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Journal articles on the topic 'Thermal Hall effect'

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Published: 10 December 2022
Last updated: 29 January 2023

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1

Maksimov, L. A., and T. V. Khabarova. "Thermal Hall-Senftleben effect." Physics of the Solid State 50, no. 10 (October 2008): 1836–40. http://dx.doi.org/10.1134/s1063783408100089.

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2

Murakami, Shuichi, and Akihiro Okamoto. "Thermal Hall Effect of Magnons." Journal of the Physical Society of Japan 86, no. 1 (January 15, 2017): 011010. http://dx.doi.org/10.7566/jpsj.86.011010.

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3

Ideue, T., T. Kurumaji, S. Ishiwata, and Y. Tokura. "Giant thermal Hall effect in multiferroics." Nature Materials 16, no. 8 (May 15, 2017): 797–802. http://dx.doi.org/10.1038/nmat4905.

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4

Yokoi, T., S. Ma, Y. Kasahara, S. Kasahara, T. Shibauchi, N. Kurita, H. Tanaka, et al. "Half-integer quantized anomalous thermal Hall effect in the Kitaev material candidate α-RuCl3." Science 373, no. 6554 (July 29, 2021): 568–72. http://dx.doi.org/10.1126/science.aay5551.

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Half-integer thermal quantum Hall conductance has recently been reported for the two-dimensional honeycomb material α-RuCl3. We found that the half-integer thermal Hall plateau appears even for a magnetic field with no out-of-plane components. The measured field-angular variation of the quantized thermal Hall conductance has the same sign structure as the topological Chern number of the pure Kitaev spin liquid. This observation suggests that the non-Abelian topological order associated with fractionalization of the local magnetic moments persists even in the presence of non-Kitaev interactions in α-RuCl3.
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5

Bruin, J. A. N., R. R. Claus, Y. Matsumoto, N. Kurita, H. Tanaka, and H. Takagi. "Robustness of the thermal Hall effect close to half-quantization in α-RuCl3." Nature Physics 18, no. 4 (February 17, 2022): 401–5. http://dx.doi.org/10.1038/s41567-021-01501-y.

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AbstractA key feature of quantum spin liquids is the predicted formation of fractionalized excitations. They are expected to produce changes in the physical response, providing a way to observe the quantum spin liquid state1. In the honeycomb magnet α-RuCl3, a quantum spin liquid has been proposed to explain the behaviour observed on applying an in-plane magnetic field H||. Previous work reported that the thermal Hall conductivity took on a half-integer quantized value and suggested this as a signature of a fractionalized Majorana edge mode predicted to exist in Kitaev quantum spin liquids2. However, the temperature and magnetic-field range of the half-quantized signal2–4 and its association with Majorana edge modes are still under debate5,6. Here we present a comprehensive study of the thermal Hall conductivity in α-RuCl3 showing that approximately half-integer quantization exists in an extended region of the phase diagram, particularly across a plateau-like parameter regime for H|| exceeding 10 T and temperature below 6.5 K. At lower fields, the thermal Hall conductivity exhibits correlations with complex anomalies in the longitudinal thermal conductivity and magnetization, and is suppressed by cooling to low temperatures. Our results can be explained by the existence of a topological state in magnetic fields above 10 T.
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6

Owerre, S. A. "Topological thermal Hall effect due to Weyl magnons." Canadian Journal of Physics 96, no. 11 (November 2018): 1216–23. http://dx.doi.org/10.1139/cjp-2018-0059.

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We present the first theoretical evidence of zero magnetic field topological (anomalous) thermal Hall effect due to Weyl magnons in stacked noncoplanar frustrated kagomé antiferromagnets. The Weyl magnons in this system result from macroscopically broken time-reversal symmetry by the scalar spin chirality of noncoplanar chiral spin textures. Most importantly, they come from the lowest excitation, therefore they can be easily observed experimentally at low temperatures due to the population effect. Similar to electronic Weyl nodes close to the Fermi energy, Weyl magnon nodes at the lowest excitation are the most important. Indeed, we show that the topological (anomalous) thermal Hall effect in this system arises from nonvanishing Berry curvature due to Weyl magnon nodes at the lowest excitation, and it depends on their distribution (distance) in momentum space. The present result paves the way to directly probe low excitation Weyl magnons and macroscopically broken time-reversal symmetry in three-dimensional frustrated magnets with the anomalous thermal Hall effect.
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7

Szelecka, Agnieszka, Jacek Kurzyna, and Loic Bourdain. "Thermal stability of the krypton Hall effect thruster." Nukleonika 62, no. 1 (March 1, 2017): 9–15. http://dx.doi.org/10.1515/nuka-2017-0002.

