Journal articles on the topic 'Chiral magnetic effect'

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1

Fukushima, Kenji. "Chiral Magnetic Effect." Progress of Theoretical Physics Supplement 193 (2012): 15–19. http://dx.doi.org/10.1143/ptps.193.15.

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2

Ali-Akbari, M., and S. F. Taghavi. "-Corrected Chiral Magnetic Effect." Nuclear Physics B 872, no. 1 (July 2013): 127–40. http://dx.doi.org/10.1016/j.nuclphysb.2013.03.011.

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3

Dong, Ren-Da, Ren-Hong Fang, De-Fu Hou, and Duan She. "Chiral magnetic effect for chiral fermion system." Chinese Physics C 44, no. 7 (June 29, 2020): 074106. http://dx.doi.org/10.1088/1674-1137/44/7/074106.

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4

Fu, Wei-Jie, and Yue-Liang Wu. "Chiral Magnetic Effect and Chiral Phase Transition." Communications in Theoretical Physics 55, no. 1 (January 2011): 123–27. http://dx.doi.org/10.1088/0253-6102/55/1/23.

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5

Li, Qiang, Dmitri E. Kharzeev, Cheng Zhang, Yuan Huang, I. Pletikosić, A. V. Fedorov, R. D. Zhong, J. A. Schneeloch, G. D. Gu, and T. Valla. "Chiral magnetic effect in ZrTe5." Nature Physics 12, no. 6 (February 8, 2016): 550–54. http://dx.doi.org/10.1038/nphys3648.

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6

Li, Wei, and Gang Wang. "Chiral Magnetic Effects in Nuclear Collisions." Annual Review of Nuclear and Particle Science 70, no. 1 (October 19, 2020): 293–321. http://dx.doi.org/10.1146/annurev-nucl-030220-065203.

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The interplay of quantum anomalies with strong magnetic fields and vorticity in chiral systems could lead to novel transport phenomena, such as the chiral magnetic effect (CME), the chiral magnetic wave (CMW), and the chiral vortical effect (CVE). In high-energy nuclear collisions, these chiral effects may survive the expansion of a quark–gluon plasma fireball and be detected in experiments. The experimental searches for the CME, the CMW, and the CVE have aroused extensive interest over the past couple of decades. The main goal of this article is to review the latest experimental progress in the search for these novel chiral transport phenomena at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory and the Large Hadron Collider at CERN. Future programs to help reduce uncertainties and facilitate the interpretation of the data are also discussed.
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7

Grieninger, Sebastian, and Sergio Morales-Tejera. "Far from equilibrium Chiral Magnetic Effect in Strong Magnetic Fields from Holography." EPJ Web of Conferences 258 (2022): 10007. http://dx.doi.org/10.1051/epjconf/202225810007.

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We study the real time evolution of the chiral magnetic effect out-ofequilibrium in strongly coupled anomalous field theories. We match the parameters of our model to QCD parameters and draw lessons of possible relevance for the realization of the chiral magnetic effect in heavy ion collisions. In particular, we find an equilibration time of about ~ 0:35 fm/c in presence of the chiral anomaly for plasma temperatures of order T ~ 300 - 400 MeV.
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8

FU, WEI-JIE, YU-XIN LIU, and YUE-LIANG WU. "CHIRAL MAGNETIC EFFECT AND QCD PHASE TRANSITIONS WITH EFFECTIVE MODELS." International Journal of Modern Physics A 26, no. 25 (October 10, 2011): 4335–65. http://dx.doi.org/10.1142/s0217751x11054541.

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We study the influence of the chiral phase transition on the chiral magnetic effect. The chiral electric current density along the magnetic field, the electric charge difference between on each side of the reaction plane, and the azimuthal charged-particle correlations as functions of the temperature during the QCD phase transitions are calculated. It is found that with the decrease of the temperature, the chiral electric current density, the electric charge difference, and the azimuthal charged-particle correlations all get a sudden suppression at the critical temperature of the chiral phase transition, because the large quark constituent mass in the chiral symmetry broken phase quite suppresses the axial anomaly and the chiral magnetic effect. We suggest that the azimuthal charged-particle correlations (including the correlators divided by the total multiplicity of produced charged particles which are used in current experiments and another kind of correlators not divided by the total multiplicity) can be employed to identify the occurrence of the QCD phase transitions in RHIC energy scan experiments.
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9

Chernodub, Maxim N., and Alberto Cortijo. "Non-Hermitian Chiral Magnetic Effect in Equilibrium." Symmetry 12, no. 5 (May 6, 2020): 761. http://dx.doi.org/10.3390/sym12050761.

