Pub Date : 2024-07-03DOI: 10.1007/s11128-024-04474-y
She-Xiang Jiang, Jin Shi
In this paper, a new scheme for asymmetric cyclic controlled teleportation of arbitrary three-dimensional unknown quantum states is proposed by performing three-dimensional Bell-state measurements and three-dimensional Hadamard transformation. The entangled state of thirteen-qutrit acts as the quantum channel to connect senders and receivers, which is constructed by a three-qutrit entangled state and five two-qutrit entangled states. In this scheme, Alice wants to transmit an arbitrary unknown single-qutrit state to Bob, at the same time, Bob wants to transmit an arbitrary unknown two-qutrit entangled state to Charlie and Charlie wants to transmit an arbitrary unknown three-qutrit entangled state to Alice under the control of the supervisor David. Participants can reconstruct the original states and make the scheme perfectly by performing appropriate unitary operation. Then, the scheme can be generalized to realize the asymmetric cyclic controlled quantum teleportation of N (N > 3) participants in the three-dimensional system, and come up with two universal schemes are determined by the parity of the participant. Furthermore, the scheme is investigated in two different noisy channels: amplitude-damping noise and phase-damping noise, and calculated the fidelities of the output states. It is demonstrated that the fidelities only depend on the coefficients of the initial state and the decoherence noisy rate. The security of the scheme is briefly analyzed and compares with the previous schemes in terms of efficiency. The proposed scheme contributes to advancing understanding of high-dimensional quantum teleportation.
{"title":"Multi-party three-dimensional asymmetric cyclic controlled quantum teleportation in noisy environment","authors":"She-Xiang Jiang, Jin Shi","doi":"10.1007/s11128-024-04474-y","DOIUrl":"https://doi.org/10.1007/s11128-024-04474-y","url":null,"abstract":"<p>In this paper, a new scheme for asymmetric cyclic controlled teleportation of arbitrary three-dimensional unknown quantum states is proposed by performing three-dimensional Bell-state measurements and three-dimensional Hadamard transformation. The entangled state of thirteen-qutrit acts as the quantum channel to connect senders and receivers, which is constructed by a three-qutrit entangled state and five two-qutrit entangled states. In this scheme, Alice wants to transmit an arbitrary unknown single-qutrit state to Bob, at the same time, Bob wants to transmit an arbitrary unknown two-qutrit entangled state to Charlie and Charlie wants to transmit an arbitrary unknown three-qutrit entangled state to Alice under the control of the supervisor David. Participants can reconstruct the original states and make the scheme perfectly by performing appropriate unitary operation. Then, the scheme can be generalized to realize the asymmetric cyclic controlled quantum teleportation of <i>N</i> (<i>N</i> > 3) participants in the three-dimensional system, and come up with two universal schemes are determined by the parity of the participant. Furthermore, the scheme is investigated in two different noisy channels: amplitude-damping noise and phase-damping noise, and calculated the fidelities of the output states. It is demonstrated that the fidelities only depend on the coefficients of the initial state and the decoherence noisy rate. The security of the scheme is briefly analyzed and compares with the previous schemes in terms of efficiency. The proposed scheme contributes to advancing understanding of high-dimensional quantum teleportation.</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-07-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514374","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-07-02DOI: 10.1007/s11128-024-04470-2
Przemysław Kościk
We study the ground-state entanglement between two atoms in a two-dimensional isotropic harmonic trap. We consider a finite-range soft-core interaction that can be applied to simulate various atomic systems. We provide detailed results on the dependence of the correlations on the parameters of the system. Our investigations show that in the hardcore limit, the wave function can be approximated as the product of the radial and angular components regardless of the interaction range. This implies that the radial and angular correlations are independent of one another. However, correlations within the radial and angular components persist and are heavily influenced by the interaction range. The radial correlations are generally weaker than the angular correlations. When soft-core interactions are considered, the correlations exhibit more complex behavior.