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Abstract The Krypton Large IMpulse Thruster (KLIMT) ESA/PECS project, which has been implemented in the Institute of Plasma Physics and Laser Microfusion (IPPLM) and now is approaching its final phase, was aimed at incremental development of a ~500 W class Hall effect thruster (HET). Xenon, predominantly used as a propellant in the state-of-the-art HETs, is extremely expensive. Krypton has been considered as a cheaper alternative since more than fifteen years; however, to the best knowledge of the authors, there has not been a HET model especially designed for this noble gas. To address this issue, KLIMT has been geared towards operation primarily with krypton. During the project, three subsequent prototype versions of the thruster were designed, manufactured and tested, aimed at gradual improvement of each next exemplar. In the current paper, the heat loads in new engine have been discussed. It has been shown that thermal equilibrium of the thruster is gained within the safety limits of the materials used. Extensive testing with both gases was performed to compare KLIMT’s thermal behaviour when supplied with krypton and xenon propellants.
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8

Blanter, Ya M., D. V. Livanov, and M. O. Rodin. "Thermal conductivity in the quantum Hall effect regime." Journal of Physics: Condensed Matter 6, no. 9 (February 28, 1994): 1739–48. http://dx.doi.org/10.1088/0953-8984/6/9/015.

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9

Zhang, Hantao, and Ran Cheng. "Magnon thermal Edelstein effect detected by inverse spin Hall effect." Applied Physics Letters 117, no. 22 (November 30, 2020): 222402. http://dx.doi.org/10.1063/5.0030368.

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10

HAN, Jung Hoon. "Electromagnetism without Electrons: A Brief History of Thermal Hall Effect." Physics and High Technology 29, no. 6 (June 30, 2020): 14–20. http://dx.doi.org/10.3938/phit.29.020.

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The past decade has witnessed the rise of the thermal Hall measurement as a sensitive probe of transport properties in solids. Experiments performed on a wide range of materials, such as magnetic insulators, spin ice, kagome spin liquids with both ferromagnetic and antiferromagnetic exchange interactions, a quantum paraelectric, and even high-Tc cuprates, showed the existence of thermal Hall transport phenomena caused by neutral excitations. There is little doubt that an era of electromagnetism without electrons has dawned. This review covers a brief and somewhat personal account of the theory and the experimental developments of the thermal Hall effect as a new discipline of condensed matter physics over the past decade.
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11

Shitade, Atsuo. "Anomalous Thermal Hall Effect in a Disordered Weyl Ferromagnet." Journal of the Physical Society of Japan 86, no. 5 (May 15, 2017): 054601. http://dx.doi.org/10.7566/jpsj.86.054601.

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12

Teixeira, Patrícia H. O., Ronnie Rodrigo Rego, Fabio Wagner Pinto, Jefferson de Oliveira Gomes, and Christoph Löpenhaus. "Application of Hall effect for assessing grinding thermal damage." Journal of Materials Processing Technology 270 (August 2019): 356–64. http://dx.doi.org/10.1016/j.jmatprotec.2019.02.019.

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13

Kane, C. L., and Matthew P. A. Fisher. "Quantized thermal transport in the fractional quantum Hall effect." Physical Review B 55, no. 23 (June 15, 1997): 15832–37. http://dx.doi.org/10.1103/physrevb.55.15832.

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14

Singh, M., and R. K. Gupta. "Hall Effect on Thermal Instability of Viscoelastic Dusty Fluid in Porous Medium." International Journal of Applied Mechanics and Engineering 18, no. 3 (August 1, 2013): 871–86. http://dx.doi.org/10.2478/ijame-2013-0052.