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We analyze the chiral magnetic effect for non-Hermitian fermionic systems using the bi-orthogonal formulation of quantum mechanics. In contrast to the Hermitian counterparts, we show that the chiral magnetic effect takes place in equilibrium when a non-Hermitian system is considered. The key observation is that for non-Hermitian charged systems, there is no strict charge conservation as understood in Hermitian systems, so the Bloch theorem preventing currents in the thermodynamic limit and in equilibrium does not apply.
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10

Huang, Xu-Guang, Wei-Tian Deng, Guo-Liang Ma, and Gang Wang. "Chiral magnetic effect in isobaric collisions." Nuclear Physics A 967 (November 2017): 736–39. http://dx.doi.org/10.1016/j.nuclphysa.2017.05.071.

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11

Shevchenko, V. I. "Quantum measurements and chiral magnetic effect." Nuclear Physics B 870, no. 1 (May 2013): 1–15. http://dx.doi.org/10.1016/j.nuclphysb.2013.01.004.

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12

Buividovich, P. V. "Axial Magnetic Effect and Chiral Vortical Effect with free lattice chiral fermions." Journal of Physics: Conference Series 607 (May 14, 2015): 012018. http://dx.doi.org/10.1088/1742-6596/607/1/012018.

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13

Kumar, Anup, Prakash Mondal, and Claudio Fontanesi. "Chiral Magneto-Electrochemistry." Magnetochemistry 4, no. 3 (August 18, 2018): 36. http://dx.doi.org/10.3390/magnetochemistry4030036.

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Magneto-electrochemistry (MEC) is a unique paradigm in science, where electrochemical experiments are carried out as a function of an applied magnetic field, creating a new horizon of potential scientific interest and technological applications. Over time, detailed understanding of this research domain was developed to identify and rationalize the possible effects exerted by a magnetic field on the various microscopic processes occurring in an electrochemical system. Notably, until a few years ago, the role of spin was not taken into account in the field of magneto-electrochemistry. Remarkably, recent experimental studies reveal that electron transmission through chiral molecules is spin selective and this effect has been referred to as the chiral-induced spin selectivity (CISS) effect. Spin-dependent electrochemistry originates from the implementation of the CISS effect in electrochemistry, where the magnetic field is used to obtain spin-polarized currents (using ferromagnetic electrodes) or, conversely, a magnetic field is obtained as the result of spin accumulation.
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14

Huang, Anping, Yin Jiang, Shuzhe Shi, Jinfeng Liao, and Pengfei Zhuang. "Out-of-equilibrium chiral magnetic effect from chiral kinetic theory." Physics Letters B 777 (February 2018): 177–83. http://dx.doi.org/10.1016/j.physletb.2017.12.025.

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15

Wang, Gang, and Liwen Wen. "Experimental Results on Chiral Magnetic and Vortical Effects." Advances in High Energy Physics 2017 (2017): 1–17. http://dx.doi.org/10.1155/2017/9240170.

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Various novel transport phenomena in chiral systems result from the interplay of quantum anomalies with magnetic field and vorticity in high-energy heavy-ion collisions and could survive the expansion of the fireball and be detected in experiments. Among them are the chiral magnetic effect, the chiral vortical effect, and the chiral magnetic wave, the experimental searches for which have aroused extensive interest. The goal of this review is to describe the current status of experimental studies at Relativistic Heavy-Ion Collider at BNL and the Large Hadron Collider at CERN and to outline the future work in experiment needed to eliminate the existing uncertainties in the interpretation of the data.
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16

Zhao, Jie. "Charge dependent particle correlations motivated by chiral magnetic effect and chiral vortical effect." EPJ Web of Conferences 141 (2017): 01010. http://dx.doi.org/10.1051/epjconf/201714101010.

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17

Liao, Jinfeng. "Chiral Magnetic Effect in Heavy Ion Collisions." Nuclear Physics A 956 (December 2016): 99–106. http://dx.doi.org/10.1016/j.nuclphysa.2016.02.027.