{"title":"Radial and angular correlations in a confined system of two atoms in two-dimensional geometry","authors":"Przemysław Kościk","doi":"10.1007/s11128-024-04470-2","DOIUrl":"https://doi.org/10.1007/s11128-024-04470-2","url":null,"abstract":"<p>We study the ground-state entanglement between two atoms in a two-dimensional isotropic harmonic trap. We consider a finite-range soft-core interaction that can be applied to simulate various atomic systems. We provide detailed results on the dependence of the correlations on the parameters of the system. Our investigations show that in the hardcore limit, the wave function can be approximated as the product of the radial and angular components regardless of the interaction range. This implies that the radial and angular correlations are independent of one another. However, correlations within the radial and angular components persist and are heavily influenced by the interaction range. The radial correlations are generally weaker than the angular correlations. When soft-core interactions are considered, the correlations exhibit more complex behavior.</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-07-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514375","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-26DOI: 10.1007/s11128-024-04465-z
Abdulbasit M. A. Sabaawi, Mohammed R. Almasaoodi, Sándor Imre
Orthogonal frequency-division multiplexing (OFDM) is a crucial modulation method used in contemporary digital communication systems for its significant spectral efficiency, low latency, and robustness in challenging environments. This work examines the novel use of OFDM in quantum communication, an area that offers exceptional security and efficiency in information transfer using quantum mechanics principles. In the rapidly evolving field of quantum computing, understanding, and mitigating quantum bit errors is paramount. This paper presents a rigorous analysis of bit error rates (BER) in quantum circuits, focusing on the impact of the quantum Fourier transform and its inverse, contrasted against quantum circuits employing dynamic gate sequences. Our research methodology encompasses simulations over a diverse set of parameters, including varying qubit counts ranging from 2 to 8 and theta angles (15, 30, 45, and 60°), as well as random theta values, utilizing the advanced capabilities of the Qiskit framework. Our findings indicate that quantum OFDM substantially improves quantum communication, lowering errors and boosting security. The quantum model outperforms the reference model in BER, with further enhancements as qubits increase.
{"title":"Exploiting OFDM method for quantum communication","authors":"Abdulbasit M. A. Sabaawi, Mohammed R. Almasaoodi, Sándor Imre","doi":"10.1007/s11128-024-04465-z","DOIUrl":"https://doi.org/10.1007/s11128-024-04465-z","url":null,"abstract":"<p>Orthogonal frequency-division multiplexing (OFDM) is a crucial modulation method used in contemporary digital communication systems for its significant spectral efficiency, low latency, and robustness in challenging environments. This work examines the novel use of OFDM in quantum communication, an area that offers exceptional security and efficiency in information transfer using quantum mechanics principles. In the rapidly evolving field of quantum computing, understanding, and mitigating quantum bit errors is paramount. This paper presents a rigorous analysis of bit error rates (BER) in quantum circuits, focusing on the impact of the quantum Fourier transform and its inverse, contrasted against quantum circuits employing dynamic gate sequences. Our research methodology encompasses simulations over a diverse set of parameters, including varying qubit counts ranging from 2 to 8 and theta angles (15, 30, 45, and 60°), as well as random theta values, utilizing the advanced capabilities of the Qiskit framework. Our findings indicate that quantum OFDM substantially improves quantum communication, lowering errors and boosting security. The quantum model outperforms the reference model in BER, with further enhancements as qubits increase.</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514376","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-25DOI: 10.1007/s11128-024-04461-3
Juan Carlos Garcia-Escartin
This paper presents a hybrid variational quantum algorithm that finds a random eigenvector of a unitary matrix with a known quantum circuit. The algorithm is based on the SWAP test on trial states generated by a parametrized quantum circuit. The eigenvector is described by a compact set of classical parameters that can be used to reproduce the found approximation to the eigenstate on demand. This variational eigenvector finder can be adapted to solve the generalized eigenvalue problem, to find the eigenvectors of normal matrices and to perform quantum principal component analysis on unknown input mixed states. These algorithms can all be run with low-depth quantum circuits, suitable for an efficient implementation on noisy intermediate-scale quantum computers and, with some restrictions, on linear optical systems. In full-scale quantum computers, where there might be optimization problems due to barren plateaus in larger systems, the proposed algorithms can be used as a primitive to boost known quantum algorithms. Limitations and potential applications are discussed.
