Lande-like formula for the g factors of hole-nanowire subband edges
被引:15
作者:
Csontos, D.
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Massey Univ, Inst Fundamental Sci, Palmerston North 4442, New Zealand
Massey Univ, MacDiarmid Inst Adv Mat & Nanotechnol, Palmerston North 4442, New ZealandMassey Univ, Inst Fundamental Sci, Palmerston North 4442, New Zealand
Csontos, D.
[1
,2
]
Zulicke, U.
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Massey Univ, MacDiarmid Inst Adv Mat & Nanotechnol, Palmerston North 4442, New ZealandMassey Univ, Inst Fundamental Sci, Palmerston North 4442, New Zealand
Zulicke, U.
[2
]
Brusheim, P.
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Lund Univ, Div Solid State Phys, S-22100 Lund, SwedenMassey Univ, Inst Fundamental Sci, Palmerston North 4442, New Zealand
Brusheim, P.
[3
]
Xu, H. Q.
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Lund Univ, Div Solid State Phys, S-22100 Lund, SwedenMassey Univ, Inst Fundamental Sci, Palmerston North 4442, New Zealand
Xu, H. Q.
[3
]
机构:
[1] Massey Univ, Inst Fundamental Sci, Palmerston North 4442, New Zealand
[2] Massey Univ, MacDiarmid Inst Adv Mat & Nanotechnol, Palmerston North 4442, New Zealand
[3] Lund Univ, Div Solid State Phys, S-22100 Lund, Sweden
We have analyzed theoretically the Zeeman splitting of hole-quantum-wire subband edges. As is typical for any bound state, their g factor depends on both an intrinsic g factor of the material and an additional contribution arising from a finite bound-state orbital angular momentum. We discuss the quantum-confinement-induced interplay between bulk-material and orbital effects, which is nontrivial due to the presence of strong spin-orbit coupling. A compact analytical formula is provided that elucidates this interplay and can be useful for predicting Zeeman splitting in generic hole-wire geometries.