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Статті в журналах з теми "Condensed matter physics not elsewhere classified"

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Автор: Grafiati

Опубліковано: 10 грудня 2022

Оновлено: 28 січня 2023

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1

Leggett, Anthony J. "Matchmaking Between Condensed Matter and Quantum Foundations, and Other Stories: My Six Decades in Physics." Annual Review of Condensed Matter Physics 11, no. 1 (March 10, 2020): 1–16. http://dx.doi.org/10.1146/annurev-conmatphys-031119-050704.

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I present some rather selective reminiscences of my long career in physics, from my doctoral work to the present. I do not spend time on topics such as the nuclear magnetic resonance behavior of 3He, as I have reviewed the history extensively elsewhere, but rather concentrate, first, on my long-running project to make condensed matter physics relevant to questions in the foundations of quantum mechanics, and second, on various rather “quirky” problems such as an attempt to amplify the effects of the parity violation due to the weak interaction to a macroscopic level, and an unconventional proposal for the mechanism of the first-order phase transition between the A and B phases of superfluid liquid 3He.

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2

King, Alex. "Classified." MRS Bulletin 25, no. 3 (March 2000): 104. http://dx.doi.org/10.1557/mrs2000.23.

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3

COFFEY, MARK W. "ON HYPERGEOMETRIC SERIES REDUCTIONS FROM INTEGRAL REPRESENTATIONS, THE KAMPÉ DE FÉRIET FUNCTION AND ELSEWHERE." International Journal of Modern Physics B 19, no. 30 (December 10, 2005): 4483–93. http://dx.doi.org/10.1142/s0217979205032814.

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Single variable hypergeometric functions pFq arise in connection with the power series solution of the Schrödinger equation or in the summation of perturbation expansions in quantum mechanics. For these applications, it is of interest to obtain analytic expressions, and we present the reduction of a number of cases of pFp and p+1Fp, mainly for p=2 and p=3. These and related series have additional applications in quantum and statistical physics and chemistry.

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4

HAO, BAILIN, JI QI, and BIN WANG. "PROKARYOTIC PHYLOGENY BASED ON COMPLETE GENOMES WITHOUT SEQUENCE ALIGNMENT." Modern Physics Letters B 17, no. 03 (February 10, 2003): 91–94. http://dx.doi.org/10.1142/s0217984903004968.

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We present a brief review of a series of on-going work on bacterial phylogeny. We propose a new method to infer relatedness of prokaryotes from their complete genome data without using sequence alignment, leading to results comparable with the bacteriologist's systematics as reflected in the latest 2001 edition of Bergey's Manual of Systematic Bacteriology.1 We only touch on the mathematical aspects of the method. The biological implications of our results will be published elsewhere.

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5

Chu, C. W. "THE EVOLUTION OF HTS: Tc-EXPERIMENT PERSPECTIVES." International Journal of Modern Physics B 24, no. 20n21 (August 30, 2010): 4102–49. http://dx.doi.org/10.1142/s0217979210056463.

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The rise of the superconducting transition temperature Tc has been reviewed in three major superconducting systems: the cuprate, the Fe -pnictide and the heavy fermion. While the first two systems display high Tc s , heavy fermion superconductors show low Tc but embody many crucial features found in the others. The prospect of future superconductors with higher Tc, preferably close to room temperature, is also discussed. Those interested in the detailed physics of high temperature superconductivity are referred to the article by E. Abrahams in the next chapter of this book and reviews published elsewhere.

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6

Park, Jong-Kyu. "Parametric dependencies of resonant layer responses across linear, two-fluid, drift-MHD regimes." Physics of Plasmas 29, no. 7 (July 2022): 072506. http://dx.doi.org/10.1063/5.0093079.

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Non-axisymmetric magnetic fields arising in a tokamak either by external or internal perturbations can induce complex non-ideal MHD responses in their resonant surfaces while remaining ideally evolved elsewhere. This layer response can be characterized in a linear regime by a single parameter called the inner-layer Δ, which enables outer-layer matching and the prediction of torque balance to non-linear island regimes. Here, we follow strictly one of the most comprehensive analytic treatments including two-fluid and drift MHD effects and keep the fidelity of the formulation by incorporating the numerical method based on the Riccati transformation when quantifying the inner-layer Δ. The proposed scheme reproduces not only the predicted responses in essentially all asymptotic regimes but also with continuous transitions as well as improved accuracies. In particular, the Δ variations across the inertial regimes with viscous or semi-collisional effects have been further resolved, in comparison with additional analytic solutions. The results imply greater shielding of the electromagnetic torque at the layer than what would be expected by earlier work when the viscous or semi-collisional effects can compete against the inertial effects, and also due to the intermediate regulation by kinetic Alfvén wave resonances as rotation slows down. These are important features that can alter the non-axisymmetric plasma responses including the field penetration by external fields or island seeding process in rotating tokamak plasmas.