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Abstract The effect of Hall currents and suspended dusty particles on the hydromagnetic stability of a compressible, electrically conducting Rivlin-Ericksen elastico viscous fluid in a porous medium is considered. Following the linearized stability theory and normal mode analysis the dispersion relation is obtained. For the case of stationary convection, Hall currents and suspended particles are found to have destabilizing effects whereas compressibility and magnetic field have stabilizing effects on the system. The medium permeability, however, has stabilizing and destabilizing effects on thermal instability in contrast to its destabilizing effect in the absence of the magnetic field. The critical Rayleigh numbers and the wave numbers of the associated disturbances for the onset of instability as stationary convection are obtained and the behavior of various parameters on critical thermal Rayleigh numbers are depicted graphically. The magnetic field, Hall currents and viscoelasticity parameter are found to introduce oscillatory modes in the systems, which did not exist in the absence of these parameters
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15

Witalis, E. A. "Hall Effect, or Hyperbolic Magnetohydrodynamics, HMHD." Zeitschrift für Naturforschung A 42, no. 9 (September 1, 1987): 917–21. http://dx.doi.org/10.1515/zna-1987-0902.

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The MHD theory of present magnetic fusion research is briefly reviewed with emphasis on its mathematically diffusive character. The importance of retaining the Hall effect term, neglected in ideal or resistive MHD theory, is stressed. Elliptic MHD theory is critically dismissed. The Hall effect, or Hyperbolic, MagnetoHydro-Dynamics, HMHD, is shown to follow as the consequence of a revision of plasma electrodynamics so as to account for the fundamental plasma quasineutrality. The non-validity of Newton’s third law in charged particle contexts is then central. Previously poorly understood phenomena, such as plasma edge effects and magnetic field line reconnection are found to be inherent properties in this HMHD plasma description. The “magnetic bottle” principle for high density plasma confinement is shown to be physically unsound because there will exist a no-confinement plasma boundary region with HMHD theory properties. Arguments for non-thermal fusion, provided by HMHD theory, are given.
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16

Kasahara, Y., T. Ohnishi, Y. Mizukami, O. Tanaka, Sixiao Ma, K. Sugii, N. Kurita, et al. "Majorana quantization and half-integer thermal quantum Hall effect in a Kitaev spin liquid." Nature 559, no. 7713 (July 2018): 227–31. http://dx.doi.org/10.1038/s41586-018-0274-0.

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17

Owerre, S. A. "Topological honeycomb magnon Hall effect: A calculation of thermal Hall conductivity of magnetic spin excitations." Journal of Applied Physics 120, no. 4 (July 28, 2016): 043903. http://dx.doi.org/10.1063/1.4959815.

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18

Ding, Linchao, Jahyun Koo, Changjiang Yi, Liangcai Xu, Huakun Zuo, Meng Yang, Youguo Shi, Binghai Yan, Kamran Behnia, and Zengwei Zhu. "Quantum oscillations, magnetic breakdown and thermal Hall effect in Co3Sn2S2." Journal of Physics D: Applied Physics 54, no. 45 (August 24, 2021): 454003. http://dx.doi.org/10.1088/1361-6463/ac1c2b.

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19

Samajdar, Rhine, Mathias S. Scheurer, Shubhayu Chatterjee, Haoyu Guo, Cenke Xu, and Subir Sachdev. "Enhanced thermal Hall effect in the square-lattice Néel state." Nature Physics 15, no. 12 (October 7, 2019): 1290–94. http://dx.doi.org/10.1038/s41567-019-0669-3.

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20

Kukushkin, I. V., N. J. Pulsford, K. von Klitzing, R. J. Haug, K. Ploog, H. Buhmann, M. Potemski, G. Martinez, and V. B. Timofeev. "Thermal Collapse of the Fractional-Quantum-Hall-Effect Energy Gaps." Europhysics Letters (EPL) 22, no. 4 (May 1, 1993): 287–92. http://dx.doi.org/10.1209/0295-5075/22/4/008.

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21

Aggarwal, Amrish, and Suman Makhija. "Hall effect on thermal stability of ferromagnetic fluid in porous medium in the presence of horizontal magnetic field." Thermal Science 18, suppl.2 (2014): 503–14. http://dx.doi.org/10.2298/tsci110714086a.

