines the magnetic field of each RF QFID to its own operating region, ensuring no significant superposition of magnetic fields between adjacent RF QFIDs.

[0016] In some embodiments, the superconducting vortex array layer comprises a p-wave topological superconducting material or a target-type superconducting material; the radio frequency superconducting quantum interference device is located on the projection plane of the superconducting vortex array layer to ensure that the target magnetic field can effectively penetrate and excite the vortex.

[0017] Thus, the superconducting vortex array layer comprises either p-wave topological superconducting material or the target type of superconducting material. A radio frequency superconducting quantum interference device (RF quantum interference device) is positioned on the projection plane of the superconducting vortex array layer to ensure that the target magnetic field can effectively penetrate and excite the vortices. In this way, the p-wave topological superconducting material ensures that the vortices can effectively confine non-Abelian anyons. Furthermore, the RF quantum interference device's position on the projection plane of the superconducting vortex array layer shortens the magnetic field transmission path, reduces energy loss, ensures effective magnetic field penetration of the superconducting layer, and avoids vortex excitation failure due to magnetic field attenuation.

[0018] In some embodiments, the topology of the radio frequency superconducting quantum interference device includes a periodic array and / or an aperiodic array, wherein the periodic array includes a square lattice array, a triangular lattice array, and / or a honeycomb lattice, and the spatial distribution of the target vortex array corresponds to the lattice position of the topology of the radio frequency superconducting quantum interference device.

[0019] Thus, the topology of the radio frequency superconducting quantum interference device (RFQU) includes periodic and / or aperiodic arrays. The periodic arrays include square lattice arrays, triangular lattice arrays, and / or honeycomb lattice arrays. The spatial distribution of the target vortex array corresponds to the lattice positions of the RFQU topology. In this way, through the optional design of periodic and aperiodic arrays, the arbitrary sub-distribution can meet both the regularization requirements of conventional large-scale computing and the personalized requirements of special tasks.

[0020] In some embodiments, the time-division multiplexing module is further configured to determine a second target radio frequency superconducting quantum interference device (RF-SQUID) and a second control signal corresponding to the second target RF-SQUID based on the received topology weaving instruction, and to send the second control signal to the second target interference device switch, wherein the first target RF-SQUID includes the second target RF-SQUID, and the second control signal includes a second state switching instruction and a second electrical parameter pulse signal; The second target interferometer switch is configured to couple the second electrical parameter pulse signal to the second target radio frequency superconducting quantum interference device according to the second state switching command; The second target radio frequency superconducting quantum interference device is configured to adjust the magnetic field gradient distribution of the target magnetic field according to the received second electrical parameter pulse signal, and guide the vortices in the target vortex array to move along a preset path to realize the topological weaving of the non-Abelian anyons.

[0021] Thus, the time-division multiplexing module is further configured to determine the second target RF superconducting quantum interference device (RFQU) and a corresponding second control signal based on the received topology weaving instruction, and send the second control signal to the second target interferometer switch. The first target RFQU includes the second target RFQU, and the second control signal includes a second state switching instruction and a second electrical parameter pulse signal. Next, the second target interferometer switch is configured to couple the second electrical parameter pulse signal to the second target RFQU according to the second state switching instruction. Finally, the second target RFQU is configured to adjust the magnetic field gradient distribution of the target magnetic field according to the received second electrical parameter pulse signal, guiding the vortices in the target vortex array to move along a preset path to achieve topology weaving of non-Abelian anyons. In this way, by dynamically adjusting the magnetic field gradient distribution, the vortex movement can be made smooth, reducing quantum state distortion and ensuring the integrity of quantum information. Furthermore, parsing the topology weaving instruction precisely selects the interferometers participating in the weaving, avoiding signal crosstalk and irrelevant magnetic field interference, and ensuring that the vortices move along the preset path.

[0022] In some embodiments, the non-Abelian anyon control system further includes a detection module; the detection module is configured to detect the presence state and associated quantum properties of the vortex to be tested in the target vortex array, so as to read the quantum information carried by the non-Abelian anyons in the vortex to be tested, the vortex to be tested including fused vortices obtained after the topological weaving.

[0023] Thus, the detection module is configured to detect the existence state and correlated quantum properties of the vortex to be tested in the target vortex array, in order to read the quantum information carried by the non-Abelian anyons in the vortex to be tested, including fused vortices obtained after topological weaving. In this way, the detection module constructs a transformation path from physical state to quantum information by specifically detecting the topologically woven vortex to be tested, combined with the dual detection of the fundamental existence and correlated quantum properties of the vortex.

[0024] This application also provides a non-Abelian anyon control method, the method being based on the above-described non-Abelian anyon control system, the method comprising: The received control command is parsed to determine the first target radio frequency superconducting quantum interference device and the first control signal corresponding to the first target radio frequency superconducting quantum interference device. The first control signal includes a first state switching command and a first electrical parameter pulse signal. According to the first state switching instruction, the first electrical parameter pulse signal is coupled to the first target radio frequency superconducting quantum interference device; The target magnetic field is continuously output according to the received first electrical parameter pulse signal, so that the superconducting vortex array layer forms and maintains a target vortex array that matches the topology of the radio frequency superconducting quantum interference device under the action of the target magnetic field.

[0025] Thus, the received control commands are parsed to determine the first target RF superconducting quantum interference device (RFQUID) and the corresponding first control signal, which includes a first state switching command and a first electrical parameter pulse signal. Next, according to the first state switching command, the first electrical parameter pulse signal is coupled to the first target RFQUID. Finally, a target magnetic field is continuously output according to the received first electrical parameter pulse signal, causing the superconducting vortex array layer to form and maintain a target vortex array with a topological structure matching that of the RFQUID under the influence of the target magnetic field. In this way, through precise control of the magnetic field parameters generated by the RFQUID and its topological structure, periodic or aperiodic non-Abelian anyon arrays can be formed as needed, meeting the requirements of different topological quantum computing scenarios. Furthermore, the one-to-one correspondence between the interferometer switch and the RFQUID, combined with the precise control of the target magnetic field using the electrical parameter pulse signal, avoids signal crosstalk and ensures the stability of the vortex array, thereby achieving stable binding of non-Abelian anyons.

[0026] Additional aspects and advantages of embodiments of this application will be set forth in part in the description which follows, and in part will be obvious from the description, or may be learned by practice of embodiments of this application. Attached Figure Description

[0027] The above and / or additional aspects and advantages of this application will become apparent and readily understood from the description of the embodiments taken in conjunction with the following drawings, wherein: Figure 1 This is one of the structural schematic diagrams of the non-Abel any subsystem control system according to an embodiment of this application; Figure 2 This is a schematic diagram of vortex movement according to an embodiment of this application; Figure 3 This is a schematic diagram of vortex fusion according to an embodiment of this application; Figure 4 This is a second schematic diagram of the non-Abel any subsystem control system according to an embodiment of this application; Figure 5 This is a flowchart illustrating the non-Abel anyon control method according to an embodiment of this application. Detailed Implementation

[0028] The embodiments of this application are described in detail below. Examples of the embodiments are shown in the accompanying drawings, wherein the same or similar reference numerals denote the same or similar elements or elements having the same or similar functions throughout. The embodiments described below with reference to the accompanying drawings are exemplary and are only used to explain the embodiments of this application, and should not be construed as limiting the embodiments of this application.