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7

PENG, Yongkang, Xiaoyue CHEN, Yeqiang DENG, Lei LAN, Haoyu ZHAN, Xuekai PEI, Jiahao CHEN, Yukuan YUAN, and Xishan WEN. "Kinetic study of key species and reactions of atmospheric pressure pulsed corona discharge in humid air." Plasma Science and Technology 24, no. 5 (April 13, 2022): 055404. http://dx.doi.org/10.1088/2058-6272/ac4693.

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Abstract In this study, we examined the key particles and chemical reactions that substantially influence plasma characteristics. In summarizing the chemical reaction model for the discharge process of N2–O2–H2O(g) mixed gases, 65 particle types and 673 chemical reactions were investigated. On this basis, a global model of atmospheric pressure humid air discharge plasma was developed, with a focus on the variation of charged particles densities and chemical reaction rates with time under the excitation of a 0–200 Td pulsed electric field. Particles with a density greater than 1% of the electron density were classified as key particles. For such particles, the top ranking generation or consumption reactions (i.e. where the sum of their rates was greater than 95% of the total rate of the generation or consumption reactions) were classified as key chemical reactions. On the basis of the key particles and reactions identified, a simplified global model was derived. A comparison of the global model with the simplified global model in terms of the model parameters, particle densities, reaction rates (with time), and calculation efficiencies demonstrated that both models can adequately identify the key particles and chemical reactions reflecting the chemical process of atmospheric pressure discharge plasma in humid air. Thus, by analyzing the key particles and chemical reaction pathways, the charge and substance transfer mechanism of atmospheric pressure pulse discharge plasma in humid air was revealed, and the mechanism underlying water vapor molecules’ influence on atmospheric pressure air discharge was elucidated.

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8

Lannert, C., and Matthew P. A. Fisher. "Inelastic Neutron Scattering Signal from Deconfined Spinons in a Fractionalized Antiferromagnet." International Journal of Modern Physics B 17, no. 15 (June 20, 2003): 2821–38. http://dx.doi.org/10.1142/s0217979203015802.

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We calculate the contribution of deconfined spinons to inelastic neutron scattering (INS) in the fractionalized antiferromagnet (AF*), introduced elsewhere. We find that the presence of free spin-1/2 charge-less excitations leads to a continuum INS signal above the Néel gap. This signal is found above and in addition to the usual spin-1 magnon signal, which to lowest order is the same as in the more conventional confined antiferromagnet. We calculate the relative weights of these two signals and find that the spinons contribute to the longitudinal response, where the magnon signal is absent to lowest order. Possible higher-order effects of interactions between magnons and spinons in the AF* phase are also discussed.

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9

SU, W. P. "INHOMOGENEOUS D-WAVE SUPERCONDUCTIVITY." International Journal of Modern Physics B 21, no. 23n24 (September 30, 2007): 4144–50. http://dx.doi.org/10.1142/s0217979207045323.

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To understand several peculiar features of d-wave superconductors such as the cuprates, we have studied a two-dimensional tight-binding (extended Hubbard) model in which the electrons interact with a potential which is attractive at nearest neighbor distance and repulsive elsewhere. Such a model is designed to produce d-wave superconductivity. It also yields antiferromagnetism and phase separation. In the two-phase region, due to vanishing compressibility the system can be easily rendered inhomogeneous by weak perturbations. Thus inhomogeneous superconductivity is a likely consequence of d-wave pairing. In addition to inhomogeneity the model also reproduces a phase diagram strikingly similar to the one observed in the cuprates. As such it throws some light on the nature of the pseudogap state.

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10

Prasad, Arun S. "Spin injection behavior in conducting polymer coated superparamagnetically functional microstructures." Modern Physics Letters B 28, no. 15 (June 17, 2014): 1450119. http://dx.doi.org/10.1142/s021798491450119x.

