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The anti-Jaynes-Cummings model is solvable : quantum Rabi model in rotating and counter-rotating frames ; following the experiments 反jaynes - cummings模型是可解的:在旋转和反旋转坐标系中的量子Rabi模型;在实验之后
arXiv: Quantum Physics Pub Date : 2021-03-17 DOI: 10.21203/RS.3.RS-379917/V1
Joseph Omolo
{"title":"The anti-Jaynes-Cummings model is solvable : quantum Rabi model in rotating and counter-rotating frames ; following the experiments","authors":"Joseph Omolo","doi":"10.21203/RS.3.RS-379917/V1","DOIUrl":"https://doi.org/10.21203/RS.3.RS-379917/V1","url":null,"abstract":"\u0000 This article is a response to the continued assumption, cited even in reports and reviews of recent experimental breakthroughs and advances in theoretical methods, that the antiJaynes-Cummings (AJC)interaction is an intractable energy non-conserving component of the quantum Rabi model (QRM). We present three key features of QRM dynamics : (a) the AJC interaction component has a conserved excitation number operator and is exactly solvable (b) QRM dynamical space consists of a rotating frame (RF) dominated by an exactly solved Jaynes-Cummings (JC) interaction specied by a conserved JC excitation number operator which generates the U(1) symmetry of RF and a correlated counter-rotating frame (CRF) dominated by an exactly solved antiJaynes-Cummings (AJC) interaction specied by a conserved AJC excitation number operator which generates the U(1) symmetry of CRF (c) for QRM dynamical evolution in RF, the initial atom-eld state je0i is an eigenstate of the effective AJC Hamiltonian HAJC, while the effective JC Hamiltonian HJC drives this initial state je0i into a time evolving entangled state, and, in a corresponding process for QRM dynamical evolution in CRF, the initial atom-eld state jg0i is an eigenstate of the effective JC Hamiltonian, while the effective AJC Hamiltonian drives this initial state jg0i into a time evolving entangled state, thus addressing one of the long-standing challenges of theoretical and experimental QRM dynamics; consistent generalizations of the initial states je0i , jg0i to corresponding n 0 entangled eigenstates j+en i , j 􀀀g ni of the AJC in RF and JC in CRF, respectively, provides general dynamical evolution of QRM characterized by collapses and revivals in the time evolution of the atomic, eld mode, JC and AJC excitation numbers for large initial photon numbers ; the JC and AJC excitation numbers are conserved in the respective frames RF, CRF, but each evolves with time in the alternate frame.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2021-03-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"89489392","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 2
Second law of thermodynamics for quantum correlations 量子相关的热力学第二定律
arXiv: Quantum Physics Pub Date : 2021-02-26 DOI: 10.13016/M2RSDW-ZGPS
Akram Touil, B. cCakmak, Sebastian Deffner
{"title":"Second law of thermodynamics for quantum correlations","authors":"Akram Touil, B. cCakmak, Sebastian Deffner","doi":"10.13016/M2RSDW-ZGPS","DOIUrl":"https://doi.org/10.13016/M2RSDW-ZGPS","url":null,"abstract":"B. C¸ . is supported by the BAGEP Award of the Science Academy and by the Research \u0000Fund of Bah¸ce¸sehir University (BAUBAP) under project no: BAP.2019.02.03. S.D. \u0000acknowledges support from the U.S. National Science Foundation under Grant No. \u0000DMR-2010127. This research was supported by grant number FQXi-RFP-1808 from \u0000the Foundational Questions Institute and Fetzer Franklin Fund, a donor advised fund \u0000of Silicon Valley Community Foundation (SD).","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2021-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"77517075","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 4
Optimal implementation of two-qubit linear-optical quantum filters 双量子位线性光学量子滤波器的优化实现
arXiv: Quantum Physics Pub Date : 2021-02-26 DOI: 10.1103/PhysRevA.103.062408
J. Fiurášek, Robert Stárek, M. Mičuda
{"title":"Optimal implementation of two-qubit linear-optical quantum filters","authors":"J. Fiurášek, Robert Stárek, M. Mičuda","doi":"10.1103/PhysRevA.103.062408","DOIUrl":"https://doi.org/10.1103/PhysRevA.103.062408","url":null,"abstract":"We design optimal interferometric schemes for implementation of two-qubit linear optical quantum filters diagonal in the computational basis. The filtering is realized by interference of the two photons encoding the qubits in a multiport linear optical interferometer, followed by conditioning on presence of a single photon in each output port of the filter. The filter thus operates in the coincidence basis, similarly to many linear optical unitary quantum gates. Implementation of the filter with linear optics may require an additional overhead in terms of reduced overall success probability of the filtering and the optimal filters are those that maximize the overall success probability. We discuss in detail the case of symmetric real filters and extend our analysis also to asymmetric and complex filters.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2021-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"90458850","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 1
Invariant quadratic operator associated with Linear Canonical Transformations 与线性正则变换相关的不变二次算子
arXiv: Quantum Physics Pub Date : 2021-02-01 DOI: 10.21203/RS.3.RS-174871/V1
Ravo Tokiniaina Ranaivoson, R. Andriambololona, Rakotoson Hanitriarivo