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18

Li, Qiang, and Dmitri E. Kharzeev. "Chiral magnetic effect in condensed matter systems." Nuclear Physics A 956 (December 2016): 107–11. http://dx.doi.org/10.1016/j.nuclphysa.2016.03.055.

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19

Isachenkov, M. V., and A. V. Sadofyev. "The chiral magnetic effect in hydrodynamical approach." Physics Letters B 697, no. 4 (March 2011): 404–6. http://dx.doi.org/10.1016/j.physletb.2011.02.041.

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20

Shevchenko, V. I. "Non-stationary measurements of Chiral Magnetic Effect." Annals of Physics 339 (December 2013): 371–81. http://dx.doi.org/10.1016/j.aop.2013.09.017.

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21

Huang, Xu-Guang. "Phenomenology of anomalous chiral transports in heavy-ion collisions." EPJ Web of Conferences 172 (2018): 01003. http://dx.doi.org/10.1051/epjconf/201817201003.

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High-energy Heavy-ion collisions can generate extremely hot quark-gluon matter and also extremely strong magnetic fields and fluid vorticity. Once coupled to chiral anomaly, the magnetic fields and fluid vorticity can induce a variety of novel transport phenomena, including the chiral magnetic effect, chiral vortical effect, etc. Some of them require the environmental violation of parity and thus provide a means to test the possible parity violation in hot strongly interacting matter. We will discuss the underlying mechanism and implications of these anomalous chiral transports in heavy-ion collisions.
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22

Sukenik, Nir, Francesco Tassinari, Shira Yochelis, Oded Millo, Lech Tomasz Baczewski, and Yossi Paltiel. "Correlation between Ferromagnetic Layer Easy Axis and the Tilt Angle of Self Assembled Chiral Molecules." Molecules 25, no. 24 (December 20, 2020): 6036. http://dx.doi.org/10.3390/molecules25246036.

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The spin–spin interactions between chiral molecules and ferromagnetic metals were found to be strongly affected by the chiral induced spin selectivity effect. Previous works unraveled two complementary phenomena: magnetization reorientation of ferromagnetic thin film upon adsorption of chiral molecules and different interaction rate of opposite enantiomers with a magnetic substrate. These phenomena were all observed when the easy axis of the ferromagnet was out of plane. In this work, the effects of the ferromagnetic easy axis direction, on both the chiral molecular monolayer tilt angle and the magnetization reorientation of the magnetic substrate, are studied using magnetic force microscopy. We have also studied the effect of an applied external magnetic field during the adsorption process. Our results show a clear correlation between the ferromagnetic layer easy axis direction and the tilt angle of the bonded molecules. This tilt angle was found to be larger for an in plane easy axis as compared to an out of plane easy axis. Adsorption under external magnetic field shows that magnetization reorientation occurs also after the adsorption event. These findings show that the interaction between chiral molecules and ferromagnetic layers stabilizes the magnetic reorientation, even after the adsorption, and strongly depends on the anisotropy of the magnetic substrate. This unique behavior is important for developing enantiomer separation techniques using magnetic substrates.
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23

Dvornikov, Maxim. "Magnetic fields in turbulent quark matter and magnetar bursts." International Journal of Modern Physics D 27, no. 01 (December 28, 2017): 1750184. http://dx.doi.org/10.1142/s021827181750184x.

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We analyze the magnetic field evolution in dense quark matter with unbroken chiral symmetry, which can be found inside quark and hybrid stars. The magnetic field evolves owing to the chiral magnetic effect in the presence of the electroweak interaction between quarks. In our study, we also take into account the magnetohydrodynamic turbulence effects in dense quark matter. We derive the kinetic equations for the spectra of the magnetic helicity density and the magnetic energy density as well as for the chiral imbalances. On the basis of the numerical solution of these equations, we find that turbulence effects are important for the behavior of small scale magnetic fields. It is revealed that, under certain initial conditions, these magnetic fields behave similarly to the electromagnetic flashes of some magnetars. We suggest that fluctuations of magnetic fields, described in frames of our model, which are created in the central regions of a magnetized compact star, can initiate magnetar bursts.
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24

Fang, Ren-Hong, Ren-Da Dong, De-Fu Hou, and Bao-Dong Sun. "Thermodynamics of the System of Massive Dirac Fermions in a Uniform Magnetic Field." Chinese Physics Letters 38, no. 9 (October 1, 2021): 091201. http://dx.doi.org/10.1088/0256-307x/38/9/091201.

