Tuesday, March 15, 2022
3:00PM - 3:12PM
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K54.00001: Observation of room temperature topological Hall effect in thin film magnetic insulator/heavy metal bilayers
Sanyum Channa, Xin Yu Zheng, Zbigniew Galazka, Lauren Riddiford, Jacob J Wisser, Egecan Cogulu, Haowen Ren, Andrew D Kent, Yuri Suzuki
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Tuesday, March 15, 2022
3:12PM - 3:24PM
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K54.00002: Resonance structures of direct and Hall currents in topological spin-Hall effect
Andrei S Zadorozhnyi
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Tuesday, March 15, 2022
3:24PM - 3:36PM
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K54.00003: Theory of Hall effects with chiral magnetic textures and spin-orbit coupling
Zachariah M Addison, Nishchhal Verma, Mohit Randeria
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Tuesday, March 15, 2022
3:36PM - 3:48PM
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K54.00004: Metastable zero-field skyrmion lattice at room temperature in van der Waals (Fe0.5Co0.5)5GeTe2
Ying-Ting Chan, Hongrui Zhang, Rui Chen, Xiang Chen, Jie Yao, Robert J Birgeneau, Ramamoorthy Ramesh, Weida Wu
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Tuesday, March 15, 2022
3:48PM - 4:00PM
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K54.00005: Hall viscosity at angular momentum compensation point
Bom Soo Kim
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Tuesday, March 15, 2022
4:00PM - 4:12PM
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K54.00006: Spin-polarized STM Study of Cr2Te3 Thin Films
Joseph E Murray
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Tuesday, March 15, 2022
4:12PM - 4:48PM
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K54.00007: Skyrmions, emergent magnetic monopoles, and their electromagnetic responses in cubic chiral magnets
Invited Speaker:
Yukako Fujishiro
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Tuesday, March 15, 2022
4:48PM - 5:00PM
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K54.00008: Distinguishing Hump-shape Hall Effects withKarplus-Luttinger and Topological Origins
Zhi Shiuh Lim, May Inn Sim, Lin Er Chow, Ganesh Ji Omar, Anjan Soumyanarayanan, Ariando Ariando
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Tuesday, March 15, 2022
5:00PM - 5:12PM
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K54.00009: Magnetoresistance in Helical Antiferromagnet Eu Metal Thin Films
Narendra Shrestha
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Tuesday, March 15, 2022
5:12PM - 5:24PM
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K54.00010: Spin Dynamics in Fe3Sn2 frustrated kagome ferromagnet for room-temperature Skyrmion based technology
Nirel Bernstein, Ranen Ben-Shalom, Elichai Frohlich, Hang Li, Wenhong Wang, Amir Capua
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Tuesday, March 15, 2022
5:24PM - 6:00PM
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K54.00011: Topological Hall and Nernst effects in spin-chiral magnets
Invited Speaker:
Max Hirschberger
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