{"title":"Invariant quadratic operator associated with Linear Canonical Transformations","authors":"Ravo Tokiniaina Ranaivoson, R. Andriambololona, Rakotoson Hanitriarivo","doi":"10.21203/RS.3.RS-174871/V1","DOIUrl":"https://doi.org/10.21203/RS.3.RS-174871/V1","url":null,"abstract":"The main purpose of this work is to identify the general quadratic operator which is invariant under the action of Linear Canonical Transformations (LCTs). LCTs are known in signal processing and optics as the transformations which generalize certain useful integral transforms. In quantum theory, they can be identified as the linear transformations which keep invariant the canonical commutation relations characterizing the coordinates and momenta operators. In this paper, LCTs corresponding to a general pseudo-Euclidian space are considered. Explicit calculations are performed for the monodimensional case to identify the corresponding LCT invariant operator then multidimensional generalizations of the obtained results are deduced. It was noticed that the introduction of a variance-covariance matrix, of coordinate and momenta operators, and a pseudo-orthogonal representation of LCTs facilitate the identification of the invariant quadratic operator. According to the calculations carried out, the LCT invariant operator is a second order polynomial of the coordinates and momenta operators. The coefficients of this polynomial depend on the mean values and the statistical variances-covariances of these coordinates and momenta operators themselves. The eigenstates of the LCT invariant operator are also identified with it and some of the main possible applications of the obtained results are discussed.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2021-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"90025062","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Diagonalization of the Hamiltonian for finite-sized dispersive media: Canonical quantization with numerical mode decomposition 有限尺寸色散介质哈密顿量的对角化:正则量化与数值模态分解
arXiv: Quantum Physics Pub Date : 2021-01-28 DOI: 10.1103/PhysRevA.103.063707
D. Na, Jie Zhu, W. Chew
{"title":"Diagonalization of the Hamiltonian for finite-sized dispersive media: Canonical quantization with numerical mode decomposition","authors":"D. Na, Jie Zhu, W. Chew","doi":"10.1103/PhysRevA.103.063707","DOIUrl":"https://doi.org/10.1103/PhysRevA.103.063707","url":null,"abstract":"We present a new math-physics modeling approach, called canonical quantization with numerical mode-decomposition, for capturing the physics of how incoming photons interact with finite-sized dispersive media, which is not describable by the previous Fano-diagonalization methods. The main procedure is to (1) study a system where electromagnetic (EM) fields are coupled to non-uniformly distributed Lorentz oscillators in Hamiltonian mechanics, (2) derive a generalized Hermitian eigenvalue problem for conjugate pairs in coordinate space, (3) apply computational electromagnetics methods to find a countably/finite set of time-harmonic eigenmodes that diagonalizes the Hamiltonian, and (4) perform the subsequent canonical quantization with mode-decomposition. Moreover, we provide several numerical simulations that capture the physics of full quantum effects, impossible by classical Maxwell's equations, such as non-local dispersion cancellation of an entangled photon pair and Hong-Ou-Mandel (HOM) effect in a dispersive beam splitter.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2021-01-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"72566860","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 11
Making Mistakes Saves the Single World of the Extended Wigner’s Friend Experiment 犯错拯救了扩展维格纳朋友实验的单一世界
arXiv: Quantum Physics Pub Date : 2021-01-27 DOI: 10.21203/RS.3.RS-149814/V1
S. Łukaszyk
{"title":"Making Mistakes Saves the Single World of the Extended Wigner’s Friend Experiment","authors":"S. Łukaszyk","doi":"10.21203/RS.3.RS-149814/V1","DOIUrl":"https://doi.org/10.21203/RS.3.RS-149814/V1","url":null,"abstract":"\u0000 The Extended Wigner’s Friend thought experiment comprising a quantum system containing an agent who draws conclusions, upon observing the outcome of a measurement of a qubit prepared in two non-orthogonal versions by another agent led its authors to conclude that quantum theory cannot consistently describe the use of itself. It has also been proposed that this thought experiment is equivalent to coherent entangled state (Bell type) experiments. It is argued in this paper that the assumption of the freedom of choice of the first Wigner’s friend invalidates such equivalency. It is also argued that the assumption of locality (physical space) introduces superfluous identity of indiscernibles metric axiom, which is invalid in quantum domain and generally disproven by the Ugly duckling mathematical theorem.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2021-01-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"88401681","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
On the mean value of the force operator for 1D particles in the step potential. 一维粒子在阶跃势中力算子的平均值。
arXiv: Quantum Physics Pub Date : 2021-01-17 DOI: 10.1590/1806-9126-rbef-2020-0422
S. Vincenzo
{"title":"On the mean value of the force operator for 1D particles in the step potential.","authors":"S. Vincenzo","doi":"10.1590/1806-9126-rbef-2020-0422","DOIUrl":"https://doi.org/10.1590/1806-9126-rbef-2020-0422","url":null,"abstract":"In the one-dimensional Klein-Fock-Gordon theory, the probability density is a discontinuous function at the point where the step potential is discontinuous. Thus, the mean value of the external classical force operator cannot be calculated from the corresponding formula of the mean value. To resolve this issue, we obtain this quantity directly from the Klein-Fock-Gordon equation in Hamiltonian form, or the Feshbach-Villars wave equation. Not without surprise, the result obtained is not proportional to the average of the discontinuity of the probability density but to the size of the discontinuity. In contrast, in the one-dimensional Schr\"odinger and Dirac theories this quantity is proportional to the value that the respective probability density takes at the point where the step potential is discontinuous. We examine these issues in detail in this paper. The presentation is suitable for the advanced undergraduate level.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2021-01-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82126841","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 1
