Spin-orbit-mediated control of electron and hole spins in InSb ...

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$Planungsraster FP C SoSe2013 Di. 13:30-18:00 h Gruppe \ Tag 9.4 ...$

Spin-blockade – strong coupling • Dip at B = 0 • Likely due to spin-orbit coupling (as also seen for electrons) • But, very different angular dependence than electrons…
Spin-blockade anisotropy – strong coupling Electrons: B SO B k T - (1,1) E B SO S(1,1) T 0 (1,1) T + (1,1) B SO S(0,2)
Page 1 and 2: Spin-orbit-mediated control of elec
Page 3 and 4: Right Gate (mV) 300 400 500 InSb do
Page 5 and 6: Energy (μeV) Electric dipole spin
Page 7 and 8: g-factor g-factor anisotropy in an
Page 9 and 10: Electric dipole spin resonance - st
Page 11 and 12: Angular dependence of SOI • antic
Page 13 and 14: Angular dependence of SOI B SO B φ
Page 15 and 16: Coherent control of electron spin i
Page 17 and 18: Ramsey sequence InSb qubit coherenc
Page 19 and 20: Selective coherent control • larg
Page 21 and 22: From electron spins to hole spins E
Page 23 and 24: Bandgap of our InSb nanowires Bandg
Page 25 and 26: Hole quantum dots Gate tuning from
Page 27 and 28: Double quantum dots with holes Sche
Page 29 and 30: Hole spin blockade • B = 0 peak i
Page 31 and 32: Hyperfine coupling: holes vs. elect
Page 33 and 34: Electric-dipole spin resonance of h
Page 35: Electric-dipole spin resonance of h
Page 39: Summary InSb nanowires, so far: •

Spin-orbit-mediated control of electron and hole spins in InSb ...

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