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Автор: Grafiati

Опубліковано: 10 грудня 2022

Оновлено: 28 січня 2023

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1

Hahn, Y., and P. Krstic. "Stark mixing of degenerate states." Journal of Physics B: Atomic, Molecular and Optical Physics 26, no. 12 (June 28, 1993): L297—L302. http://dx.doi.org/10.1088/0953-4075/26/12/003.

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2

Hannabuss, K. C., and D. C. Latimer. "Fermion mixing in quasifree states." Journal of Physics A: Mathematical and General 36, no. 4 (January 15, 2003): L69—L79. http://dx.doi.org/10.1088/0305-4470/36/4/101.

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3

Lund, A. P., T. C. Ralph, and P. van Loock. "Entangled non-Gaussian states formed by mixing Gaussian states." Journal of Modern Optics 55, no. 13 (July 20, 2008): 2083–94. http://dx.doi.org/10.1080/09500340801986932.

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4

Bender, M., and P.-H. Heenen. "Configuration mixing of mean-field states." Journal of Physics G: Nuclear and Particle Physics 31, no. 10 (September 12, 2005): S1611—S1616. http://dx.doi.org/10.1088/0954-3899/31/10/042.

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5

Franzini, Paula J., and Frederick J. Gilman. "Mixing oftt¯bound states with theZboson." Physical Review D 32, no. 1 (July 1, 1985): 237–46. http://dx.doi.org/10.1103/physrevd.32.237.

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6

Rossi, G. C., and G. Veneziano. "Isospin mixing of narrow pentaquark states." Physics Letters B 597, no. 3-4 (September 2004): 338–45. http://dx.doi.org/10.1016/j.physletb.2004.07.042.

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7

Fortune, H. T. "Configuration mixing among11/2−states inF19." Physical Review C 35, no. 3 (March 1, 1987): 1141–44. http://dx.doi.org/10.1103/physrevc.35.1141.

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8

He, Xiao-Gang, Xue-Qian Li, Xiang Liu, and Xiao-Qiang Zeng. "Mixing of pentaquark and molecular states." European Physical Journal C 44, no. 3 (November 2005): 419–30. http://dx.doi.org/10.1140/epjc/s2005-02383-9.

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9

He, Xiao-Gang, Xue-Qian Li, Xiang Liu, and Xiao-Qiang Zeng. "Mixing of pentaquark and molecular states." European Physical Journal C 44, no. 3 (November 2005): 459. http://dx.doi.org/10.1140/epjc/s2005-02420-9.

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10

Lieb, Elliott H., and Anna Vershynina. "Upper bounds on mixing rates." Quantum Information and Computation 13, no. 11&12 (November 2013): 986–94. http://dx.doi.org/10.26421/qic13.11-12-5.

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Анотація:

We prove upper bounds on the rate, called "mixing rate", at which the von Neumann entropy of the expected density operator of a given ensemble of states changes under non-local unitary evolution. For an ensemble consisting of two states, with probabilities of p and 1-p, we prove that the mixing rate is bounded above by 4\sqrt{p(1-p)} for any Hamiltonian of norm 1. For a general ensemble of states with probabilities distributed according to a random variable X and individually evolving according to any set of bounded Hamiltonians, we conjecture that the mixing rate is bounded above by a Shannon entropy of a random variable $X$. For this general case we prove an upper bound that is independent of the dimension of the Hilbert space on which states in the ensemble act.

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11

Trappenburg, Margo. "Against Segregation: Ethnic Mixing in Liberal States." Journal of Political Philosophy 11, no. 3 (August 4, 2003): 295–319. http://dx.doi.org/10.1111/1467-9760.00179.

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12

Simonov, Yu A. "Mixing of meson, hybrid, and glueball states." Physics of Atomic Nuclei 64, no. 10 (October 2001): 1876–86. http://dx.doi.org/10.1134/1.1414936.

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13

LAHIRI, AVIJIT, GAUTAM GHOSH, and SANKHASUBHRA NAG. "MIXING AND DECOHERENCE TO NEAREST SEPARABLE STATES." International Journal of Quantum Information 07, no. 04 (June 2009): 829–46. http://dx.doi.org/10.1142/s0219749909005432.