[0029] Topology-protected qubits are constructed based on non-Abelian anyons. Thanks to the topological degeneracy of non-Abelian anyons, the quantum information in topology-protected qubits is naturally immune to local perturbations, which can meet the fault tolerance threshold requirements of topological quantum computing.

[0030] In related technologies, the preparation and weaving of non-Abelian anyons mainly rely on local probe manipulation techniques. However, local probe manipulation techniques have unavoidable limitations. Specifically, the physical volume of the local probe is much larger than the operating unit of the non-Abelian anyon, which is a superconducting vortex, typically on the nanometer scale. Thus, during the preparation stage, the local probe cannot precisely locate the vortex generation position, easily leading to disordered distribution of non-Abelian anyons and difficulty in forming a regular manipulation array. During the weaving stage, the local probe cannot precisely control the vortex's trajectory, causing the weaving path of the anyon to deviate from the preset logic, directly affecting the accuracy of quantum gate operations.

[0031] Furthermore, direct contact between the local probe and the superconducting vortex layer generates mechanical stress, which can easily damage the microcrystalline structure of the superconducting layer, causing instability of non-Abelian anyons. This forces the experiment to be interrupted or reinitialized, significantly increasing operational costs. Moreover, local probe manipulation technology is highly sensitive to environmental stability; even minor vibrations, temperature fluctuations, and electromagnetic interference can alter the relative position of the probe and the superconducting layer or damage the superconducting properties, leading to a substantial decrease in the success rate of non-Abelian anyon fabrication and weaving.

[0032] Based on the above issues, please refer to Figure 1 This application provides a non-Abelian anyon control system 1000, which includes a time division multiplexing module 100, an interferometer switch 200, a radio frequency superconducting quantum interference device 300, and a superconducting vortex array layer 400. The interferometer switch 200 and the radio frequency superconducting quantum interference device 300 are in one-to-one correspondence. The time-division multiplexing module 100 is configured to parse the received control command, determine the first target radio frequency superconducting quantum interference device 310 and the first control signal corresponding to the first target radio frequency superconducting quantum interference device 310, and send the first control signal to the first target interference device switch 200. The radio frequency superconducting quantum interference device 300 includes the first target radio frequency superconducting quantum interference device 310, the first target interference device switch 200 corresponds to the first target radio frequency superconducting quantum interference device 310, and the first control signal includes a first state switching command and a first electrical parameter pulse signal. The first target interferometer switch 200 is configured to couple a first electrical parameter pulse signal to the first target radio frequency superconducting quantum interference device 310 according to a first state switching instruction; The first target radio frequency superconducting quantum interference device 310 is configured to generate a target magnetic field according to the received first electrical parameter pulse signal, so that the superconducting vortex array layer 400 forms a target vortex array under the action of the target magnetic field that matches the topology of the radio frequency superconducting quantum interference device 300, wherein each vortex in the target vortex array is used to bind a non-Abelian anyon.

[0033] Specifically, non-Abelian anyons refer to quasi-particle excited states in condensed matter physics that possess non-Abelian statistical properties. They are information carriers for topological quantum computing, and their topological properties can achieve noise protection for quantum information.

[0034] The non-Abelian anyon control system 1000 provided in this application is composed of multiple functional modules such as a time division multiplexing module 100, an interferometer switch 200, a radio frequency superconducting quantum interference device 300, and a superconducting vortex array layer 400, which can realize the preparation, weaving, and related quantum information processing of non-Abelian anyons.

[0035] The time division multiplexing module 100 can be understood as the central brain of the control system. It is responsible for receiving external control commands, parsing the command content, determining the target execution components and corresponding control signals, and can divide control resources in the time dimension to achieve efficient control of multiple devices.

[0036] Interferometer switch 200 can be understood as a signal bridge connecting time division multiplexing module 100 and radio frequency superconducting quantum interference device 300. It corresponds one-to-one with radio frequency superconducting quantum interference device 300, and is responsible for receiving and executing state switching instructions and precisely coupling electrical parameter pulse signals.

[0037] The radio frequency superconducting quantum interference device 300 refers to a superconducting device consisting of a single Josephson junction and a superconducting loop. It can be understood as a magnetic field generator that can generate a magnetic field with controllable intensity and polarity under the drive of an electrical parameter pulse signal.

[0038] The superconducting vortex array layer 400 refers to a thin film layer made of p-wave topological superconducting material or type II superconducting material. It is equivalent to a platform for carrying non-Abelian anyons. Under the action of an external magnetic field, it will be excited to form vortices, and each vortex can stably bind a non-Abelian anyon.

[0039] Control commands refer to the instruction signals input from the outside to the time division multiplexing module 100, which include operational requirements related to the preparation and regulation of non-Abelian anyons, and are used to trigger the operation of the non-Abelian anyon control system 1000.

[0040] The first target radio frequency superconducting quantum interference device 310 refers to the specific radio frequency superconducting quantum interference device 300 determined from all radio frequency superconducting quantum interference devices 300 after the time division multiplexing module 100 parses the control instructions, and is used to perform the vortex array preparation task.

[0041] The first control signal refers to the control signal matched by the time-division multiplexing module 100 for the first target radio frequency superconducting quantum interference device 310, including the core instructions and parameters for implementing the operation of the interference device, specifically divided into a first state switching instruction and a first electrical parameter pulse signal. It should be noted that the first control signal may include first electrical parameter pulse signals used to control different radio frequency superconducting quantum interference devices, meaning that the non-Abelian anyon control system provided in this application embodiment can generate multiple non-Abelian anyons in parallel.

[0042] The first state switching instruction is used to control the on / off state of the first target interferometer switch 200, ensuring that the first electrical parameter pulse signal can be accurately coupled to the first target radio frequency superconducting quantum interferometer 310.

[0043] The first electrical parameter pulse signal includes key electrical parameters such as voltage, current, polarity, and amplitude, which can drive the first target radio frequency superconducting quantum interference device 310 to generate the target magnetic field.

[0044] The first target interferometer switch 200 refers to the interferometer switch 200 corresponding to the first target radio frequency superconducting quantum interference device 310. It only responds to the control signal corresponding to the first target radio frequency superconducting quantum interference device 310 it is paired with, and is used to receive the first state switching command sent by the time division multiplexing module 100. It is responsible for the coupling of the first electrical parameter pulse signal with the first target radio frequency superconducting quantum interference device 310.

[0045] The target magnetic field refers to the magnetic field generated by the radio frequency superconducting quantum interference device 300 according to the first electrical parameter pulse signal, which satisfies the control command. Its polarity, intensity and distribution are precisely defined by the first electrical parameter pulse signal.

