information thermodynamics on feedback process
DESCRIPTION
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 engineTRANSCRIPT
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 (Maxwells demon)
Szilard engine Feedback by time-varying potential Cold damping
Summary 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 Maxwells demon: violation of thermodynamic second law
(1867)
Demon as a memory device: measurement-> information stored
Szilard engine: tractable model (1929) Shannon entropy: Landauers
principle: measurement as thermodynamic process, erasure of memory
(1961) Erasure Measurement Landauers principle Bennet, others:
Erasure process can resolve the paradox of demon. can be negative!
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. 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 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 Up to Step 3
(quasi-static)
Maximum extraction of work In sudden expansion (no work, no heat)
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 Step 2: Measurement Conditional
probability of outcomeformeasuring Joint PDF for : PDF for Cond PDF
Step 3: Switch the potential
Work done at Step 3 Step 4: protocol change in time Total work
Mutual information Shannon entropy Total entropy change
Quasi-static process Generalization of the optimal protocol
suggested by Parrondo, Horowitz, Sagawa (Nature Phys, 2015) 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 Expected for other feedback processes
Repeated with time delay and interval V. Summary The thermodynamic
second law should hold at any instant, not only for cycle. It was
proven for a few examples via the informationthermodynamics based
on the mutual information. The paradox of Maxwells demon is
resolved. The feedback process for cold damping is presented.