Chains of mini-boson stars Shi-Xian Sun1 Yong-Qiang Wang2 and Li Zhao3 aLanzhou Center for Theoretical Physics Key Laboratory of Theoretical Physics of Gansu

2025-04-30 0 0 1023.33KB 15 页 10玖币
侵权投诉
Chains of mini-boson stars
Shi-Xian Sun1, Yong-Qiang Wang2, and Li Zhao 3
aLanzhou Center for Theoretical Physics, Key Laboratory of Theoretical Physics of Gansu
Province, School of Physical Science and Technology, Lanzhou University, Lanzhou
730000, People’s Republic of China
bInstitute of Theoretical Physics &Research Center of Gravitation, Lanzhou University,
Lanzhou 730000, People’s Republic of China
Abstract
In this paper, we re-investigate the stationary, soliton-like solutions in the model of the
Einstein gravity coupled to a free and complex scalar field, which have been known as
mini-boson stars. With numerical method, we find that in addition to the usual single
mini-boson star solutions, there exist a novel family of solutions interpreted as chains
of boson stars, which is made of some boson stars along the symmetry axis. We show
the configuration of two types of chains, including an even number of constituents and
an odd number of constituents. Furthermore, we also study the effect of the frequency
of the complex scalar field on the ADM mass Mand the U(1) scalar charge Q. It
is interesting to note that the existence of chains of boson stars does not require the
introduction of a complex scalar field with self-interacting potential.
1sunshx20@lzu.edu.cn
2yqwang@lzu.edu.cn
3lizhao@lzu.edu.cn, corresponding author
arXiv:2210.09265v1 [gr-qc] 17 Oct 2022
1 Introduction
It is well known that the most general stationary solution of the vacuum Einstein equation in
a four-dimensional spacetime is described by a so-called Kerr geometry, which is a rotating
black hole only with two parameters, the black-hole mass and angular momentum. The
above uniqueness of the Kerr black hole is sometimes referred to as the “no-hair” theorem.
When considering the model of a free scalar field minimally coupled to Einstein’s gravity,
one could find that it is difficult to obtain analytical or numerical black hole solutions for
a long time. Until the last few years, a novel family of solutions of Kerr black holes with
scalar hair was presented by Herdeiro and Radu in [1]. Furthermore, when restrictions on
the stationary solution of compact object with event horizon are lifted, there exist a family
of horizonless solutions, which have become well-known as boson stars (BSs).
The study of BSs has a long history. Firstly, in the 1960s, a family of spherically
symmetric BSs were discovered by Kaup in the four-dimensional Einstein gravity coupled
to a free, complex scalar field with the constant angular frequency of the phase of the field in
the complex plane [2, 3]. Due to little astrophysical interest in directed searches for a boson
star, BSs with rotational symmetry were not studied until the 1990s. The first rotating
solutions of boson stars in the Einstein-Klein-Gordon theory were found in [4]. BSs with a
free scalar field without self-interaction were well known as mini-boson stars (BSs), which
can then be extended to the self-interacting BSs case [5], the excited case of scalar field
with nodes [6] and the multistate boson stars [7, 8]. There are also studies on the solutions
of the self-gravitating solitons in Einstein-Proca or Einstein-Dirac models [9, 10]. Another
interest of BSs in astronomy is to investigate their application to axions [11, 12], cosmic
dark matter [13, 14], and black hole mimickers [15, 16, 17]. In addition, the collisions of
binary BSs have been studied extensively [18, 19, 20, 21, 22, 23, 24], which offers a possible
way to detect the BSs with the gravitational waves generated by the merger of binary stars.
Recently, by introducing the self-interaction potential with the type of quartic and sextic
terms, which was studied in literatures on the Q-balls in the field theory, a novel family of
solutions interpreted as chains of boson stars, which is made of some boson stars along the
symmetry axis, was obtained in the Einstein-Klein-Gordon theory [25]. Such solutions can
be divided into two classes, including even chains and odd chains according to the parity
at the two sides of the equatorial plane. The obvious difference is that in the case of even-
numbered chains, the curve of the relationship between mass and frequency could form a
spiral pattern similar to the case of a single boson star, while odd-numbered star chains
can form a kind of loop pattern, which is very different from the case of a single boson
2
star. Moreover, in the second branch of odd-numbered star chains with loop patterns, the
system of star chains turn into a radially excited spherically symmetric boson star. Rotating
generalizations of chains of boson stars with the sextic potential also been studied in [26].
It is worth noting that in flat spacetime there does not exist the chain of multisoliton in
the free scalar field model. So, it will be interesting to see whether there are solutions of the
chains of mini-boson stars without the self-interaction potential in the model of free scalar
field coupled to gravity. In the present paper, we numerically solve the coupled system of
nonlinear partial differential equations of scalar field and Einstein equations, and obtain a
family of chains of mini -BSs, which can be divided into two classes, including even chains
and odd chains. Moreover, we also study the effect of the frequency of the complex scalar
field on the ADM mass and the Noether charge.
This paper is organized as follows. In Sect. 2, we briefly review the model of a free,
complex scalar field coupled to Einstein’s gravity. The boundary conditions are analyzed
in Sect. 3. We show the numerical results of two types of BSs chains in Sect. 4. The
conclusion and discussion are given in the last section. Throughout this paper, Roman
letters a,b,c, . . . denote spacetime indices ranging from 0 to 3.
Note added: when we are finishing this project, we notice that there appears a paper
[27], which overlaps with our results of chains of BSs with two constituents.
2 The Model
Let us introduce the model of Einstein gravity coupled to a free, complex massive scalar
field in four-dimensional spacetime. The Lagrangian density reads
S=Zd4xgR
16πG − ∇aψaψµ2ψψ,(2.1)
where Gand µare the Newton’s constant and the mass of the scalar field ψ, respectively.
Note that we consider mini-boson stars without self-interaction potential, and the term
proportional to µ2is known as a mass term. The above action is invariant under a global
U(1) transformation ψψe, where θis constant. Variation of the action (2.1) with
respect to the complex scalar field ψand the metric could lead to the following Klein-
Gordon (KG) equation of the scalar field
ψ=µ2ψ , (2.2)
3
摘要:

Chainsofmini-bosonstarsShi-XianSun1,Yong-QiangWang2,andLiZhao3aLanzhouCenterforTheoreticalPhysics,KeyLaboratoryofTheoreticalPhysicsofGansuProvince,SchoolofPhysicalScienceandTechnology,LanzhouUniversity,Lanzhou730000,People'sRepublicofChinabInstituteofTheoreticalPhysics&ResearchCenterofGravitation,La...

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