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Information Thermodynamics on Feedback Process

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Presentation on theme: "Information Thermodynamics on Feedback Process"— Presentation transcript:

1 Information Thermodynamics on Feedback Process
KIAS Workshop on Quantum Information and Thermodynamics – Nov, 2015, Busan Information Thermodynamics on Feedback Process Chulan Kwon Myongji University Outline Feedback process (Maxwell’s demon) Szilard engine Feedback by time-varying potential Cold damping Summary

2 I. Feedback Process Inside memory device: measurement, erasure
used Bit (binary digit) Information process empty erased Hidden process erasure measurement system state measurement outcome memory state protocol, external field feedback Inside memory device: measurement, erasure At post-measurement: (Szilard) information engine

3 Maxwell’s demon: violation of thermodynamic second law (1867)
Demon as a memory device: measurement-> information stored Szilard engine: tractable model (1929) Shannon entropy: Landauer’s principle: measurement as thermodynamic process, erasure of memory (1961) Erasure Measurement Landauer’s principle Bennet, others: Erasure process can resolve the paradox of demon. can be negative!

4 Mutual information Measurement
Memory and system as a composite system (T. Sagawa and his group, since 2008) Mutual information Measurement Potential shape change depending on X will be used as a measurement error In the post-measurement process.

5 measurement Post-measurement zero correlation zero mutual information at pre-measurement lower entropy higher mutual information at measurement higher entropy lower mutual information in post-measurement Total entropy change of the composite system and the heat bath in post-measurement Sagawa and Ueda, PRL, 2012 with the aid of fluctuation theorem Szilard engine Exorcism of demon

6 II. Szilard Engine Revisiting: Sagawa & Ueda, PRE, 2012
Step 1: thermal equilibrium Step 2: insertion of partition and measurement Step 3: quasi-static expansion according to measurement up to volume fraction Step 4: removing partition

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8 Up to Step 3 (quasi-static)
Maximum extraction of work In sudden expansion (no work, no heat)

9 Feedback control by time-varying potential
Revisiting: Abreu & Seifert, EPL, 2011; Sagawa & Ueda, 2012 Time-varying potential Overdamped motion Step 1: Thermal equilibrium at the beginning

10 Step 2: Measurement Conditional probability of outcome for measuring Joint PDF for : PDF for Cond PDF

11 Step 3: Switch the potential
Work done at Step 3

12 Step 4: protocol change in time

13 Total work Mutual information Shannon entropy

14 Total entropy change Quasi-static process Generalization of the optimal protocol suggested by Parrondo, Horowitz, Sagawa (Nature Phys, 2015)

15 IV. Cold damping (with J. Um & H. Park) Kim & Qian, PRL, 2007; Jourdan et al, Nanotechnology, 2007; Ito & Sano, PRE, 2011 y E feedback v v measure

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17 Expected for other feedback processes
Repeated with time delay and interval

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23 V. Summary The thermodynamic second law should hold at any instant, not only for cycle. It was proven for a few examples via the information thermodynamics based on the mutual information. The paradox of Maxwell’s demon is resolved. The feedback process for cold damping is presented.


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