[0046] The target vortex array refers to the collection of vortices formed by the superconducting vortex array layer 400 under the action of the target magnetic field. Its spatial topology is perfectly matched with the array layout of the radio frequency superconducting quantum interference device 300, ensuring the ordered distribution of non-Abelian anyons.

[0047] First, after the control command is input to the time division multiplexing module 100, the time division multiplexing module 100 parses the control command, first identifies the first target radio frequency superconducting quantum interference device 310 that needs to be activated, and then generates the corresponding first state switching command and first electrical parameter pulse signal according to the array topology requirements.

[0048] Subsequently, the module sends these control signals, namely the first control signals, to the first target interferometer switch 200, which corresponds one-to-one with the first target radio frequency superconducting quantum interference device 310.

[0049] The first target interferometer switch 200 turns on the signal channel according to the first state switching command, and couples the electrical parameter pulse signal to the first target radio frequency superconducting quantum interferometer 310 without distortion.

[0050] The first target radio frequency superconducting quantum interference device 310 converts the electrical parameter pulse signal into a target magnetic field, which acts on the superconducting vortex array layer 400. Under the excitation of the target magnetic field, the superconducting vortex array layer 400 forms a target vortex array, with each vortex binding a non-Abelian anyon, ultimately completing the full-link transformation from control commands to the array of non-Abelian anyons.

[0051] In summary, the non-Abelian anyon control system 1000 provided in this application includes a time-division multiplexing module 100, an interferometer switch 200, a radio frequency superconducting quantum interference device (RF-SUBET) 300, and a superconducting vortex array layer 400. The interferometer switch 200 and the RF-SUBET 300 correspond one-to-one. The time-division multiplexing module 100 is configured to parse received control commands, determine a first target RF-SUBET 310 and a first control signal corresponding to the first target RF-SUBET 310, and send the first control signal to the first target interferometer switch 200. The RF-SUBET 300 includes the first target RF-SUBET 310, and the first target interferometer switch 200 corresponds to the first target RF-SUBET 310. The first control signal includes a first state switching command and a first electrical parameter pulse signal. Next, the first target interferometer switch 200 is configured to couple a first electrical parameter pulse signal to the first target radio frequency superconducting quantum interference device (RF-QFID) 310 according to a first state switching command. Then, the first target RF-QFID 310 is configured to generate a target magnetic field based on the received first electrical parameter pulse signal, causing the superconducting vortex array layer 400 to form a target vortex array under the influence of the target magnetic field, matching the topology of the RF-QFID 300. Each vortex in the target vortex array is used to confine a non-Abelian anyon. Thus, through precise control of the magnetic field parameters generated by the RF-QFID 300 and its topology, periodic or aperiodic non-Abelian anyon arrays can be formed as needed, meeting the requirements of different topological quantum computing scenarios. Furthermore, the interferometer switch 200 and the RF-QFID 300 correspond one-to-one, and the precise control of the target magnetic field by the electrical parameter pulse signal avoids signal crosstalk and ensures the stability of the vortex array, thereby achieving stable confinement of non-Abelian anyons.

[0052] In some implementations, the time-division multiplexing module 100 is configured to: The control commands are parsed to determine the addressing signals; Based on the pre-configured addressing signal-RF superconducting quantum interference device 300 mapping relationship, the first target RF superconducting quantum interference device 310 is determined according to the addressing signal; The control command is parsed to determine the first state switching command and the first electrical parameter pulse signal. The first electrical parameter pulse signal includes a polarity parameter and an amplitude parameter. The polarity parameter is used to determine the polarity of the target magnetic field, and the amplitude parameter is used to control the strength of the target magnetic field.

[0053] Specifically, the addressing signal refers to the identification signal parsed from the control command and used to locate the target device. It can be a specific code, address code or parameter combination, and has uniqueness to ensure that different radio frequency superconducting quantum interference devices 300 can be accurately distinguished.

[0054] The addressing signal-RF superconducting quantum interference device 300 mapping relationship refers to the corresponding rules pre-stored in the time division multiplexing module 100, which binds each unique addressing signal to a certain RF superconducting quantum interference device 300 in the system. It is equivalent to the address book of RF superconducting quantum interference device 300, which is used to quickly lock the target RF superconducting quantum interference device 300 through the addressing signal.

[0055] The first target radio frequency superconducting quantum interference device 310 refers to the specific radio frequency superconducting quantum interference device 300 that needs to perform this magnetic field generation task, as determined by the time division multiplexing module 100 based on the addressing signal and mapping relationship.

[0056] The polarity parameter refers to the key sub-parameter in the first electrical parameter pulse signal, which is used to define the magnetic pole direction of the target magnetic field. It can be divided into positive polarity parameters and negative polarity parameters.

[0057] The amplitude parameter refers to another key sub-parameter in the first electrical parameter pulse signal, which is used to adjust the intensity of the electrical signal, thereby controlling the strength of the magnetic field generated by the radio frequency superconducting quantum interference device 300, and ensuring that the magnetic field strength meets the requirements of the superconducting vortex array layer 400 to excite vortices.

[0058] The time division multiplexing module 100 first decodes and extracts the received control commands, and separates the addressing signal used to locate the first target radio frequency superconducting quantum interference device 310 from the complex command information.

[0059] Next, the time division multiplexing module 100 calls the pre-configured addressing signal-RF superconducting quantum interference device 300 mapping relationship, compares the addressing signal parsed in the first step with the entries in the mapping table one by one, quickly locks the corresponding RF superconducting quantum interference device 300, and defines it as the first target RF superconducting quantum interference device 310.

[0060] After locking onto the first target radio frequency superconducting quantum interference device 310, the time-division multiplexing module 100 re-parses the control commands, extracting the first state switching command for controlling the interferometer switch 200, and the first electrical parameter pulse signal for driving the device to generate a magnetic field. The first electrical parameter pulse signal explicitly includes polarity and amplitude parameters—the polarity parameter directly determines the magnetic pole direction of the target magnetic field, and the amplitude parameter directly controls the strength of the target magnetic field, ensuring that the magnetic field meets the requirements of the superconducting vortex array layer 400 to form a specific vortex.

[0061] Thus, the control command is parsed to determine the addressing signal. Next, based on the pre-configured addressing signal-RF superconducting quantum interference device (RFQFID) 300 mapping relationship, the first target RFQFID 310 is determined according to the addressing signal. Then, the control command is parsed again to determine the first state switching command and the first electrical parameter pulse signal. The first electrical parameter pulse signal includes a polarity parameter and an amplitude parameter; the polarity parameter is used to determine the polarity of the target magnetic field, and the amplitude parameter is used to control the strength of the target magnetic field. In this way, through the addressing signal-RFQFID 300 mapping relationship, it can be ensured that the control signal is accurately delivered to the target RFQFID 300, avoiding signal crosstalk and malfunctions.

