Energy cost of information transfer
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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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]”
From Quantum speed limits: from Heisenberg’s uncertainty principle to optimal quantum control (2017) · cites this paper as [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.”
From Quantum speed limits: from Heisenberg’s uncertainty principle to optimal quantum control (2017) · cites this paper as [25]
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].”
From Quantum speed limits: from Heisenberg’s uncertainty principle to optimal quantum control (2017) · cites this paper as [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
- Publisher
- American Physical Society (APS)
- 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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