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Conductance of a quantum wire at low electron density
Konstantin Matveev
Materials Science DivisionMaterials Science DivisionArgonne National LaboratoryArgonne National Laboratory Boulder School, 7/25/2005
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Outline
1. Quantum wires and Quantum Point Contacts
2. Experiments:• quantization of conductance, • 0.7 anomaly, • 0.5 plateau
3. Theoretical ideas:• spin polarization, • Wigner crystal
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One-dimensional conductors
Top view:
One-dimensional electron system
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Quantum Point Contacts2D electron gas confined
by a split gateExperiment: B.J. Van Wees et al., 1988;
also, D.A. Wharam et al., 1988
Conductance (1/Resistance) vs. Vg
Electron motion acrossthe channel is quantized
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Conductance of a Quantum WireApplied bias results in uncompensated current
I = e∆nvF
∆n =1
h∆pF =
1
h
dpFdEF
eV =e
hvFVElectron density:
I =e2
hV G=
e2
hCurrent: Conductance:
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Shape of the conductance stepsL. I. Glazman, G. B. Lesovik, D. E. Khmel'nitskii, R. I. Shekhter, 1988
The energy of the transverse motion of electrons is inversely proportional to the square of the width d(x) of the channel
V (x) ∼π2h2
2md2(x)
Constriction creates a potential barrier for electrons
How does the barrier affect the conductance?
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Landauer formula
Only a fraction of electrons cross the barrier!
Current: I = e∆nvF T(EF)
is the transmission coefficient of the barrier at the Fermi energy
T(EF)
G=e2
hT(EF)Conductance:
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Transmission coefficientParabolic-potential approximation:
E. C. Kemble, 1935
V (x) = −12mΩ2x2
Conductance as a function of the Fermi energy
2 accounts for electron spinsG0 = 2
e2
h
T(EF) =1
exp³−2πEFhΩ
´+1
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Shape of the conductance stepsExperiment:Kristensen et al., 1998
• Good agreement with theory at low temperatures;
• Noticeable deviations at higher temperatures.
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0.7 AnomalyConductance vs. gate voltage at different temperatures:
Thomas et al., 1996 Cronenwett et al., 2001
As the temperature grows, the conductance develops a shoulder near 0.7× 2e
2
h
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0.5 PlateauThomas et al., 2000 Reilly et al., 2001
0.5× 2e2
hSeveral experiments show a plateau of conductance at
This 0.5 plateau tends to appear in longer samples
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Magnetic field dependenceConductance vs. gate voltage at different B:
Thomas et al., 1996Cronenwett et al., 2001
0.7-anomaly evolves toward the spin-polarized plateau at 0.5
2e2
h
Spin-polarization effect?
Wang & Berggren, 1997Spivak & Zhou, 2000Flambaum & Kuchiev, 2000Hirose, Li & Wingreen, 2001...
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One-dimensional ferromagnetism?
• Two-dimensional electron gas is paramagnetic.• Is one-dimensional electron system ferromagnetic?
No! The ground state of a system of one-dimensionalspin-1/2 fermions has the lowest spin possible.
E. Lieb and D. Mattis, 1962;D. Mattis, The Theory of Magnetism.
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Interacting one-dimensional electrons: Bosonization
One-dimensional electron liquid is an elastic medium
H =p2
2mn+1
2mnv2F
µdu
dx
¶2u(x) is displacement of the medium, p(x) is momentum density, n is electron density.
In a non-interacting system the waves propagate at Fermi velocity vF
In the presence of interactions vF is replaced by plasmonvelocity s
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Quantized resistance
u(0, t) = u0 cosωt
Applied current: I = enu
Density of elastic energy:
Energy carried away by plasmons in unit time:
hHi= hmnu2i= m
e2nI2
W = 2hHivF =2mvF
e2nI2 = I2R
µn =
2kFπ
¶R =
2mvF
e2n≡ h
2e2Resistance:
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Interacting electronsOne-dimensional model with non-interacting leads
[Maslov & Stone; Ponomarenko;Safi and Schulz, 1995]
In the dc limit plasmon wavelength
ω → 0λ→∞
Plasmons are emitted in the non-interacting region
h
2e2Resistance is still
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Wigner crystalOne-dimensional electrons at low density n→ 0
Compare kinetic and interaction energies:
Ekin =h2k2F2m
∝ n2, ECoul =e2
r∝ n.
