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Symmetry fractionalization: Symmetry-protected topological phases of the bond-alternating spin-1/2 Heisenberg chain
, Article Journal of Physics Condensed Matter ; Vol. 26, issue. 45 , 2014 ; ISSN: 09538984 ; Langari, A ; Rezakhani, A. T ; Sharif University of Technology
2014
Abstract
We study different phases of the one-dimensional bond-alternating spin-1/2 Heisenberg model by using the symmetry fractionalization mechanism. We employ the infinite matrix-product state representation of the ground state (through the infinite-size density matrix renormalization group algorithm) to obtain inequivalent projective representations and commutation relations of the (unbroken) symmetry groups of the model, which are used to identify the different phases. We find that the model exhibits trivial as well as symmetry-protected topological phases. The symmetry-protected topological phases are Haldane phases on even/odd bonds, which are protected by the time-reversal (acting on the spin...
Quantum discord and non-Markovianity of quantum dynamics
, Article Physical Review A - Atomic, Molecular, and Optical Physics ; Volume 85, Issue 5 , 2012 ; 10502947 (ISSN) ; Mani, A ; Rezakhani, A. T ; Sharif University of Technology
2012
Abstract
The problem of recognizing (non-)Markovianity of a quantum dynamics is revisited through analyzing quantum correlations. We argue that instantaneouslyvanishing quantum discord provides a necessary and sufficient condition for Markovianity of a quantum map. This is used to introduce a measure of non-Markovianity. This measure, however, requires demanding knowledge about the system and the environment. By using a quantum correlation monogamy property and an ancillary system, we propose a simplified measure with fewer requirements. Non-Markovianity is thereby decided by quantum state tomography of the system and the ancilla
Dissipative quantum metrology in manybody systems of identical particles
, Article New Journal of Physics ; Vol. 16, issue , January , 2014 ; Alipour, S ; Rezakhani, A. T ; Sharif University of Technology
2014
Abstract
Estimation of physical parameters is essential in almost any part of science and technology. The enhancement of performance in this task (e.g. beating the standard classical shot-noise limit) using available physical resources is a major goal in metrology. Quantum metrology in closed systems has indicated that entanglement in such systems may be a useful resource. However, whether in open quantum systems such enhancements may still show up is not yet fully understood. Here, we consider a dissipative (open) quantum system of identical particles in which a parameter of the open dynamics itself is to be estimated. We employ a recently developed dissipative quantum metrology framework, and...
Quantum metrology in open systems: Dissipative cramer-rao bound
, Article Physical Review Letters ; Volume 112, Issue 12 , 2014 ; 00319007 (ISSN) ; Mehboudi, M ; Rezakhani, A. T ; Sharif University of Technology
American Physical Society
2014
Abstract
Estimation of parameters is a pivotal task throughout science and technology. The quantum Cramér-Rao bound provides a fundamental limit of precision allowed to be achieved under quantum theory. For closed quantum systems, it has been shown how the estimation precision depends on the underlying dynamics. Here, we propose a general formulation for metrology scenarios in open quantum systems, aiming to relate the precision more directly to properties of the underlying dynamics. This feature may be employed to enhance an estimation precision, e.g., by quantum control techniques. Specifically, we derive a Cramér-Rao bound for a fairly large class of open system dynamics, which is governed by a...
Quantum ergodicity for a class of non-generic systems
, Article Journal of Physics A: Mathematical and Theoretical ; Volume 49, Issue 5 , 2015 ; 17518113 (ISSN) ; Bakhshinezhad, F ; Rezakhani, A. T ; Sharif University of Technology
2015
Abstract
We examine quantum normal typicality and ergodicity properties for quantum systems whose dynamics are generated by Hamiltonians which have residual degeneracy in their spectrum and resonance in their energy gaps. Such systems can be considered atypical in the sense that degeneracy, which is usually a sign of symmetry, is naturally broken in typical systems due to stochastic perturbations. In particular, we prove a version of von Neumann's quantum ergodic theorem, where a modified condition needs to hold in order to have normal typicality and ergodicity. As a result, we show that degeneracy of spectrum does not considerably modify the condition of the theorem, whereas the existence of...