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Анотація:

We consider a class of entangled states of a quantum system (S) and a second system (A) where pure states of the former are correlated with mixed states of the latter, and work out the entanglement measure with reference to the nearest separable state. Such "pure-mixed" entanglement is expected when the system S interacts with a macroscopic measuring apparatus in a quantum measurement, where the quantum correlation is destroyed in the process of environment-induced decoherence whereafter only the classical correlation between S and A remains, the latter being large compared to the former. We present numerical evidence that the entangled S–A state drifts towards the nearest separable state through decoherence, with an additional tendency of equimixing among relevant groups of apparatus states.

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14

Chen, Hao. "Constraints on the mixing of bipartite states." Journal of Mathematical Physics 46, no. 12 (December 2005): 122101. http://dx.doi.org/10.1063/1.2138048.

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15

BALARAS, ELIAS, UGO PIOMELLI, and JAMES M. WALLACE. "Self-similar states in turbulent mixing layers." Journal of Fluid Mechanics 446 (October 23, 2001): 1–24. http://dx.doi.org/10.1017/s0022112001005626.

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Анотація:

Large-eddy simulations of temporally evolving turbulent mixing layers have been carried out. The effect of the initial conditions and the size of the computational box on the turbulent statistics and structures is examined in detail. A series of calculations was initialized using two different realizations of a spatially developing turbulent boundary-layer with their free streams moving in opposite directions. Computations initialized with mean flow plus random perturbations with prescribed moments were also conducted. In all cases, the initial transitional stage, from boundary-layer turbulence or random noise to mixing-layer turbulence, was followed by a self-similar period. The self-similar periods, however, differed considerably: the growth rates and turbulence intensities showed differences, and were affected both by the initial condition and by the computational domain size. In all simulations the presence of quasi-two-dimensional spanwise rollers was clear, together with ‘braid’ regions with quasi-streamwise vortices. The development of these structures, however, was different: if strong rollers were formed early (as in the cases initialized by random noise), a well-organized pattern persisted throughout the self-similar period. The presence of boundary layer turbulence, on the other hand, inhibited the growth of the inviscid instability, and delayed the formation of the roller–braid patterns. Increasing the domain size tended to make the flow more three-dimensional.

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16

Blasone, M., A. Capolupo, S. Capozziello, and G. Vitiello. "Neutrino mixing, flavor states and dark energy." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 588, no. 1-2 (April 2008): 272–75. http://dx.doi.org/10.1016/j.nima.2008.01.050.

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17

Hong, Jin, Seok-Jin Kang, Tetsuji Miwa, and Robert Weston. "Mixing of ground states in vertex models." Journal of Physics A: Mathematical and General 31, no. 28 (July 17, 1998): L515—L525. http://dx.doi.org/10.1088/0305-4470/31/28/001.

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18

Chu, King-Wai, Yuefan Deng, and John Reinitz. "Parallel Simulated Annealing by Mixing of States." Journal of Computational Physics 148, no. 2 (January 1999): 646–62. http://dx.doi.org/10.1006/jcph.1998.6134.

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19

Bajer, J. "Nonclassical states generated via four-wave mixing." Czechoslovak Journal of Physics 40, no. 6 (June 1990): 646–63. http://dx.doi.org/10.1007/bf01597860.

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20

Saghai, B., and Z. Li. "Configuration Mixing of Quark States in Baryons." Few-Body Systems 47, no. 1-2 (September 16, 2009): 105–15. http://dx.doi.org/10.1007/s00601-009-0071-2.

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21

Dai, L. R., L. Yuan, N. Zheng, X. S. Kang, S. L. Yuan, and D. Zhang. "The possible strangeness dibaryon states in a chiral quark model." Modern Physics Letters A 30, no. 09 (March 11, 2015): 1550048. http://dx.doi.org/10.1142/s0217732315500480.

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Анотація:

Considering the mixing of scalar mesons, the ΩΩ and Ξ*Ω systems are dynamically investigated within the framework of the chiral SU(3) quark model by solving the resonating group method (RGM) equation. The model parameters are taken from our previous work, which gave a good description of the energies of the baryon ground states, the binding energy of deuteron, and the experimental data of the nucleon–nucleon (NN) and nucleon–hyperon (NY) scattering processes. Two different mixing cases, one is the ideal mixing and another is 19° mixing, are discussed. The results show that no matter what kind of mixing is adopted, the ΩΩ and Ξ*Ω systems are still bound states. It is also shown that they are deeply bound if 19° mixing is adopted.

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22

Giacosa, Francesco. "Chiral anomaly and strange-nonstrange mixing." EPJ Web of Conferences 199 (2019): 05012. http://dx.doi.org/10.1051/epjconf/201919905012.

