Abstract
We apply the technique of Gaussian regularization to the grand canonical pressure partition function to show that under physically meaningful boundary conditions (non-existence of external confining vessels, i.e., no fixed volumes) the energy density and similar intensive quantities have, in a statistical bootstrap model of extended hadrons (Van der Waals type volume corrections), indeed the singularity claimed in previous papers. Earlier results obtained with an entirely different technique (which had been criticized) are recovered and shown to be correct. The technique used here is useful in all cases where the volume is not imposed from the outside, but results from the internal dynamics of the system as is generally the case in high energy physics and astrophysics.
Similar content being viewed by others
References
J. Baacke: Acta Phys. Pol.B8, 625 (1977)
This fact has been known already to cosmic ray physicists and has been stated in so many papers that it is impossible to list them all. Let two more recent ones represent the whole lot:
A.T. Laasanen et al.: Phys. Rev. Lett.38, 1 (1977)
G.W. Van Appeldoorn, et al.: Z. Phys. C—Particles and Fields,7, 235 (1981)
We do not consider here Monte Carlo lattice calculations which indeed may cover both sides and do suggest a phase transition, but which cannot exhibit singularities in the strict sense. See, e.g., J. Engels, F. Karsch, I. Montvay, H. Satz: Phys. Lett.102B, 332 (1981) and references therein
R. Hagedorn, J. Rafelski: Phys. Lett.97B, 136 (1980)
R. Hagedorn, J. Rafelski: From hadron gas to quark matter I. In: Statistical mechanics of quarks and hadrons, H. Satz (Ed.), Amsterdam: North Holland 1981
N. Cabibbo, G. Parisi: Phys. Lett.59B, 67 (1974)
J.I. Kapusta: Nucl. Phys.B148, 461 (1979);
O.K. Kalashnikov, V.V. Klimov: Phys. Lett.88B, 328 (1979);
J. Kuti, J. Polonyi, K. Szalachani: Phys. Lett.98B, 199 (1981);
J. Rafelski, R. Hagedorn: From hadron gas to quark matter II. In: H. Satz (Ed.)loc. cit.
S.A. Chin: Phys. Lett.78B, 552 (1978).
E. Shuryak: Phys. Rep.61, 71 (1980).
V.V. Dixit, F. Karsch, H. Satz: Phys. Lett.101B, 412 (1981)
E.A. Guggenheim: J. Chem. Phys.7, 103 (1939)
I. Prigogine: Physica16, 133 (1950)
A. Münster Statistical thermodynamics, Chap. 3.1, 3.2, Berlin, Heidelberg, New York: Springer 1969
A. Münster:loc. cit
A. Chodos et al.: Phys. Rev.D9, 3471 (1974)
B. Touschek: Nuovo CimentoB58, 295 (1968)
R. Hagedorn, I. Montvay, J. Rafelski: In: Hadronic matter at extreme energy density, N. Cabibbo, L. Sertorio (Eds.) New York: Plenum Press 1980
R. Hagedorn, J. Rafelski: Commun. Math. Phys.83, 563–578 (1982).
M.I. Gorenstein, V.K. Petrov, G.M. Zinovjev: Phys. Lett.106B, 327 (1981)
J. Kapusta: Nucl. Phys.B196, 1 (1982)
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Hagedorn, R. The pressure ensemble as a tool for describing the hadron-quark phase transition. Z. Phys. C - Particles and Fields 17, 265–281 (1983). https://doi.org/10.1007/BF01578153
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01578153