[0062] In some embodiments, the first target radio frequency superconducting quantum interference device 310 includes a plurality of radio frequency superconducting quantum interference devices 300, the first control signal further includes timing parameters, and the time division multiplexing module 100 is configured to: Based on the pre-configured topology-RF superconducting quantum interference device 300 mapping table, the control commands are parsed to determine multiple addressing signals; Based on the topology-RF superconducting quantum interference device 300 mapping table, the first target RF superconducting quantum interference device 310 is determined according to multiple addressing signals; Based on timing parameters, the first state switching command and the first electrical parameter pulse signal are sent to the first target interferometer switch 200.

[0063] Specifically, multiple addressing signals refer to a set of identification signals parsed from the control command for locating multiple target interferometers. Each addressing signal corresponds to one radio frequency superconducting quantum interference device 300, and the entire set of signals corresponds one-to-one with the set of interferometers required for the target topology, possessing uniqueness and correlation.

[0064] The first target radio frequency superconducting quantum interference device 310 refers to the specific radio frequency superconducting quantum interference device 300 that the time division multiplexing module 100 determines, based on the addressing signal and the addressing signal-radio frequency superconducting quantum interference device 300 mapping relationship, to perform this magnetic field generation task. With the coordinated operation of all the first target radio frequency superconducting quantum interference devices 310, a magnetic field distribution that meets the topological requirements and usage needs can be generated.

[0065] Timing parameters refer to the time scheduling rules for sending control signals, including the order, interval, and synchronization trigger time of sending the first state switching command and the first electrical parameter pulse signal, which are used to ensure that the magnetic field generation and state switching of multiple first target radio frequency superconducting quantum interference devices 310 are synchronized.

[0066] The time division multiplexing module 100 first decodes and extracts the received control commands, separating multiple addressing signals from the complex command information to locate the first target radio frequency superconducting quantum interference device 310.

[0067] Next, the time division multiplexing module 100 calls the pre-configured addressing signal-RF superconducting quantum interference device 300 mapping relationship, compares the addressing signal parsed in the first step with the entries in the mapping table one by one, quickly locks the corresponding RF superconducting quantum interference device 300, and defines it as the first target RF superconducting quantum interference device 310.

[0068] After locking onto the first target radio frequency superconducting quantum interference device 310, the time-division multiplexing module 100 re-parses the control commands, extracting the first state switching command for controlling the interferometer switch 200, and the first electrical parameter pulse signal for driving the device to generate a magnetic field. The first electrical parameter pulse signal explicitly includes polarity and amplitude parameters—the polarity parameter directly determines the magnetic pole direction of the target magnetic field, and the amplitude parameter directly controls the strength of the target magnetic field, ensuring that the magnetic field meets the requirements of the superconducting vortex array layer 400 to form a specific vortex.

[0069] In this way, the control commands are parsed to determine multiple addressing signals. Next, based on the topology-RF superconducting quantum interference device (RFQFID) 300 mapping table, the first target RFQFID 310 is determined according to the multiple addressing signals. Finally, based on timing parameters, the first state switching command and the first electrical parameter pulse signal are sent to the first target interferometer switch 200. Thus, by using timing parameters, the state switching and magnetic field generation of multiple RFQFIDs 300 can maintain a high degree of coordination, preventing magnetic field distribution disorder caused by asynchronous signal transmission, thereby enabling parallel operation.

[0070] In some embodiments, the polarity parameter includes a positive polarity parameter and a negative polarity parameter. If the polarity parameter is a positive polarity parameter, the first target radio frequency superconducting quantum interference device 310 outputs a first magnetic pole magnetic field; if the polarity parameter is a negative polarity parameter, the first target radio frequency superconducting quantum interference device 310 outputs a second magnetic pole magnetic field.

[0071] Specifically, the positive polarity parameter refers to one of the values ​​of the polarity parameter. It is an instruction parameter that triggers the first target radio frequency superconducting quantum interference device 310 to output a specific magnetic field. Its encoding form matches the system's preset first magnetic field driving logic and has unique identification.

[0072] The negative polarity parameter refers to another value of the polarity parameter, which forms a mutually exclusive relationship with the positive polarity parameter. It is used to trigger the first target radio frequency superconducting quantum interference device 310 to output a second magnetic pole magnetic field opposite to the first magnetic pole. Its encoding form also uniquely corresponds to the second magnetic pole magnetic field driving logic preset by the system.

[0073] The first magnetic pole magnetic field refers to the magnetic field output by the first target radio frequency superconducting quantum interference device 310 under the drive of the positive polarity parameter, which is usually an N pole magnetic field.

[0074] The second magnetic field refers to the magnetic field output by the first target radio frequency superconducting quantum interference device 310 under the drive of the negative polarity parameter. It is opposite in polarity to the first magnetic field and is usually the S-pole magnetic field.

[0075] Thus, the polarity parameters include positive and negative polarity parameters. If the polarity parameter is positive, the first target RF superconducting quantum interference device 310 outputs a first magnetic pole magnetic field; if the polarity parameter is negative, the first target RF superconducting quantum interference device 310 outputs a second magnetic pole magnetic field. This ensures that the magnetic field polarity of each first target RF superconducting quantum interference device 310 can be accurately predicted and controlled, avoiding disordered vortex directions caused by magnetic pole chaos, thereby ensuring the topological integrity of the target vortex array.

[0076] In some implementations, the radio frequency superconducting quantum interference device 300 consists of a single Josephson junction and a superconducting loop.

[0077] Specifically, a Josephson junction refers to a core functional structure consisting of two superconducting materials sandwiching a thin insulating layer or a normal metal layer, exhibiting the Josephson effect. The Josephson effect refers to the ability to transmit superconducting current under zero-voltage conditions and to sensitively respond to external electrical signals, enabling precise control over the on / off state, direction, and magnitude of the superconducting current.

[0078] A superconducting loop is a closed loop made of superconducting materials. It has zero resistance and can minimize energy loss during current transmission, providing a channel for the formation and maintenance of stable superconducting current.

[0079] Without a superconducting loop, the superconducting current generated by the Josephson junction cannot form a closed loop, producing only a transient and weak magnetic field, insufficient to meet the continuous magnetic field required for vortex excitation. Without a single Josephson junction, the current in the superconducting loop cannot be actively controlled, remaining in a fixed state, unable to switch magnetic field polarity and intensity, and unable to adapt to the requirements of vortex arrays with different topologies. Using multiple Josephson junctions leads to severe signal interference, complex control logic, and reduced magnetic field control accuracy.

[0080] Thus, the radio frequency superconducting quantum interference device 300 consists of a single Josephson junction and a superconducting loop. In this way, the single Josephson junction can avoid interference from multiple junctions, making current regulation more precise, thereby ensuring that the polarity and strength of the target magnetic field are perfectly matched with the control command, and guaranteeing the orderliness of the target vortex array.