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As a first step, a simple and pedagogical recall of the η-η′ system is presented, in which the role of the axial anomaly, related to the heterochiral nature of the multiplet of (pseudo)scalar states, is underlined. As a consequence, η is close to the octet and η′ to the singlet configuration. On the contrary, for vector and tensor states, which belong to homochiral multiplets, no anomalous contribution to masses and mixing is present. Then, the isoscalar physical states are to a very good approximation nonstrange and strange, respectively. Finally, for pseudotensor states, which are part of an heterochiral multiplet (just as pseudoscalar ones), a sizable anomalous term is expected: η2(1645) roughly corresponds to the octet and η2(1870) to the singlet.

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23

NOWAKOWSKI, MAREK. "QUANTUM INSTABILITY FOR MIXED STATES." Modern Physics Letters A 17, no. 31 (October 10, 2002): 2039–48. http://dx.doi.org/10.1142/s0217732302008642.

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The analysis of the time evolution of unstable states which are linear superposition of other, observable, states can, in principle, be carried out in two distinct, non-equivalent ways. One of the methods, usually employed for the neutral kaon system, combines the mixing and instability into one single step which then results in unconventional properties of the mass-eigenstates. An alternative method is to remain within the framework of a Lagrangian formalism and to perform the mixing prior to the instability analysis. Staying close to the [Formula: see text] system, we compare both methods pointing out some of their shortcomings and advantages.

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24

Shaik, Sason, and A. Chandrasekhar Reddy. "Transition states, avoided crossing states and valence-bond mixing: fundamental reactivity paradigms." Journal of the Chemical Society, Faraday Transactions 90, no. 12 (1994): 1631. http://dx.doi.org/10.1039/ft9949001631.

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25

Auerbach, N., J. D. Bowman, and V. Spevak. "Nearby Doorway States, Parity Doublets, and Parity Mixing in Compound Nuclear States." Physical Review Letters 74, no. 14 (April 3, 1995): 2638–41. http://dx.doi.org/10.1103/physrevlett.74.2638.

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26

Lian-Rong, Dai, Liu Jia, and Zhang Dan. "Multiquark states and the mixing of scalar meson." Chinese Physics C 33, no. 12 (December 2009): 1397–400. http://dx.doi.org/10.1088/1674-1137/33/12/064.

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27

Holm, David A., and Murray Sargent III. "Quantum theory of multiwave mixing. VIII. Squeezed states." Physical Review A 35, no. 5 (March 1, 1987): 2150–63. http://dx.doi.org/10.1103/physreva.35.2150.

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28

Suryadharma, Radius N. S., Alexander A. Iskandar, and May-On Tjia. "Photonic states mixing beyond the plasmon hybridization model." Journal of Applied Physics 120, no. 4 (July 28, 2016): 043105. http://dx.doi.org/10.1063/1.4959258.

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29

Borrajo, Marta, Tomás R. Rodríguez, and J. Luis Egido. "Symmetry conserving configuration mixing method with cranked states." Physics Letters B 746 (June 2015): 341–46. http://dx.doi.org/10.1016/j.physletb.2015.05.030.

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30

NEKRASOV, M. L. "PSEUDOSCALAR QUARK STATES MIXING AND AXIAL WARD IDENTITIES." International Journal of Modern Physics A 07, no. 32 (December 30, 1992): 8069–80. http://dx.doi.org/10.1142/s0217751x92003641.

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Анотація:

The η-, η′-meson system is investigated in a relativistic invariant approach of composite operators under assumptions of completeness and quark nature of mesons. New advanced solutions of axial Ward identities have been obtained. The connection of the decays constants and other parameters of the η-, η′-meson system with the mixing angle and the pion and kaon constants has been established. In the approach under consideration the improved PCAC formulas for the decays η→γγ, η′→γγ have been determined and the basic parameter values of the η-, η′-meson system have been evaluated. The effect of the nonet symmetry breaking obtained in this system exceeds the usually expected value and is estimated as ≃50%. The value of the pseudoscalar mixing angle is estimated as θp=−14.5°±1.0°.

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31

Farber, Paul. "Race-mixing and science in the United States." Endeavour 27, no. 4 (December 2003): 166–70. http://dx.doi.org/10.1016/j.endeavour.2003.08.007.

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32

van Enter, Aernout, and Jacek Miȩkisz. "Typical Ground States for Large Sets of Interactions." Journal of Statistical Physics 181, no. 5 (September 29, 2020): 1906–14. http://dx.doi.org/10.1007/s10955-020-02647-4.

