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/ 29 ContextEnergy costAngular Mtm costImpactSummary 1 Erasure of information under conservation laws Joan Vaccaro Centre for Quantum Dynamics Griffith University Brisbane, Australia Steve Barnett SUPA University of Strathclyde Glasgow, UK
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ContextEnergy costAngular Mtm costImpactSummary / 292 Landauer erasure Landauer, IBM J. Res. Develop. 5, 183 (1961) 0 0 1 forward process: 0 0 1 0 time reversed: ? Erasure is irreversible Minimum cost 0 0/1 BEFORE erasureAFTER erasure # microstates environment heat Context Hide the past of the memory in a reservoir (who’s past is unknown) ?
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ContextEnergy costAngular Mtm costImpactSummary / 293 Exorcism of Maxwell’s demon 1871 Maxwell’s demon extracts work of Q from thermal reservoir by collecting only hot gas particles. (Violates 2 nd Law: reduces entropy of whole gas) QQ Thermodynamic Entropy 1982 Bennet showed full cycle requires erasure of demon’s memory which costs at least Q : Bennett, Int. J. Theor. Phys. 21, 905 (1982) Cost of erasure is commonly expressed as entropic cost: This is regarded as the fundamental cost of erasing 1 bit. BUT this result is implicitly associated with an energy cost: QQ work
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ContextEnergy costAngular Mtm costImpactSummary / 294 Different Paradigm all states are degenerate in energy maximisation of entropy subject to conservation of angular momentum cost of erasure is angular momentum Conventional Paradigm maximisation of entropy subject to conservation of energy cost of erasure is work S
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ContextEnergy costAngular Mtm costImpactSummary / 295 Example to set the stage… single-electron atoms with ground state spin angular momentum memory: spin-1/2 atoms in equal mixture reservoir: spin-1 atoms all in m j = 1 state (spin polarised) independent optical trapping potentials (dipole traps) atoms exchange spin angular momentum via collisions when traps brought together erasure of memory by loss of spin polarisation of reservoir – the cost of erasure is spin angular momentum 1/2 1/2 11 1 11 1 11 1
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ContextEnergy costAngular Mtm costImpactSummary / 296 1/2 1/2 11 1 11 1 11 1 Example to set the stage… single-electron atoms with ground state spin angular momentum memory: spin-1/2 atoms in equal mixture reservoir: spin-1 atoms all in m j = 1 state (spin polarised) independent optical trapping potentials (dipole traps) atoms exchange spin angular momentum via collisions when traps brought together erasure of memory by loss of spin polarisation of reservoir – the cost of erasure is spin angular momentum
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ContextEnergy costAngular Mtm costImpactSummary / 297 Impact This talk Energy Cost Conventional paradigm: ▀ conservation of energy ▀ simple 2-state atomic model New paradigm: ▀ conservation of angular momentum ▀ energy degenerate states of different spin Angular Momentum Cost ▀ New mechanism ▀ statements of the 2 nd Law E Shannon cost work entropy E thermal reservoirspin reservoir Proc. R. Soc. A 467 1770 (2011)
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ContextEnergy costAngular Mtm costImpactSummary / 298 System: 0/1 Memory bit: 2 degenerate atomic states Thermal reservoir: multi-level atomic gas at temperature T Energy cost
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ContextEnergy costAngular Mtm costImpactSummary / 299 Thermalise memory bit while increasing energy gap 0/1
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ContextEnergy costAngular Mtm costImpactSummary / 2910 raise energy of state (e.g. Stark or Zeeman shift) 0/1 Work to raise state from E to E+dE Thermalise memory bit while increasing energy gap
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ContextEnergy costAngular Mtm costImpactSummary / 2911 0/1 Work to raise state from E to E+dE Total work raise energy of state (e.g. Stark or Zeeman shift) Thermalise memory bit while increasing energy gap
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ContextEnergy costAngular Mtm costImpactSummary / 2912 0/1 Work to raise state from E to E+dE Total work raise energy of state (e.g. Stark or Zeeman shift) Thermalise memory bit while increasing energy gap Thermalisation of memory bit: Bring the system to thermal equilibrium at each step in energy: i.e. maximise the entropy of the system subject to conservation of energy. This is erasure in the paradigm of thermal reservoirs