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We construct the grand partition function of the system of massive Dirac fermions in a uniform magnetic field from Landau levels, through which all thermodynamic quantities can be obtained. Making use of the Abel–Plana formula, these thermodynamic quantities can be expanded as power series with respect to the dimensionless variable b = 2eB/T 2. The zero-field magnetic susceptibility is expanded at zero mass, and the leading order term is logarithmic. We also calculate scalar, vector current, axial vector current and energy-momentum tensor of the system through ensemble average approach. Mass correction to chiral separation effect is discussed. For massless chiral fermions, our results recover the chiral magnetic effect for right- and left-handed fermions, as well as chiral separation effect.
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25

Yang, Ji-Chong, Qing-Qing Mao, and Yu Shi. "Generation of magnetic skyrmions through pinning effect." Modern Physics Letters B 33, no. 02 (January 20, 2019): 1950040. http://dx.doi.org/10.1142/s0217984919500404.

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Based on analytical estimation and lattice simulation, a proposal is made that magnetic skyrmions can be generated through the pinning effect in 2D chiral magnetic materials, in the absence of an external magnetic field or magnetic anisotropy. In our simulation, stable magnetic skyrmions can be generated in the pinning areas. The properties of the skyrmions are studied for various values of ferromagnetic exchange strength and the Dzyaloshinskii–Moriya interaction strength.
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26

Kumar, Rajesh, and Arvind Kumar. "η mesons in hot magnetized nuclear matter." Chinese Physics C 46, no. 2 (February 1, 2022): 024109. http://dx.doi.org/10.1088/1674-1137/ac3bc7.

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Abstract interactions are investigated in hot magnetized asymmetric nuclear matter using the chiral SU(3) model and chiral perturbation theory (ChPT). In the chiral model, the in-medium properties of η-mesons are calculated using medium modified scalar densities under the influence of an external magnetic field. Further, in a combined chiral model and ChPT approach, off-shell contributions of the interactions are evaluated from the ChPT effective Lagrangian, and the in-medium effect of scalar densities are incorporated from the chiral SU(3) model. We find that the magnetic field has a significant effect on the in-medium mass and optical potential of η mesons, and we observe a deeper mass-shift in the combined chiral model and ChPT approach than in the solo chiral SU(3) model. In both approaches, no additional mass-shift is observed due to the uncharged nature of η mesons in the presence of a magnetic field.
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27

Liu, Xuan, Xiaohui Liu, and Shijie Xie. "Chiral resistance effect in an organic helical heterojunction device." Applied Physics Letters 121, no. 11 (September 12, 2022): 113502. http://dx.doi.org/10.1063/5.0098584.

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Chiral-induced spin selectivity has stimulated the investigation of chiral electronics and spintronics. In this theoretical work, we propose chiral resistance (CR) in a heterojunction constituted by two adjacent molecules with different chiralities. We study chirality-dependent transport properties in such a non-magnetic helical heterojunction and find that chiral-induced spin–orbit coupling and chiral-induced spinterface will affect the electron transmission through the device and lead to large CR at low bias. We demonstrate the dependence of CR on the molecule length, the chirality-inversion ratio, and the chirality mismatch. Our studies are helpful to understand the transport properties in a helical heterojunction, and the proposed CR effect could be used to design future spintronics devices.
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28

Wang, Zhiwen, Jinghua Liang, and Hongxin Yang. "Strain-Enabled Control of Chiral Magnetic Structures in MnSeTe Monolayer." Chinese Physics Letters 40, no. 1 (January 1, 2023): 017501. http://dx.doi.org/10.1088/0256-307x/40/1/017501.

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Chiral magnetic states are promising for future spintronic applications. Recent progress of chiral spin textures in two-dimensional magnets, such as chiral domain walls, skyrmions, and bimerons, have been drawing extensive attention. Here, via first-principles calculations, we show that biaxial strain can effectively manipulate the magnetic parameters of the Janus MnSeTe monolayer. Interestingly, we find that both the magnitude and the sign of the magnetic constants of the Heisenberg exchange coupling, Dzyaloshinskii–Moriya interaction and magnetocrystalline anisotropy can be tuned by strain. Moreover, using micromagnetic simulations, we obtain the distinct phase diagram of chiral spin texture under different strains. Especially, we demonstrate that abundant chiral magnetic structures including ferromagnetic skyrmion, skyrmionium, bimeron, and antiferromagnetic spin spiral can be induced in the MnSeTe monolayer. We also discuss the effect of temperature on these magnetic structures. The findings highlight the Janus MnSeTe monolayer as a good candidate for spintronic nanodevices.
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29

Teryaev, O. V., and D. A. Shohonov. "Chiral Magnetic Effect and the Heisenberg–Euler Lagrangian." Physics of Particles and Nuclei Letters 19, no. 4 (July 26, 2022): 317–19. http://dx.doi.org/10.1134/s1547477122040203.