{"title":"Finding eigenvectors with a quantum variational algorithm","authors":"Juan Carlos Garcia-Escartin","doi":"10.1007/s11128-024-04461-3","DOIUrl":"https://doi.org/10.1007/s11128-024-04461-3","url":null,"abstract":"<p>This paper presents a hybrid variational quantum algorithm that finds a random eigenvector of a unitary matrix with a known quantum circuit. The algorithm is based on the SWAP test on trial states generated by a parametrized quantum circuit. The eigenvector is described by a compact set of classical parameters that can be used to reproduce the found approximation to the eigenstate on demand. This variational eigenvector finder can be adapted to solve the generalized eigenvalue problem, to find the eigenvectors of normal matrices and to perform quantum principal component analysis on unknown input mixed states. These algorithms can all be run with low-depth quantum circuits, suitable for an efficient implementation on noisy intermediate-scale quantum computers and, with some restrictions, on linear optical systems. In full-scale quantum computers, where there might be optimization problems due to barren plateaus in larger systems, the proposed algorithms can be used as a primitive to boost known quantum algorithms. Limitations and potential applications are discussed.\u0000</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-06-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514386","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-25DOI: 10.1007/s11128-024-04377-y
Yuxin Ji, Qinghui Chen, Rui Wang, Naihua Ji, Hongyang Ma
Quantum error correction techniques are important for implementing fault-tolerant quantum computation, and topological quantum error correcting codes provide feasibility for implementing large-scale fault-tolerant quantum computation. Here, we propose a deep reinforcement learning framework for implementing quantum error correction algorithms for errors on heavy hexagonal codes. Specifically, we construct the double deep Q learning model with policy reuse method, so that the decoding agent does not have to explore the learning from scratch when dealing with new error syndrome, but instead reuses past policies, which can reduce the computational complexity. And the double deep Q network can avoid the problem of threshold being overestimated and get the true decoding threshold. Our experimental results show that the error correction accuracy of our decoder can reach 91.86%. Different thresholds are obtained according to the code distance, which is 0.0058 when the code distance is 3, 5, 7, and 0.0065 when the code distance is 5, 7, 9, both higher than that of the classical minimum weight perfect matching decoder. Compared to the threshold of the MWPM decoder under the depolarizing noise model, the threshold of our decoder is improved by 32.63%, which enables better fault-tolerant quantum computation.
{"title":"Quantum error correction for heavy hexagonal code using deep reinforcement learning with policy reuse","authors":"Yuxin Ji, Qinghui Chen, Rui Wang, Naihua Ji, Hongyang Ma","doi":"10.1007/s11128-024-04377-y","DOIUrl":"https://doi.org/10.1007/s11128-024-04377-y","url":null,"abstract":"<p>Quantum error correction techniques are important for implementing fault-tolerant quantum computation, and topological quantum error correcting codes provide feasibility for implementing large-scale fault-tolerant quantum computation. Here, we propose a deep reinforcement learning framework for implementing quantum error correction algorithms for errors on heavy hexagonal codes. Specifically, we construct the double deep <i>Q</i> learning model with policy reuse method, so that the decoding agent does not have to explore the learning from scratch when dealing with new error syndrome, but instead reuses past policies, which can reduce the computational complexity. And the double deep <i>Q</i> network can avoid the problem of threshold being overestimated and get the true decoding threshold. Our experimental results show that the error correction accuracy of our decoder can reach 91.86%. Different thresholds are obtained according to the code distance, which is 0.0058 when the code distance is 3, 5, 7, and 0.0065 when the code distance is 5, 7, 9, both higher than that of the classical minimum weight perfect matching decoder. Compared to the threshold of the MWPM decoder under the depolarizing noise model, the threshold of our decoder is improved by 32.63%, which enables better fault-tolerant quantum computation.</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-06-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514387","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-24DOI: 10.1007/s11128-024-04453-3
Kyo Inoue, Toshimori Honjo
A quantum conference key agreement (QCKA) protocol based on differential-phase-shift quantum key distribution is presented, which provides a common secret key for secure communication between more than two parties. In the proposed protocol, one party simultaneously broadcasts a weak coherent pulse train with {0, π} phases to multiple parties that measure the phase differences between adjacent pulses using a delay interferometer followed by photon detectors, and the transmitter and receivers share secret key bits from the coincident counts in the receivers. The system setup and operation are simpler than those of conventional QCKA schemes that use a multipartite quantum entanglement state. The key creation performance is evaluated by considering the eavesdropping probability. The results indicate that the proposed scheme offers better performance than the conventional entanglement-based QCKA system.
