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Landauer's Principle


Landauer's principle bounds the heat transferred to an initially thermal reservoir when another system's von Neumann entropy decreases. In a finite-dimensional formulation, let the initial density matrix be rho_(SR)=rho_S tensor rho_R, with rho_R=e^(-betaH)/Tr(e^(-betaH)), a Hermitian matrix H, and beta=1/(k_BT)>0. Here k_B is Boltzmann's constant and T is the temperature. A unitary matrix U produces rho_(SR)^'=Urho_(SR)U^|.

Using natural logarithms, write S for von Neumann entropy, DeltaS=S(rho_S)-S(rho_S^'), and DeltaQ=Tr[H(rho_R^'-rho_R)]. Then

 betaDeltaQ=DeltaS+I(S^':R^')+D(rho_R^'Orho_R)>=DeltaS,

where D is quantum relative entropy and I(S^':R^')=D(rho_(SR)^'Orho_S^' tensor rho_R^') is quantum mutual information. Both quantities are nonnegative, yielding the bound (Reeb and Wolf 2014).

Resetting an unbiased bit to a definite value decreases entropy by ln2, giving

 DeltaQ>=k_BTln2.

This is not a heat cost for every logical operation. Initial independence, a thermal reservoir, and unitary joint evolution are essential hypotheses of this formulation. Finite reservoirs generally require a stronger bound (Reeb and Wolf 2014).


See also

Density Matrix, Mutual Information, Quantum Relative Entropy, von Neumann Entropy

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References

Landauer, R. "Irreversibility and Heat Generation in the Computing Process." IBM J. Res. Devel. 5, 183-191, 1961. https://doi.org/10.1147/rd.53.0183.Reeb, D. and Wolf, M. M. "An Improved Landauer Principle with Finite-Size Corrections." New J. Phys. 16, 103011, 2014. https://doi.org/10.1088/1367-2630/16/10/103011.

Cite this as:

Weisstein, Eric W. "Landauer's Principle." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/LandauersPrinciple.html

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