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30

Brandenburg, Axel, Yutong He, Tina Kahniashvili, Matthias Rheinhardt, and Jennifer Schober. "Relic Gravitational Waves from the Chiral Magnetic Effect." Astrophysical Journal 911, no. 2 (April 1, 2021): 110. http://dx.doi.org/10.3847/1538-4357/abe4d7.

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31

Sun, Yifeng, Che Ming Ko, and Feng Li. "Chiral magnetic effect in the anomalous transport model." Journal of Physics: Conference Series 832 (April 25, 2017): 012042. http://dx.doi.org/10.1088/1742-6596/832/1/012042.

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32

Mizher, Ana Julia, Alfredo Raya, and Cristián Villavicencio. "The pseudo chiral magnetic effect in QED 3." Nuclear and Particle Physics Proceedings 270-272 (January 2016): 181–84. http://dx.doi.org/10.1016/j.nuclphysbps.2016.02.036.

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33

Kharzeev, Dmitri E. "The Chiral Magnetic Effect and anomaly-induced transport." Progress in Particle and Nuclear Physics 75 (March 2014): 133–51. http://dx.doi.org/10.1016/j.ppnp.2014.01.002.

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34

Tang, A. H. "Probe chiral magnetic effect with signed balance function." Chinese Physics C 44, no. 5 (April 28, 2020): 054101. http://dx.doi.org/10.1088/1674-1137/44/5/054101.

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35

Fukushima, Kenji, Dmitri E. Kharzeev, and Harmen J. Warringa. "Electric-current susceptibility and the Chiral Magnetic Effect." Nuclear Physics A 836, no. 3-4 (May 2010): 311–36. http://dx.doi.org/10.1016/j.nuclphysa.2010.02.003.

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36

L'YI*, Won Sik. "Spontaneous Symmetry Breaking and the Chiral Magnetic Effect." New Physics: Sae Mulli 64, no. 5 (May 30, 2014): 523–25. http://dx.doi.org/10.3938/npsm.64.523.

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37

Mandal, Tanumoy, and Prashanth Jaikumar. "Effect of Strong Magnetic Field on Competing Order Parameters in Two-Flavor Dense Quark Matter." Advances in High Energy Physics 2017 (2017): 1–11. http://dx.doi.org/10.1155/2017/6472909.

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We study the effect of strong magnetic field on competing chiral and diquark order parameters in a regime of moderately dense quark matter. The interdependence of the chiral and diquark condensates through nonperturbative quark mass and strong coupling effects is analyzed in a two-flavor Nambu-Jona-Lasinio (NJL) model. In the weak magnetic field limit, our results agree qualitatively with earlier zero-field studies in the literature that find a critical coupling ratioGD/GS~1.1below which chiral or superconducting order parameters appear almost exclusively. Above the critical ratio, there exists a significant mixed broken phase region where both gaps are nonzero. However, a strong magnetic fieldB≳1018 G disrupts this mixed broken phase region and changes a smooth crossover found in the weak-field case to a first-order transition for both gaps at almost the same critical density. Our results suggest that in the two-flavor approximation to moderately dense quark matter strong magnetic field enhances the possibility of a mixed phase at high density, with implications for the structure, energetics, and vibrational spectrum of neutron stars.
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38

Sigl, Günter, and Natacha Leite. "Chiral magnetic effect in protoneutron stars and magnetic field spectral evolution." Journal of Cosmology and Astroparticle Physics 2016, no. 01 (January 14, 2016): 025. http://dx.doi.org/10.1088/1475-7516/2016/01/025.

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39

Liu, Juan, and Song Shi. "Chiral Chemical Potential and Magnetic Effects on QCD Matter in NJL Model with a Self-Consistent Method." Symmetry 14, no. 3 (March 1, 2022): 502. http://dx.doi.org/10.3390/sym14030502.