Topological input-output theory for directional amplification 定向放大的拓扑输入输出理论
arXiv: Quantum Physics Pub Date : 2020-12-17 DOI: 10.1103/PHYSREVA.103.033513
T. Ramos, J. Garc'ia-Ripoll, D. Porras
{"title":"Topological input-output theory for directional amplification","authors":"T. Ramos, J. Garc'ia-Ripoll, D. Porras","doi":"10.1103/PHYSREVA.103.033513","DOIUrl":"https://doi.org/10.1103/PHYSREVA.103.033513","url":null,"abstract":"We present a topological approach to the input-output relations of photonic driven-dissipative lattices acting as directional amplifiers. Our theory relies on a mapping from the optical non-Hermitian coupling matrix to an effective topological insulator Hamiltonian. This mapping is based on the singular value decomposition of non-Hermitian coupling matrices, whose inverse matrix determines the linear input-output response of the system. In topologically non-trivial regimes, the input-output response of the lattice is dominated by singular vectors with zero singular values that are the equivalent of zero-energy states in topological insulators, leading to directional amplification of a coherent input signal. In such topological amplification regime, our theoretical framework allows us to fully characterize the amplification properties of the quantum device such as gain, bandwidth, added noise, and noise-to-signal ratio. We exemplify our ideas in a one-dimensional non-reciprocal photonic lattice, for which we derive fully analytical predictions. We show that the directional amplification is near quantum-limited with a gain growing exponentially with system size, $N$, while the noise-to-signal ratio is suppressed as $1/sqrt{N}$. This points out to interesting applications of our theory for quantum signal amplification and single-photon detection.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2020-12-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"90704153","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 11
Self-consistency of the two-point energy measurement protocol 两点能量测量方案的自一致性
arXiv: Quantum Physics Pub Date : 2020-12-17 DOI: 10.1103/PHYSREVA.103.042214
M. Mohammady
{"title":"Self-consistency of the two-point energy measurement protocol","authors":"M. Mohammady","doi":"10.1103/PHYSREVA.103.042214","DOIUrl":"https://doi.org/10.1103/PHYSREVA.103.042214","url":null,"abstract":"The Two-Point energy Measurement (TPM) protocol defines the work done on a system undergoing unitary evolution as the difference in energy measurement outcomes performed before and after such evolution. By noting that energy measurements on the system can be modelled as a unitary premeasurement interaction between the system and a measurement apparatus, followed by measurement of the apparatus by a pointer observable, we show that it is possible to design a measurement scheme for the TPM protocol on the system that simultaneously acts as a TPM protocol for the compound of system-plus-apparatus so as to reveal the total work distribution. We further demonstrate that: (i) the average total work will be the change in average energy, given the total unitary evolution, for all initial system states and system unitary processes; and (ii) the total work distribution will be identical to the system-only work distribution, for all system states, if and only if the unitary premeasurements conserve the total energy of system-plus-apparatus for all system states.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2020-12-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78089252","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 1
Adiabatic sensing technique for optimal temperature estimation using trapped ions 利用俘获离子估算最佳温度的绝热传感技术
arXiv: Quantum Physics Pub Date : 2020-12-16 DOI: 10.1103/PHYSREVRESEARCH.3.013244
Aleksandrina V. Kirkova, Weibin Li, P. Ivanov
{"title":"Adiabatic sensing technique for optimal temperature estimation using trapped ions","authors":"Aleksandrina V. Kirkova, Weibin Li, P. Ivanov","doi":"10.1103/PHYSREVRESEARCH.3.013244","DOIUrl":"https://doi.org/10.1103/PHYSREVRESEARCH.3.013244","url":null,"abstract":"We propose an adiabatic method for optimal phonon temperature estimation using trapped ions which can be operated beyond the Lamb-Dicke regime. The quantum sensing technique relies on a time-dependent red-sideband transition of phonon modes, described by the non-linear Jaynes-Cummings model in general. A unique feature of our sensing technique is that the relevant information of the phonon thermal distributions can be transferred to the collective spin-degree of freedom. We show that each of the thermal state probabilities is adiabatically mapped onto the respective collective spin-excitation configuration and thus the temperature estimation is carried out simply by performing a spin-dependent laser fluorescence measurement at the end of the adiabatic transition. We characterize the temperature uncertainty in terms of the Fisher information and show that the state projection measurement saturates the fundamental quantum Cram'er-Rao bound for quantum oscillator at thermal equilibrium.","PeriodicalId":8484,"journal":{"name":"arXiv: Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2020-12-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78293661","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 6
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