Yosi Avron Martin Fraas Gian Michele Graf …Yosi Avron, Martin Fraas, Gian Michele Graf Adiabatic...
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Adiabatic response of open systems
Yosi Avron Martin Fraas Gian Michele Graf
December 17, 2015
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QuestionAre topological phase protected form contact with the world?
Choosing:
Observables and states=⇒ immunity
Ω
system
bath
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QuestionAre topological phase protected form contact with the world?
Choosing:
Observables and states=⇒ immunity
Ω
system
bath
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Ambiguity: Which transport coefficients?Open vs. isolated systems
Vanchor Ffriction
Fspring
F as response to V .Which F?
Open systems
Ffriction = −ν V
Fspring = ν V
FTotal = P = 0 V
Isolated system
Ffriction = 0
Fspring = FTotal
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Ambiguity: Which transport coefficients?Open vs. isolated systems
Vanchor Ffriction
Fspring
F as response to V .Which F?
Open systems
Ffriction = −ν V
Fspring = ν V
FTotal = P = 0 V
Isolated system
Ffriction = 0
Fspring = FTotal
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Sources of ambiguitiesTensor product & Observables
Bath?System
Ambiguous tensor decomposition
Hsystem ⊗Hbath = H′system ⊗H′bath
Ambiguous observables of sub-system
H = Hs ⊗ 1 + Hinteraction + 1⊗ Hb
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Sources of ambiguitiesTensor product & Observables
Bath?System
Ambiguous tensor decomposition
Hsystem ⊗Hbath = H′system ⊗H′bath
Ambiguous observables of sub-system
H = Hs ⊗ 1 + Hinteraction + 1⊗ Hb
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Sources of ambiguitiesTensor product & Observables
Bath?System
Ambiguous tensor decomposition
Hsystem ⊗Hbath = H′system ⊗H′bath
Ambiguous observables of sub-system
H = Hs ⊗ 1 + Hinteraction + 1⊗ Hb
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Ambiguity in fluxes (aka rates aka currents)
Bath
SystemIleft→right
Isystem→bath
Q =∑
j<0 a∗j aj
Q ⊗ 1Ileft→right = i [Hs ,Q]
ITotal = i [Hs+b,Q ⊗ 1]
Formulate an ITotal as a property of the system
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Ambiguity in fluxes (aka rates aka currents)
Bath
SystemIleft→right
Isystem→bath
Q =∑
j<0 a∗j aj
Q ⊗ 1Ileft→right = i [Hs ,Q]
ITotal = i [Hs+b,Q ⊗ 1]
Formulate an ITotal as a property of the system
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Krauss maps
Krauss maps
|ψ〉s+B (0) |ψ〉s+B (t)Unitary
Kraussρs(t)ρs(0)
Trb Trb
Kraus: Positivity and Trace preserving
ρ 7→∑
KjρK†j ,
∑K †j Kj = 1
KρK † = (K√ρ)(K
√ρ)† ≥ 0
Tr ρ 7→∑
Tr KjρK†j = Tr
(∑K †j Kj
)ρ
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Krauss maps
Krauss maps
|ψ〉s+B (0) |ψ〉s+B (t)Unitary
Kraussρs(t)ρs(0)
Trb Trb
Kraus: Positivity and Trace preserving
ρ 7→∑
KjρK†j ,
∑K †j Kj = 1
KρK † = (K√ρ)(K
√ρ)† ≥ 0
Tr ρ 7→∑
Tr KjρK†j = Tr
(∑K †j Kj
)ρ
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Lindbladians
Generators of Krauss maps
ρ 7→ ρ+ δt Lρ︸ ︷︷ ︸generator
ρ 7→∑
KjρK†j︸ ︷︷ ︸
positive
K0 = 1 + δt Γ0, Kj =√δt Γj ,
∑K †j Kj = 1
trace preserving: Γ0 + Γ†0 +∑
Γ†j Γj = 0
Solve for Γ0: Γ0 = −iH − 12
∑Γ†j Γj
Lindbladians
L ρ = −i [H, ρ] +Dρ
Dρ =∑
2ΓjρΓ†j − Γ†j Γjρ− ρΓ†j Γj
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Lindbladians
Generators of Krauss maps
ρ 7→ ρ+ δt Lρ︸ ︷︷ ︸generator
ρ 7→∑
KjρK†j︸ ︷︷ ︸
positive
K0 = 1 + δt Γ0, Kj =√δt Γj ,
