Cited by 252Advanced Thermodynamics and Statistical MechanicsError Correcting Code TechniquesQuantum-Dot Cellular Automata

Energy cost of information transfer

Bekenstein, Jacob D.·1981·Physical Review Letters

Abstract

From thermodynamic and causality considerations a general upper bound on the rate at which information can be transferred in terms of the message energy is inferred. This bound is consistent with Shannon's bounds for a band-limited channel. It prescribes the minimum energy cost for information transferred over a given time interval. As an application, a fundamental upper bound of ${10}^{15}$ operations/sec on the speed of an ideal digital computer is established.

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Crossref · 10.1103/physrevlett.46.623

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  • The maximum bound gives the highest rate at which quantum information can be communicated.

    “In particular, equation (2) sets the maximal rate with which quant um information can be communicated [25]”
  • Bekenstein showed that essentially the same information-transfer bound follows from thermodynamic and causality considerations alone.

    “Regardless, Bekenstein showed essentially the same fundamental bound on information transfer can be formulated from purely thermodynamic and causality considerations.”
  • For orthogonal initial and final states at high temperature, equation (44) reduces to the Bremermann-Bekenstein bound.

    “It is worth noting that if initial and final states are orthogonal and in the limit of high temper atures, equation (44) simplifies to the Bremermann-Bekenstein bound [25].”
  • The serial nature of computation at the black-hole limit can be deduced from the fact that black holes attain the Bekenstein bound, k_B RE/ħcS = 1/2π.

    “As noted above, the serial nature of computation at the black-hole limit can be deduced from the fact that black holes attain the Beckenstein bound 20 -22 , k B RE/ ¯ hcS = 1 / 2 π .”

    From Ultimate physical limits to computation (2000) · cites this paper as [21]

  • As ordinary matter obeys the Bekenstein bound, k_B RE/ħcS > 1/2π, as one compresses the computer t_com/t_flip ≈ k_B RE/ħcS will remain greater than one, so the operation will still be somewhat parallel.

    “As ordinary matter obeys the Beckenstein bound 20 -22 , k B RE/ ¯ hcS > 1 / 2 π , however, as one compresses the computer t com /tfl ip ≈ k B RE/ ¯ hcS will remain greater than one: i.e., the operation will still be somewhat parallel.”

    From Ultimate physical limits to computation (2000) · cites this paper as [21]

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Authors
Bekenstein, J. D.
Affiliations
Princeton University (US)
Corresponding author
Bekenstein, Jacob D.
Venue
Physical Review Letters
Published
1981-03-09
Volume
46
Issue
10
Pages
623-626
ISSN
0031-9007 (ISSN-L)
OpenAlex
W2072161052
Cited by
252
References
9
Citations by year
2026: 6 · 2025: 11 · 2024: 16 · 2023: 15 · 2022: 27 · 2021: 17 · 2020: 13 · 2019: 10 · 2018: 7 · 2017: 17 · 2016: 13 · 2015: 14 · 2014: 6 · 2013: 2 · 2012: 1
FWCI
7.91
Type
journal article
Language
en
Open access
closed
Locations
Physical Review Letters (publishedVersion)
Topics
  • Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Advanced Thermodynamics and Statistical Mechanics
  • Physical Sciences › Computer Science › Computer Networks and Communications › Error Correcting Code Techniques
  • Physical Sciences › Computer Science › Computational Theory and Mathematics › Quantum-Dot Cellular Automata
Keywords
information transmission, energy costs, thermodynamics of computation, causality, bandwidth-limited channels

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