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![Page 1: Disorder effects in 2D ferromagnetic semiconductor structures: GaAs/InGaAs/GaAs quantum well with remote Mn delta-layer B. Aronzon, A. Davydov, K. Kugel,](https://reader033.fdocuments.in/reader033/viewer/2022051315/56649e895503460f94b8db9f/html5/thumbnails/1.jpg)
Disorder effects in 2D ferromagnetic semiconductor structures:
GaAs/InGaAs/GaAs quantum well with remote Mn delta-layer
B. Aronzon, A. Davydov, K. Kugel, V. Tripathi, K. Dhochak, A. Lashkul and E. Lahderanta
1. Introduction. Structure description. Proofs of 2D and ferromagnetic ordering.2. Disorder effects. Resistivity.3. Disorder effects. Noise.4. The nature of ferromagnetic ordering. Models.5. Conclusion.
Semiconductor spintronics. 2 problems. Tc and 2D
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2
Quantum well with Mn delta layer
2D
GaAs, 15-18 nm
-layer Mn
spacer GaAs, 3 nm
QW InGaAs, 9-10 nm
-layer С
Buffer layer GaAs, 0.5 μm
cap-layer GaAs, 30-40 nm
Substratei-GaAs (100)
Awshalom et al., 2004Zaicev, et al., 2009Aronzon et al., 2006, 2009, 2010, 2011, 2012Wegscheider et al., 2007, 2010Dietl et al. 2010Sapega et al. 2012
Buffer GaAs, 25 нм
cap-layer GaAs, 60-80 нм
δ-layer Mn
spacer GaAs, 1-5 нм
QW InGaAs, 9-10 нм
GaAs, 5 нмδ-Be
SubstrateGaAs, (100)
B.N. Zvonkov et al.N. Novgorod
Y. Furdyna et al.Buffalo
Parametes of the samplesParametes of the samples
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3
-12 -8 -4 0 4 8 12
5000
10000
15000
20000
25000T=5KB _I_ xy
Rx
x, O
hm
B, T
0 4 8 1214600
14800
15000
15200
Rxx
, Ohm
B, T
T=5K
B in plane
Quantum Hall Effect
Mn 0.5ML
10 200
20
40n
s = 4.56*1011cm-2
Rxx
, KO
hm
B, T
GaAs(Mn)/In0.17
Ga0.83
As/GaAs
d=10nm,
0 10 20 300
10
20
30
40
InGaAs/GaAs QW
Rxy
, KO
hm
B, T
Rk = h/e2
2D
J. Appl. Phys. 107, 023905 (2010)
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Transport proofs for ferromagnetism
Pure carbon doping (Sample 5) shows no resistance anomaly. Samples 1 and 4 show hysteresis in magnetisation curve. [ JETP Lett. (2008)] Anomalous Hall effect observed in all samples doped with Mn.
? Metal - insulator transition under rise of
Mn content ?
Resistivity Anomalous Hall effect
Hall resistance dependes on spin-orbit interaction and carrier polarization
RHd= yx = R0B + RsM
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Formation of charge carrier puddles in the quantum well (QW) from competition of doping disorder and nonlinear screening.
z0
Partially ionized Mn dopants
Typical potential fluctuation Vfluc
Location of holes in thetransverse direction
Hole wavefunction in transversedirection
After Gergel’ and Suris paper and Shklovskii and Efros
Fluctuation potential
Schematic of the quantum well potential (shown inverted). Dashed (blue) line represents the quantum well potential in the absence of fluctuations and the solid (red) line shows the potential well with an attractive fluctuation potential. The dotted line indicates the Mn dopants at a distance from the left face of the quantum well.