[0081] In some embodiments, the radio frequency superconducting quantum interference device 300 is in the shape of a ring, and the target magnetic field output by the ring-shaped radio frequency superconducting quantum interference device 300 is rotationally symmetrically distributed, and the magnetic field strength of the target magnetic field gradually decreases outward along the ring axis.

[0082] Specifically, the ring shape refers to the geometry of the superconducting loop in the radio frequency superconducting quantum interference device 300.

[0083] Rotationally symmetric distribution refers to the spatial distribution characteristics of the target magnetic field. Specifically, with the central axis of the circular interferometer as the axis of symmetry, the magnitude and direction of the magnetic field in each radial direction are completely consistent in any plane perpendicular to the axis. The magnetic field lines are distributed in a ring around the axis without obvious bias.

[0084] The annular axis refers to the geometric center axis of the annular interferometer, which is a virtual straight line passing through the center of the annular ring and perpendicular to the plane of the annular ring. It is the central reference for the rotational symmetry distribution of the magnetic field, and the magnetic field strength decreases to both sides outward with the peak value of this axis.

[0085] The gradual decrease in magnetic field strength along the annular axis outwards refers to the intensity gradient characteristic of the target magnetic field. Specifically, along the annular axis, the magnetic field strength reaches its maximum value at the intersection of the annular axis and the superconducting vortex array layer 400, and then steadily decreases according to electromagnetic laws as it moves away from this intersection. This ensures that the magnetic field energy of each radio frequency superconducting quantum interference device 300 is concentrated in its corresponding local region, effectively reducing mutual interference between adjacent magnetic fields in an arrayed layout and providing spatial compatibility for collaborative operation of multiple interferometers.

[0086] Thus, the radio frequency superconducting quantum interference device (RFQFID) 300 is ring-shaped, and the target magnetic field output by the ring-shaped RFQFID 300 is rotationally symmetrically distributed, with the magnetic field strength gradually decreasing outward along the ring axis. This rotational symmetry ensures precise alignment between the vortex center and the interferometer axis, preventing vortex offset or distortion, and ensuring that the topology of the target vortex array is consistent with the topology of the RFQFID 300, thereby improving the accuracy of vortex excitation. Furthermore, the gradual decrease in magnetic field strength outward along the ring axis confines the magnetic field of each RFQFID 300 to its own operating region, ensuring no significant superposition of magnetic fields between adjacent RFQFID 300 devices.

[0087] In some embodiments, the superconducting vortex array layer 400 includes a p-wave topological superconducting material or a target-type superconducting material; the radio frequency superconducting quantum interference device 300 is located on the projection plane of the superconducting vortex array layer 400 to ensure that the target magnetic field can effectively penetrate and excite the vortex.

[0088] Specifically, p-wave topological superconducting materials refer to a class of superconducting materials possessing topological order and p-wave pairing properties. These materials exhibit a unique internal electron pairing mechanism, where vortices formed under magnetic field influence can stably bind Majorana zero modes. For example, strontium-ruthenium oxide (Sr₂RuO₄) is an adaptable material for carrying non-Abelian anyons.

[0089] Target category superconducting materials refer to those that, while not p-wave topological superconductors, belong to type II superconductors. These materials possess the fundamental characteristic of generating vortices under magnetic field influence, satisfying application scenarios without special requirements for anyon statistical properties, and thus have broad applicability. Examples include copper oxide YBa₂Cu₃O₇ and iron-based superconductors LaFeAsO.

[0090] Thus, the superconducting vortex array layer 400 comprises p-wave topological superconducting materials or target-type superconducting materials. The radio frequency superconducting quantum interference device (RFQU) 300 is located on the projection plane of the superconducting vortex array layer 400 to ensure that the target magnetic field can effectively penetrate and excite vortices. In this way, the p-wave topological superconducting material ensures that vortices can effectively confine non-Abelian anyons. Furthermore, the RFQU 300's location on the projection plane of the superconducting vortex array layer 400 shortens the magnetic field transmission path, reduces energy loss, ensures effective magnetic field penetration of the superconducting layer, and avoids vortex excitation failure due to magnetic field attenuation.

[0091] In some embodiments, the topology of the radio frequency superconducting quantum interference device 300 includes a periodic array and / or an aperiodic array. The periodic array includes a square lattice array, a triangular lattice array, and / or a honeycomb lattice. The spatial distribution of the target vortex array corresponds to the lattice position of the topology of the radio frequency superconducting quantum interference device 300.

[0092] Specifically, the topology of the radio frequency superconducting quantum interference device 300 refers to the arrangement and positional relationship of multiple radio frequency superconducting quantum interference devices 300 in space, which is the basis for determining the distribution of the target vortex array.

[0093] Periodic arrays refer to array structures formed by repeating the arrangement of radio frequency superconducting quantum interference devices 300 according to a fixed pattern. Their grid positions follow a uniform geometric period, and they have the characteristics of regular arrangement and strong reproducibility, which facilitates large-scale standardized preparation and control.

[0094] Square grid array is a type of periodic array. The radio frequency superconducting quantum interference device 300 is arranged at the vertex positions of a square grid, with equal spacing between adjacent interferometers and perpendicular lines between grid points. It is the most basic and widely used periodic layout.

[0095] Triangular lattice arrays are a type of periodic array. The radio frequency superconducting quantum interference device 300 is arranged at the vertices of an equilateral triangular lattice, with three adjacent interferometers evenly distributed around each lattice point, resulting in a higher space utilization rate than square lattice arrays.

[0096] A honeycomb grid array is a type of periodic array. The radio frequency superconducting quantum interference device 300 is arranged at the vertex positions of a honeycomb grid, and the grid distribution exhibits hexagonal symmetry, combining regularity and spatial compactness.

[0097] A non-periodic array refers to an array structure of a radio frequency superconducting quantum interference device 300 that does not follow a fixed period and whose arrangement position is flexibly designed according to specific topological calculation requirements. It has no uniform repetition pattern and can adapt to irregular arbitrary sub-distribution requirements.

[0098] The spatial distribution and grid position correspondence means that the grid position of each radio frequency superconducting quantum interference device 300 is matched one-to-one with the position of the vortex excited on the superconducting vortex array layer 400. When the radio frequency superconducting quantum interference device 300 is activated at a certain grid point, a vortex will be excited at the corresponding position, ensuring that the arrangement of the vortex array is completely synchronized with the interferometer array.

[0099] Thus, the topology of the radio frequency superconducting quantum interference device 300 includes periodic arrays and / or aperiodic arrays. The periodic arrays include square lattice arrays, triangular lattice arrays, and / or honeycomb lattice arrays. The spatial distribution of the target vortex array corresponds to the lattice positions of the topology of the radio frequency superconducting quantum interference device 300. In this way, through the optional design of periodic and aperiodic arrays, the arbitrary sub-distribution can meet both the regularization requirements of conventional large-scale computing and the personalized requirements of special tasks.