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ContextEnergy costAngular Mtm costImpactSummary / 2913 an irreversible process based on random interactions to bring the system to maximum entropy subject to a conservation law the conservation law restricts the entropy the entropy “flows” from the memory bit to the reservoir Principle of Erasure: 0/1 E E work
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ContextEnergy costAngular Mtm costImpactSummary / 2914 System: ●spin ½ ½ particles ●no B or E fields so spins states are energy degenerate ● collisions between particles cause spin exchanges 0/1 Memory bit: single spin ½ particle Reservoir: collection of N spin ½ particles. Possible states Simple representation: # of spin up multiplicity (copy): 1,2,… n particles are spin up Angular Momentum Cost
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ContextEnergy costAngular Mtm costImpactSummary / 2915 0/1 Angular momentum diagram states Memory bit: Reservoir: # of spin up multiplicity (copy) 1,2,… state number of states with
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ContextEnergy costAngular Mtm costImpactSummary / 2916 Reservoir as “canonical” ensemble (exchanging not energy) Maximise entropy of reservoir subject to Total is conserved Reservoir : Bigger spin bath :
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ContextEnergy costAngular Mtm costImpactSummary / 2917 Reservoir as “canonical” ensemble (exchanging not energy) Maximise entropy of reservoir subject to Total is conserved Reservoir : Bigger spin bath : Average spin
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ContextEnergy costAngular Mtm costImpactSummary / 2918 0/1 Erasure protocol Reservoir : Memory spin :
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ContextEnergy costAngular Mtm costImpactSummary / 2919 0/1 Reservoir : Coupling Memory spin : Erasure protocol
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ContextEnergy costAngular Mtm costImpactSummary / 2920 Reservoir : 0/1 Increase J z using ancilla in memory (control) ancilla (target) this operation costs Memory spin : and CNOT operation Erasure protocol
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ContextEnergy costAngular Mtm costImpactSummary / 2921 0/1 Reservoir : Coupling Memory spin : Erasure protocol
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ContextEnergy costAngular Mtm costImpactSummary / 2922 0/1 Reservoir : Repeat Final state of memory spin & ancilla memory erased ancilla in initial state Memory spin : Erasure protocol
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ContextEnergy costAngular Mtm costImpactSummary / 2923 Reservoir : Repeat Final state of memory spin & ancilla memory erased ancilla in initial state 0/1 Memory spin : Total cost: The CNOT operation on state of memory spin consumes angular momentum. For step m : memory ( m -1) m th ancilla m=0 term includes cost of initial state Erasure protocol
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ContextEnergy costAngular Mtm costImpactSummary / 2924 Single thermal reservoir: - used for both extraction and erasure Impact QQ erased memory work QQ heat engine cycle entropy No net gain
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ContextEnergy costAngular Mtm costImpactSummary / 2925 cycle Two Thermal reservoirs: - one for extraction, - one for erasure Q1Q1 work entropy increased entropy Net gain if T 1 > T 2 T1T1 T2T2 Q2Q2 work erased memory & Q energy decrease heat engine
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ContextEnergy costAngular Mtm costImpactSummary / 2926 spin reservoir cycle entropy Here: Thermal and Spin reservoirs: - extract from thermal reservoir - erase with spin reservoir spin QQ work erased memory & Q energy decrease increased entropy Gain if T 1 > 0 heat engine T1T1
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ContextEnergy costAngular Mtm costImpactSummary / 2927 Shannon cost work entropy E thermal reservoirspin reservoir New mechanism: 2 nd Law Thermodynamics Kelvin-Planck It is impossible for a heat engine to produce net work in a cycle if it exchanges heat only with bodies at a single fixed temperature. S 0 Schumacher (yesterday) “There can be no physical process whose sole effect is the erasure of information” applies to thermal reservoirs only Shannon entropy general
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ContextEnergy costAngular Mtm costImpactSummary / 2928 ▀ cost of erasure depends on the conservation law ▀ thermal reservoir is a resource for erasure: cost is ▀ spin reservoir is a resource for erasure: cost is where ▀ 2 nd Law is obeyed: total entropy is not decreased ▀ New mechanism Summary Shannon cost work entropy E thermal reservoirspin reservoir
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ContextEnergy costAngular Mtm costImpactSummary / 2929 Spinning as a resource… xkcd.com
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