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Model of nanoscale inhomogeneitiesModel of nanoscale inhomogeneities
z0
2
20
2
1log16 z+
R+
en'ze=zV c
2a2
fluc
RMS potential fluctuation:
n’a - Density of ionized Mnatoms
Screening length correspondsto carrier density p:
p
n'=R a
c
/
[Kennett, Tripathi, PRB (2006)]
PRB, 2011
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Electrical resistanceElectrical resistance: : Role of ferromagnetic correlationsRole of ferromagnetic correlations
Mijij
ijA
D=
TJ+TE=T
ξ/expθcos
/θcos1/exp0ρρ
Vb a r r i e r
i j
θi j
EA + J(1-cos θ
i j )
Extra energy cost due to spin orientation
Di j
Resistivity anomalycorresponds to rapid change of magnetic contribution.
Cosine term changes appreciably whenmagnetic correlation length becomes ofthe order of droplet separation.
PRB, 2011
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Observed temperature dependence of resistance for (a) Sample 4, in units of the resistance at 70 K, and (b) Sample 1, in units of the resistance at 90 K (points), andtheoretical fits (solid lines). Sample 4 is near the percolation threshold and Sample 1 is well-insulating. The fits were made using Eq. (13). Parameters such as the activation energy EA and the droplet separation D1 were chosen close to the values obtained from the droplet model. The magnetic parameters J and TC were then varied to obtain the above fits. In both cases, the best fit value of TC was significantly larger than the temperature, at which the resistance anomaly (hump or shoulder) was observed.
Resistivity
PRB, 2011
Two phase system
Tc
Tс – local transition in magnetic islands
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9
Power spectral density of electrical noise
10 100
1E-16
1E-15
1E-14
1E-13
at 150Hz
Pow
er S
pect
ral D
ensi
ty (
Hz
-1)
T (K)
at 10Hz
0,1 1 10 100 1000
1E-14
1E-13
1E-12
Pow
er S
pect
al d
ensi
ty x
freq
uenc
y
frequency, Hz
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
0 1 2 3 4 5
23K
22.6K
21.4K
21.5K
20.9K
20.6K
20.3K
20.1K
18.94K
18.94K
0.15
0 10 20 30 40 50 60 70 80 90
1,5x104
2,0x104
Rxx
, Ohm
T, K
4417
Percolation transitionin magnetic subsystem?
There are no transitions in transport properties.
PRB, 2012
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10
Noise fit: Frequency dependenceNoise fit: Frequency dependenceThe long-time dependence of the resistivity autocorrelation functionSρ(t) extracted from the noise data at T = 4.0 K together with fits. The red curve is a fit to Sρ(t)=A/t1.05 + Bln(t/t0), blue curve is a fit to Sρ(t) = A/t2/5 + Bln(t/t0). In 2D, Sρ(t ) ∼ t−1 behavior is expected for a disordered RKKY ferromagnet and Sρ (t ) ∼ t−2/5 for double-exchange ferromagnets. The logarithmic time dependence indicates 1/f noise contributions. The fit to the RKKY model is better than to the double exchange.
Frequency dependence of noise at T = 4 K (solid curve) together with fits to the low- and high-frequency regimes. At the low-frequency end, the dashed curve and the dotted curve are fits to Sρ ∼ A − Bf2 and Sρ ∼ A − B lnf − Cf,respectively. At the high-frequency end, the fit is to Sρ ∼Af−1.53. 1.53
ρf~fS
PRB, 2012
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Noise fit: Temperature dependenceNoise fit: Temperature dependence
Sample 4f = 150Hz
TefS cT /
~ 2
Fit to TC= 52K
PRB, 2012
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Curie temperature dependence on the depth of quantum well
-4 -2 0 2 4 60
0,2
0,4
0,6
z
q0z
u0=3
51015
max
80 100 120 140 160 180
0
10
20
30
40
Tc,
K
E, meV
Mn 0,25 MC Mn 0,3 MC
5570
5765
5569
5572
5764
5763
J. Phys. Conf. Ser. 2013
55 and 57 set
48 set Mn 0.5 Ml
0.10 0.15 0.2020
25
30
35
40
Tc,
K
E, eV
4836
4834
4843
4831
4832 -4846
110 meV
U=100 meV U=140 meV U=180 meV
GaAs GaAs GaAs
Mn
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131 2 3 4 525
30
Tc,
K
d, nm
Buffer GaAs, 25 нм
cap-layer GaAs, 60-80 нм
δ-layer Mn
spacer GaAs, 1-5 нм
QW InGaAs, 9-10 нм
GaAs, 5 нм
δ-Be
SubstrateGaAs, (100)
MBE
1 2 3 4 522
24
26
28
30
32
5575Mn 0,3In 0,3
Tc,
K
d, nm
5574Mn 0,3In 0,3 5570
Mn 0,3In 0,3
GaAs, 15-18 nm
-layer Mnspacer GaAs, 3 nm
QW InGaAs, 9-10 nm
-layer С
Buffer layer GaAs, 0.5 μm
cap-layer GaAs, 30-40 nm
Substratei-GaAs (100)
CVD
Curie temperature dependence on the spacer thickness
Mech
J. Phys. Conf. Ser. 2013
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Models
M=0
GaAs
Mn
GaMnAs GaInAs
GaAsGaMnAs GaInAs
Itinerant FM ordering in GaMnAs layer. (S.Caprara et al. PRB (2011)).
