Volume 345, Issue 2-3 e240012
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Dirac spinor scattering states with positive-energy in rotating spheroid models

Zhi-Fu Gao

Zhi-Fu Gao

Xinjiang Astronomical Observatory, CAS, Urumqi, Xinjiang, China

Xinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal University, Yining, Xinjiang, China

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Ci-Xing Chen

Ci-Xing Chen

Department of Astronomy, University of Sciences and Technology of China, CAS, Hefei, Anhui, China

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Na Wang

Na Wang

Xinjiang Astronomical Observatory, CAS, Urumqi, Xinjiang, China

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Xin-Jun Zhao

Corresponding Author

Xin-Jun Zhao

Xinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal University, Yining, Xinjiang, China

Correspondence

Xin-Jun Zhao, Xinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal University, Yining, Xinjiang 83500, China.

Email: [email protected]

Zhao-Jun Wang, Xinjiang University of Science and Technology, Korla, Xinjiang 841000, China.

Email: [email protected]

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Zhao-Jun Wang

Corresponding Author

Zhao-Jun Wang

Xinjiang University of Science and Technology, Korla, Xinjiang, China

Correspondence

Xin-Jun Zhao, Xinjiang Laboratory of Phase Transitions and Microstructures in Condensed Matters, College of Physical Science and Technology, Yili Normal University, Yining, Xinjiang 83500, China.

Email: [email protected]

Zhao-Jun Wang, Xinjiang University of Science and Technology, Korla, Xinjiang 841000, China.

Email: [email protected]

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First published: 17 February 2024
Citations: 5

Abstract

There are many rotating spheroids in the universe, and many astronomers and physicists have used theoretical methods to study the characteristics of stellar gravity since Newton's time. This paper derives the solutions of eight scattering states ( ϕ ( 0 ) , χ ( 0 ) , ϕ ( 1 ) , χ ( 1 ) , ϕ ( 2 ) $$ \Big({\phi}^{(0)},{\chi}^{(0)},{\phi}^{(1)},{\chi}^{(1)},{\phi}^{(2)} $$ , χ ( 2 ) , ϕ ( 3 ) $$ {\chi}^{(2)},{\phi}^{(3)} $$ , and χ ( 3 ) ) $$ {\chi}^{(3)}\Big) $$ for the Dirac equation with positive-energy E = im $$ E= im $$ , and establishes the relationship between the differential scattering cross section σ i ( p , θ , φ ) $$ {\sigma}_i\left(p,\theta, \varphi \right) $$ and the stellar density μ $$ \mu $$ . It is found that: (1) For the eight scattering states, their average scattering cross-sections σ i $$ \overline{\sigma_i} $$ are proportional to μ 2 $$ {\mu}^2 $$ , and depend on the star's radius, and the higher the stellar density μ $$ \mu $$ , the greater the sensitivity of σ i $$ \overline{\sigma i} $$ to the change of μ $$ \mu $$ ; (2) For the four scattering states χ ( i ) , i = 0 , 1 , 2 , 3 $$ {\chi}^{(i)},i=0,1,2,3 $$ , their average scattering amplitudes f ( p , θ ) $$ \overline{f}\left(p,\theta \right) $$ and σ ( p , θ ) $$ \overline{\sigma}\left(p,\theta \right) $$ depend on the mass m $$ m $$ of the particles; while for the other four scattering states ϕ ( i ) $$ {\phi}^{(i)} $$ , i = 0 , 1 , 2 , 3 $$ i=0,1,2,3 $$ , then f $$ \overline{f} $$ and σ $$ \overline{\sigma} $$ are independent of m $$ m $$ . This study links the gravitational characteristics of stars with the scattering cross section, creating a new method for studying the gravitational characteristics, which helps to reveal the mystery of the gravity of rotating ellipsoidal stars.

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