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The NJL model of one-flavor quark is employed to study the properties of QCD mater with finite temperature, external magnetic field, and chiral chemical potential. Through the mean-field approximation and a self-consistent method, a non-perturbative quark propagator is proposed to deduce the gap equations, and it can be proved that besides the classic vacuum condensate, there are non-zero statistical averages of a quark current and quark magnetic moment. Through a rigorous algebraic method, the quark current leads to a modified chiral magnetic effect. Through a numerical method, the quark magnetic moment is non-zero in the chiral breaking phase, and its relation with chiral chemical potential is studied.
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40

Dayi, Ömer F., and Mahmut Elbistan. "A semiclassical formulation of the chiral magnetic effect and chiral anomaly in even d + 1 dimensions." International Journal of Modern Physics A 31, no. 13 (May 8, 2016): 1650074. http://dx.doi.org/10.1142/s0217751x16500743.

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In terms of the matrix valued Berry gauge field strength for the Weyl Hamiltonian in any even space–time dimensions a symplectic form whose elements are matrices in spin indices is introduced. Definition of the volume form is modified appropriately. A simple method of finding the path integral measure and the chiral current in the presence of external electromagnetic fields is presented. It is shown that within this new approach the chiral magnetic effect as well as the chiral anomaly in even [Formula: see text] dimensions are accomplished straightforwardly.
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41

Mukherjee, Tamal K., and Soma Sanyal. "Particle temperature and the chiral vortical effect in the early universe." Modern Physics Letters A 32, no. 32 (October 12, 2017): 1750178. http://dx.doi.org/10.1142/s0217732317501784.

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We study the effect of hotter or colder particles on the evolution of the chiral magnetic field in the early universe. We are interested in the temperature-dependent term in the chiral vortical effect (CVE). There are no changes in the magnetic energy spectrum at large length scales but in the Kolmogorov regime we do find a difference. Our numerical results show that the Gaussian peak in the magnetic spectrum becomes negatively skewed. The negatively skewed peak can be fitted with a beta distribution. Analytically, one can relate the non-Gaussianity of the distribution to the temperature-dependent vorticity term. The vorticity term is therefore responsible for the beta distribution in the magnetic spectrum. Since the beta distribution has already been used to model turbulent dispersion in fluids, hence it seems that the presence of hotter or colder particles may lead to turbulence in the magnetized plasma.
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42

Gómez Dumm, D., M. F. Izzo Villafañe, S. Noguera, V. P. Pagura, and N. N. Scoccola. "Strong magnetic fields in a nonlocal Polyakov chiral quark model." EPJ Web of Conferences 172 (2018): 02007. http://dx.doi.org/10.1051/epjconf/201817202007.

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We study the behavior of strongly interacting matter under an external constant magnetic field in the context of nonlocal chiral quark models that incorporate a coupling to the Polyakov loop. We find that at zero temperature the behavior of the quark condensates shows the expected magnetic catalysis effect, our predictions being in good quantitative agreement with lattice QCD results. On the other hand when the analysis is extended to the case of finite temperature our results show that nonlocal models naturally lead to the Inverse Magnetic Catalysis effect for both the chiral restoration and deconfinement transition temperatures.
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43

Chernodub, Maxim N., Julien Garaud, and Dmitri E. Kharzeev. "Chiral Magnetic Josephson Junction as a Base for Low-Noise Superconducting Qubits." Universe 8, no. 12 (December 14, 2022): 657. http://dx.doi.org/10.3390/universe8120657.

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The lack of space inversion symmetry endows non-centrosymmetric superconducting materials with various interesting parity-breaking phenomena, including the anomalous Josephson effect. Our paper considers a Josephson junction of two non-centrosymmetric superconductors connected by a uniaxial ferromagnet. We show that this “Chiral Magnetic Josephson junction” (CMJ junction) exhibits a direct analog of the Chiral Magnetic Effect, which has already been observed in Weyl and Dirac semimetals. We suggest that the CMJ can serve as an element of a qubit with a Hamiltonian tunable by the ferromagnet’s magnetization. The CMJ junction avoids using an offset magnetic flux in inductively shunted qubits, thus enabling a simpler and more robust architecture. Furthermore, when the uniaxial ferromagnet’s easy axis is directed across the junction, the resulting “chiral magnetic qubit” provides robust protection from the noise caused by magnetization fluctuations.
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44

Zubkov, Mikhail, Zakhar Khaidukov, and Ruslan Abramchuk. "Momentum Space Topology and Non-Dissipative Currents †." Universe 4, no. 12 (December 12, 2018): 146. http://dx.doi.org/10.3390/universe4120146.