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This paper deals with the theoretical investigation of the effect of Hall currents on the thermal stability of a ferromagnetic fluid heated from below in porous medium. For a fluid layer between two free boundaries, an exact solution is obtained using a linearized stability theory and normal mode analysis. A dispersion relation governing the effects of medium permeability, a uniform horizontal magnetic field, magnetization and Hall currents is derived. For the case of stationary convection, it is found that the magnetic field and magnetization have a stabilizing effect on the system, as such their effect is to postpone the onset of thermal instability whereas Hall currents are found to hasten the onset of thermal instability. The medium permeability hastens the onset of convection under certain conditions. The principle of exchange of stabilities is not valid for the problem under consideration whereas in the absence of Hall currents (hence magnetic field), it is valid under certain conditions.
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22

Sharma, R. C., and Sunil. "Thermal instability of a compressible finite-Larmor-radius Hall plasma in a porous medium." Journal of Plasma Physics 55, no. 1 (February 1996): 35–45. http://dx.doi.org/10.1017/s002237780001864x.

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The thermal instability of a compressible plasma in a porous medium is considered in the presence of a uniform vertical magnetic field to include the Hall-current and finite-Larmor-radius effects. The system is found to be stable for (cp/g) β < 1, where cp, β and g are the specific heat at constant-pressure, the uniform adverse temperature gradient and the acceleration due to gravity respectively. The uniform vertical magnetic field, Hall-current and finite. Laimor-radius effects introduce oscillatory modes in the system for (cp/g) β ≤ 1, which were non-existent in their absence. The Hall current and finite Larmor radius (FLR) individually have destabilizing and stabilizing effects respectively on the system. In their simultaneous presence there is competition between the destabilizing role of the Hall current and the stabilizing role of the FLR, and each succeeds in stabilizing a certain wavenumber range. In the absence of a magnetic field (and hence the absence of an FLR and Hall current), the destabilizing effect of medium permeability is seen, but in the presence of a magnetic field (and hence the presence of an FLR and Hall current), the medium permeability may have a stabilizing or a destabilizing effect on the thermal instability of the plasma. The effect of compressibility is found to postpone the onset of thermal instability in plasma.
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23

Zhuo, Fengjun, Hang Li, and Aurélien Manchon. "Topological thermal Hall effect and magnonic edge states in kagome ferromagnets with bond anisotropy." New Journal of Physics 24, no. 2 (February 1, 2022): 023033. http://dx.doi.org/10.1088/1367-2630/ac51a8.

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Abstract The magnon band topology due to the Dzyaloshinskii–Moriya interaction (DMI) and its relevant topological thermal Hall effect has been extensively studied in kagome lattice magnets. In this theoretical investigation, we report a new mechanism for phase transitions between topological phases of magnons in kagome ferromagnets by tuning the anisotropic nearest-neighbor ferromagnetic interaction and DMI. Using the linear spin-wave theory, we calculate the Chern number and thermal Hall conductivity of magnons in low temperature regime. We show the magnon band structures and magnonic edge states in each topological phase. From the topological phase diagram, we find a sign reversal of the thermal Hall conductivity upon tuning the modulation factors. We explicitly demonstrate the correspondence of thermal Hall conductivity with the propagation direction of the magnonic edge states. Finally, we discuss candidate materials as experimental realizations of our theoretical model.
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24

Aggarwal, Amrish Kumar, and Anushri Verma. "Effect of hall currents on thermal instability of dusty couple stress fluid." Archives of Thermodynamics 37, no. 3 (September 1, 2016): 3–18. http://dx.doi.org/10.1515/aoter-2016-0016.

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Abstract In this paper, effect of Hall currents on the thermal instability of couple-stress fluid permeated with dust particles has been considered. Following the linearized stability theory and normal mode analysis, the dispersion relation is obtained. For the case of stationary convection, dust particles and Hall currents are found to have destabilizing effect while couple stresses have stabilizing effect on the system. Magnetic field induced by Hall currents has stabilizing/destabilizing effect under certain conditions. It is found that due to the presence of Hall currents (hence magnetic field), oscillatory modes are produced which were non-existent in their absence.
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25

WATTS, S. M., S. VON MOLNáR, and M. JAIME. "HIGH-FIELD HALL EFFECT AND BAND STRUCTURE OF HALF-METALLIC CrO2 FILMS." International Journal of Modern Physics B 16, no. 20n22 (August 30, 2002): 3334–37. http://dx.doi.org/10.1142/s0217979202014346.