[0100] In some embodiments, the time-division multiplexing module 100 is further configured to determine the second target radio frequency superconducting quantum interference device 320 and a second control signal corresponding to the second target radio frequency superconducting quantum interference device 320 according to the received topology weaving instruction, and send the second control signal to the second target interference device switch 220, wherein the first target radio frequency superconducting quantum interference device 310 includes the second target radio frequency superconducting quantum interference device 320, and the second control signal includes a second state switching instruction and a second electrical parameter pulse signal; The second target interferometer switch 220 is configured to couple a second electrical parameter pulse signal to the second target radio frequency superconducting quantum interference device 320 according to a second state switching command; The second target radio frequency superconducting quantum interference device 320 is configured to adjust the magnetic field gradient distribution of the target magnetic field according to the received second electrical parameter pulse signal, and guide the vortices in the target vortex array to move along a preset path to achieve topological weaving of non-Abelian anyons.

[0101] Specifically, topology weaving instructions refer to externally input operation instructions, including key information such as the movement path of non-Abelian arbitrarys, timing rules, target positions, and cooperative logic. These instructions are the core basis for triggering and guiding topology weaving operations.

[0102] The second target radio frequency superconducting quantum interference device 320 refers to the radio frequency superconducting quantum interference device 300 that participates in magnetic field modulation during the topology weaving stage. It is a subset of the first target radio frequency superconducting quantum interference device 310, ensuring that the weaving operation is carried out based on the already formed target vortex array and avoiding conflicts with the initialization logic.

[0103] The second control signal refers to the control signal generated for the weaving operation, which consists of a second state switching command and a second electrical parameter pulse signal. The second state switching command is used to control the on / off state of the interferometer switch 200, and the second electrical parameter pulse signal is used to adjust the strength, polarity, and gradient distribution of the magnetic field to adapt to the dynamic changes in the magnetic field during the weaving stage. It should be noted that the received second control signal may include second electrical parameter pulse signals used to control different radio frequency superconducting quantum interference devices, meaning that the non-Abelian anyon control system provided in this application can control multiple non-Abelian anyons in parallel.

[0104] The second target interferometer switch 220 refers to the signal transmission switch that corresponds one-to-one with the second target radio frequency superconducting quantum interference device 320. It is responsible for receiving and executing the second state switching command, and coupling the second electrical parameter pulse signal to the target interferometer without distortion, thereby avoiding signal crosstalk and mistransmission.

[0105] Magnetic field gradient distribution refers to the spatial variation characteristics of magnetic field strength, that is, the magnetic field strength varies at different locations, forming a gradient difference between high field strength and low field strength. It is the physical basis for generating directional forces and guiding vortices to move along a predetermined path.

[0106] The preset path refers to the non-Abelian arbitrary child movement trajectory specified in the topology weaving instruction, which consists of multiple consecutive interferometer lattice points to ensure that the weaving operation is carried out in an orderly manner according to the preset quantum logic.

[0107] Topological weaving refers to quantum operations formed by moving, exchanging positions, or entangled non-Abelian anyons along a predetermined path. It can utilize the topological properties of anyons to generate quantum entanglement, thus enabling the logic gate function of topological quantum computing. It should be noted that adiabatic weaving can be achieved by controlling the vortex velocity during topological weaving.

[0108] First, the topology weaving command is input to the time-division multiplexing module 100. This module, as the core control unit of the system, first parses the path planning and timing requirements in the command, and then selects the second target RF superconducting quantum interference device (RFQUANDAV) 320 from the first target RFQU 310 to participate in the weaving operation. Next, the time-division multiplexing module 100 generates a second control signal according to the command requirements, including a second state switching command and a second electrical parameter pulse signal. The second state switching command specifies the on / off timing of the second target interferometer switch 220, ensuring that signal transmission matches the vortex movement rhythm. The second electrical parameter pulse signal sets key parameters such as polarity, amplitude, and timing parameters for each second target interferometer according to the magnetic field gradient adjustment requirements.

[0109] Subsequently, the time-division multiplexing module 100 sends the second control signal to the corresponding second target interferometer switch 220. The second target interferometer switch 220 precisely controls the on / off state according to the second state switching command, stably coupling the second electrical parameter pulse signal to the second target radio frequency superconducting quantum interference device 320. After receiving the signal, these second target radio frequency superconducting quantum interference devices 320 adjust the strength and polarity of their own output magnetic field to form a preset magnetic field gradient distribution in a specific region of the superconducting vortex array layer 400. That is, based on the difference in magnetic field strength at different locations, a directional "magnetic field thrust" is generated, driving the vortices in the target vortex array that bind non-Abelian anyons to move strictly along the preset path planned by the topological weaving command. During the movement, multiple second target radio frequency superconducting quantum interference devices 320 work collaboratively under the unified timing control of the time-division multiplexing module 100. Some second target radio frequency superconducting quantum interference devices 320 enhance the magnetic field, while others weaken the magnetic field, continuously optimizing the magnetic field gradient distribution to ensure uniform vortex movement speed and precise path, avoiding collisions or annihilation.

[0110] Please see Figure 2 , Figure 2 This diagram illustrates the movement of a vortex. The top, middle, and bottom images correspond to times t1, t2, and t3, respectively. At time t1, the A-band radio frequency superconducting quantum interference device (RFQUAD) is activated, generating a magnetic field and creating a vortex anyon in the superconducting vortex layer. At time t2, RFQUAD element A is deactivated, while RFQUAD element B is activated. The magnetic field at element B induces the vortex to move towards element B until it reaches a stable position. At time t3, during the vortex movement, its speed increases as it approaches element B.

[0111] Please see Figure 3 , Figure 3This diagram illustrates vortex fusion. The top, middle, and bottom images correspond to times t4, t5, and t6, respectively. At time t1, both radio frequency superconducting quantum interference devices (RFQIs) A and B are activated, generating magnetic fields and creating a vortex anyon in the superconducting vortex layer. At time t2, RFQI element A is deactivated, and the magnetic field at element B induces the vortex at A to move towards element B. At time t3, during the vortex movement, the vortex's speed increases as it approaches element B.

[0112] Thus, the time-division multiplexing module 100 is further configured to determine the second target RF superconducting quantum interference device 320 and a second control signal corresponding to the second target RF superconducting quantum interference device 320 according to the received topology weaving instruction, and send the second control signal to the second target interference device switch 220. The first target RF superconducting quantum interference device 310 includes the second target RF superconducting quantum interference device 320, and the second control signal includes a second state switching instruction and a second electrical parameter pulse signal. Next, the second target interference device switch 220 is configured to couple the second electrical parameter pulse signal to the second target RF superconducting quantum interference device 320 according to the second state switching instruction. Finally, the second target RF superconducting quantum interference device 320 is configured to adjust the magnetic field gradient distribution of the target magnetic field according to the received second electrical parameter pulse signal, guiding the vortices in the target vortex array to move along a preset path to achieve topology weaving of non-Abelian anyons. In this way, by dynamically adjusting the magnetic field gradient distribution, the vortex movement can be made smooth, reducing quantum state distortion and ensuring the integrity of quantum information. Furthermore, the topology weaving instructions are analyzed to accurately select the interferometers involved in the weaving, avoiding signal crosstalk and irrelevant magnetic field interference, and ensuring that the vortex moves along the preset path.