∑K †j Kj = 1
trace preserving: Γ0 + Γ†0 +∑
Γ†j Γj = 0
Solve for Γ0: Γ0 = −iH − 12
∑Γ†j Γj
Lindbladians
L ρ = −i [H, ρ] +Dρ
Dρ =∑
2ΓjρΓ†j − Γ†j Γjρ− ρΓ†j Γj
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Lindbladians
Generators of Krauss maps
ρ 7→ ρ+ δt Lρ︸ ︷︷ ︸generator
ρ 7→∑
KjρK†j︸ ︷︷ ︸
positive
K0 = 1 + δt Γ0, Kj =√δt Γj ,
∑K †j Kj = 1
trace preserving: Γ0 + Γ†0 +∑
Γ†j Γj = 0
Solve for Γ0: Γ0 = −iH − 12
∑Γ†j Γj
Lindbladians
L ρ = −i [H, ρ] +Dρ
Dρ =∑
2ΓjρΓ†j − Γ†j Γjρ− ρΓ†j Γj
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Lindbladians
Schrodinger and HeisenbergStates and Observables
Adjoint (Banach space)
Tr(XAρ
)= Tr
((A∗X )ρ
) Observables
‖X‖ <∞
States
Trρ <∞
L ρ = −i [H, ρ] + 2ΓρΓ† − Γ†Γρ− ρΓ†Γ
L∗ X = +i [H,X ] + [Γ†,X ]Γ + Γ†[X , Γ]
Schrodinger and Heisenberg
ρ = Lρ, X = L∗X
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Lindbladians
Schrodinger and HeisenbergStates and Observables
Adjoint (Banach space)
Tr(XAρ
)= Tr
((A∗X )ρ
) Observables
‖X‖ <∞
States
Trρ <∞
L ρ = −i [H, ρ] + 2ΓρΓ† − Γ†Γρ− ρΓ†Γ
L∗ X = +i [H,X ] + [Γ†,X ]Γ + Γ†[X , Γ]
Schrodinger and Heisenberg
ρ = Lρ, X = L∗X
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Lindbladians
Schrodinger and HeisenbergStates and Observables
Adjoint (Banach space)
Tr(XAρ
)= Tr
((A∗X )ρ
) Observables
‖X‖ <∞
States
Trρ <∞
L ρ = −i [H, ρ] + 2ΓρΓ† − Γ†Γρ− ρΓ†Γ
L∗ X = +i [H,X ] + [Γ†,X ]Γ + Γ†[X , Γ]
Schrodinger and Heisenberg
ρ = Lρ, X = L∗X
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Lindbladians
Schrodinger and HeisenbergStates and Observables
Adjoint (Banach space)
Tr(XAρ
)= Tr
((A∗X )ρ
) Observables
‖X‖ <∞
States
Trρ <∞
L ρ = −i [H, ρ] + 2ΓρΓ† − Γ†Γρ− ρΓ†Γ
L∗ X = +i [H,X ] + [Γ†,X ]Γ + Γ†[X , Γ]
Schrodinger and Heisenberg
ρ = Lρ, X = L∗X
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Lindbladians
Fluxes (aka rates) L∗QTwo notions of currents in open systems
Bath
SystemIleft→right
Isystem→bath
Q
Left-right current
Ileft→right = i [H,Q] = i Ad(H)Q
Flux: Total current
ITotal = Q = L∗Q
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Lindbladians
Fluxes (aka rates) L∗QTwo notions of currents in open systems
Bath
SystemIleft→right
Isystem→bath
Q
Left-right current
Ileft→right = i [H,Q] = i Ad(H)Q
Flux: Total current
ITotal = Q = L∗Q
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Lindbladians
Fluxes (aka rates) L∗QTwo notions of currents in open systems
Bath
SystemIleft→right
Isystem→bath
Q
Left-right current
Ileft→right = i [H,Q] = i Ad(H)Q
Flux: Total current
ITotal = Q = L∗Q
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Lindbladians
Loop currents are not rates
Fluxes vanish in stationary states:
Iloop = − ∂∂φH 6= L
∗Q
φ
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Stationary states
Stationary states of LTowards adiabatic theory of fluxes
L∗1 = 0 =⇒ 0 ∈Spectrum(L)
σ1σ3
σ2
σ1
generic KerLKerL
If dimH <∞ dim Ker L=1 generically
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Stationary states
Stationary states of LTowards adiabatic theory of fluxes
L∗1 = 0 =⇒ 0 ∈Spectrum(L)
σ1σ3
σ2
σ1
generic KerLKerL
If dimH <∞ dim Ker L=1 generically
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Fluxes
Fluxes vanish in stationary states
Fluxes vanish in stationary states:
Tr Q σ = 0
Tr Qσ = Tr (L∗Q)σ = Tr QLσ = 0
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Fluxes
Adiabatic expansion for fluxesSlow manifold
Adiabatic evolutions
ερ = Ltρ, ε 1
Adiabatic expansion
ρt = σt +εL−1σt +. . .
