from fully quantum thermodynamical identities to a second ...€¦ · outlook and open questions...
TRANSCRIPT
![Page 1: From fully quantum thermodynamical identities to a second ...€¦ · Outlook and open questions Fluctuations of states Probabilistic transformation (LOCC: Vidal 1999, Jonathan &](https://reader034.vdocuments.mx/reader034/viewer/2022050609/5fb0d2469b96a466e52fa641/html5/thumbnails/1.jpg)
From fully quantum thermodynamical identities to a second law equality
Alvaro Alhambra, Lluis Masanes, Jonathan Oppenheim, Chris Perry
Fluctuating StatesPhys. Rev. X 6, 041016 (2016)
Fluctuating WorkPhys. Rev. X 6, 041017 (2016)
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Information
TheoryPhysics
Lord Spekkens
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Quantum Information Thermodynamics
stochasticthermodynamics
open systems
majorizationtheory
optimal control
finite timethermodynamics
heat devices
foundations of statistical mechanics
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MaxwellSzilardLandauerBennett
4
W=kTlog2
Thermodynamics is an information theory
R L
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What do we mean by W=kTlog2?(consider the limit of perfect erasure)
A)W=kTlog2 on average, but there will be fluctuations around this value.
B)We can achieve perfect erasure.
C)By using slightly more work on average, you can sometimes gain work when you erase.
D)None of these statements are true.
E)This quiz is undecidable.
![Page 6: From fully quantum thermodynamical identities to a second ...€¦ · Outlook and open questions Fluctuations of states Probabilistic transformation (LOCC: Vidal 1999, Jonathan &](https://reader034.vdocuments.mx/reader034/viewer/2022050609/5fb0d2469b96a466e52fa641/html5/thumbnails/6.jpg)
What do we mean by W=kTlog2?(consider the limit of perfect erasure)
A)W=kTlog2 on average, but there will be fluctuations around this value.
B)We can achieve perfect erasure.
C)By using slightly more work on average, you can sometimes gain work when you erase.
D)None of these statements are true.
E)This quiz is undecidable.
![Page 7: From fully quantum thermodynamical identities to a second ...€¦ · Outlook and open questions Fluctuations of states Probabilistic transformation (LOCC: Vidal 1999, Jonathan &](https://reader034.vdocuments.mx/reader034/viewer/2022050609/5fb0d2469b96a466e52fa641/html5/thumbnails/7.jpg)
What do we mean by W=kTlog2?(consider the limit of perfect erasure)
A)W=kTlog2 on average, but there will be fluctuations around this value.
B)We can achieve perfect erasure.
C)By using slightly more work on average, you can sometimes gain work when you erase.
D)None of these statements are true.
E)This quiz is undecidable.
![Page 8: From fully quantum thermodynamical identities to a second ...€¦ · Outlook and open questions Fluctuations of states Probabilistic transformation (LOCC: Vidal 1999, Jonathan &](https://reader034.vdocuments.mx/reader034/viewer/2022050609/5fb0d2469b96a466e52fa641/html5/thumbnails/8.jpg)
Fluctuating work in erasure
∑s , w
P(s ' ,w∣s)eβ(Es '−Es+w )=1
∑s ' , w
P(s ' , w∣s)=1
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Main Results
● QIT strengthening of Stochastic Thermodynamics
● Generalisations of doubly-stochastic maps, majorisation
● Second law of thermodynamics as an equality (fine grained free energy)
● Fully quantum identity Stochastic Thermodynamics
● Fluctuations of work and of states
● Proof and quantification of third law of thermodynamics
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Outline
● Review of thermodynamics (Macroscopic, QIT)
● Equalities for work fluctuations
● Quantum identities
● Outlook
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Outline
● Review of thermodynamics (Macroscopic, QIT)
● Equalities for work fluctuations
● Quantum identities
● Outlook
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3 laws of thermodynamics
0) If R1 is in equilibrium with R2 and R3 then R2 is in equilibrium with R3
1) dE = dQ – dW (energy conservation)
2) Heat can never pass from a colder body to a warmer body without some other change occuring. – Clausius
3) One can never attain T=0 in a finite number of steps
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The second law
Heat can never pass from a colder body to a warmer body without some other change occurring – Clausius
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The second law
In any cyclic process⟨W ⟩≤Δ F
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Free Energy
F = <E> – TS<W> rev = F(ρ initial) – F(ρ final )ρ initial → ρ final iff <W>≤ΔF
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Free Energy
F = <E> – TS<W> rev = F(ρ initial) – F(ρ final )ρ initial → ρ final iff <W>≤ΔF This is just the first order
term of an equality!