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The Hall effect of (100)- and (110)-oriented films of the half-metallic ferromagnetic oxide CrO2, fabricated by both chemical vapor deposition and high pressure, thermal decomposition methods, has been examined in large magnetic fields up to 60 T. In all cases the Hall effect exhibits a sign reversal from positive to negative with increasing field, which we take as evidence for multi-band behavior. (110) films fabricated by both methods exhibit this sign reversal at relatively low fields. The data may be fit with a simple two-band model, which indicates the existence of highly mobile holes of p-like parentage, along with a much larger number of heavy, d-like electrons. In the (100) film the sign reversal is at much higher field. The parameters obtained from the fits allow us (with help from band structure calculations) to infer the band structure near the Fermi level and how it depends on sample strain and other structural characteristics. These details will be important for understanding carrier transport through interfaces such as for spin injection or other "spintronics" applications.
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26

Furukawa, Shunsuke, and Tsutomu Momoi. "Effects of Dzyaloshinskii–Moriya Interactions in Volborthite: Magnetic Orders and Thermal Hall Effect." Journal of the Physical Society of Japan 89, no. 3 (March 15, 2020): 034711. http://dx.doi.org/10.7566/jpsj.89.034711.

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27

Sharma, R. C., and V. K. Bhardwaj. "Finite Larmor Radius and Hall Effects on Thermal Instability of a Plasma in Porous Medium." Zeitschrift für Naturforschung A 49, no. 4-5 (May 1, 1994): 547–51. http://dx.doi.org/10.1515/zna-1994-4-505.

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Abstract The thermal instability of a plasma in a porous medium in the presence of a finite Larmor radius (FLR) and Hall effects is considered. Oscillatory m odes due to the presence of a magnetic field (and hence the presence of FLR and Hall effects) are introduced. For stationary convection, the FLR may have a stabilizing or destabilizing effect, but a completely stabilizing one for a certain wave-number range. Similarly, the Hall currents may have a stabilizing or destabilizing effect but a completely stabilizing one for the same wave-number range under certain condition, whereas the medium permeability always has a destabilizing effect for stationary convection.
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28

Mehta, C. B., M. Singh, and S. Kumar. "Thermal convection of magneto compressible couple-stress fluid saturated in a porous medium with Hall current." International Journal of Applied Mechanics and Engineering 21, no. 1 (February 1, 2016): 83–93. http://dx.doi.org/10.1515/ijame-2016-0005.

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Abstract An investigation is made on the effect of Hall currents on thermal instability of a compressible couple-stress fluid in the presence of a horizontal magnetic field saturated in a porous medium. The analysis is carried out within the framework of the linear stability theory and normal mode technique. A dispersion relation governing the effects of viscoelasticity, Hall currents, compressibility, magnetic field and porous medium is derived. For the stationary convection a couple-stress fluid behaves like an ordinary Newtonian fluid due to the vanishing of the viscoelastic parameter. Compressibility, the magnetic filed and couple-stress parameter have stabilizing effects on the system whereas Hall currents and medium permeability have a destabilizing effect on the system, but in the absence of Hall current couple-stress has a destabilizing effect on the system. It has been observed that oscillatory modes are introduced due to the presence of viscoelasticity, magnetic field porous medium and Hall currents which were non-existent in their absence.
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29

Shirokura, Takanori, and Pham Nam Hai. "Giant spin Hall effect in half-Heusler alloy topological semimetal YPtBi grown at low temperature." AIP Advances 12, no. 12 (December 1, 2022): 125116. http://dx.doi.org/10.1063/5.0117613.

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Half-Heusler alloy topological semimetal YPtBi is a promising candidate for an efficient spin source material having both large spin Hall angle θSH and high thermal stability. However, high-quality YPtBi thin films with low bulk carrier density are usually grown at 600 °C, which exceeds the limitation of 400 °C for back end of line (BEOL) process. Here, we investigate the crystallinity and spin Hall effect of YPtBi thin films grown at lower growth temperature down to 300 °C. Although both effective spin Hall angle and spin Hall conductivity degraded with lowering the growth temperature to 300 °C due to degradation of the interfacial spin transparency, they were recovered by reducing the sputtering Ar gas pressure. We achieved a giant θSH up to 7.8 and demonstrated efficient spin–orbit torque magnetization switching by ultralow current density of ∼105 A/cm2 in YPtBi grown at 300 °C with the Ar gas pressure of 1 Pa. Our results provide the recipe to achieve giant θSH in YPtBi grown at lower growth temperature suitable for BEOL process.
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30

Nakai, Ryota, Shinsei Ryu, and Kentaro Nomura. "Finite-temperature effective boundary theory of the quantized thermal Hall effect." New Journal of Physics 18, no. 2 (February 10, 2016): 023038. http://dx.doi.org/10.1088/1367-2630/18/2/023038.