[0113] Please see Figure 4 In some embodiments, the non-Abelian anyon control system 1000 further includes a detection module 500; the detection module 500 is configured to detect the existence state and associated quantum properties of the vortex to be tested in the target vortex array, so as to read the quantum information carried by the non-Abelian anyon in the vortex to be tested, including the fused vortex obtained by topological weaving.

[0114] Specifically, the detection module 500 refers to the functional component in the non-Abelian anyon control system 1000 responsible for state perception and information reading. By collecting physical signals and analyzing key characteristics, it transforms the physical state of the vortex into identifiable quantum information and provides feedback signals to the non-Abelian anyon control system 1000.

[0115] The vortex to be tested refers to a specific vortex that needs to be detected and its information read. It is the core detection object of the detection module 500, covering the initial vortex in the preparation stage and the fused vortex after the weaving stage.

[0116] A fused vortex refers to a single vortex formed by multiple vortices moving to the same position and merging after a topological weaving operation. Its correlated quantum properties integrate the quantum information of the original multiple vortices and are the key object for reading quantum computing results.

[0117] The existence state refers to the physical existence and stability of the vortex under test in the superconducting vortex array layer 400, including whether the vortex is generated, whether it remains intact, and whether it is accidentally annihilated or merged.

[0118] Related quantum properties: Physical properties directly related to non-Abelian anyon quantum states, usually the parity of fermion parity, are the core physical carriers of quantum information, and their changes directly reflect the evolution of quantum states.

[0119] Quantum information refers to information stored based on the principles of quantum mechanics, with qubits as the basic unit, and is the core processing object of quantum computing.

[0120] The detection module 500 first docks with the superconducting vortex array layer 400 to determine the detection range of the vortex to be tested, including the initial vortex generated during the preparation stage and the fused vortex formed after topological weaving.

[0121] For the initial vortex, the detection module 500 determines the existence state of the vortex by collecting physical signals such as magnetic field distribution signal and charge response signal. If the detected magnetic field peak reaches a preset threshold and the signal is stable without attenuation, the vortex is determined to exist effectively and carry a non-Abelian anyon; if the signal is weak or there is no signal, it is determined to be an invalid vortex and does not carry anyon.

[0122] For fused vortices, after confirming their existence and stable state, the detection module 500 analyzes related quantum properties such as fermion parity parity odd and even. That is, by detecting quantum signals such as the ground state energy transition characteristics and magnetic field polarity changes after vortex fusion, it distinguishes between odd and even parity.

[0123] Thus, the detection module 500 is configured to detect the existence state and correlated quantum properties of the vortex to be tested in the target vortex array, in order to read the quantum information carried by the non-Abelian anyons in the vortex to be tested, including fused vortices obtained after topological weaving. In this way, the detection module 500 constructs a transformation path from physical state to quantum information by specifically detecting the topologically woven vortex to be tested, combined with the dual detection of the fundamental existence and correlated quantum properties of the vortex.

[0124] Please see Figure 5 This application also provides a non-Abelian anyon control method, based on the aforementioned non-Abelian anyon control system 1000, the method comprising: 01: Parse the received control commands to determine the first target radio frequency superconducting quantum interference device and the first control signal corresponding to the first target radio frequency superconducting quantum interference device; 02: According to the first state switching instruction, the first electrical parameter pulse signal is coupled to the first target radio frequency superconducting quantum interference device; 03: Continuously output the target magnetic field according to the received first electrical parameter pulse signal, so that the superconducting vortex array layer forms and maintains a target vortex array that matches the topology of the radio frequency superconducting quantum interference device under the action of the target magnetic field.

[0125] Specifically, the control commands are first decoded to extract core information such as the topology requirements and vortex density of the vortex array. Then, combined with the pre-configured addressing signal-RF superconducting quantum interference device (RFQFID) 300 mapping relationship, an RFQFID 300 that meets the magnetic field distribution requirements is selected and designated as the first target RFQFID 310. Finally, a first control signal is generated according to the command requirements. The first control signal includes a first state switching command and a first electrical parameter pulse signal. The first state switching command specifies the on / off timing of the first target interferometer switch 200, while the first electrical parameter pulse signal sets specific parameters such as voltage amplitude and current frequency according to the magnetic field strength and polarity requirements, ensuring that the signal matches the hardware characteristics of the target interferometer.

[0126] The first target interferometer switch 200 connects the signal transmission channel under a preset timing sequence, and couples the first electrical parameter pulse signal to the corresponding first target radio frequency superconducting quantum interferometer 310 without loss or crosstalk.

[0127] After receiving the first electrical parameter pulse signal, the first target radio frequency superconducting quantum interference device 310 outputs a corresponding N-pole / S-pole magnetic field according to the polarity parameter of the pulse signal, and controls the magnetic field strength according to the amplitude parameter, ultimately forming a target magnetic field that matches its own topological structure. This target magnetic field penetrates into the superconducting vortex array layer 400, causing the material within the layer to generate a topological response and form an ordered target vortex array.

[0128] Thus, the received control commands are parsed to determine the first target RF superconducting quantum interference device 310 and the first control signal corresponding to it. The first control signal includes a first state switching command and a first electrical parameter pulse signal. Next, according to the first state switching command, the first electrical parameter pulse signal is coupled to the first target RF superconducting quantum interference device 310. Finally, according to the received first electrical parameter pulse signal, a target magnetic field is continuously output to cause the superconducting vortex array layer 400 to form and maintain a target vortex array matching the topology of the RF superconducting quantum interference device 300 under the action of the target magnetic field. In this way, through precise control of the magnetic field parameters generated by the RF superconducting quantum interference device 300 and its topology, periodic or aperiodic non-Abelian anyson arrays can be formed as needed to meet the requirements of different topological quantum computing scenarios. Furthermore, the interferometer switch 200 and the radio frequency superconducting quantum interference device 300 correspond one-to-one. Combined with the precise control of the target magnetic field by the electrical parameter pulse signal, signal crosstalk can be avoided and the stability of the vortex array can be ensured, thereby achieving stable binding of non-Abelian anyons.

[0129] This application also provides a computer-readable storage medium containing a computer program. When the computer program is executed by one or more processors, it causes the one or more processors to perform the method of this application.

[0130] It is understood that a computer program includes computer program code. Computer program code can be in the form of source code, object code, executable files, or some intermediate form. Computer-readable storage media can include: any entity or device capable of carrying computer program code, recording media, USB flash drives, portable hard drives, magnetic disks, optical disks, computer memory, read-only memory (ROM), random access memory (RAM), and software distribution media, etc.