Averkiev et al. – resonance tunneling.PRB (2012).
EF
Mn layer – GaMnAs
Tс – local transition in magnetic islands
Two phase system
Tc
L
Meilikhov et al. – overlapping of the wave function tails with GaMnAs layer.
JETP Letters (2008)
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15
THANKS FOR YOUR
ATTENTION!
Disorder and magnetic interactions affect strongly both transport and magnetic properties of the structures and could explain the temperature dependence of resistance and noise quantitatively.
Conclusion
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Model of nanoscale inhomogeneitiesModel of nanoscale inhomogeneities
z0
Assume Gaussian white noisedistribution for ionized dopants:
r'rn'=nr'nrn a 2
Fluctuation charge in circle ofradius R:
2
a
R
n'=Rn
2
Disorder screened by holes in QW: ca Rn'=Rn=p //2
PRB, 2011
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Ferromagnetic correlations: modelsFerromagnetic correlations: models
cc
ccM
TT,TTa
TT,TTa=
2/exp
≫/1/ξ
I. Isotropic 2D Heisenberg ferromagnet
II. Uniaxial 2D Heisenberg ferromagnet
jij
i SSJ=H No long-range magnetic orderat finite temperature.
KJ
TT
SKSSJ=H
c
ijzj
iji
/ln~
20
2
0γ
0
0
~/1/
2/exp
≫/
ξ
TT,TTa
TTT,TTa
TT,TTa
= cc
cc
M
M. Bander, D. Mills, PRB (1988) 1.25= for Ising
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Voltage noise: mVoltage noise: magnetic fluctuationsagnetic fluctuations
,,DCe+CTJS ijMijD
ααααα
22ρ ω
ξ/ω0,/ρ/ω
Resistivity noise from magnetic fluctuations
q,eqdT
=r,C riqαβ
2αβαβ Im
2
Autocorrelation functionof magnetisation
Autocorrelation function contains information on dynamics, and can shedlight on the mechanism of ferromagnetism.
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Magnetic correlations: dynamicsMagnetic correlations: dynamics
q,iq+
T=q,
M /1 2
0αβαβResistivity noise is sensitive to
the dynamics of the ferromagnet:
Interested in two broad universality classes depending on whether the dynamics has a hydrodynamic description:
2
0ω/const. Mq,
=q,
Model A: No conserved order parametere.g. anisotropic Heisenberg
Model B: Conserved order parametere.g. Isotropic Heisenberg 2
q,Dq=q,
0ω
Hohenberg, Halperin, RMP (1977)
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0 10 20 30 40 50 60 70 80
0
2
4
A
(GaAs)1-yMny
a/a, %
InхGa1-хAs
yM
n
0.0
0.1
0.2
0.3
0 10 20 30 40 50 60 70 80
0
2
4
0.0
0.1
0.2
0.3
0.4
B (GaAs)1-yMny
InхGa1-хAs
z, nм
yM
n
Sample 4831
sample4834
Mn content
40
GaAs, 15-18 nm
50-layer Mn
spacer GaAs, 3 nm
QW InGaAs, 9-10 nm
-layer С
Buffer layer GaAs, 0.5 μm
cap-layer GaAs, 30-40 nm
Substratei-GaAs (100)
z, nm
.0
55
60
Profile of the deviation of the lattice constant from its value for GaAs along the sample depth (z)
X-ray diagnostics of the samplesX-ray diagnostics of the samples2D
J. Appl. Phys. 107, 023905 (2010)
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Noise fit: Frequency dependenceNoise fit: Frequency dependence
1.53ρ
f~fSModel A:
Model B:
~ f −2
~ f −1
CffBA~fS lnρ
2ρ BfA~fS (Model A)
(Model B)Sample 4T=4K
Model A: Random TelegraphModel B: Diffusive spin dynamics
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GaInAs GaAsGaAs(Mn)
2D conductivity channel
z
E0
Mn
L
0
Carrier-mediated FM via carriers in the quantum well.
