Rotational band properties of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msup><mml:mrow /><mml:mn>173</mml:mn></mml:msup></mml:math>W

Wang, H. X.; Zhang, Y. H.; Zhou, Xiao Hong; Liu, M. L.; Ding, Bing; Li, G. S.; Zhou, Haibiao; Guo, S.; Qiang, Y. H.; Oshima, M.; Koizumi, M.; Toh, Y.; Kimura, A.; Harada, Hideo; Furutaka, Kazuyoshi; Kitatani, Fumito; Nakamura, Shôji; Hatsukawa, Y.; Ohta, M.; Hara, K.; Kin, Tadahiro; Meng, J.

doi:10.1103/physrevc.86.044305

Cited by 45 publications

(85 citation statements)

References 23 publications

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“…Their energy and momentum are subtracted from all final observables. The (3+1)D CLVisc hydrodynamic model [10,11] is used to provide spatial and time information on the local temperature and fluid velocity of the bulk QGP medium during jet propagation. Initial production of jet shower partons per hard nucleon-nucleon collisions is simulated through standard Monte Carlo programs such as Pyhtia.…”

Section: Lbt Modelmentioning

confidence: 99%

E-by-e jet suppression, anisotropy, medium response and hard-soft tomography

Cao

Wei

et al. 2019

Nuclear Physics A

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The Linear Boltzmann Transport (LBT) model for jet propagation and interaction in quark-gluon plasma (QGP) has been used to study jet quenching in high-energy heavy-lion collisions. The suppression of single inclusive jet production, medium modification of γ-jet correlation, jet profiles and fragmentation functions as observed in experiments at Large Hadron Collider (LHC) can be described well by LBT in which jet-induced medium response is shown to play an essential role. In event-by-event simulations of jet quenching within LBT, jet azimuthal anisotropies are found to correlate linearly with the anisotropic flows of bulk hadrons from the underlying hydrodynamic events.

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Section: Lbt Modelmentioning

confidence: 99%

E-by-e jet suppression, anisotropy, medium response and hard-soft tomography

Cao

Wei

et al. 2019

Nuclear Physics A

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“…[45,46] Based on the GCB, deterministic photon-spin quantum interfaces (entangling gates) could be built, and several schemes for scalable QIP with single QD spins and single photons have been proposed. [47][48][49][50][51][52][53][54][55][56][57][58][59][60][61][62][63] In particular, universal quantum controlled gates on photons, [64][65][66][67][68] electron spins, [69][70][71][72][73] and photon-spin hybrid systems [74,75] could be implemented. In 2011, Young et al [76] experimentally investigated the QD-induced phase shift in a pillar microcavity.…”

Section: Introductionmentioning

confidence: 99%

High‐Fidelity Universal Quantum Controlled Gates on Electron‐Spin Qubits in Quantum Dots Inside Single‐Sided Optical Microcavities

et al. 2019

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Semiconductor quantum‐dot (QD) spins hold great promise in quantum information science and technology. The implementation of high‐fidelity quantum gates on QD‐spin qubits is of great importance. Here, two schemes are presented to implement two universal quantum controlled gates, that is, the two‐qubit controlled‐not gate and the three‐qubit Toffoli gate, on stationary electron‐spin qubits in QDs inside single‐sided optical microcavities, based on the cavity‐assisted photon scattering under the balance condition. Compared with the previous schemes based on the ideal giant circular birefringence, the present schemes use the balance condition of the single‐sided QD‐cavity system, which can be achieved in both the weak‐ and strong‐coupling regimes of cavity quantum electrodynamics. Under the balance condition, the noise caused by the unbalanced reflectance between the coupled and uncoupled QD‐cavity systems can be efficiently depressed, so that the fidelity of each quantum gate operation can be increased to unity in principle. The schemes exhibit the possibility of realizing high‐fidelity and scalable quantum computing with single QD spins and single photons using the feasible and robust light–matter quantum interface. These high‐fidelity quantum controlled gates can lead to more efficient construction of quantum circuits for quantum computing, and provide a convenient avenue for quantum networking.

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“…However, the channel noise will induce decoherence and degrade the entanglement between the quantum systems. Entanglement concentration [11][12][13][14][15][16][17][18][19][20][21][22][23] is an operation which converts a partially entangled state to a more or maximally entangled state. Since the first entanglement concentration protocol (ECP), the well known Schmidt projection, was proposed by Bennett et al [11], its realization on the various physical systems has been reported.…”

mentioning

confidence: 99%

“…Since the first entanglement concentration protocol (ECP), the well known Schmidt projection, was proposed by Bennett et al [11], its realization on the various physical systems has been reported. The examples include ECPs with linear optical elements in the principle of Schmidt projection [12,13], nonlocal-photon ECP with linear [17] or nonlinear optical elements [18,19], and ECP based on electron-spin systems [20] or on circuit quantum electrodynamics [21,22], etc.…”

mentioning

confidence: 99%

Phononic entanglement concentration via optomechanical interactions

Chen

Zhang

et al. 2019

Phys. Rev. A

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Low dissipation, tunable coupling to other quantum systems, and unique features of phonons in the aspects of propagation, detection and others suggest the applications of quantized mechanical resonators in phonon-based quantum information processing (QIP) in a way different from their photonic counterpart. In this paper, we propose the first protocol of entanglement concentration for nonlocal phonons from quantized mechanical vibration. We combine the optomechanical cross-Kerr interaction with the Mach-Zehnder interferometer and, by means of twice optomechanical interactions and the photon analysis with respect to the output of the interferometer, achieve ideal entanglement concentration about less-entangled nonlocal phonon Bell and Greenberger-Horne-Zeilinger states. Our protocol is useful for preserving the entangled phonons for the use of high quality phonon-based QIP in future.PACS numbers: I. INTRODUCTIONQuantum entanglement is a quantum resource indispensable in the areas, such as quantum key distribution [1-3], quantum teleportation [4], quantum secure direct communication [5][6][7][8] and quantum dense coding [9,10]. In quantum communications, an entangled state is usually used for building a quantum channel between remote parties. However, the channel noise will induce decoherence and degrade the entanglement between the quantum systems. Entanglement concentration [11][12][13][14][15][16][17][18][19][20][21][22][23] is an operation which converts a partially entangled state to a more or maximally entangled state. Since the first entanglement concentration protocol (ECP), the well known Schmidt projection, was proposed by Bennett et al [11], its realization on the various physical systems has been reported. The examples include ECPs with linear optical elements in the principle of Schmidt projection [12,13], nonlocal-photon ECP with linear [17] or nonlinear optical elements [18,19], and ECP based on electron-spin systems [20] or on circuit quantum electrodynamics [21,22], etc.

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Rotational band properties of173W

Cited by 45 publications

References 23 publications

E-by-e jet suppression, anisotropy, medium response and hard-soft tomography

E-by-e jet suppression, anisotropy, medium response and hard-soft tomography

High‐Fidelity Universal Quantum Controlled Gates on Electron‐Spin Qubits in Quantum Dots Inside Single‐Sided Optical Microcavities

Phononic entanglement concentration via optomechanical interactions

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