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31

Singh, Rajan, Zhaochu Luo, Ziyao Lu, Awais Siddique Saleemi, Chengyue Xiong, and Xiaozhong Zhang. "Thermal stability of NDR-assisted anomalous Hall effect based magnetic device." Journal of Applied Physics 125, no. 20 (May 28, 2019): 203901. http://dx.doi.org/10.1063/1.5088916.

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32

Tinsman, Colin, Gang Li, Caroline Su, Tomoya Asaba, Benjamin Lawson, Fan Yu, and Lu Li. "Probing the thermal Hall effect using miniature capacitive strontium titanate thermometry." Applied Physics Letters 108, no. 26 (June 27, 2016): 261905. http://dx.doi.org/10.1063/1.4955069.

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33

Kagan, Yu, and L. A. Maksimov. "Anomalous Hall effect in the phonon thermal conductivity of paramagnetic dielectrics." Journal of Experimental and Theoretical Physics 107, no. 4 (October 2008): 632–41. http://dx.doi.org/10.1134/s1063776108100105.

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34

Gupta, Urvashi, Parul Aggarwal, and Kumar Wanchoo. "Thermal convection of dusty compressible Rivlin-Ericksen viscoelastic fluid with hall currents." Thermal Science 16, no. 1 (2012): 177–92. http://dx.doi.org/10.2298/tsci110128113g.

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An investigation is made on the effect of Hall currents and suspended particles on the hydromagnetic stability of a compressible, electrically conducting Rivlin-Ericksen elastico-viscous fluid. The perturbation equations are analyzed in terms of normal modes after linearizing the relevant set of hydromagnetic equations. A dispersion relation governing the effects of viscoelasticity, magnetic field, Hall currents, compressibility and suspended particles is derived. For the stationary convection Rivlin-Ericksen fluid behaves like an ordinary Newtonian fluid due to the vanishing of the viscoelastic parameter. Compressibility and magnetic field are found to have a stabilizing effect on the system whereas Hall currents and suspended particles hasten the onset of thermal instability. These analytic results are confirmed numerically and the effects of various parameters on the stability parameter are depicted graphically. The critical Rayleigh numbers and the wavenumbers of the associated disturbances for the onset of instability as stationary convection are obtained and the behavior of various parameters on critical thermal Rayleigh numbers has been depicted graphically. It has been observed that oscillatory modes are introduced due to the presence of viscoelasticity, suspended particles and Hall currents which were not existing in the absence of these parameters.
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35

Singh, Mahinder, and Chander Bhan Mehta. "Hall Effect on Bénard Convection of Compressible Viscoelastic Fluid through Porous Medium." Journal of Fluids 2013 (October 10, 2013): 1–8. http://dx.doi.org/10.1155/2013/910531.

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An investigation made on the effect of Hall currents on thermal instability of a compressible Walter’s B′ elasticoviscous fluid through porous medium is considered. The analysis is carried out within the framework of linear stability theory and normal mode technique. For the case of stationary convection, Hall currents and compressibility have postponed the onset of convection through porous medium. Moreover, medium permeability hasten postpone the onset of convection, and magnetic field has duel character on the onset of convection. The critical Rayleigh numbers and the wave numbers of the associated disturbances for the onset of instability as stationary convection have been obtained and the behavior of various parameters on critical thermal Rayleigh numbers has been depicted graphically. The magnetic field, Hall currents found to introduce oscillatory modes, in the absence of these effects the principle of exchange of stabilities is valid.
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36

Zeini, B., A. Freimuth, B. Büchner, M. Galffy, R. Gross, A. P. Kampf, M. Kläser, G. Müller-Vogt, and L. Winkler. "Thermal conductivity and thermal Hall effect in Bi- and Y-based high-T c superconductors." European Physical Journal B 20, no. 2 (March 2001): 189–208. http://dx.doi.org/10.1007/pl00011098.