U(z)
(z)
(z)
GaAs GaAs
GaInAs
E.Z. Meilkhov and R.M. Farzetdinova, JETP Letters (2008)
M
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23
Mn
(z)
MnGaAs
GaInAsThere is 2D spin – polarized collective state in the GaMnAs aria. The corresponding wave function is expanded inside quantum well and acts on carriers causing their spin-polarization.
FM ordering occurs in GaMnAs layer due to itinerant mechanism. Carriers in the quantum well do not invoolved. V.V. Tugushev et al.PRB (2009)
FM ordering inside Mn layer M
From Lucev et al. PRB 2009
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Модель
M=0
GaAs
Mn
GaMnAs GaInAs
GaAsGaMnAs GaInAs
ФМ упорядочение в GaMnAs слое обусловлено обменом спинов Mn через носители в этом же слое. Носители из квантовой ямы в обмене почти не участвуют (S.Caprara et al.PRB (2011)). Вблизи дельта слоя возникает 2D спин – поляризованное состояние. Волновая функция проникает из дельта слоя в квантовую яму, вызывая спиновую поляризацию дырок.
Аверкиев и др. – резонансное туннелирование,Мейлихов и др. – перекрытие хвостов
волновой функции из КЯ в слой GaMnAs
EF
Mn – содержащий слой GaMnAs
Tс – локальный ФМ в островках
Двухфазная среда
Tc
L
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Voltage noise: frequency dependenceVoltage noise: frequency dependence
Freq. dependence of the voltage noise for temperatures below resistivity anomaly.
f S f ~ f −0.53
f S f ~ f ?
Sample 4
Freq. dependence is not 1/f. Random telegraph? Griffiths?
Characteristic frequency
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ConclusionsConclusions At low carrier density, competition of disorder and nonlinear screening causes formation of charge puddles in 2DHG.
Resistance anomaly arises when magnetic correlation length becomes comparable with a relevant length scale. Anomaly not evidence for a phase transition.
In 2D (unlike 3D) resistance anomaly may occur far below Curie temperature.
Noise is non-1/f over a large window of frequencies. Data in reasonable agreement with both Model A (Random Telegraph) and Model B (Diffusive spin dynamics).
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27
намагниченность
-2 -1 0 1 2-1.0x10-4
-5.0x10-5
0.0
5.0x10-5
1.0x10-4
Mn in QW sampleT = 3 K
M (
em
u)
B (T)
0 20 40 60 80 1000.0
1.0x10-5
2.0x10-5
3.0x10-5
4.0x10-5
Mn in QW sample B = 1 TM
(e
mu
)T (K)
ZFC FC
Ferromagnet
Exchange bias of hysteresis loop
Известен для двухвазных систем с ферро- и антиферромагнитными включениями,например, в манганитах.
В чем причина необычного вида гистерезиса?