Coulomb energy dominates:
Electrons form a Wigner crystal and stay near their lattice sites
Density excitations are elastic waves in the crystal (plasmons)
H =p2
2mn+1
2nms2
µdu
dx
¶2
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Spin couplingTo first approximation the spins do not interact
Weak exchange due to tunneling through the Coulomb barrier
J ∼ expÃ− π√naB
!
Hσ =Xl
JSl · Sl+1, J > 0Antiferromagnetic spin chain:
Note: charge and spin are not coupled!
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Spin-charge separation?
• Exchange constant depends on electron density. Thus J=J(l).
• The density at site l depends on the number of electrons that moved through the wire: J=J[l+q(t)].
Electric current (a charge excitation)affects coupling between the spins!
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Spin contribution to the resistance
The spin Hamiltoniandepends on q(t) ∝ I. Thus the applied current excites not only charge, but also spin waves:
Hσ =XJ [l+ q(t)]Sl ·Sl+1
W = I2h
2e2+ I2Rσ = I2R
These processes give an additive contribution to the resistance
R =h
2e2+Rσ
How do we find Rσ?
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Approximation: XY model
The Jordan-Wigner transformation converts theproblem to that of non-interacting fermions:
Hσ =Xl
Jl³Sxl S
xl+1+ S
yl Syl+1
´, Jz ≡ 0
Hσ =1
2
Xl
Jl³a†l al+1+ a
†l+1al
´
J is large in the leads, butsmall in the constriction
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Jordan-Wigner transformation
Raising and lowering operators
can be expressed in terms of fermionic operators:
S±l = Sxl ± iSyl
Then the Hamiltonian of a spin chain
S+l = a†l exp
⎛⎝iπ l−1Xj=1
a†jaj
⎞⎠ , Szl = a†l al−
1
2
transforms to
H =Xl
[J⊥(Sxl Sxl+1+ Syl S
yl+1)+ JzS
zl Szl+1]
H =Xl
1
2J⊥
³a†l al+1+ a†l+1al
´+ Jz
µa†l al+
1
2
¶µa†l+1al+1+
1
2
¶
XY model: Non-interacting fermionsJz = 0
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Resistance due to scattering of excitations
1. At T ¿ J very few fermions are scattered by the barrier:
Jl = J [l+ q(t)]
The fermions near the Fermi level pick up energy from the oscillating barrier, leading to dissipation W = I2Rσ
Long wire limit
Rσ =h
2e2nF(J)
Rσ =h
4e2
Z Ã−∂nF∂E
![1− T(E)]dE
Exact result:
2. At T À J most excitations are backscattered, and resistance saturates:
Rσ ∝ e−J/T
Rσ =h
4e2
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Activated temperature dependenceKristensen et al., 2000
The temperature dependence of 0.7 structure fits to
G=2e2
h−GA exp
µ−TAT
¶Activation temperature
TA ∼ 1K
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Isotropic exchange
The true excitations of the spin chain are spinons, with the dispersion relation
²(q) =πJ
2sinq, 0 < q < π
J = J [l+ q(t)]
Spinons with energies below πJ/2 pass through; all others are reflected and contribute to Rσ
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Conductance of a Wigner crystal wire
At T ¿ J only an exponentially small fraction of the spinons are reflected:
Rσ ∝ expµ−πJ2T
¶, T ¿ J
At higher temperatures Rσ grows, and saturates at
Rσ =h
2e2, T À J
The conductance of the wire
G =1
h2e2+Rσ
changes from at T ¿ J to at T À J.2e2
h
e2
h
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High temperature
At J ¿ T all spin excitations are reflected by the barrier (c.f. XY model)
Analogy: high B
B
When spins in the wire are polarized, no excitations pass through; expect G=
e2
h
Check with bosonization:
ψ = ei(φρ±φσ)/√2In the leads
Boundary conditions at x = 0
φσ =πq(t)√2
φρ=πq(t)√2
Rσ = Rρ=h
2e2
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Conclusions1. At low density of electrons in a quantum wire, they
form a Wigner crystal
2. The spins of electrons in the Wigner crystal are weakly coupled, and the propagation of spin excitations through the wire is impeded.
3. As a result, the conductance of the wire decreases by a factor of 2.
4. No spin polarization is required!