Bound entanglement in quantum phase transitions
, Article Physical Review A - Atomic, Molecular, and Optical Physics ; Volume 81, Issue 4 , 2010 ; 10502947 (ISSN) ; Alipour, S ; Rezakhani, A. T ; Sharif University of Technology
2010
Abstract
We investigate quantum phase transitions in which a change in the type of entanglement from bound entanglement to either free entanglement or separability may occur. In particular, we present a theoretical method to construct a class of quantum spin-chain Hamiltonians that exhibit this type of quantum criticality. Given parameter-dependent two-site reduced density matrices (with prescribed entanglement properties), we lay out a reverse construction for a compatible pure state for the whole system, as well as a class of Hamiltonians for which this pure state is a ground state. This construction is illustrated through several examples
Unreliability of mutual information as a measure for variations in total correlations
, Article Physical Review A ; Volume 101, Issue 4 , 2020 ; Tuohino, S ; Rezakhani, A. T ; Ala-Nissila, T ; Sharif University of Technology
American Physical Society
2020
Abstract
Correlations disguised in various forms underlie a host of important phenomena in classical and quantum systems, such as information and energy exchanges. The quantum mutual information and the norm of the correlation matrix are both considered as proper measures of total correlations. We demonstrate that, when applied to the same system, these two measures can actually show significantly different behavior except at least in two limiting cases: when there are no correlations and when there is maximal quantum entanglement. We further quantify the discrepancy by providing analytic formulas for time derivatives of the measures for an interacting bipartite system evolving unitarily. We argue...
Correlation-enabled energy exchange in quantum systems without external driving
, Article Physical Review A ; Volume 105, Issue 2 , 2022 ; 24699926 (ISSN) ; Alipour, S ; Rezakhani, A. T ; Ala Nissila, T ; Sharif University of Technology
American Physical Society
2022
Abstract
We study the role of correlation in mechanisms of energy exchange between an interacting bipartite quantum system and its environment by decomposing the energy of the system to local and correlation-related contributions. When the system Hamiltonian is time independent, no external work is performed. In this case, energy exchange between the system and its environment occurs only due to the change in the state of the system. We investigate the possibility of a special case where the energy exchange with the environment occurs exclusively due to changes in the correlation between the constituent parts of the bipartite system, while their local energies remain constant. We find sufficient...
Shortcuts to adiabaticity in driven open quantum systems: Balanced gain and loss and non-markovian evolution
, Article Quantum ; Volume 4 , 2020 ; Chenu, A ; Rezakhani, A. T ; del Campo, A ; Sharif University of Technology
Verein zur Forderung des Open Access Publizierens in den Quantenwissenschaften
2020
Abstract
A universal scheme is introduced to speed up the dynamics of a driven open quantum system along a prescribed trajectory of interest. This framework generalizes counterdiabatic driving to open quantum processes. Shortcuts to adiabaticity designed in this fashion can be implemented in two alternative physical scenarios: one characterized by the presence of balanced gain and loss, the other involves non-Markovian dynamics with time-dependent Lindblad operators. As an illustration, we engineer superadiabatic cooling, heating, and isothermal strokes for a two-level system, and provide a protocol for the fast thermalization of a quantum oscillator. © 2020 Paideia. All rights reserved
Quantum imaging as an ancilla-assisted process tomography
, Article Physical Review A - Atomic, Molecular, and Optical Physics ; Volume 94, Issue 4 , 2016 ; 10502947 (ISSN) ; Afsary, M ; Alipour, S ; Rezakhani, A. T ; Sharif University of Technology
American Physical Society
2016
Abstract
We show how a recent experiment of quantum imaging with undetected photons can basically be described as an (a partial) ancilla-assisted process tomography in which the object is described by an amplitude-damping quantum channel. We propose a simplified quantum circuit version of this scenario, which also enables one to recast quantum imaging in quantum computation language. Our analogy and analysis may help us to better understand the role of classical and/or quantum correlations in imaging experiments. © 2016 American Physical Society
Symmetrization and entanglement of arbitrary states of qubits
, Article Physics Letters, Section A: General, Atomic and Solid State Physics ; Volume 313, Issue 5-6 , 2003 , Pages 330-337 ; 03759601 (ISSN) ; Karimipour, V ; Memarzadeh, L ; Rezakhani, A. T ; Sharif University of Technology
Elsevier
2003
Abstract
Given two arbitrary pure states |φ〉 and |ψ〉 of qubits or higher level states, we provide arguments in favor of states of the form (1/√2)(|ψ〉|φ〉 + i|φ〉|ψ〉) instead of symmetric or anti-symmetric states, as natural candidates for optimally entangled states constructed from these states. We show that such states, firstly have on the average a high value of concurrence, secondly can be constructed by a universal unitary operator independent of the input states. We also show that these states are the only ones which can be produced with perfect fidelity, by any quantum operation designed for intertwining two pure states with a relative phase. A probabilistic method is proposed for producing any...
