Using Relativistic Quantum Geometry we study back-reaction effects of space-time inside the causal horizon of a static de Sitter metric, in order to make a quantum thermodynamical description of space-time. We found a finite number of discrete energy levels for a scalar field from a polynomial condition of the confluent hypergeometric functions expanded around $$r=0$$. As in the previous work, we obtain that the uncertainty principle is valid for each energy level on sub-horizon scales of space-time. We found that temperature and entropy are dependent on the number of sub-states on each energy’s level and the Bekenstein–Hawking temperature of each energy level is recovered when the number of sub-states of a given level tends to infinity. We...
We consider the quantum birth of a hot FRW universe from a vacuum-dominated quantum fluctuation with...
The notions of temperature, entropy and 'evaporation', usually associated with spacetimes with horiz...
It is suggested that the Planck h = m(sub k)c Lambda(sub k) and the Boltzmann k = m(sub k)c nu(sub k...
Using Relativistic Quantum Geometry we study back-reaction effects of space-time inside the causal h...
A general formalism for understanding the thermodynamics of horizons in spherically symmetric spacet...
We study space-time back-reaction configuration in the interior of a Schwarzschild Black-Hole (B-H) ...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
International audienceWe go forward in completing the Standard Model of the Universe back in time wi...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
The idea of Thermodynamical Einstein's Dream sounds that spacetime geometry is an effect of quantum ...
International audienceWe go forward in completing the Standard Model of the Universe back in time wi...
We consider the quantum birth of a hot FRW universe from a vacuum-dominated quantum fluctuation with...
We consider the quantum birth of a hot FRW universe from a vacuum-dominated quantum fluctuation with...
The notions of temperature, entropy and 'evaporation', usually associated with spacetimes with horiz...
It is suggested that the Planck h = m(sub k)c Lambda(sub k) and the Boltzmann k = m(sub k)c nu(sub k...
Using Relativistic Quantum Geometry we study back-reaction effects of space-time inside the causal h...
A general formalism for understanding the thermodynamics of horizons in spherically symmetric spacet...
We study space-time back-reaction configuration in the interior of a Schwarzschild Black-Hole (B-H) ...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
International audienceWe go forward in completing the Standard Model of the Universe back in time wi...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
We investigate the thermodynamical properties of quantum fields in curved spacetime. Our approach is...
The idea of Thermodynamical Einstein's Dream sounds that spacetime geometry is an effect of quantum ...
International audienceWe go forward in completing the Standard Model of the Universe back in time wi...
We consider the quantum birth of a hot FRW universe from a vacuum-dominated quantum fluctuation with...
We consider the quantum birth of a hot FRW universe from a vacuum-dominated quantum fluctuation with...
The notions of temperature, entropy and 'evaporation', usually associated with spacetimes with horiz...
It is suggested that the Planck h = m(sub k)c Lambda(sub k) and the Boltzmann k = m(sub k)c nu(sub k...