{"title":"Quantum conference key agreement based on differential-phase-shift quantum key distribution","authors":"Kyo Inoue, Toshimori Honjo","doi":"10.1007/s11128-024-04453-3","DOIUrl":"https://doi.org/10.1007/s11128-024-04453-3","url":null,"abstract":"<p>A quantum conference key agreement (QCKA) protocol based on differential-phase-shift quantum key distribution is presented, which provides a common secret key for secure communication between more than two parties. In the proposed protocol, one party simultaneously broadcasts a weak coherent pulse train with {0, <i>π</i>} phases to multiple parties that measure the phase differences between adjacent pulses using a delay interferometer followed by photon detectors, and the transmitter and receivers share secret key bits from the coincident counts in the receivers. The system setup and operation are simpler than those of conventional QCKA schemes that use a multipartite quantum entanglement state. The key creation performance is evaluated by considering the eavesdropping probability. The results indicate that the proposed scheme offers better performance than the conventional entanglement-based QCKA system.</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-06-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514385","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-24DOI: 10.1007/s11128-024-04440-8
Cong Xu, Qing-Hua Zhang, Shao-Ming Fei
Uncertainty principle is one of the most fundamental features in quantum mechanics and plays a significant role in quantum information processing. We establish tighter summation form of the uncertainty relations based on metric-adjusted skew information via operator representation of observables, which improves the existing results. By employing the methodologies of sampling coordinates of observables, we also present tighter product form of the uncertainty relations. Detailed examples are given to illustrate the advantages of our uncertainty relations.
{"title":"The summation and product forms of the uncertainty relations based on metric-adjusted skew information","authors":"Cong Xu, Qing-Hua Zhang, Shao-Ming Fei","doi":"10.1007/s11128-024-04440-8","DOIUrl":"https://doi.org/10.1007/s11128-024-04440-8","url":null,"abstract":"<p>Uncertainty principle is one of the most fundamental features in quantum mechanics and plays a significant role in quantum information processing. We establish tighter summation form of the uncertainty relations based on metric-adjusted skew information via operator representation of observables, which improves the existing results. By employing the methodologies of sampling coordinates of observables, we also present tighter product form of the uncertainty relations. Detailed examples are given to illustrate the advantages of our uncertainty relations.\u0000</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-06-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514384","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-24DOI: 10.1007/s11128-024-04460-4
Hao Sun, Fenzhuo Guo, Haifeng Dong, Fei Gao
The sharing of quantum nonlocality has been the subject of much recent research for two-qubit and three-qubit entangled systems. In this paper, we discuss nonlocality sharing with unsharp measurement based on Mermin–Ardehali–Belinskii–Klyshko (MABK) inequality for the N-qubit generalized Greenberger–Horne–Zeilinger (GHZ) system. In the one-sided sequential measurements scenario, we determine a state range associated with k within which ( k+1 ) independent observers can share the standard N-partite nonlocality with the other ((N-1)) sides, as well as a state range where arbitrarily many independent observers can do the same. Similarly, as to the m-sided sequential measurements scenario, we also identify a state range influenced by k within which ( k+1 ) independent observers in each of m sides can share the standard N-partite nonlocality with the other ((N-m)) sides, and a state range where arbitrarily many independent observers can do so. Crucially, all of our nonlocality sharing findings result from a measurement strategy in which every sequential observer employs unequal sharpness measurements. As a special case, for the three-qubit maximally entangled GHZ state, we demonstrate that an unbounded number of observers can share the nonlocality in the one-sided sequential measurements scenario. This outcome further underscores the importance of unequal sharpness measurements in recycling qubits for generating quantum nonlocality.
