Topological phases in superconductor/noncollinear …DPG-Frühjahrstagung 2016 — TT 68.3...
Transcript of Topological phases in superconductor/noncollinear …DPG-Frühjahrstagung 2016 — TT 68.3...
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s-wave SC
Topological phases in superconductor/noncollinear
magnet interfaces with strong spin–orbit coupling
Henri Menke Alexander Toews Andreas P. SchnyderMax Planck Institute for Solid State Research, Stuttgart, Germany
DPG-Frühjahrstagung 2016 — TT 68.3
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Motivation
STM tip
superconductor
• p-wave superconductors are rare in nature
• Topological phase of a superconductor
• This phase can be induced in tailored materialsSee talk by A. Yazdani, TT 26.4
• Topological superconductors host Majorana edge states
• Majorana edge states are robust against disorder
• Candidate for fault tolerant quantum storage
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Noncollinear Magnets• Collinearity of two vectors means that they are linearly dependent
a = γb , γ is scalar
• Example of a noncollinear spin texture
θ
Bn = B(sinθn cosφn, sinθn sinφn, cosθn)>
θ = θn+1 − θn = 2π3 , φn = 0� 2/10
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Noncollinear Magnets• Collinearity of two vectors means that they are linearly dependent
a = γb , γ is scalar
• Example of a noncollinear spin texture
θ
Bn = B(sinθn cosφn, sinθn sinφn, cosθn)>
θ = θn+1 − θn = 2π3 , φn = 0� 2/10
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Hamiltonian
s-wave SC
• Tight-binding approximation
• superconductive s-wave pairing
• sd coupling
• Rashba-type spin–orbit coupling lk = sinkxy
H = t∑〈i,j〉,σ
c†i,σcj,σ − µ∑i,σc†i,σci,σ +∆
∑i
(c†i,↑c
†i,↓ + ci,↓ci,↑
)+∑i,α,β
(Bi ·σ)αβc†i,αci,β + λ∑i
[(c†i−δx ,↓ci,↑ − c
†i+δx ,↓ci,↑
)+ h.c.]
P. M. R. Brydon et al., Phys. Rev. B 91, 064505 (2015)
S. Nadj-Perge et al., Phys. Rev. B 88, 020407 (2013)
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Hamiltonian
s-wave SC
• Tight-binding approximation
• superconductive s-wave pairing
• sd coupling
• Rashba-type spin–orbit coupling lk = sinkxy
H = t∑〈i,j〉,σ
c†i,σcj,σ − µ∑i,σc†i,σci,σ +∆
∑i
(c†i,↑c
†i,↓ + ci,↓ci,↑
)+∑i,α,β
(Bi ·σ)αβc†i,αci,β + λ∑i
[(c†i−δx ,↓ci,↑ − c
†i+δx ,↓ci,↑
)+ h.c.]
P. M. R. Brydon et al., Phys. Rev. B 91, 064505 (2015)
S. Nadj-Perge et al., Phys. Rev. B 88, 020407 (2013)
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sd vs. Rashba
• It can be shown that the effects of spin–orbit coupling can be
mapped to a helical spin texture by a unitary transformation in spin
space.
• Ferromagnetic spin texture
Bn = B =
BxByBz
• Spin–orbit coupling
λ ≠ 0
vs.
• Helical spin texture
Bn = B
sinθn cosφnsinθn sinφn
cosθn
• No spin–orbit coupling
λ = 0
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Topological Invariant
• Transform Hamiltonian to Majorana representation
b2n−1,σ = fn,σ + f †n,σ , b2n,σ = −i(fn,σ − f †n,σ )
H = i4
∑qb†qA(q)bq
• Bulk Z2 invariant ν ∈ {0,1}
(−1)ν =∏a
Pf[A(Λa)]√det[A(Λa)]
=∏a
sgn(Pf[A(Λa)]
) = ±1Λa ∈ {0, π} are the time-reversal invariant momenta.
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Topological Invariant
• Transform Hamiltonian to Majorana representation
b2n−1,σ = fn,σ + f †n,σ , b2n,σ = −i(fn,σ − f †n,σ )
H = i4
∑qb†qA(q)bq
• Bulk Z2 invariant ν ∈ {0,1}
(−1)ν =∏a
Pf[A(Λa)]√det[A(Λa)]
=∏a
sgn(Pf[A(Λa)]
) = ±1Λa ∈ {0, π} are the time-reversal invariant momenta.
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Comparison• Helical spin texture, α = cosθ/2 and β = sinθ/2.
Pf[A(q)] = B2 − [µ − 2tα cos(q)]2 − [∆0 − 2itβ sin(q)]2
S. Nadj-Perge et al., Phys. Rev. B 88, 020407 (2013)
• Ferromagnetic spin texture with spin–orbit coupling
Pf[A(q)] = |B|2 − [µ − 2t cos(q)]2 − [∆0 − 2iλ sin(q)]2
Parameter matching
t ← tα , λ← tβ• Helical spin texture with spin–orbit coupling
Pf[A(q)] = B2 − [µ − 2tα cos(q)+ 2λβ cos(q)]2
− [∆0 − 2itβ sin(q)− 2λα sin(q)]2
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Comparison• Helical spin texture, α = cosθ/2 and β = sinθ/2.
Pf[A(q)] = B2 − [µ − 2tα cos(q)]2 − [∆0 − 2itβ sin(q)]2
S. Nadj-Perge et al., Phys. Rev. B 88, 020407 (2013)
• Ferromagnetic spin texture with spin–orbit coupling
Pf[A(q)] = |B|2 − [µ − 2t cos(q)]2 − [∆0 − 2iλ sin(q)]2
Parameter matching
t ← tα , λ← tβ• Helical spin texture with spin–orbit coupling
Pf[A(q)] = B2 − [µ − 2tα cos(q)+ 2λβ cos(q)]2
− [∆0 − 2itβ sin(q)− 2λα sin(q)]2
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Numerical Evidence• Helical spin texture, θ = 2π/3, t = 2∆
1 12 24 36 480
0.1
0.2
0.3
Site index
LDO
S
λ = 0
−1 −0.5 0 0.50
0.2
0.4
0.6
E/∆
λ = 0
• Ferromagnetic spin texture with spin–orbit coupling, t = ∆
1 12 24 36 480
0.1
0.2
0.3
Site index
LDO
S
λ = √3
−1 −0.5 0 0.50
0.2
0.4
0.6
E/∆
λ = √3
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Edge State Fragility• Can we spoil the topological phase with strong spin–orbit coupling?
0 1 2 3 4 5
−1
−0.5
0
0.5
1
λ/∆
E/∆
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Edge State Fragility• Can we spoil the topological phase with strong spin–orbit coupling?
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Outlook & Ongoing Research• Two-dimensional systems with noncollinear and noncoplanar spin
textures S. Nakosai et al., Phys. Rev. B 88, 180503 (2013)
−1 −0.5 0 0.5 1−1
−0.5
0
0.5
1
kx/π
E/∆
noncollinear
−1 −0.5 0 0.5 1−1
−0.5
0
0.5
1
kx/π
noncoplanar
0
0.2
0.4
• Computation of the edge currents
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References & Further Reading
[1] P. M. R. Brydon, S. Das Sarma, H.-Y. Hui, and J. D. Sau, Phys. Rev. B 91, 064505
(2015).
[2] S. Nadj-Perge, I. K. Drozdov, B. A. Bernevig, and A. Yazdani, Phys. Rev. B 88,
020407 (2013).
[3] S. Nakosai, Y. Tanaka, and N. Nagaosa, Phys. Rev. B 88, 180503 (2013).