J.M. Isidro

Dr. J.M. Isidro

Universidad Politécnica de Valencia
orcid

Research Focus & Metrics

Academic Career Length

35Years (1992-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 June 2009 in Geothermics
Verified
Journal Article
Closed access
TBTatyana V. Bandos
Tatyana V. Bandos
ÁMÁlvaro Montero
Álvaro Montero
EFEsther Fernández
Esther Fernández
JGJuan Luis González-Santander
Juan Luis González-Santander
JIJ.M. Isidro
J.M. Isidro
Javier UrchueguíaJavier Urchueguía
Javier Urchueguía

1 June 1993 in Nuclear Physics B
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Journal Article
Closed access
JIJ.M. Isidro
J.M. Isidro
JLJ.M.F. Labastida
J.M.F. Labastida
ARA.V. Ramallo
A.V. Ramallo

3 July 2012 in International Journal of Geometric Methods in Modern Physics
Verified
Journal Article
Closed access
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DAD. Acosta
D. Acosta
Pedro Fernández de Córdoba CastelláPedro Fernández de Córdoba Castellá
Pedro Fernández de Córdoba Castellá
JIJ.M. Isidro
J.M. Isidro
JGJuan Luis González-Santander
Juan Luis González-Santander

6 March 2013 in International Journal of Geometric Methods in Modern Physics
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Journal Article
Open access
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DAD. Acosta
D. Acosta
Pedro Fernández de Córdoba CastelláPedro Fernández de Córdoba Castellá
Pedro Fernández de Córdoba Castellá
JIJ.M. Isidro
J.M. Isidro
JGJuan Luis González-Santander
Juan Luis González-Santander
We present an explicit correspondence between quantum mechanics and the classical theory of irreversible thermodynamics as developed by Onsager, Prigogine et al. Our correspondence maps irreversible Gaussian Markov processes into the semiclassical approximation of quantum mechanics. Quantum-mechanical propagators are mapped into thermodynamical probability distributions. The Feynman path integral also arises naturally in this setup. The fact that quantum mechanics can be translated into thermodynamical language provides additional support for the conjecture that quantum mechanics is not a fundamental theory but rather an emergent phenomenon, i.e. an effective description of some underlying degrees of freedom.

1 May 1997 in Nuclear Physics B
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Journal Article
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JIJ.M. Isidro
J.M. Isidro
AMAvijit Mukherjee
Avijit Mukherjee
JNJoão P. Nunes
João P. Nunes
HSHoward J. Schnitzer
Howard J. Schnitzer

16 April 2004 in Physical Review D
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IBIgor A. Bandos
Igor A. Bandos
JIJ.M. Isidro
J.M. Isidro
We elaborate a full superfield description of the interacting system of dynamical D=4, N=1 supergravity and a dynamical superstring. As far as a minimal formulation of simple supergravity is used, such a system should contain as well the tensor (real linear) multiplet which describes the dilaton and the two-superform gauge field whose pullback provides the Wess-Zumino term for the superstring. The superfield action is given by the sum of the Wess-Zumino action for D=4, N=1 superfield supergravity, the superfield action for the tensor multiplet in curved superspace, and the Green-Schwarz superstring action. The latter includes the coupling to the tensor multiplet both in the Nambu-Goto and in the Wess-Zumino terms. We derive superfield equations of motion including, besides the superfield supergravity equations with the source, the source-full superfield equations for the linear multiplet. The superstring equations keep the same form as for the superstring in supergravity and 2-superform background. The analysis of gauge symmetries shows that the superfield description of the interacting system is gauge equivalent to the dynamical system described by the sum of the spacetime, component action for supergravity interacting with the tensor multiplet, and of the purely bosonic string action.