Rashba spin-orbit coupling and spin relaxation in silicon quantum wells

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a

r

X

i

v

:

c

o

n

d

-

m

at/0401615v2 [cond-mat.mes-hall] 27 Jul 2004

T

1T

2

k·p

Step graded SiGeSi CapSi Cap

Doped SiGe donor layer

(P or Sb)

Strained Si 2DEG

SiGe virtual substrateStrained Si QW (empty)28

Strained Si 2DEG backgate

SiGe barrier/spacer

Donor layer

SiGe virtual substrateStep graded SiGe

electron

qubit

induced

charge12-201025204 (nm)

4

< 60

6-10

< 30 (nm)SiGe barrier/spacer

E

ESchottky gates

Device 1 (D1)Device 2 (D2)SiGe barrier/spacer

E

z∼106

E

z>105

E

z≈en

s

4πǫ

Sid2=3×105,

d=20

3×107

g

0=2.00232

∆g

󰀄≈−0.003∆g

⊥≈−0.004∆g

g

Ge=1.4

∆gV

H

SO=󰀁zz

H2D

R=α(p

y−p

x)∝E

z(󰀘σ×p)

z,

E

c

E

z

α

α=2PP

z∆

d

2󰀁E

v1E

v2󰀅

1

E

v2󰀇

e󰀍E

z󰀎,

zP=󰀁󰀍X|p

x|S󰀎/imP

z=󰀁󰀍Z|p

z|S󰀎/im

d=0.044E

v1=3.1

E

v2=7

m

PP

z

PP

z

2mP2

(z)/󰀁2

≈22

α≈1.66×10−6

󰀍E

z󰀎

k=0

α≈5.94αe/󰀁=

0.55/√

4πns

02040608022.533.544.55x 10-7

Time (s)

Magnetic field angle, θT

1

T

2

n

s=3x10 m-2

µ=9 m2

/Vs

E=2.3 MV/m

α=3.8 m/s(a)

0204060801.41.61.822.22.42.62.833.2x 10-7

Time (s)

Magnetic field angle, θT

1

T

2

n

s=4x10 m-2

µ=5 m2

/Vs

E=3.1 MV/mα=5.1 m/s(b)

1515

0204060800.511.52x 10-7

Time (s)

Magnetic field angle, θT

1

T

2n

s

µ=20 m2

/Vs

E=3.1 MV/m

α=5.1 m/s(c)

02040608000.20.40.60.811.21.41.6x 10-7

Time (s)

Magnetic field angle, θT

1

T

2n

s

µ=50 m2

/Vs

E=3.8 MV/m

α=6.4 m/s(d)

=4x10 m-215

=4x10 m-215

θ=0

α

H2D

R=α(p

y−p

x)

󰀘pε

󰀘p=ε

F󰀘p′ε

󰀘p′=ε

F,ε

F

T

2,T

1,2×2ρ󰀍σ

i󰀎=Tr{σ

iρ}.

H,dρ/dt=i

n =

9x10

8

7

6

5

13

24

Mobility, µ (m /Vs)T (µsec)-2s

α = 1 m/s

2

2010203040500102030m15

T

2α=1

µn

sα2T

2(α)=T

2(α=1)/α2

B=0.33

H

1

ρ

int=exp(−iH

0t/󰀁)ρexp(iH

0t/󰀁),

int

󰀁󰀎

ρ

int,Hint

1(t)󰀐

,

Hint

1(t)=exp(iH

0t/󰀁)H

1exp(−iH

0t/󰀁).

ρ

int(t)=ρ

int(0)+i

dt=i

󰀁󰀇

2󰀑

t

0dt′󰀆󰀆

ρ

int(0),Hint

1(t′

)󰀈

,Hint

1(t)󰀈

.

zH

0=󰀁ω

z/2.󰀎

Hint

1(t)󰀐

ss′′=

󰀁

i=x,yhi

(t)σi

ss′′

󰀅

i

dt󰀇

2=󰀏

s′′

s′′′ρ

ss′′(0)󰀎

Hint

1(t′

)󰀐

s′′s′′′󰀎

Hint

1(t)󰀐

s′′′s′ei(s′′

−s′′′

)t′

ei(s′′′

−s′

)t

+󰀏

s′′s′′′󰀎

Hint

1(t)󰀐

ss′′ei(s−s′′

)t󰀎

Hint

1(t)󰀐

s′′s′′′ei(s′′

−s′′′

)t′

ρ

s′′′s′(0)

−󰀏

s′′s′′′󰀎

Hint

1(t′

)󰀐

ss′′ei(s−s′′

)t′

ρint

s′′s′′′(0)󰀎

Hint

1(t)󰀐

s′′′s′ei(s′′′

−s′

)t

−󰀏

s′′s′′′󰀎

Hint

1(t)󰀐

ss′′ei(s−s′′

)t

ρint

s′′s′′′(0)ei(s′′′

−s′

)t′󰀎

Hint

1(t′

)󰀐

s′′′s′,est

=eǫ

st

.

hi(t)hj(t′)σi

ss′′σj

s′′s′′′

=󰀏

i=x,y,zχi

(t−t′

)σi

ss′′σi

s′′s′′′,

τ=t−t′χi

(τ)=

󰀁󰀇

−2󰀂

++

󰀁󰀇

−2󰀂

+−

dt=d[Tr(σz

ρ)]

dt(ρ

++−ρ

−−)

=2󰀅

i

󰀁󰀇

2

[χx

c)+χy

c)]󰀍σ

z󰀎

1/T

1=2[χx

c)+χy

c)]/󰀁2

.

d󰀍σx

󰀎

dt=d1/T

2(θ)=󰀎

cos2

θχx

L)+χy

L)+2sin2

θχx

(0)󰀐

/󰀁2

.

xt=0hx

,

hxexp(−t/τ

p)

2α2

p2

Fe−t/τ

p,

χx,y

(ω)=α2

p2

Fτ2pTB󰀃z

2=420

TB⊥z

2=140

TB󰀃z

2=

TB⊥z

2=

µ∼92

n

s∼3×1015−2TB󰀃z

2TB⊥z

2

TB󰀃z

1TB⊥z

1

TB󰀃z

2TB⊥z

2

TB󰀃z

1TB⊥z

1

TB󰀃z

2=µ

TB⊥z

2=

TB󰀃z

2=

TB⊥z

2=

µ∼52

n

s∼4×1015−2TB󰀃z

2TB⊥z

2

TB󰀃z

2TB⊥z

2

TB󰀃z

1TB⊥z

1

TB󰀃z

2=105

TB⊥z

2=49

TB󰀃z

2=

TB⊥z

2=

T

2=2󰀁/󰀋√