Non-extensive self-consistent thermodynamical theory

In experimental physics, researchers have proposed non-extensive self-consistent thermodynamic theory to describe phenomena observed in the Large Hadron Collider (LHC). This theory investigates a fireball for high-energy particle collisions, while using Tsallis non-extensive thermodynamics. Fireballs lead to the bootstrap idea, or self-consistency principle, just as in the Boltzmann statistics used by Rolf Hagedorn. Assuming the distribution function gets variations, due to possible symmetrical change, Abdel Nasser Tawfik applied the non-extensive concepts of high-energy particle production.

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enIn experimental physics, researchers have proposed non-extensive self-consistent thermodynamic theory to describe phenomena observed in the Large Hadron Collider (LHC). This theory investigates a fireball for high-energy particle collisions, while using Tsallis non-extensive thermodynamics. Fireballs lead to the bootstrap idea, or self-consistency principle, just as in the Boltzmann statistics used by Rolf Hagedorn. Assuming the distribution function gets variations, due to possible symmetrical change, Abdel Nasser Tawfik applied the non-extensive concepts of high-energy particle production.
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enIn experimental physics, researchers have proposed non-extensive self-consistent thermodynamic theory to describe phenomena observed in the Large Hadron Collider (LHC). This theory investigates a fireball for high-energy particle collisions, while using Tsallis non-extensive thermodynamics. Fireballs lead to the bootstrap idea, or self-consistency principle, just as in the Boltzmann statistics used by Rolf Hagedorn. Assuming the distribution function gets variations, due to possible symmetrical change, Abdel Nasser Tawfik applied the non-extensive concepts of high-energy particle production. The motivation to use the non-extensive statistics from Tsallis comes from the results obtained by Bediaga et al. They showed that with the substitution of the Boltzmann factor in Hagedorn's theory by the q-exponential function, it was possible to recover good agreement between calculation and experiment, even at energies as high as those achieved at the LHC, with q>1.
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Non-extensive self-consistent thermodynamical theory
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enNon-extensive self-consistent thermodynamical theory
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Abdel Nasser Tawfik
Boltzmann statistics
Bosons
Category:Experimental particle physics
Category:Nuclear physics
Category:Principles
Density of states
Distribution function (physics)
Entropy
Experimental physics
Fermions
Fireball concept
High-energy particle
High energy physics
Jean Cleymans
Large Hadron Collider
LHC
Mass spectrum
Partition function (statistical mechanics)
Rolf Hagedorn
Self-consistency principle in high energy physics
Thermofractals
Tsallis entropy
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Non-extensive self-consistent thermodynamical theory
Q17104959
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Category:Experimental particle physics
Category:Nuclear physics
Category:Principles
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