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Resource Theories
lass of operations
In reversible theories and under minor assumptions, relative entropy distance to free states is the unique measure of the resource(Horodecki et. al. 2011)
In thermodynamics, will turn out to be the Gibbs state and the measure is
But thermodynamics can also be irreversible
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What is Thermodynamics??
A resource theoretic approach: Γ• (ρs, Hs) • adding free states ρB, HB
• work system ρW, Hw
• energy conserving unitaries U (1st law) [U, Hs + Hw + HB ] = 0
• tracing out • can allow changing Hamiltonian by adding switch bit• translation invariant on W: [U,ΔW]=0 [ΔW,Hw]=i
Streater (1995)Janzig et. al. (2000)Horodecki, JO (2011)Skrzypczyk et. al. (2013)Brandao et. al. (2015)
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Work
or in the micro - regime
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Broadest definition of thermo
Includes other paradigms (Brandao et. al. 2011)
• Hint
• H(t)
• implicit battery: arbitrary U, and take W=trHρ-trHUρU†
• Implemented using very crude control (Perry et. al. 2016)
• c.f. catalytic transformations (Brandao et. al. 2015)
What is the cost of a state transformation? (2nd law)
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What do we mean by work?
•No work: Ruch, Mead (1975); Janzig (2000); Horodecki et. al. (2003); Horodecki, JO (2011)
•Deterministic or worst case work: Dahlsten et al. (2010); Del Rio et. al. (2011); Horodecki, JO (2011); Aaberg (2011); Faist et. al. (2013), Egloff (2015)
•Average work: Brandao et. al. (2011); Skrzypczyk et. al. (2013); Korzekwa et.
al (2015)
•Fluctuating work: Jarzynski (1997); Crooks (1999); Tasaki (1999)
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Outline
● Review of thermodynamics (Macroscopic, QIT)
● Equalities for work fluctuations
● Quantum identities
● Outlook
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When can we go from ρ to σ?(2nd law)
Many Second Laws
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H=0 (Noisy Operations), no workmajorisation
ρ→σ iff ρ≻σ ∑k
p(k )≥∑k
q (k )∀ kp(1)≥ p(2)≥p(3) ...
Horodecki et. al. 2003
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(Thermal Operations), deterministic work
thermo-majorisation
(β-ordering)
Horodecki, JO (2011)Ruch, Mead, (75)
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Fluctuating work
∑s , w
P(s ' ,w∣s)eβ(Es '−Es+w )=1
f s :=E s+Tlog p(s)
F=⟨ f s ⟩
=⟨E ⟩−TS
⟨eβ(f s '− f s+w)⟩=1 2nd law equality
∑s ' , w
P(s ' , w∣s)=1
Classical derivation: Seifert (2012)
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Corrections to second law
f s :=E s+TlogP (s)
F=⟨ f s ⟩
=⟨E ⟩−TS
⟨eβ(f s '− f s+w)⟩=1
Standard 2nd law⟨ f s '−f s+w ⟩≤0 W≤Δ F
∑k=1
Nβ
k
k !⟨( f s '− f s+w)
k⟩≤0
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Fluctuating work in erasure
∑s , w
P(s ' ,w∣s)eβ(Es '−Es+w )=1
Same considerations apply to non-deterministic case
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What do we mean by W=kTlog2?(consider the limit of perfect erasure)
A)W=kTlog2 on average, but there will be fluctuations around this value.
B)We can achieve perfect erasure.
C)By using slightly more work on average, you can sometimes gain work when you erase.
D)None of these statements are true.
E)This quiz is undecidable.