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A nanoferrite superparamagnetic system synthesized through co-precipitation method and subsequently dispersed in a medium of de-ionized water was encapsulated with a matrix polymer under constant sonication using chemical oxidative polymerization technique. The polymer coated functional microstructure thus obtained shows enhanced magnetization as evidenced from the results reported elsewhere. The magnetic core crystal growth and anti-spin canting hypothesis were given to be the most general justification behind the unusual enhancement in magnetization and more specifically the rationale could understand recently in accordance with spin injection behavior in functional core-shell microstructures. In this paper, an attempt has been made to correlate the previous magnetization results with spin injection behavior, in conjunction with the thermo gravimetric and dielectric results.

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11

Frank, P., M. Beckmann, and G. Himmel. "Analytical description of low-frequency electron density and temperature oscillations." Journal of Plasma Physics 55, no. 1 (February 1996): 25–34. http://dx.doi.org/10.1017/s0022377800018638.

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Low-frequency density and temperature oscillations (ω « νj, ωcj, where νj is the collision frequency with neutrals and ωcj is the cyclotron frequency; j = i, e) observed in magnetized radiofrequency-produced plasmas with electron density and temperature gradients across the magnetic field are analysed using a local two-fluid model. This model incorporates the electron energy equation. The resulting dispersion relation permits study of the parameter dependence of the complex angular wave frequency. Instability is found in the case where the election density and temperature gradients have opposite signs. This instability is classified as a low-frequency drift wave, and the criteria for its onset are obtained.

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12

Tauheed, A., M. S. Z. Chaghtai, and K. Rahimullah. "Classified Lines and Energy Levels of Mo V." Physica Scripta 31, no. 5 (May 1, 1985): 369–78. http://dx.doi.org/10.1088/0031-8949/31/5/011.

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13

Liu, Qianwei, Bixin Jin, Qin Li, Huanzhi Yang, Yunjun Luo, and Xiaoyu Li. "Self-sorting assembly of artificial building blocks." Soft Matter 18, no. 13 (2022): 2484–99. http://dx.doi.org/10.1039/d2sm00153e.

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Strategies for fabricating artificial self-sorting systems are summarized and classified into five main categories based on their interactive mechanisms, focusing on supramolecular and polymeric species, to provide guidance for the future studies.

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14

Weisbuch, Claude, and Henri Benisty. "Microcavities in Ecole Polytechnique Fédérale de Lausanne, Ecole Polytechnique (France) and elsewhere: past, present and future." physica status solidi (b) 242, no. 11 (September 2005): 2345–56. http://dx.doi.org/10.1002/pssb.200560972.

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15

Hamioud, Farida, and A. A. Mubarak. "The mechanical, optoelectronic and thermoelectric properties of NiYSn (Y = Zr and Hf) alloys." International Journal of Modern Physics B 31, no. 23 (September 14, 2017): 1750170. http://dx.doi.org/10.1142/s0217979217501703.

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First-principle calculations are performed using DFT as implemented in Wien2k code to compute the mechanical, electronic, optical and thermoelectric properties of NiYSn (Y = Zr and Hf) alloys. The computed lattice constants, bulk modulus and cohesive energy of these alloys at 0 K and 0 GPa are performed. NiZrSn and NiHfSn are found to be anisotropic and elastically stable. Furthermore, both alloys are confirmed to be thermodynamically stable by the calculated values of the standard enthalpy of formation. The Young’s and shear moduli values show that NiZrSn seems to be stiffer than NiHfSn. The optical properties are performed using the dielectric function. Some beneficial optoelectronic applications are found as exposed in the optical spectra. Moreover, the alloys are classified as good insulators for solar heating. The thermoelectric properties as a function of temperature are computed utilizing BoltzTrap code. The major charge carriers are found to be electrons and the alloys are classified as [Formula: see text]-type doping alloys.

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16

Wells, D. R. "Containment forces in stable plasma configurations." Laser and Particle Beams 6, no. 3 (August 1988): 539–44. http://dx.doi.org/10.1017/s0263034600005450.

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It is demonstrated that finite pressure gradients can be maintained in the lowest free energy state (‘relaxed state’) of a plasma configuration. The pressure forces are supported by the Magnus Force in a compressible adiabatic plasma if mass motions are considered. It has been demonstrated elsewhere that these forces can be of the same order of magnitude as the Lorentz forces in some laboratory plasmas.

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17

"Classified." MRS Bulletin 17, no. 4 (April 1992): 78–80. http://dx.doi.org/10.1557/s088376940004118x.

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18

"Classified." MRS Bulletin 17, no. 8 (August 1992): 78–80. http://dx.doi.org/10.1557/s0883769400041956.

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19

"Classified." MRS Bulletin 18, no. 3 (March 1993): 109–12. http://dx.doi.org/10.1557/s0883769400044080.

