Thirumalai Anand
Department of Physics, DigiPen Institute of Technology, 9931 Willows Road NE, Redmond, Washington, 98052, United States.
J Phys Chem A. 2025 Mar 6;129(9):2161-2172. doi: 10.1021/acs.jpca.4c07546. Epub 2025 Feb 25.
In addition to harboring intense global magnetic fields, neutron stars also have outer envelopes that are subjected to high pressures. The outermost layer of a neutron star's envelope consists of a thin atmosphere, which in turn sits atop an ocean layer of condensed matter. The pressure at the topmost layer of the ocean is generally estimated to be around ≳ 10 GPa. The envelope is thought to be dynamic, with mixing between the layers, and this investigation seeks to delineate the energy landscape of neutral atoms from the atmosphere, which can get trapped inside denser surrounding material of the ocean layer below during mixing. The high-pressure environment is modeled as a quantum confined model by means of a spherical cavity using a piecewise potential () and a confining radius (). A range of pressures and magnetic field strengths ( T) are considered, and the two most astrophysically relevant atoms (hydrogen and helium) are studied herein, and, to the best of the author's knowledge, this is the first study to investigate the combination of the two effects in neutron star atmospheres. The energies of the first few low-lying states of each of hydrogen and helium atoms are computed (at the Hartree-Fock level of the theory for the latter), and the findings indicate that the binding energies of the states are considerably altered in such an environment. At the pressures relevant to the ocean layer ( ≳ 10 GPa), it was found that the negative parity states of both hydrogen and helium do not survive as the energy shift introduced by the confinement is large enough to render them unbound. The positive parity states of these atoms do, however, survive at such pressures (albeit with somewhat lesser binding energies, for the case of helium) in neutron star envelopes. At lower pressures ∼ 10 GPa, representing material in the lower reaches of the atmosphere though not at ocean layer depths, the energy landscape is still found to be appreciably altered for both the positive and the negative parity states of hydrogen and helium. Higher in the atmosphere, the energy shifts were found to diminish to negligible amounts for pressures relevant to the photosphere of the neutron star ( ∼ 10 GPa). Overall, the study reveals that incorporating the effect of high pressure is important when studying the structure of atoms in the intense magnetic fields present in neutron star envelopes, as significant shifts in the computed energies will have bearing on any subsequent computations of oscillator strengths, transition wavelengths, as well as calculations of relative abundance of atoms and ions in atmosphere models. Thus, the results are relevant to understanding the spectra of neutron stars.
除了拥有极强的全球磁场外,中子星还有承受高压的外层。中子星外层的最外层由一层稀薄的大气组成,而这层大气又位于一层凝聚态物质的海洋之上。通常估计海洋最顶层的压力约为≳10吉帕斯卡。人们认为外层是动态的,各层之间存在混合,本研究旨在描绘来自大气的中性原子的能量图景,这些原子在混合过程中可能被困在下方海洋层密度更大的周围物质中。通过使用分段势()和限制半径()的球形腔,将高压环境建模为量子限制模型。考虑了一系列压力和磁场强度(特斯拉),并在此研究了两种在天体物理学中最相关的原子(氢和氦),据作者所知,这是第一项研究中子星大气中这两种效应组合的研究。计算了氢和氦原子各自的前几个低能态的能量(对于后者,在理论的哈特里 - 福克水平上),研究结果表明,在这样的环境中,这些态的结合能会发生相当大的变化。在与海洋层相关的压力(≳10吉帕斯卡)下,发现氢和氦的负宇称态都无法存在,因为限制引入的能量位移足够大,使其变为非束缚态。然而,在中子星外层中,这些原子的正宇称态在这样的压力下确实存在(尽管对于氦来说,结合能稍小一些)。在较低压力(∼10吉帕斯卡)下,代表大气下游但并非海洋层深度的物质,氢和氦的正宇称态和负宇称态的能量图景仍然被发现有明显改变。在大气较高处,对于与中子星光球相关的压力(∼10吉帕斯卡),能量位移被发现减小到可以忽略不计的程度。总体而言,该研究表明,在研究中子星外层存在的强磁场中原子的结构时,纳入高压效应很重要,因为计算出的能量的显著位移将对随后任何关于振子强度、跃迁波长的计算以及大气模型中原子和离子相对丰度的计算产生影响。因此,这些结果与理解中子星的光谱相关。