量子非局域性的共享一直是近年来二量子比特和三量子比特纠缠系统研究的主题。本文基于 N 量子位广义格林伯格-霍恩-泽林格(GHZ)系统的 Mermin-Ardehali-Belinskii-Klyshko (MABK)不等式,讨论了非尖锐测量的非局域性共享。在单边顺序测量场景中,我们确定了一个与k相关的状态范围,在这个范围内,( k+1 )个独立观测者可以与其他((N-1))边共享标准的N边非局域性,以及一个任意多个独立观测者都可以这样做的状态范围。同样,对于 m 边顺序测量的情况,我们也确定了一个受 k 影响的状态范围,在这个范围内,m 边中每边的( k+1 )个独立观察者可以与其他((N-m))边共享标准的 N 边非位置性,还有一个任意多的独立观察者可以这样做的状态范围。最重要的是,我们所有的非局域性共享发现都来自于一种测量策略,在这种策略中,每个顺序观测者都采用了不相等的锐度测量。作为一个特例,对于三量子位最大纠缠 GHZ 状态,我们证明了在单边顺序测量的情况下,无限制数量的观察者可以共享非局域性。这一结果进一步强调了回收量子比特中不等锐度测量对产生量子非位置性的重要性。
{"title":"Multipartite standard nonlocality sharing by m-sided independent sequential observers","authors":"Hao Sun, Fenzhuo Guo, Haifeng Dong, Fei Gao","doi":"10.1007/s11128-024-04460-4","DOIUrl":"https://doi.org/10.1007/s11128-024-04460-4","url":null,"abstract":"<p>The sharing of quantum nonlocality has been the subject of much recent research for two-qubit and three-qubit entangled systems. In this paper, we discuss nonlocality sharing with unsharp measurement based on Mermin–Ardehali–Belinskii–Klyshko (MABK) inequality for the <i>N</i>-qubit generalized Greenberger–Horne–Zeilinger (GHZ) system. In the one-sided sequential measurements scenario, we determine a state range associated with <i>k</i> within which <span>( k+1 )</span> independent observers can share the standard <i>N</i>-partite nonlocality with the other <span>((N-1))</span> sides, as well as a state range where arbitrarily many independent observers can do the same. Similarly, as to the <i>m</i>-sided sequential measurements scenario, we also identify a state range influenced by <i>k</i> within which <span>( k+1 )</span> independent observers in each of <i>m</i> sides can share the standard <i>N</i>-partite nonlocality with the other <span>((N-m))</span> sides, and a state range where arbitrarily many independent observers can do so. Crucially, all of our nonlocality sharing findings result from a measurement strategy in which every sequential observer employs unequal sharpness measurements. As a special case, for the three-qubit maximally entangled GHZ state, we demonstrate that an unbounded number of observers can share the nonlocality in the one-sided sequential measurements scenario. This outcome further underscores the importance of unequal sharpness measurements in recycling qubits for generating quantum nonlocality.</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-06-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141514379","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-24DOI: 10.1007/s11128-024-04456-0
Sarallah Keshavarz, Mohammad Reza Reshadinezhad, Shekoofeh Moghimi
Quantum circuits are one of the best platforms to implement quantum algorithms. Concerning fault-tolerant quantum circuit, the Clifford + T gate set supports quantum circuits against decoherence error. However, they cause physical resource overheads like many qubits and the use of T gates as a high-cost computing element. This work focuses on low T-cost fault tolerant quantum ALU implementation using Clifford + T gate set. Three new different designs of quantum ALU are proposed by introducing a new quantum logic unit, and new low-cost fault tolerant implementations of full adder and subtractor circuits. We present a novel lemma in synthesizing quantum NCV-based circuits to Clifford + T quantum circuits. This lemma shows how an NCV-based structure with less CNOT layer can lead to an improvement in T-count and T-depth criteria in Clifford + T equivalent circuit. We analyze the effect of applying our proposed lemma in implementing low-cost fault tolerant Clifford + T circuits by some examples on adder and subtractors and ALUs. Comparison of the designs shows 50%, 40%, 36%, and 69% superior functionality of our proposed ALU module in terms of T-count, T-depth, number of qubits, and number of calculated operations compared to the existing counterpart, respectively. The proposed lemma can be used as a simplification step in quantum circuit synthesis algorithms and can be extended to use in quantum synthesis tools.
