optical hall effect
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Nanophotonics ◽  
2021 ◽  
Vol 0 (0) ◽  
Author(s):  
S. Azar Oliaei Motlagh ◽  
Vadym Apalkov

Abstract We propose an ultrafast all-optical anomalous Hall effect in two-dimensional (2D) semiconductors of hexagonal symmetry such as gapped graphene (GG), transition metal dichalcogenides (TMDCs), and hexagonal boron nitride (h-BN). To induce such an effect, the material is subjected to a sequence of two strong-field single-optical-cycle pulses: A chiral pump pulse followed within a few femtoseconds by a probe pulse linearly polarized in the armchair direction of the 2D lattice. Due to the effect of topological resonance, the first (pump) pulse induces a large chirality (valley polarization) in the system, while the second pulse generates a femtosecond pulse of the anomalous Hall current. The proposed effect is fundamentally the fastest all-optical anomalous Hall effect possible in nature. It can be applied to ultrafast all-optical storage and processing of information, both classical and quantum.


2021 ◽  
Author(s):  
Muhammad Bilal ◽  
Wen Xu ◽  
Hua Wen ◽  
Xingjia Cheng ◽  
Yiming Xiao ◽  
...  

2021 ◽  
Author(s):  
Young-Gwan Choi ◽  
Manh-Ha Doan ◽  
Youngkuk Kim ◽  
Gyung-Min Choi

Abstract The ordinary Hall effect refers to generation of a transverse voltage upon exertion of an electric field in the presence of an out-of-plane magnetic field. While a linear Hall effect is commonly observed in systems with breaking time-reversal symmetry via an applied external magnetic field or their intrinsic magnetization1, 2, a nonlinear Hall effect can generically occur in non-magnetic systems associated with a nonvanishing Berry curvature dipole3. Here we report, observations of a nonlinear optical Hall effect in a Weyl semimetal WTe2 without an applied magnetic field at room temperature. We observe an optical Hall effect resulting in a polarization rotation of the reflected light, referred to as the nonlinear Kerr rotation. The nonlinear Kerr rotation linearly depends on the charge current and optical power, which manifests the fourth-order nonlinearity. We quantitatively determine the fourth-order susceptibility, which exhibits strong anisotropy depending on the directions of the charge current and the light polarization. Employing symmetry analysis of Berry curvature multipoles, we demonstrate that the nonlinear Kerr rotations can arise from the Berry curvature hexapole allowed by the crystalline symmetries of WTe2. There also exist marginal signals that are incompatible with the symmetries, which suggest a hidden phase associated with the nonlinear process.


Carbon ◽  
2021 ◽  
Vol 172 ◽  
pp. 248-259
Author(s):  
Nerijus Armakavicius ◽  
Philipp Kühne ◽  
Jens Eriksson ◽  
Chamseddine Bouhafs ◽  
Vallery Stanishev ◽  
...  

2020 ◽  
Vol 91 (8) ◽  
pp. 083903
Author(s):  
Sean Knight ◽  
Stefan Schöche ◽  
Philipp Kühne ◽  
Tino Hofmann ◽  
Vanya Darakchieva ◽  
...  

2020 ◽  
Vol 101 (24) ◽  
Author(s):  
X. N. Zhao ◽  
W. Xu ◽  
Y. M. Xiao ◽  
J. Liu ◽  
B. Van Duppen ◽  
...  

2019 ◽  
Vol 100 (23) ◽  
Author(s):  
Qianfan Chen ◽  
Maria Erukhimova ◽  
Mikhail Tokman ◽  
Alexey Belyanin

2019 ◽  
Vol 123 (24) ◽  
Author(s):  
Shenhe Fu ◽  
Chaoheng Guo ◽  
Guohua Liu ◽  
Yongyao Li ◽  
Hao Yin ◽  
...  

2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Prakash Uprety ◽  
Indra Subedi ◽  
Maxwell M. Junda ◽  
Robert W. Collins ◽  
Nikolas J. Podraza

AbstractElectrical transport parameters for active layers in silicon (Si) wafer solar cells are determined from free carrier optical absorption using non-contacting optical Hall effect measurements. Majority carrier transport parameters [carrier concentration (N), mobility (μ), and conductivity effective mass (m*)] are determined for both the n-type emitter and p-type bulk wafer Si of an industrially produced aluminum back surface field (Al-BSF) photovoltaic device. From measurements under 0 and ±1.48 T external magnetic fields and nominally “dark” conditions, the following respective [n, p]-type Si parameters are obtained: N = [(3.6 ± 0.1) × 1018 cm−3, (7.6 ± 0.1) × 1015 cm−3]; μ = [166 ± 6 cm2/Vs, 532 ± 12 cm2/Vs]; and m* = [(0.28 ± 0.03) × me, (0.36 ± 0.02) × me]. All values are within expectations for this device design. Contributions from photogenerated carriers in both regions of the p-n junction are obtained from measurements of the solar cell under “light” 1 sun illumination (AM1.5 solar irradiance spectrum). From analysis of combined dark and light optical Hall effect measurements, photogenerated minority carrier transport parameters [minority carrier concentration (Δp or Δn) and minority carrier mobility (μh or μe)] under 1 sun illumination for both n- and p-type Si components of the solar cell are determined. Photogenerated minority carrier concentrations are [(7.8 ± 0.2) × 1016 cm−3, (2.2 ± 0.2) × 1014 cm−3], and minority carrier mobilities are [331 ± 191 cm2/Vs, 766 ± 331 cm2/Vs], for the [n, p]-type Si, respectively, values that are within expectations from literature. Using the dark majority carrier concentration and the effective equilibrium minority carrier concentration under 1 sun illumination, minority carrier effective lifetime and diffusion length are calculated in the n-type emitter and p-type wafer Si with the results also being consistent with literature. Solar cell device performance parameters including photovoltaic device efficiency, open circuit voltage, fill factor, and short circuit current density are also calculated from these transport parameters obtained via optical Hall effect using the diode equation and PC1D solar cell simulations. The calculated device performance parameters are found to be consistent with direct current-voltage measurement demonstrating the validity of this technique for electrical transport property measurements of the semiconducting layers in complete Si solar cells. To the best of our knowledge, this is the first method that enables determination of both minority and majority carrier transport parameters in both active layers of the p-n junction in a complete solar cell.


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