On a suggestion relating topological and quantum mechanical entanglements
, Article Physics Letters, Section A: General, Atomic and Solid State Physics ; Volume 327, Issue 5-6 , 2004 , Pages 380-390 ; 03759601 (ISSN) ; Karimipour, V ; Memarzadeh, L ; Rezakhani, A. T ; Sharif University of Technology
Elsevier
2004
Abstract
We analyze a recent suggestion [New J. Phys. 4 (2002) 73], [quant-ph/0304091] on a possible relation between topological and quantum mechanical entanglements. We show that a one to one correspondence does not exist, neither between topologically linked diagrams and entangled states, nor between braid operators and quantum entanglers. We also add a new dimension to the question of entangling properties of unitary operators in general. © 2004 Elsevier B.V. All rights reserved
Analysis of the quantum Zeno effect for quantum control and computation
, Article Journal of Physics A: Mathematical and Theoretical ; Volume 46, Issue 7 , 2013 ; 17518113 (ISSN) ; Paz Silva, G. A ; Rezakhani, A. T ; Lidar, D. A ; Sharif University of Technology
2013
Abstract
Within quantum information, many methods have been proposed to avoid or correct the deleterious effects of the environment on a system of interest. In this work, expanding on our earlier paper (Paz-Silva et al 2012 Phys. Rev. Lett. 108 080501), we evaluate the applicability of the quantum Zeno effect as one such method. Using the algebraic structure of stabilizer quantum error correction codes as a unifying framework, two open-loop protocols are described which involve frequent non-projective (i.e. weak) measurement of either the full stabilizer group or a minimal generating set thereof. The effectiveness of the protocols is measured by the distance between the final state under the protocol...
Binding energy of bipartite quantum systems: Interaction, correlations, and tunneling
, Article Physical Review A ; Volume 101, Issue 1 , 2020 ; Bathaee, M ; Bakhshinezhad, F ; Rezakhani, A. T ; Bahrampour, A. R ; Sharif University of Technology
American Physical Society
2020
Abstract
We provide a physically motivated definition for the binding energy (or bond dissociation) of a bipartite quantum system. We consider coherently applying an external field to cancel out the interaction between the subsystems, to break their bond and separate them as systems from which no work can be extracted coherently by any cyclic evolution. The minimum difference between the average energies of the initial and final states obtained this way is defined as the binding energy of the system. We show that the final optimal state is a passive state. We discuss how the required evolution can be realized through a sequence of control pulses. The utility of our definition is illustrated through...
Correlations in quantum thermodynamics: Heat, work, and entropy production
, Article Scientific Reports ; Volume 6 , 2016 ; 20452322 (ISSN) ; Benatti, F ; Bakhshinezhad, F ; Marcantoni, S ; Rezakhani, A. T ; Sharif University of Technology
Nature Publishing Group
2016
Abstract
We provide a characterization of energy in the form of exchanged heat and work between two interacting constituents of a closed, bipartite, correlated quantum system. By defining a binding energy we derive a consistent quantum formulation of the first law of thermodynamics, in which the role of correlations becomes evident, and this formulation reduces to the standard classical picture in relevant systems. We next discuss the emergence of the second law of thermodynamics under certain-but fairly general-conditions such as the Markovian assumption. We illustrate the role of correlations and interactions in thermodynamics through two examples
Entropy production and non-markovian dynamical maps
, Article Scientific Reports ; Volume 7, Issue 1 , 2017 ; 20452322 (ISSN) ; Alipour, S ; Benatti, F ; Floreanini, R ; Rezakhani, A. T ; Sharif University of Technology
2017
Abstract
In the weak-coupling limit approach to open quantum systems, the presence of the bath is eliminated and accounted for by a master equation that introduces dissipative contributions to the system reduced dynamics: within this framework, there are no bath entropy contributions to the entropy balance. We show that, as a consequence, the entropy production fails to be positive for a class of physically legitimate, that is completely positive and trace preserving, non-Markovian dynamical maps. Moreover, in absence of the semigroup property, if the reduced dynamics has a thermal asymptotic state, this need not be stationary. Then even the integrated entropy production becomes negative. These...