JETP Letters, 2008
Magn
Загадка 3
Диэлектрический образец
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28
-8 -6 -4 -2 0 2 4 6 8
-8
0
8 10K
M
(e
mu
)
B (T)
НамагниченностьМалое содержание Mn
Magn
JETP Letters, 2007
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29
Model
Mn rich lake
Ferromagnetic regionQW, high carrier
concentration
Magnetic moment of the lake is pinned by Jf-af
The percolation transition in magnetic system affect scattering and results in decrease of resistance – reason of the noise.
Antiferromagnetic region
Jf
Jf-af
M
Mn delta layer
spacer
2DEG
Due to shape anisotropymagnetic moment of Mn layer aligns along
Due to quantizationspin of heavy holes aligns perpendicularly
Is the exchange possible?Yes, due to high Fermi energy and disorder. dqw=10 nm, rloc= 20-30 nm, K in plane is about Kz
JETP Letters, 2008PSS, 2008
Magn
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Nature for AFM regions
Tugushev et al. PRB (2009)
Magn
Fig from Lutcev et al. PRB (2009)
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31
Magnetization
-2 -1 0 1 2-8.0x10-5
-4.0x10-5
0.0
4.0x10-5
8.0x10-5
M (
em
u)
B (T)
Mn in qw4831T = 3 K
0 20 40 60 80 100
0.0
1.0x10-5
2.0x10-5
3.0x10-5
4.0x10-5
Spin glass
Mn in qw4831 B = 1 T
M (
em
u)
T (K)
ZFC FC
-2 -1 0 1 2-1.0x10-4
-5.0x10-5
0.0
5.0x10-5
1.0x10-4
Mn in qw4834T = 3 K
M (
em
u)
B (T)
Metallic sampleLow Mn content
0 20 40 60 80 1000.0
1.0x10-5
2.0x10-5
3.0x10-5
4.0x10-5
Mn in qw4834 B = 1 TM
(e
mu
)
T (K)
ZFC FC
Ferromagnet
Insulator sampleHigh Mn content
Exchange bias of hysteresis loop
Known for two phase systems with ferro - and anti-ferro inclusions,for example, phase separation in manganites
What is thereason forunusualhysteresisloop?
JETP Letters, 2008
Mag
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Model of nanoscale inhomogeneities Model of nanoscale inhomogeneities 11Formation of charge carrier puddles in the quantum well (QW) from competition of doping disorder and nonlinear screening.
Partially ionized Mn dopants
Typical potential fluctuation
(Gergel' & Suris, JETP (1978))
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Estimate of the droplet sizesEstimate of the droplet sizes
Virial theorem:
pnflucnmax, R,zV=
k0n
22
2
1
2m
Droplet charge distributed over subbands:
22
2m
222
211
1
122
22
1
2
21
pmax,pmax,pa
max,max,max,max,
Rk+
Rk=Rn'
EEkk=EE
Solve these nonlinearequations to get dropletsize
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T= 77 K
T= 5 K
Results of the calculationsResults of the calculations
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Флуктуационный потенциал и температурная зависимость сопротивления
Вслед за работой Гергель, Сурис, ЖЭТФ (1978)
PRB 2011
Загадка 1Расчетная температура не совпадает с максимумом R(T).Две температуры?
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AHE temperature dependence
-2 0 2
-200
-100
0
100
200
T=4.6 K; p=3.1*1011
cm-2,
=350 cm2/Vs
T=33 K;
p=3.3*1011
cm-2,
=850 cm2/Vs
T=100 K; p=1.4*1012
cm-2,
=1000 cm2/Vs
T=77K; p=1*1012
cm-2,
=1200 cm2/Vs
T=50 K; p=5*1011
cm-2,
=1100 cm2/Vs
RA
HE
, Ohm
B, T
0 20 40 60 80 100-300
-200
-100
0
100
200
300
p=4*1011 cm-2
p=650 cm2/V*s
at T=30 K;
3 T
0.3T
1 T
RA
HE, O
hm
T, K
AHE change sign with T
Two contributions intrinsic and side-jump
AHE
0 20 40 60 80 100-200
-100
0
100
10
20
Bsa
tur, T
RA
HE, O
hm
T, K
5569
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37
-4 -2 0 2 4
-40
-20
0
20
40
Rxy
a, O
hm
0.5 ML
B, T
17 K
-4 -2 0 2 4
-400
-200
0
200
1.2 ML
Rxy
a, O
hm
B, T
55 K
2/ xxaxy
axy
2/ xxnxy
nxy
heaxy /07.0 2 hea
xy /17.0 2he /1.0 22Dрасчет
222
22
1
c
cnxy m
рe 2// nxy
axy
nxy
axy
S.Y. Liu, X.L. Lei, Phys. Rev. B 72, 195329 (2005).V.K. Dugaev, P. Bruno, M. Taillefumier, B. Canals, C. Lacroix, Phys. Rev. 71, 224423 (2005).
