Predicting the borderline between the classical and quantum regimes in 4He gas from the second virial coefficient

Author:

Ghassib H.B.1,Sandouqa A.S.2,Joudeh B.R.34,Mosameh S.M.5

Affiliation:

1. Department of Physics, The University of Jordan, Amman, Jordan.

2. Department of Applied Sciences, Faculty of Engineering Technology, Al-Balqa’ Applied University, Amman, Jordan.

3. Applied Physics Department, Tafila Technical University, Tafila, Jordan.

4. Department of Computer Science, College of Shari’a and Islamic Studies in Al Ahsaa, Al Imam Muhammad Ibn Saud Islamic University (IMSIU), Saudi Arabia.

5. Department of Applied Sciences, Irbid University College, Al-Balqa’ Applied University, Irbid, Jordan.

Abstract

The second Virial coefficient in both classical and quantum regimes of 4He gas is investigated in the temperature range 4.2–10 K. Full quantum mechanical and classical treatments are undertaken to calculate this coefficient. The main input in computing the quantum coefficient is the “effective” phase shifts. These are determined within the framework of the Galitskii–Migdal–Feynman formalism, using two interatomic potentials. The borderline between the classical and quantum regimes is found to depend on the temperature, the number density, and the interparticle potential.

Publisher

Canadian Science Publishing

Subject

General Physics and Astronomy

Reference28 articles.

1. R.P. Feynman. Statistical Mechanics. Benjamin, Reading, MA. 1972.

2. K. Huang. Statistical Mechanics, 2nd ed. Wiley, New York. 1987.

3. A.L. Fetter and J.D. Walecka. Quantum Theory of Many-Particle Systems. McGraw-Hill, New York. 1971.

4. A study of the Galitskii-Feynman T matrix for liquid 3He

5. Composite pairs and effective two-body scattering in a many-body medium

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