σ0
σt
ρt = ρ0 + ερ1 + . . .
ε0 : Ltρ0 = 0 =⇒ ρ0 = σt
σt instantaneous stationary state
ε1 : σt = Ltρ1
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Fluxes
Adiabatic expansion for fluxesSlow manifold
Adiabatic evolutions
ερ = Ltρ, ε 1
Adiabatic expansion
ρt = σt +εL−1σt +. . .
σ0
σt
ρt = ρ0 + ερ1 + . . .
ε0 : Ltρ0 = 0 =⇒ ρ0 = σt
σt instantaneous stationary state
ε1 : σt = Ltρ1
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Fluxes
Adiabatic expansion for fluxesSlow manifold
Adiabatic evolutions
ερ = Ltρ, ε 1
Adiabatic expansion
ρt = σt +εL−1σt +. . .
σ0
σt
ρt = ρ0 + ερ1 + . . .
ε0 : Ltρ0 = 0 =⇒ ρ0 = σt
σt instantaneous stationary state
ε1 : σt = Ltρ1
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Fluxes
Adiabatic expansion for fluxesSlow manifold
Adiabatic evolutions
ερ = Ltρ, ε 1
Adiabatic expansion
ρt = σt +εL−1σt +. . .
σ0
σt
ρt = ρ0 + ερ1 + . . .
ε0 : Ltρ0 = 0 =⇒ ρ0 = σt
σt instantaneous stationary state
ε1 : σt = Ltρ1
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Fluxes
Adiabatic expansion for fluxesSlow manifold
Adiabatic evolutions
ερ = Ltρ, ε 1
Adiabatic expansion
ρt = σt +εL−1σt +. . .
σ0
σt
ρt = ρ0 + ερ1 + . . .
ε0 : Ltρ0 = 0 =⇒ ρ0 = σt
σt instantaneous stationary state
ε1 : σt = Ltρ1
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Fluxes
Q in adiabatically evolving stateNo need to invert L
The magic
Tr Q ρt ≈ Tr Qσt
ρ = σt + εL−1σt + . . .
Ltρt = εLL−1σ + · · · ≈ εσt
Tr Qρt = 1εTr L
∗Qρt = Tr QLtρt ≈ Tr Qσt
The irrelevant dynamics
Adiabatic fluxes oblivious to L. Only care about σ
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Fluxes
Q in adiabatically evolving stateNo need to invert L
The magic
Tr Q ρt ≈ Tr Qσt
ρ = σt + εL−1σt + . . .
Ltρt = εLL−1σ + · · · ≈ εσt
Tr Qρt = 1εTr L
∗Qρt = Tr QLtρt ≈ Tr Qσt
The irrelevant dynamics
Adiabatic fluxes oblivious to L. Only care about σ
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Fluxes
Sharing stationary states.
Sharing instantaneous stationary states
KerLt = Ker(Ad Ht)
Example: D = γAd2(H)
σ
photon
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Fluxes
Geometry of transportTransport coefficients
φ control plane σ = (∂µσ) φµ
Tr Qρt︸ ︷︷ ︸response
≈ Tr (Q∂µσ) φµ︸︷︷︸driving
Transport coefficient
Fµ = Tr (Q∂µσ)
Oblivious to L, cares bout σ
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Fluxes
Transport coefficients & Adiabatic curvature
‘U(φ) = e iQµφµ
σ(φ) = U(φ)σU∗(φ)
∂µσ = i [Qµ, σ]
Transport coefficients
Fµν = iTr [Qµ,Qν ]σ
If σ projections
Fmuν = i Tr σ[∂µσ, ∂νσ]
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Fluxes
Conclusions and OverviewViews of the QHE
Macroscopic
L∗Q = ∂∂AH
Index=ChernGap condition?
A. Fraas and Graf, JSP(2012) arxiv1202.5750
φ1φ2
Multiply connected
∂∂AH
ChernDissipation: Kahler geometry
A. Fraas, Kenneth and Graf,NJP (2011) arxiv1008.4079
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