Negentropy

Source: Wikipedia, the free encyclopedia.

In

What is Life?[1] Later, French physicist Léon Brillouin shortened the phrase to néguentropie (negentropy).[2][3] In 1974, Albert Szent-Györgyi proposed replacing the term negentropy with syntropy. That term may have originated in the 1940s with the Italian mathematician Luigi Fantappiè, who tried to construct a unified theory of biology and physics. Buckminster Fuller
tried to popularize this usage, but negentropy remains common.

In a note to

What is Life?
Schrödinger explained his use of this phrase.

... if I had been catering for them [physicists] alone I should have let the discussion turn on free energy instead. It is the more familiar notion in this context. But this highly technical term seemed linguistically too near to energy for making the average reader alive to the contrast between the two things.

Information theory

In

Gaussian distribution is the one with the highest entropy. Negentropy measures the difference in entropy between a given distribution and the Gaussian distribution with the same mean and variance. Thus, negentropy is always nonnegative, is invariant by any linear invertible change of coordinates, and vanishes if and only if
the signal is Gaussian.

Negentropy is defined as

where is the differential entropy of the Gaussian density with the same mean and variance as and is the differential entropy of :

Negentropy is used in

entropy, which is used in independent component analysis.[7][8]

The negentropy of a distribution is equal to the Kullback–Leibler divergence between and a Gaussian distribution with the same mean and variance as (see Differential entropy § Maximization in the normal distribution for a proof). In particular, it is always nonnegative.

Correlation between statistical negentropy and Gibbs' free energy

Gibbs energy
) and its capacity for entropy (the amount by which the entropy of the body can be increased without changing the energy of the body or increasing its volume) respectively.

There is a physical quantity closely linked to

Massieu for the isothermal process[10][11][12] (both quantities differs just with a figure sign) and then Planck for the isothermal-isobaric process.[13] More recently, the Massieu–Planck thermodynamic potential, known also as free entropy, has been shown to play a great role in the so-called entropic formulation of statistical mechanics,[14] applied among the others in molecular biology[15] and thermodynamic non-equilibrium processes.[16]

where:
is entropy
is negentropy (Gibbs "capacity for entropy")
is the Massieu potential
is the partition function
the Boltzmann constant

In particular, mathematically the negentropy (the negative entropy function, in physics interpreted as free entropy) is the convex conjugate of LogSumExp (in physics interpreted as the free energy).

Brillouin's negentropy principle of information

In 1953, Léon Brillouin derived a general equation[17] stating that the changing of an information bit value requires at least energy. This is the same energy as the work

Leó Szilárd's engine produces in the idealistic case. In his book,[18]
Brillouin further explored this problem concluding that any cause of this bit value change (measurement, decision about a yes/no question, erasure, display, etc.) will require the same amount of energy.

See also

Notes

  1. ^ Schrödinger, Erwin, What is Life – the Physical Aspect of the Living Cell, Cambridge University Press, 1944
  2. ^ Brillouin, Leon: (1953) "Negentropy Principle of Information", J. of Applied Physics, v. 24(9), pp. 1152–1163
  3. ^ Léon Brillouin, La science et la théorie de l'information, Masson, 1959
  4. ^ Aapo Hyvärinen, Survey on Independent Component Analysis, node32: Negentropy, Helsinki University of Technology Laboratory of Computer and Information Science
  5. ^ Aapo Hyvärinen and Erkki Oja, Independent Component Analysis: A Tutorial, node14: Negentropy, Helsinki University of Technology Laboratory of Computer and Information Science
  6. ^ Ruye Wang, Independent Component Analysis, node4: Measures of Non-Gaussianity
  7. ^ P. Comon, Independent Component Analysis – a new concept?, Signal Processing, 36 287–314, 1994.
  8. ^ Didier G. Leibovici and Christian Beckmann, An introduction to Multiway Methods for Multi-Subject fMRI experiment, FMRIB Technical Report 2001, Oxford Centre for Functional Magnetic Resonance Imaging of the Brain (FMRIB), Department of Clinical Neurology, University of Oxford, John Radcliffe Hospital, Headley Way, Headington, Oxford, UK.
  9. ^ Willard Gibbs, A Method of Geometrical Representation of the Thermodynamic Properties of Substances by Means of Surfaces, Transactions of the Connecticut Academy, 382–404 (1873)
  10. ^ Massieu, M. F. (1869a). Sur les fonctions caractéristiques des divers fluides. C. R. Acad. Sci. LXIX:858–862.
  11. ^ Massieu, M. F. (1869b). Addition au precedent memoire sur les fonctions caractéristiques. C. R. Acad. Sci. LXIX:1057–1061.
  12. ^ Massieu, M. F. (1869), Compt. Rend. 69 (858): 1057.
  13. ^ Planck, M. (1945). Treatise on Thermodynamics. Dover, New York.
  14. ^ Antoni Planes, Eduard Vives, Entropic Formulation of Statistical Mechanics Archived 2008-10-11 at the Wayback Machine, Entropic variables and Massieu–Planck functions 2000-10-24 Universitat de Barcelona
  15. ^ John A. Scheilman, Temperature, Stability, and the Hydrophobic Interaction, Biophysical Journal 73 (December 1997), 2960–2964, Institute of Molecular Biology, University of Oregon, Eugene, Oregon 97403 USA
  16. ^ Z. Hens and X. de Hemptinne, Non-equilibrium Thermodynamics approach to Transport Processes in Gas Mixtures, Department of Chemistry, Catholic University of Leuven, Celestijnenlaan 200 F, B-3001 Heverlee, Belgium
  17. ^ Leon Brillouin, The negentropy principle of information, J. Applied Physics 24, 1152–1163 1953
  18. ^ Leon Brillouin, Science and Information theory, Dover, 1956