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Анотація:

AbstractWe discuss what ground states for generic interactions look like. We note that a recent result, due to Morris, implies that the behaviour of ground-state measures for generic interactions is similar to that of generic measures. In particular, it follows from his observation that they have singular spectrum and that they are weak mixing, but not mixing.

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33

Huo, Juntao, Kangyuan Li, Bowen Zang, Meng Gao, Li-Min Wang, Baoan Sun, Maozhi Li, Lijian Song, Jun-Qiang Wang, and Wei-Hua Wang. "High Mixing Entropy Enhanced Energy States in Metallic Glasses." Chinese Physics Letters 39, no. 4 (April 1, 2022): 046401. http://dx.doi.org/10.1088/0256-307x/39/4/046401.

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Owing to the nonequilibrium nature, the energy state of metallic glasses (MGs) can vary a lot and has a critical influence on the physical properties. Exploring new methods to modulate the energy state of glasses and studying its relationship with properties have attracted great interests. Herein, we systematically investigate the energy state, mixing entropy and physical properties of Zr–Ti–Cu–Ni–Be multicomponent high entropy MGs by experiments and simulations. We find that the energy state increases along with the increase of mixing entropy. The yield strength and thermal stability of MGs are also enhanced by high mixing entropy. These results may open a new door on regulation of energy states and thus physical properties of MGs.

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34

MA, BO-QIANG. "NEUTRINO OSCILLATIONS: FROM STANDARD AND NON-STANDARD VIEWPOINTS." International Journal of Modern Physics: Conference Series 01 (January 2011): 291–96. http://dx.doi.org/10.1142/s2010194511000420.

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In the standard model of neutrino oscillations, the neutrino flavor states are mixtures of mass-eigenstates, and the phenomena are well described by the neutrino mixing matrix, i.e., the PMNS matrix. I review the recent progress on parametrization of the neutrino mixing matrix. Besides that I also discuss on the possibility to describe the neutrino oscillations by a non-standard model in which the neutrino mixing is caused by the Lorentz violation (LV) contribution in the effective field theory for LV. We assume that neutrinos are massless and that neutrino flavor states are mixing states of energy eigenstates. In our calculation the neutrino mixing parts depend on LV parameters and neutrino energy. The oscillation amplitude varies with the neutrino energy, thus neutrino experiments with energy dependence may test and constrain the Lorentz violation scenario for neutrino oscillation.

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35

ROBERTS, W., and MUSLEMA PERVIN. "HEAVY BARYONS IN A QUARK MODEL." International Journal of Modern Physics A 23, no. 19 (July 30, 2008): 2817–60. http://dx.doi.org/10.1142/s0217751x08041219.

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A quark model is applied to the spectrum of baryons containing heavy quarks. The model gives masses for the known heavy baryons that are in agreement with experiment, but for the doubly-charmed baryon Ξcc, the model prediction is too heavy. Mixing between the ΞQ and Ξ′Q states is examined and is found to be small for the lowest lying states. In contrast with this, mixing between the Ξbc and Ξ′bc states is found to be large, and the implication of this mixing for properties of these states is briefly discussed. We also examine heavy-quark spin-symmetry multiplets, and find that many states in the model can be placed in such multiplets. We compare our predictions with those of a number of other authors.

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36

Abdulvahabova, S. G., and I. G. Afandiyeva. "Population of 0+ excited states in reactions with transmission of two nucleons." Izvestiya vysshikh uchebnykh zavedenii. Fizika, no. 3 (2021): 121–25. http://dx.doi.org/10.17223/00213411/64/3/121.

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Анотація:

Properties of 0+ excited states, generated by the pair and quadrupole-quadrupole interactions in some isotopes of the rare-earth region, are studied. The excitation energies for 0+ states, E (0)- and E (2)-transitions, Rasmussen parameter X and cross sections for two nucleon transfer reactions are calculeted taking into account the mixing of excited states with different values. The contribution of mixing excited states underestimates the values of the calculated physical quantities.

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37

Fanchi, John R. "Neutrino Flavor Transitions as Mass State Transitions." Symmetry 11, no. 8 (July 24, 2019): 948. http://dx.doi.org/10.3390/sym11080948.

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Анотація:

Experiments have shown that transitions occur between electron neutrino, muon neutrino, and tau neutrino flavors. Some experiments indicate the possible existence of a fourth neutrino known as the sterile neutrino. The question arises: do all neutrino flavors participate in transitions between flavors? These transitions are viewed as mass state transitions in parametrized relativistic dynamics (PRD). PRD frameworks have been developed for neutrino flavor transitions associated with the mixing of two mass states or the mixing of three mass states. This paper presents an extension of the framework to neutrino flavor transitions associated with the mixing of four mass states.

