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Information thermodynamics for a feedback control with time delay I. Feedback control: the exorcism of Maxwell’s demon II. Post-measurement process III.Multi-step feedback control with time delay IV. Cold damping V. Summary NSPCS14, KIAS, July 8-11, 2014 In collaboration with Jaegon Um, Uni-Wuerzburg, Germany Jae Dong Noh, University of Seoul, K Hyunggyu Park, KIAS, Korea Chulan Kwon Myongji University, Korea [email protected]

Information thermodynamics for a feedback control with time delay

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NSPCS14, KIAS, July 8-11, 2014. Information thermodynamics for a feedback control with time delay. Chulan Kwon Myongji University, Korea [email protected]. In collaboration with Jaegon Um, Uni-Wuerzburg , Germany Jae Dong Noh, University of Seoul, Korea Hyunggyu Park, KIAS, Korea. - PowerPoint PPT Presentation

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Page 1: Information thermodynamics  for a feedback control  with time delay

Information thermodynamics for a feedback control

with time delay

I. Feedback control: the exorcism of Maxwell’s demonII. Post-measurement processIII. Multi-step feedback control with time delayIV. Cold dampingV. Summary

NSPCS14, KIAS, July 8-11, 2014

In collaboration withJaegon Um, Uni-Wuerzburg, Germany

Jae Dong Noh, University of Seoul, KoreaHyunggyu Park, KIAS, Korea

Chulan KwonMyongji University, Korea

[email protected]

Page 2: Information thermodynamics  for a feedback control  with time delay

I. Feedback control: the exorcism of a Maxwell’s demon

1. The paradox of Maxwell’s demon: the violation of 2nd law -- Maxwell (1867), Szilard (1929), Landauer(1961), ….

Szilard engine

• Demonic entropy The state of demon? • Landauer’s principle Nothing to do with the system’s time evolution

Incomplete exorcism

Page 3: Information thermodynamics  for a feedback control  with time delay

2. Feedback control

feedback

measurement

measurement outcome

system state

protocol, external field

erasure

empty usederased

Hiddenprocess

memory state

Post-measurement process observable

Fluctuation theorem

PROPER EXORCISM OF MAXWELL’S DEMON

Bitinformation process

Generalized 2nd law T. Sagawa and M. Ueda, PRL (2012); NJP (2013)

Page 4: Information thermodynamics  for a feedback control  with time delay

II. Fluctuation theorem for post-measurement process

measurement feedback

10

Measurement

Post-measurement

Schematic view

Page 5: Information thermodynamics  for a feedback control  with time delay

Probability of measurementoutcome given system state

Post-measurement processby feedback control

Page 6: Information thermodynamics  for a feedback control  with time delay

Environmentalentropy production

trajectory

time-reverse trajectory

anomalous entropy production due to odd-parity force

Schnackenberg, 1976, master equation

Page 7: Information thermodynamics  for a feedback control  with time delay

Total entropy production

Fluctuation Theorem

Mutualinformation

Page 8: Information thermodynamics  for a feedback control  with time delay

Less correlation, less information

higher entropylower mutual information in post-measurement

more correlation, more information

lower entropyhigher mutual information at measurement

Page 9: Information thermodynamics  for a feedback control  with time delay

III. Multi-step feedback control with time delay

Page 10: Information thermodynamics  for a feedback control  with time delay

Total entropy production

Fluctuation theorem

Generalized 2nd law

Page 11: Information thermodynamics  for a feedback control  with time delay

IV. Cold damping

E

v

y

measure

Kim & Qian, PRL, 2007; Jourdan et al, Nanotechnology, 2007; Ito & Sano, PRE, 2011

feedback

v

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V. Summary

• The paradox of Maxwell’s demon is resolved by the information thermodynamics of the feedback control.• The observable post-measurement process satisfies the fluctuation theorem, which is the true exorcism of Maxwell’s demon, with no knowledge about hidden process in Maxwell’s demon or memory device such as measurement, erasure.• The multi-step feedback control with time delay is studied:

• The cold damping problem is revisited. Temperature depends on time delay and time interval between measurement steps. • An experimental study is expected.