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37

Wen, Han, Eric Bennett, and David G. Wiesler. "Shielding of Piezoelectric Ultrasonic Probes in Hall Effect Imaging." Ultrasonic Imaging 20, no. 3 (July 1998): 206–20. http://dx.doi.org/10.1177/016173469802000305.

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This paper addresses significant sources of electromagnetic noise in Hall effect imaging. Hall effect imaging employs large electrical pulses for signal generation and high sensitivity ultrasonic probes for signal reception. Coherent noise arises through various coupling mechanisms between the excitation pulse and the probe. In this paper, the coupling mechanisms are experimentally isolated and theoretically analyzed. Several methods of shielding the probe from electromagnetic interference are devised and tested. These methods are able to reduce the noise to levels below the random thermal noise, thereby improving the signal-to-noise ratio in HEI by two orders of magnitude.
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38

Ben-Abdallah, P. "Photon Thermal Hall Effect." Physical Review Letters 116, no. 8 (February 23, 2016). http://dx.doi.org/10.1103/physrevlett.116.084301.

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39

Ott, A., S. A. Biehs, and P. Ben-Abdallah. "Anomalous photon thermal Hall effect." Physical Review B 101, no. 24 (June 15, 2020). http://dx.doi.org/10.1103/physrevb.101.241411.

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40

"Thermal Hall effect in a paramagnet." Journal Club for Condensed Matter Physics, March 30, 2015. http://dx.doi.org/10.36471/jccm_march_2015_02.

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41

Mandal, Debottam, Kamal Das, and Amit Agarwal. "Magnus Nernst and thermal Hall effect." Physical Review B 102, no. 20 (November 12, 2020). http://dx.doi.org/10.1103/physrevb.102.205414.

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42

Long, Wen, Hui Zhang, and Qing-feng Sun. "Quantum thermal Hall effect in graphene." Physical Review B 84, no. 7 (August 5, 2011). http://dx.doi.org/10.1103/physrevb.84.075416.

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43

Yan, Yonghong, Weiguo Ye, Haifei Wu, and Hui Zhao. "Electronic thermal Hall effect in silicene." European Physical Journal B 90, no. 10 (October 2017). http://dx.doi.org/10.1140/epjb/e2017-80394-x.

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44

Freimuth, A., and B. Zeini. "Thermal conductivity and thermal Hall effect from vortex motion." Physical Review B 67, no. 5 (February 25, 2003). http://dx.doi.org/10.1103/physrevb.67.052504.

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45

Guo, Shucheng, Youming Xu, Ran Cheng, Jianshi Zhou, and Xi Chen. "Thermal Hall effect in insulating quantum materials." Innovation, July 2022, 100290. http://dx.doi.org/10.1016/j.xinn.2022.100290.

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46

Carnahan, Caitlin, Yinhan Zhang, and Di Xiao. "Thermal Hall effect of chiral spin fluctuations." Physical Review B 103, no. 22 (June 17, 2021). http://dx.doi.org/10.1103/physrevb.103.224419.

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47

Huang, Ze-Min, Bo Han, and Xiao-Qi Sun. "Torsion, energy magnetization, and thermal Hall effect." Physical Review B 105, no. 8 (February 3, 2022). http://dx.doi.org/10.1103/physrevb.105.085104.

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48

Idrisov, Edvin G., Ivan P. Levkivskyi, and Eugene V. Sukhorukov. "Thermal drag effect in quantum Hall circuits." Physical Review B 106, no. 12 (September 30, 2022). http://dx.doi.org/10.1103/physrevb.106.l121405.

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49

Gromov, Andrey, and Alexander G. Abanov. "Thermal Hall Effect and Geometry with Torsion." Physical Review Letters 114, no. 1 (January 6, 2015). http://dx.doi.org/10.1103/physrevlett.114.016802.

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50

Nandy, S., A. Taraphder, and Sumanta Tewari. "Planar thermal Hall effect in Weyl semimetals." Physical Review B 100, no. 11 (September 17, 2019). http://dx.doi.org/10.1103/physrevb.100.115139.

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