[0131] In this specification, the terms "specifically," "furthermore," "particularly," "understandably," etc., refer to specific features, structures, materials, or characteristics described in connection with embodiments or examples that are included in at least one embodiment or example of this application. In this specification, the illustrative expressions of the above terms do not necessarily refer to the same embodiment or example. Furthermore, the specific features, structures, materials, or characteristics described may be combined in any suitable manner in one or more embodiments or examples. Moreover, without contradiction, those skilled in the art can combine and integrate the different embodiments or examples described in this specification, as well as the features of different embodiments or examples.

[0132] Any process or method described in the flowchart or otherwise herein can be understood as representing a module, segment, or portion of code comprising one or more executable instructions for implementing a particular logical function or process, and the scope of the preferred embodiments of this application includes additional implementations in which functions may be performed not in the order shown or discussed, including substantially simultaneously or in reverse order depending on the function involved, as will be understood by those skilled in the art to which embodiments of this application pertain.

[0133] Although embodiments of this application have been shown and described above, it is understood that the above embodiments are exemplary and should not be construed as limiting this application. Those skilled in the art can make changes, modifications, substitutions and variations to the above embodiments within the scope of this application.

Claims

1. A non-Abelian any subsystem control system, characterized in that, The non-Abelian anyon control system includes a time-division multiplexing module, an interferometer switch, a radio frequency superconducting quantum interference device (RF quantum interference device), and a superconducting vortex array layer, wherein the interferometer switch and the RF quantum interference device are in one-to-one correspondence. The time-division multiplexing module is configured to parse the received control command, determine the first target radio frequency superconducting quantum interference device (RF-SQFID) and a first control signal corresponding to the first target RF-SQFID, and send the first control signal to the first target interference device switch. The RF-SQFID includes the first target RF-SQFID, the first target interference device switch corresponds to the first target RF-SQFID, and the first control signal includes a first state switching command and a first electrical parameter pulse signal. The first target interferometer switch is configured to couple the first electrical parameter pulse signal to the first target radio frequency superconducting quantum interference device according to the first state switching instruction; The first target radio frequency superconducting quantum interference device is configured to generate a target magnetic field based on a received first electrical parameter pulse signal, so that the superconducting vortex array layer forms a target vortex array under the action of the target magnetic field that matches the topology of the radio frequency superconducting quantum interference device, wherein each vortex in the target vortex array is used to bind one of the non-Abelian anyons.

2. The system according to claim 1, characterized in that, The time-division multiplexing module is configured as follows: The control command is parsed to determine the addressing signal; Based on the pre-configured addressing signal-RF superconducting quantum interference device (RFQUMP) mapping relationship, the first target RFQUMP is determined according to the addressing signal. The control command is parsed to determine the first state switching command and the first electrical parameter pulse signal, wherein the first electrical parameter pulse signal includes a polarity parameter and an amplitude parameter, the polarity parameter is used to determine the polarity of the target magnetic field, and the amplitude parameter is used to control the strength of the target magnetic field.

3. The system according to claim 2, characterized in that, The first target radio frequency superconducting quantum interference device includes multiple radio frequency superconducting quantum interference devices, the first control signal further includes timing parameters, and the time division multiplexing module is configured as follows: The control command is parsed to determine multiple addressing signals; Based on the addressing signal-RF superconducting quantum interference device (RFQID) mapping relationship, the first target RFQID is determined according to multiple addressing signals. Based on the timing parameters, the first state switching command and the first electrical parameter pulse signal are sent to the first target interferometer switch.

4. The system according to claim 2, characterized in that, The polarity parameter includes a positive polarity parameter and a negative polarity parameter. If the polarity parameter is the positive polarity parameter, the first target radio frequency superconducting quantum interference device outputs a first magnetic pole magnetic field; if the polarity parameter is the negative polarity parameter, the first target radio frequency superconducting quantum interference device outputs a second magnetic pole magnetic field.

5. The non-Abelian any subsystem control system according to claim 1, characterized in that, The radio frequency superconducting quantum interference device consists of a single Josephson junction and a superconducting loop.

6. The non-Abelian any subsystem control system according to claim 5, characterized in that, The radio frequency superconducting quantum interference device is circular in shape, and the target magnetic field output by the circular radio frequency superconducting quantum interference device is rotationally symmetrically distributed, and the magnetic field strength of the target magnetic field gradually decreases outward along the axis of the circular ring.

7. The non-Abelian any subcontrol system according to claim 1, characterized in that, The superconducting vortex array layer comprises a p-wave topological superconducting material or a target-type superconducting material; the radio frequency superconducting quantum interference device is located on the projection plane of the superconducting vortex array layer to ensure that the target magnetic field can effectively penetrate and excite the vortex.

8. The non-Abelian any subcontrol system according to claim 1, characterized in that, The topology of the radio frequency superconducting quantum interference device includes a periodic array and / or a non-periodic array. The periodic array includes a square lattice array, a triangular lattice array, and / or a honeycomb lattice. The spatial distribution of the target vortex array corresponds to the lattice position of the topology of the radio frequency superconducting quantum interference device.

9. The non-Abelian any subsystem control system according to claim 1, characterized in that, The time-division multiplexing module is further configured to determine a second target radio frequency superconducting quantum interference device (RF-SQU) and a second control signal corresponding to the second target RF-SQU according to the received topology weaving instruction, and send the second control signal to the second target interference device switch, wherein the first target RF-SQU includes the second target RF-SQU, and the second control signal includes a second state switching instruction and a second electrical parameter pulse signal; The second target interferometer switch is configured to couple the second electrical parameter pulse signal to the second target radio frequency superconducting quantum interference device according to the second state switching command; The second target radio frequency superconducting quantum interference device is configured to adjust the magnetic field gradient distribution of the target magnetic field according to the received second electrical parameter pulse signal, and guide the vortices in the target vortex array to move along a preset path to realize the topological weaving of the non-Abelian anyons.

10. The non-Abel arbitrary subcontrol system according to any one of claims 9, characterized in that, The non-Abel any subcontrol system also includes a detection module; The detection module is configured to detect the existence state and associated quantum properties of the vortex to be tested in the target vortex array, so as to read the quantum information carried by the non-Abelian anyons in the vortex to be tested, the vortex to be tested including the fused vortex obtained after the topological weaving.

11. A non-Abelian anyon control method, characterized in that, The method is based on the non-Abelian any subsystem control system as described in claims 1-10, and the method includes: The received control command is parsed to determine the first target radio frequency superconducting quantum interference device and the first control signal corresponding to the first target radio frequency superconducting quantum interference device. The first control signal includes a first state switching command and a first electrical parameter pulse signal. According to the first state switching instruction, the first electrical parameter pulse signal is coupled to the first target radio frequency superconducting quantum interference device; The target magnetic field is continuously output according to the received first electrical parameter pulse signal, so that the superconducting vortex array layer forms and maintains a target vortex array that matches the topology of the radio frequency superconducting quantum interference device under the action of the target magnetic field.

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