Characterization of two-qubit perfect entanglers
, Article Physical Review A - Atomic, Molecular, and Optical Physics ; Volume 70, Issue 5 A , 2004 , Pages 052313-1-052313-9 ; 10502947 (ISSN) ; Sharif University of Technology
2004
Abstract
The problem of the characterization of perfect entanglers was investigated. Perfect entanglers have been defined as unitary operators that can generate maximally entangled states from some suitably chosen separable states. Some well defined tools have also been used to measure the entangling properties of quantum operators and two-qubit states. It was found that such tools help to analyze perfect entanglers and also have the unique property of maximally entangling a complete set of orthonormal product vectors. The results show that the qubit gates provided minimum universal gate construction and two of them were necessary and sufficient in implementation of a generic two-qubit gate
Quantum process tomography with coherent states
, Article New Journal of Physics ; Volume 13 , 2011 ; 13672630 (ISSN) ; Scherer, A ; Mann, A ; Rezakhani, A. T ; Lvovsky, A. I ; Sanders, B. C ; Sharif University of Technology
2011
Abstract
We have developed an enhanced technique for characterizing quantum optical processes based on probing unknown quantum processes only with coherent states. Our method substantially improves the original proposal (Lobino et al 2008 Science 322 563), which uses a filtered Glauber-Sudarshan decomposition to determine the effect of the process on an arbitrary state. We introduce a new relation between the action of a general quantum process on coherent state inputs and its action on an arbitrary quantum state. This relation eliminates the need to invoke the Glauber-Sudarshan representation for states; hence, it dramatically simplifies the task of process identification and removes a potential...
Quantum phase transitions in the Kondo-necklace model: Perturbative continuous unitary transformation approach
, Article Journal of Physics Condensed Matter ; Volume 27, Issue 15 , March , 2015 ; 09538984 (ISSN) ; Rahimi Movassagh, M ; Ghassemi, N ; Kargarian, M ; Rezakhani, A. T ; Langari, A ; Sharif University of Technology
Institute of Physics Publishing
2015
Abstract
The Kondo-necklace model can describe magnetic low-energy limit of strongly correlated heavy fermion materials. There exist multiple energy scales in this model corresponding to each phase of the system. Here, we study quantum phase transition between the Kondo-singlet phase and the antiferromagnetic long-range ordered phase, and show the effect of anisotropies in terms of quantum information properties and vanishing energy gap. We employ the 'perturbative continuous unitary transformations' approach to calculate the energy gap and spin-spin correlations for the model in the thermodynamic limit of one, two, and three spatial dimensions as well as for spin ladders. In particular, we show that...
Uncontrolled disorder effects in fabricating photonic quantum simulators on a kagome geometry: A projected-entangled-pair-state versus exact- diagonalization analysis
, Article Physical Review A - Atomic, Molecular, and Optical Physics ; Vol. 89, Issue. 6 , 2014 ; ISSN: 10502947 ; Dezfouli, B. G ; Ghasemipour, F ; Rezakhani, A. T ; Saberi, H ; Sharif University of Technology
2014
Abstract
We propose a flexible numerical framework for extracting the energy spectra and photon transfer dynamics of a unit kagome cell with disordered cavity-cavity couplings under realistic experimental conditions. A projected-entangled pair state (PEPS) Ansatz to the many-photon wave function allows us to gain a detailed understanding of the effects of undesirable disorder in fabricating well-controlled and scalable photonic quantum simulators. The correlation functions associated with the propagation of two-photon excitations reveal intriguing interference patterns peculiar to the kagome geometry and promise at the same time a highly tunable quantum interferometry device with a signature for the...