量子电路是实现量子算法的最佳平台之一。关于容错量子电路,克利福德 + T 门集支持量子电路抵御退相干错误。然而,它们会造成物理资源开销,如许多量子比特和作为高成本计算元素的 T 门的使用。这项工作的重点是利用克利福德 + T 门集实现低 T 成本容错量子 ALU。通过引入新的量子逻辑单元,以及全加法器和减法器电路的新的低成本容错实现,提出了三种不同的量子 ALU 新设计。我们提出了一个将基于 NCV 的量子电路合成为 Clifford + T 量子电路的新型阶式。该 Lemma 说明了基于 NCV 的结构如何通过减少 CNOT 层来改善 Clifford + T 等效电路的 T 数和 T 深度标准。我们通过一些加法器、减法器和 ALU 的例子,分析了应用我们提出的 Lemma 实现低成本容错 Clifford + T 电路的效果。设计比较显示,与现有模块相比,我们提出的 ALU 模块在 T 数、T 深度、量子比特数和计算操作数方面的功能分别优于 50%、40%、36% 和 69%。所提出的 Lemma 可用作量子电路合成算法的简化步骤,并可扩展到量子合成工具中使用。
{"title":"T-count and T-depth efficient fault-tolerant quantum arithmetic and logic unit","authors":"Sarallah Keshavarz, Mohammad Reza Reshadinezhad, Shekoofeh Moghimi","doi":"10.1007/s11128-024-04456-0","DOIUrl":"https://doi.org/10.1007/s11128-024-04456-0","url":null,"abstract":"<p>Quantum circuits are one of the best platforms to implement quantum algorithms. Concerning fault-tolerant quantum circuit, the Clifford + T gate set supports quantum circuits against decoherence error. However, they cause physical resource overheads like many qubits and the use of T gates as a high-cost computing element. This work focuses on low T-cost fault tolerant quantum ALU implementation using Clifford + T gate set. Three new different designs of quantum ALU are proposed by introducing a new quantum logic unit, and new low-cost fault tolerant implementations of full adder and subtractor circuits. We present a novel lemma in synthesizing quantum NCV-based circuits to Clifford + T quantum circuits. This lemma shows how an NCV-based structure with less CNOT layer can lead to an improvement in T-count and T-depth criteria in Clifford + T equivalent circuit. We analyze the effect of applying our proposed lemma in implementing low-cost fault tolerant Clifford + T circuits by some examples on adder and subtractors and ALUs. Comparison of the designs shows 50%, 40%, 36%, and 69% superior functionality of our proposed ALU module in terms of T-count, T-depth, number of qubits, and number of calculated operations compared to the existing counterpart, respectively. The proposed lemma can be used as a simplification step in quantum circuit synthesis algorithms and can be extended to use in quantum synthesis tools.\u0000</p>","PeriodicalId":746,"journal":{"name":"Quantum Information Processing","volume":null,"pages":null},"PeriodicalIF":2.5,"publicationDate":"2024-06-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141530628","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-24DOI: 10.1007/s11128-024-04447-1
Ansha Tayyab, Seerat Javed, Muzzamal I. Shaukat
In this paper, we examine how finite time disentanglement can be manipulated for the quantum system out of thermal equilibrium. To this aim, we employ the Markovian master equation approach to find the rate equations and Wootter’s concurrence to analyze out of thermal equilibrium entanglement dynamics for Dicke bases. The effect of super- and sub-radiant rates on entanglement sudden death is examined for different classes of X-states. It is found that the shorter dark period is achieved at a higher transition rate of a super-radiant state. This approach allows us to analyze the further applications of quantum information technologies.
在本文中,我们研究了如何操纵量子系统在热平衡之外的有限时间不纠缠。为此,我们采用马尔可夫主方程方法来寻找速率方程,并利用 Wootter 协整来分析 Dicke 基的热平衡外纠缠动力学。针对不同类别的 X 态,研究了超辐射率和亚辐射率对纠缠猝死的影响。研究发现,超辐射态的过渡率越高,暗周期越短。通过这种方法,我们可以分析量子信息技术的进一步应用。
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