![Page 30: From fully quantum thermodynamical identities to a second ...€¦ · Outlook and open questions Fluctuations of states Probabilistic transformation (LOCC: Vidal 1999, Jonathan &](https://reader034.vdocuments.mx/reader034/viewer/2022050609/5fb0d2469b96a466e52fa641/html5/thumbnails/30.jpg)
no work to fluctuating work
doubly stochastic maps majorisation
Gibbs-stochastic maps thermo-majorisation
fluctuating work linear program
∑s
P(s '∣s)=1
∑s '
P(s ’∣s)=1
∑s
P(s '∣s)eβ(Es'−Es)=1
∑s '
P(s ’∣s)=1
∑s , w
P(s ' ,w∣s)eβ(Es '−Es+w )=1
∑s '
P(s ’∣s)=1
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Thermo-majorisation curves
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Outline
● Review of thermodynamics (Macroscopic, QIT)
● Equalities for work fluctuations
● Quantum identities
● Outlook
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Quantum identity
trW [F H 'S+HWΓSW F H S+HW
−1]1S⊗ρW=1S F H (ρ):=e
β
2H
ρ eβ
2H
∑s , w
P(s ' ,w∣s)eβ(Es '−Es+w )=1 For classical states
ΓSW=trBU ρSWBU†
c.f. Aaberg (2016)
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Quantum identity
Masanes, JO (2014)
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Generalised Gibbs-stochastic
Second Law equality
Generalised Jarzynski equality
Crooks equation1
(Petz recovery)
Fully quantum identities
1 c.f. Åberg (2016)
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Generalised Gibbs-stochastic
Second Law equality
Generalised Jarzynski equality
Crooks equation(Petz recovery)
Quantum identities w/ diagonal input
c.f. Sagawa, Ueda (2011)Schumacher (2014)Manzano (2015)
∑s , w
P(s ' ,w∣s)eβ(Es '−Es+w )=1
⟨eβ(f s '− f s+w)⟩=1
⟨eβ(w− f s)⟩=Z 'S
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Outline
● Review of thermodynamics (Macroscopic, QIT)
● Equalities for work fluctuations
● Quantum identities
● Outlook
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Outlook and open questions● Fluctuations of states
● Probabilistic transformation (LOCC: Vidal 1999, Jonathan & Plenio 1999), Alhambra et. al. (2014); Renes (2015); Narasimhachar, Gour (2016)
● Generalised third laws● Reeb, Wolf (2013)
● Thermal machines: Masanes, JO (2014)
● Fully quantum fluctuations (non-commuting case)● Recovery Maps
● Alhambra et. al. (2015), Åberg (2016), Alhambra et.al. (2016)
● Embezzlement of work? (Brandao et. al. 2015)
● Autonomous machines and clocks● Horodecki et. al. (2011), Woods et. al. (2016)
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*
ρ σ
Probabilistic state transformations
W
ρ ρ'= p*σ+(1-p*)X
V l(ρ)=∑s=1
l
p(s)
2W ρ⇒σ≤ p≤2−Wσ ⇒ρ
c.f. entanglement theoryG. Vidal (1999)Jonathan, Plenio (1999)
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Probabilistic state transformations
*2W ρ⇒σ≤ p≤2−Wσ ⇒ρ
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*
Probabilistic state transformations
∑s
T (s '∣s)e−β Es≤e−βEs '
∑s
T (s '∣s) p(s)≥p p(s ' ) Renes (2015)
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Quantitative third law(Masanes, JO; to appear in Nat. Comm.)
T '≥αT
t 2d+1
Heat Theorem (Planck 1911): when the temperature of a pure substance approaches absolute zero, its entropy approaches zero
Unattainability Principle (Nernst 1912): any thermodynamical process cannot attain absolute zero in a finite number of steps or within a finite time
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Thermal Machines
● Like Turing Machines
● In a finite time, they interact with a finite volume and inject a finite amount of work
●
● Bath of volume V has sub-exponential density of states Ω(E)
t≥1vV 1/d t≥
1uwmax
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Outlook and open questions● Fluctuations of states
● Probabilistic transformation (LOCC: Vidal 1999, Jonathan & Plenio 1999), Alhambra et. al. (2014); Renes (2015); Narasimhachar, Gour (2016)
● Generalised third laws● Reeb, Wolf (2013)
● Thermal machines: Masanes, JO (2014)
● Fully quantum fluctuations (non-commuting case)● Recovery Maps
● Alhambra et. al. (2015), Åberg (2016), Alhambra et.al. (2016)
● Embezzlement of work? (Brandao et. al. 2015)
● Autonomous machines and clocks● Horodecki et. al. (2011), Woods et. al. (2016)