TY - JOUR
T1 - Robustness of a persistent spin helix against a cubic Dresselhaus field in (001) and (110) oriented two-dimensional electron gases
AU - Iizasa, D.
AU - Sato, Dai
AU - Morita, K.
AU - Nitta, Junsaku
AU - Kohda, M.
N1 - Funding Information:
We thank T. Saito, T. Fukasawa, Y. Takeda, S. Iba, Y. Ohno, and G. Salis for fruitful discussions. This work is partially supported by Japan Society for the Promotion of Science (JSPS) (Grants No. 15H02099, No. 15H05854, No. 25220604, and No. 15H05699) and the Engineering and Physical Sciences Research Council–JSPS Core-to-Core program. D.I. thanks the Graduate Program of Spintronics at Tohoku University.
Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/10/8
Y1 - 2018/10/8
N2 - The persistent spin helix (PSH) state in III-V semiconductor quantum wells (QWs) is a promising candidate for spin-based applications because the PSH state realizes controllable spin orientation with long spin lifetime. Although the cubic Dresselhaus spin-orbit (SO) interaction is known for breaking the PSH state in both (001)-oriented and (110)-oriented QWs, it is not well understood how the distinct symmetry of cubic Dresselhaus terms β3 between (001) and (110) QWs affects the robustness of the PSH state. Here we investigate robustness of the PSH state between (001) and (110) QWs under various strengths of cubic Dresselhaus SO interaction based on numerical Monte Carlo approach and magnetoconductance simulation, respectively, representing optical spin excitation/detection and weak localization/weak antilocalization in magnetotransport. For electron spins initialized along z [001] in a (001) QW and x [001]andy [11 0] in a (110) QW, where the spin distribution is developed with the helical spin mode, a (001) QW shows a more robust PSH state against the increase of β3 than does a (110) QW. This phenomenon is contrary to numerically computed magnetoconductance, where weak localization is maintained on the variation of β3 in a (110) QW, whereas weak antilocalization appears in a (001) QW. By deriving the spin lifetime of the PSH state in a (110) QW from a diffusion equation using a random-walk approach, we demonstrate that such a difference arises directly from the magnitude and orientation of third angular harmonics in cubic Dresselhaus fields for (001) and (110) QWs.
AB - The persistent spin helix (PSH) state in III-V semiconductor quantum wells (QWs) is a promising candidate for spin-based applications because the PSH state realizes controllable spin orientation with long spin lifetime. Although the cubic Dresselhaus spin-orbit (SO) interaction is known for breaking the PSH state in both (001)-oriented and (110)-oriented QWs, it is not well understood how the distinct symmetry of cubic Dresselhaus terms β3 between (001) and (110) QWs affects the robustness of the PSH state. Here we investigate robustness of the PSH state between (001) and (110) QWs under various strengths of cubic Dresselhaus SO interaction based on numerical Monte Carlo approach and magnetoconductance simulation, respectively, representing optical spin excitation/detection and weak localization/weak antilocalization in magnetotransport. For electron spins initialized along z [001] in a (001) QW and x [001]andy [11 0] in a (110) QW, where the spin distribution is developed with the helical spin mode, a (001) QW shows a more robust PSH state against the increase of β3 than does a (110) QW. This phenomenon is contrary to numerically computed magnetoconductance, where weak localization is maintained on the variation of β3 in a (110) QW, whereas weak antilocalization appears in a (001) QW. By deriving the spin lifetime of the PSH state in a (110) QW from a diffusion equation using a random-walk approach, we demonstrate that such a difference arises directly from the magnitude and orientation of third angular harmonics in cubic Dresselhaus fields for (001) and (110) QWs.
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U2 - 10.1103/PhysRevB.98.165112
DO - 10.1103/PhysRevB.98.165112
M3 - Article
AN - SCOPUS:85054878216
VL - 98
JO - Physical Review B
JF - Physical Review B
SN - 2469-9950
IS - 16
ER -