The quantum second virial coefficient of 3He at low density in the temperature range 0.005-10 K

被引:7
|
作者
Al-Obeidat, O. T. [1 ]
Sandouqa, A. S. [1 ]
Joudeh, B. R. [2 ,3 ]
Ghassib, H. B. [4 ]
Hawamdeh, M. M. [1 ]
机构
[1] Al Balqa Appl Univ, Fac Engn Technol, Dept Phys & Basic Sci, Amman, Jordan
[2] Tafila Tech Univ, Fac Sci, Appl Phys Dept, Tafila, Jordan
[3] Al Imam Muhammad Ibn Saud Islamic Univ IMSIU, Coll Sharia & Islamic StudiesAl Ahsaa, Dept Comp Sci, Riyadh, Saudi Arabia
[4] Univ Jordan, Fac Sci, Dept Phys, Amman, Jordan
关键词
quantum second virial coefficient; Galitskii-Migdal-Feynman formalism; compressibility; equation of state; saturated vapor; EQUATION-OF-STATE; THERMOPHYSICAL PROPERTIES; SCATTERING PROPERTIES; T-MATRIX; GAS; LIQUID-HE-3; HELIUM; VALUES; ENERGY;
D O I
10.1139/cjp-2016-0907
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The quantum second virial coefficient B-q for He-3 is calculated from first principles at low density in the temperature range 0.005-10 K. By "first principles", it is meant that the many-body phase shifts are first determined within the Galitskii-Migdal-Feynman formalism; they are then plugged into the Beth-Uhlenbeck formula for B-q. A positive B-q corresponds to an overall repulsive interaction; a negative B-q represents an overall attractive interaction. The s-wave scattering length a(o) is calculated quite accurately as a function of the temperature T. The effect of the (low-density) medium on B-q is studied. B-q is then used to determine the volume of He-3 at the saturation curve. The compressibility is evaluated as a measure of the non-ideality of the system.
引用
收藏
页码:1208 / 1214
页数:7
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