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arXiv physics/9711003physics.chem-ph
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磁场中的氢分子:Pi流形的最低态和平行组态的整体基态

Hydrogen molecule in a magnetic field: The lowest states of the Pi manifold and the global ground state of the parallel configuration

T. Detmer, P. Schmelcher, L. S. Cederbaum

摘要:

研究了氢分子在平行于核间轴和磁场轴的磁场中的电子结构。$Π$流形的最低状态进行了研究自旋单重态和三重态$(M_s = -1) $以及gerade和ungerade奇偶校验的一个广泛的场强范围$0 \leq B \leq 100 a.u.$对于这两个国家与gerade奇偶校验,我们观察到一个单调下降的解离能随着场强的增加到$B = 0.1 a.u.$和亚稳态相对于解离成两个H原子发生在一定范围内的场强。对于这两个国家与ungerade宇称,我们观察到一个强烈的增加,在解离能增加的电场强度以上的一些临界场强$B_c$。作为一个主要的结果,我们确定最低的$^1Σ_g$,$^3Σ_u$和$^3Π_u$状态之间的交叉点的过渡场强度。$B \lesssim 0.18 a.u.$的整体基态是强束缚的$^1Σ_g$态。$^1Σ_g$与$^3Σ_u$和$^3Π_u$状态的交叉分别发生在$B \approx 0.18$和$B \approx0.39 a.u.$。$^3Σ_u$和$^3Π_u$态之间的跃迁发生在$B \approx 12.3 a.u.$。因此,对于$0.18 \lesssim B \lesssim 12.3 a.u.$,平行构型的氢分子的整体基态是未结合的$^3Σ_u$态。对于$B \gtrsim 12.3 a.u.$,基态是强结合的$^3Π_u$态。这一结果与磁性白矮星和中子星大气层中的化学性质有很大关系。

英文摘要:

The electronic structure of the hydrogen molecule in a magnetic field is investigated for parallel internuclear and magnetic field axes. The lowest states of the $Π$ manifold are studied for spin singlet and triplet$(M_s = -1) $ as well as gerade and ungerade parity for a broad range of field strengths $0 \leq B \leq 100 a.u.$ For both states with gerade parity we observe a monotonous decrease in the dissociation energy with increasing field strength up to $B = 0.1 a.u.$ and metastable states with respect to the dissociation into two H atoms occur for a certain range of field strengths. For both states with ungerade parity we observe a strong increase in the dissociation energy with increasing field strength above some critical field strength $B_c$. As a major result we determine the transition field strengths for the crossings among the lowest $^1Σ_g$, $^3Σ_u$ and $^3Π_u$ states. The global ground state for $B \lesssim 0.18 a.u.$ is the strongly bound $^1Σ_g$ state. The crossings of the $^1Σ_g$ with the $^3Σ_u$ and $^3Π_u$ state occur at $B \approx 0.18$ and $B \approx0.39 a.u.$, respectively. The transition between the $^3Σ_u$ and $^3Π_u$ state occurs at $B \approx 12.3 a.u.$ Therefore, the global ground state of the hydrogen molecule for the parallel configuration is the unbound $^3Σ_u$ state for $0.18 \lesssim B \lesssim 12.3 a.u.$ The ground state for $B \gtrsim 12.3 a.u.$ is the strongly bound $^3Π_u$ state. This result is of great relevance to the chemistry in the atmospheres of magnetic white dwarfs and neutron stars.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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