AHE
J. Phys. Cond. Matt. 2008, JAP2010
Аномальный эффект ХоллаХолловское сопротивление RHd= yx = R0B + RsMАномальный вклад пропорционален намагниченности и зависит от S-O взаимодействия и спиновой поляризации носителей.
axy
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Fluctuation potential
After Gergel’ and Suris paper and Shklovskii and Efros
Schematic of the quantum well potential (shown inverted). Dashed (blue) line represents the quantum well potential in the absence of fluctuations and the solid (red) line shows the potential well with an attractive fluctuation potential. The dotted line indicates the Mn dopants at a distance from the left face of the quantum well.
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Geometry of the Geometry of the dropletsdroplets
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Voltage noise: charge fluctuationsVoltage noise: charge fluctuations
Fluctuations in inter-droplet tunnellingA. L. Rakhmanov et al., PRB (2001) [phase-separated manganites]
2
2
2
2ω
1
/1
ij2
ijCE
D+
DTe
ijClocijD
ij
TJT+Ee
D
cos1///1
02
Different from characteristictime associated with resistivity.
Random-telegraph type(consistent with experiment)
Temperature dependence not in agreement with data.Need to look at magnetic contribution to noise.
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GaInAs
GaAs
V-band
FM transition in the Mn layer affects the conductivity in QW
z
Mn
GaAs
L
U(z)
Mech
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GaInAs
GaAsGaAs
V-band
z
Mn
L
U(z)
FM transitionoccurs
0 20 40 60 80 100
4.0x1011
8.0x1011
1.2x1012
1.6x1012
2.0x1012
Tcl
Tc
T, K
p, cm-2
FM transition in the Mn layer affects the conductivity in QW
0 20 40 60
9.0x1011
1.2x1012
2000
2500
3000
p, c
m-2
T, K
p, cm^-2
,
cm
2 /V
*s
mob, cm^2/V*s
QW 4831
Mech
5569
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Two-dimensionalityTwo-dimensionality
Negative magnetoresistance consistent with 2D weak localisation corrections.
Observation of Shubnikov-de Haas oscillations for fields perpendicular to plane of hole gas.
Quantum Hall effect in all samples, including Sample 1. [B. A. Aronzon et al., J. Appl. Phys. (2010)]
Sample 3 (metallic)
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Photolumiscence InGaAs/GaAs:Mn
0 4 80.0
0.5
1.0
1,33 1,34
dS = 3 nm
B = 5 T
EL
inte
nsity
h (eV)
Psa
t
reference LED
dS (nm)
dS= 3 nm
EL PL
B (T)
PC
(a)
0 5 10
0.0
0.2
0.4 (b)
reference LED
Pc(B) dependences for EL and PL
of sample 2 and of the reference sample 5 without δ-Mn layer. Inset shows polarized EL spectra; (b) Pc(9 T) values vs. ds in LEDs
with x = 0.1.
Zaitsev, Kulakovskii et al. Jetp letters 90,730 (2009)
Psat (9 T) values vs. ds
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45
1. Introduction. Structure description. Proofs of 2D and ferromagnetic ordering.2. Disorder effects. Resistivity.3. Disorder effects. Noise.4. The nature of ferromagnetic ordering. Models.5. Conclusion.
Semiconductor spintronics. 2 problems. Tc and 2D
Outline