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Relativistic heavy ion collisions represent an arena for the probe of various anomalous transport effects. Those effects, in turn, reveal the correspondence between the solid state physics and the high energy physics, which share the common formalism of quantum field theory. It may be shown that for the wide range of field–theoretic models, the response of various nondissipative currents to the external gauge fields is determined by the momentum space topological invariants. Thus, the anomalous transport appears to be related to the investigation of momentum space topology—the approach developed earlier mainly in the condensed matter theory. Within this methodology we analyse systematically the anomalous transport phenomena, which include, in particular, the anomalous quantum Hall effect, the chiral separation effect, the chiral magnetic effect, the chiral vortical effect and the rotational Hall effect.
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45

Dvornikov, Maxim, and Victor B. Semikoz. "Chiral magnetic effect in the presence of electroweak interactions as a quasiclassical phenomenon." Modern Physics Letters A 33, no. 07n08 (March 14, 2018): 1850043. http://dx.doi.org/10.1142/s0217732318500438.

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We elaborate the quasiclassical approach to obtain the modified chiral magnetic effect (CME) in the case when the massless charged fermions interact with electromagnetic fields and the background matter by the electroweak forces. The derivation of the anomalous current along the external magnetic field involves the study of the energy density evolution of chiral particles in parallel electric and magnetic fields. We consider both the particle acceleration by the external electric field and the contribution of the Adler anomaly. The condition of the validity of this method for the derivation of the CME is formulated. We obtain the expression for the electric current along the external magnetic field, which appears to coincide with our previous results based on the purely quantum approach. Our results are compared with the findings of other authors.
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46

Ibe, Yohei, and Hiroaki Sumiyoshi. "Chiral Magnetic Effect due to Inhomogeneous Magnetic Fields in Noncentrosymmetric Weyl Semimetals." Journal of the Physical Society of Japan 86, no. 5 (May 15, 2017): 054707. http://dx.doi.org/10.7566/jpsj.86.054707.

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47

Fukushima, Kenji, Dmitri E. Kharzeev, and Harmen J. Warringa. "Chiral magnetic effect." Physical Review D 78, no. 7 (October 31, 2008). http://dx.doi.org/10.1103/physrevd.78.074033.

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48

Higashikawa, Sho, Masaya Nakagawa, and Masahito Ueda. "Floquet Chiral Magnetic Effect." Physical Review Letters 123, no. 6 (August 7, 2019). http://dx.doi.org/10.1103/physrevlett.123.066403.

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49

Hayata, Tomoya. "Chiral magnetic effect of light." Physical Review B 97, no. 20 (May 3, 2018). http://dx.doi.org/10.1103/physrevb.97.205102.

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50

Yin, Lei, Defu Hou, and Hai-cang Ren. "Chiral magnetic effect and three-point function from AdS/CFT correspondence." Journal of High Energy Physics 2021, no. 9 (September 2021). http://dx.doi.org/10.1007/jhep09(2021)117.

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Abstract:
Abstract The chiral magnetic effect with a fluctuating chiral imbalance is more realistic in the evolution of quark-gluon plasma, which reflects the random gluonic topological transition. Incorporating this dynamics, we calculate the chiral magnetic current in response to space-time dependent axial gauge potential and magnetic field in AdS/CFT correspondence. In contrast to conventional treatment of constant axial chemical potential, the response function here is the AVV three-point function of the $$ \mathcal{N} $$ N = 4 super Yang-Mills at strong coupling. Through an iterative solution of the nonlinear equations of motion in Schwarzschild-AdS5 background, we are able to express the AVV function in terms of two Heun functions and prove its UV/IR finiteness, as expected for $$ \mathcal{N} $$ N = 4 super Yang-Mills theory. We found that the dependence of the chiral magnetic current on a non-constant chiral imbalance is non-local, different from hydrodynamic approximation, and demonstrates the subtlety of the infrared limit discovered in field theoretic approach. We expect our results enrich the understanding of the phenomenology of the chiral magnetic effect in the context of relativistic heavy ion collisions.
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