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20

"Classified." MRS Bulletin 20, no. 3 (March 1995): 86–88. http://dx.doi.org/10.1557/s0883769400044523.

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21

"Classified." MRS Bulletin 21, no. 2 (February 1996): 86. http://dx.doi.org/10.1557/s0883769400046352.

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22

"Classified." MRS Bulletin 18, no. 6 (June 1993): 71. http://dx.doi.org/10.1557/s0883769400047436.

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23

"Classified." MRS Bulletin 19, no. 8 (August 1994): 87–88. http://dx.doi.org/10.1557/s0883769400047874.

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24

"Classified." MRS Bulletin 19, no. 10 (October 1994): 71–72. http://dx.doi.org/10.1557/s0883769400048296.

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25

"Classified." MRS Bulletin 20, no. 1 (January 1995): 75–78. http://dx.doi.org/10.1557/s0883769400049071.

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26

"Classified." MRS Bulletin 24, no. 9 (September 1999): 76. http://dx.doi.org/10.1557/s0883769400053136.

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27

"Classified." MRS Bulletin 11, no. 5 (October 1986): 59–60. http://dx.doi.org/10.1557/s0883769400054622.

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28

"Classified." MRS Bulletin 14, no. 4 (April 1989): 76–78. http://dx.doi.org/10.1557/s0883769400055196.

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29

"Classified." MRS Bulletin 16, no. 3 (March 1991): 71. http://dx.doi.org/10.1557/s0883769400057511.

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30

"Classified." MRS Bulletin 15, no. 11 (November 1990): 107–11. http://dx.doi.org/10.1557/s0883769400058528.

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31

"Classified." MRS Bulletin 14, no. 2 (February 1989): 73–76. http://dx.doi.org/10.1557/s0883769400063569.

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32

"Classified." MRS Bulletin 13, no. 12 (December 1988): 77–80. http://dx.doi.org/10.1557/s0883769400063818.

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33

"Classified." MRS Bulletin 13, no. 9 (September 1988): 59. http://dx.doi.org/10.1557/s0883769400064538.

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34

"Classified." MRS Bulletin 13, no. 7 (July 1988): 53–55. http://dx.doi.org/10.1557/s0883769400065349.

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35

"Classified." MRS Bulletin 13, no. 5 (May 1988): 50–52. http://dx.doi.org/10.1557/s0883769400065763.

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36

"Classified." MRS Bulletin 13, no. 4 (April 1988): 71–72. http://dx.doi.org/10.1557/s0883769400066033.

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37

"Classified." MRS Bulletin 13, no. 3 (March 1988): 55. http://dx.doi.org/10.1557/s0883769400066239.

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38

"Classified." MRS Bulletin 12, no. 2 (March 1987): 98. http://dx.doi.org/10.1557/s0883769400068615.

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39

"Classified." MRS Bulletin 11, no. 2 (April 1986): 52. http://dx.doi.org/10.1557/s0883769400069621.

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40

"Classified." MRS Bulletin 23, no. 9 (September 1998): 87–88. http://dx.doi.org/10.1557/s0883769400029468.

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41

"Classified." MRS Bulletin 21, no. 11 (November 1996): 95. http://dx.doi.org/10.1557/s0883769400031973.

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42

"Classified." MRS Bulletin 22, no. 11 (November 1997): 105–11. http://dx.doi.org/10.1557/s0883769400034588.

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43

"Classified." MRS Bulletin 22, no. 12 (December 1997): 70. http://dx.doi.org/10.1557/s0883769400034801.

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44

"Classified." MRS Bulletin 21, no. 9 (September 1996): 79. http://dx.doi.org/10.1557/s0883769400036423.

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45

"Classified." MRS Bulletin 19, no. 6 (June 1994): 71–72. http://dx.doi.org/10.1557/s0883769400036836.

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46

"Classified." MRS Bulletin 18, no. 8 (August 1993): 79–80. http://dx.doi.org/10.1557/s0883769400037908.

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47

"Classified." MRS Bulletin 18, no. 9 (September 1993): 94–96. http://dx.doi.org/10.1557/s088376940003815x.

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48

"Classified." MRS Bulletin 10, no. 2 (April 1985): 20. http://dx.doi.org/10.1557/s0883769400040008.

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49

"Classified." MRS Bulletin 10, no. 5 (October 1985): 32. http://dx.doi.org/10.1557/s0883769400040306.

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50

"Classified." MRS Bulletin 31, no. 9 (September 2006): 704–11. http://dx.doi.org/10.1557/mrs2006.183.

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