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38

SINGH, K. P., T. KAKAVAND, and M. HAJIVALIEI. "LIFETIME MEASUREMENTS OF EXCITED STATES IN 73As." International Journal of Modern Physics E 13, no. 05 (October 2004): 1019–34. http://dx.doi.org/10.1142/s0218301304002569.

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Анотація:

The excited states of 73 As have been investigated via the 73 Ge ( p , n γ)73 As reaction with proton beam energies from 2.5–4.3 MeV. The lifetimes of the levels at 769.6, 860.5, 1177.8, 1188.7, 1274.9, 1344.1, 1557.1 and 1975.2 keV excitation energies have been measured for the first time using the Doppler shift attenuation method. The angular distributions have been used to assign the spins and the multipole mixing ratios using statistical theory for compound nuclear reactions. The ambiguity in the spin values for the various levels has been removed. The multipole mixing ratios for eight γ-transitions have been newly measured.

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39

Franca, Daniel S. "Perfect sampling for quantum Gibbs states." Quantum Information and Computation 18, no. 5&6 (May 2018): 361–88. http://dx.doi.org/10.26421/qic18.5-6-1.

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Анотація:

We show how to obtain perfect samples from a quantum Gibbs state on a quantum computer. To do so, we adapt one of the ``Coupling from the Past''-algorithms proposed by Propp and Wilson. The algorithm has a probabilistic run-time and produces perfect samples without any previous knowledge of the mixing time of a quantum Markov chain. To implement it, we assume we are able to perform the phase estimation algorithm for the underlying Hamiltonian and implement a quantum Markov chain such that the transition probabilities between eigenstates only depend on their energy. We provide some examples of quantum Markov chains that satisfy these conditions and analyze the expected run-time of the algorithm, which depends strongly on the degeneracy of the underlying Hamiltonian. For Hamiltonians with highly degenerate spectrum, it is efficient, as it is polylogarithmic in the dimension and linear in the mixing time. For non-degenerate spectra, its runtime is essentially the same as its classical counterpart, which is linear in the mixing time and quadratic in the dimension, up to a logarithmic factor in the dimension. We analyze the circuit depth necessary to implement it, which is proportional to the sum of the depth necessary to implement one step of the quantum Markov chain and one phase estimation. This algorithm is stable under noise in the implementation of different steps. We also briefly discuss how to adapt different ``Coupling from the Past''-algorithms to the quantum setting.

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40

Ljungberg, Peter, and Ove Axner. "Degenerate four-wave mixing from laser-populated excited states." Applied Optics 34, no. 3 (January 20, 1995): 527. http://dx.doi.org/10.1364/ao.34.000527.

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41

Mogilevtsev, D., N. Korolkova, and J. Perina. "Entangled superpositions of distinguishable states via nonlinear wave mixing." Quantum and Semiclassical Optics: Journal of the European Optical Society Part B 8, no. 6 (December 1996): 1169–78. http://dx.doi.org/10.1088/1355-5111/8/6/006.

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42

Chernyshov, V. N. "Mixing of hole states in GaAs/AlAs(110) heterostructures." Semiconductors 44, no. 10 (October 2010): 1301–7. http://dx.doi.org/10.1134/s1063782610100118.

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43

Reid, M. D., and D. F. Walls. "Generation of squeezed states via degenerate four-wave mixing." Physical Review A 31, no. 3 (March 1, 1985): 1622–35. http://dx.doi.org/10.1103/physreva.31.1622.

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44

Lundquist, Paul B., та David R. Andersen. "Solitary four-wave-mixing states in χ^(3) media". Journal of the Optical Society of America B 14, № 1 (1 січня 1997): 87. http://dx.doi.org/10.1364/josab.14.000087.

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45

Afek, I., O. Ambar, and Y. Silberberg. "High-NOON States by Mixing Quantum and Classical Light." Science 328, no. 5980 (May 13, 2010): 879–81. http://dx.doi.org/10.1126/science.1188172.

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46

Granstrom, Karl, Peter Willett, and Yaakov Bar-Shalom. "Systematic approach to IMM mixing for unequal dimension states." IEEE Transactions on Aerospace and Electronic Systems 51, no. 4 (October 2015): 2975–86. http://dx.doi.org/10.1109/taes.2015.150015.

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47

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