弱耦合等离子体环境下高电荷氢离子和类氢离子的束缚态和共振态

IF 1.3 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS
S. Mondal, A. N. Sil, S. Dutta, S. Nandi, T. K. Mukhopadhyay, J. K. Saha
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Saha","doi":"10.1002/ctpp.202400041","DOIUrl":null,"url":null,"abstract":"<p>The position of bound <span></span><math>\n <semantics>\n <mrow>\n <mn>1</mn>\n <mi>sns</mi>\n </mrow>\n <annotation>$$ 1 sns $$</annotation>\n </semantics></math> (<span></span><math>\n <semantics>\n <mrow>\n <mi>n</mi>\n <mo>=</mo>\n <mn>1</mn>\n <mo>−</mo>\n <mn>5</mn>\n </mrow>\n <annotation>$$ n=1-5 $$</annotation>\n </semantics></math>) states as well as doubly excited resonance <span></span><math>\n <semantics>\n <mrow>\n <mn>2</mn>\n <mi>sns</mi>\n </mrow>\n <annotation>$$ 2 sns $$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <mn>2</mn>\n <mi>pnp</mi>\n </mrow>\n <annotation>$$ 2 pnp $$</annotation>\n </semantics></math> (<span></span><math>\n <semantics>\n <mrow>\n <mi>n</mi>\n <mo>=</mo>\n <mn>2</mn>\n <mo>−</mo>\n <mn>3</mn>\n </mrow>\n <annotation>$$ n=2-3 $$</annotation>\n </semantics></math>) states of <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mo> </mo>\n <mn>1</mn>\n </msup>\n <msup>\n <mi>S</mi>\n <mi>e</mi>\n </msup>\n </mrow>\n <annotation>$$ {}^1{\\mathrm{S}}^e $$</annotation>\n </semantics></math> symmetry has been determined for highly charged He-like ions (<span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mi>C</mi>\n <mrow>\n <mn>4</mn>\n <mo>+</mo>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathrm{C}}^{4+} $$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mi>Mg</mi>\n <mrow>\n <mn>10</mn>\n <mo>+</mo>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathrm{Mg}}^{10+} $$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mi>Al</mi>\n <mrow>\n <mn>11</mn>\n <mo>+</mo>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathrm{Al}}^{11+} $$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mi>Si</mi>\n <mrow>\n <mn>12</mn>\n <mo>+</mo>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathrm{Si}}^{12+} $$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mi>S</mi>\n <mrow>\n <mn>14</mn>\n <mo>+</mo>\n </mrow>\n </msup>\n </mrow>\n <annotation>$$ {\\mathrm{S}}^{14+} $$</annotation>\n </semantics></math>, and Ar<sup>16+</sup>) along with their respective one-electron thresholds (<span></span><math>\n <semantics>\n <mrow>\n <mn>1</mn>\n <mi>s</mi>\n </mrow>\n <annotation>$$ 1s $$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <mn>2</mn>\n <mi>s</mi>\n </mrow>\n <annotation>$$ 2s $$</annotation>\n </semantics></math>, and <span></span><math>\n <semantics>\n <mrow>\n <mn>2</mn>\n <mi>p</mi>\n </mrow>\n <annotation>$$ 2p $$</annotation>\n </semantics></math>) under weakly coupled plasma environment. 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引用次数: 0

摘要

在弱耦合等离子体环境下,测定了高电荷类氦离子(、、、、和Ar16+)的束缚()态和双激发共振对称态()的位置及其各自的单电子阈值(、、和)。之所以选择这些特定离子及其各自的电荷状态,是因为它们经常出现在天体物理和实验室等离子体中。在处理氦离子和类氦离子时,分别采用了具有多分量明确相关的海勒拉斯(Hylleraas)类型基础和纯指数基础集的里兹变分法。在不同等离子体条件下,采用稳定法测定了几个低洼共振态的共振宽度。等离子体嵌入离子的束缚态和共振态的电离电位都有所降低。很明显,来自不同主导构型的共振态的宽度(或寿命)随等离子体屏蔽长度的变化而变化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Bound and resonance states of highly charged H- and He-like ions under weakly coupled plasma environment

The position of bound 1 sns $$ 1 sns $$ ( n = 1 5 $$ n=1-5 $$ ) states as well as doubly excited resonance 2 sns $$ 2 sns $$ , 2 pnp $$ 2 pnp $$ ( n = 2 3 $$ n=2-3 $$ ) states of 1 S e $$ {}^1{\mathrm{S}}^e $$ symmetry has been determined for highly charged He-like ions ( C 4 + $$ {\mathrm{C}}^{4+} $$ , Mg 10 + $$ {\mathrm{Mg}}^{10+} $$ , Al 11 + $$ {\mathrm{Al}}^{11+} $$ , Si 12 + $$ {\mathrm{Si}}^{12+} $$ , S 14 + $$ {\mathrm{S}}^{14+} $$ , and Ar16+) along with their respective one-electron thresholds ( 1 s $$ 1s $$ , 2 s $$ 2s $$ , and 2 p $$ 2p $$ ) under weakly coupled plasma environment. These particular ions and their respective charge states are selected due to their frequent occurrence in astrophysical and laboratory plasmas. Ritz variational method with multi-exponent explicitly correlated Hylleraas type basis and pure-exponential basis set are adopted for tackling He- and H-like ions, respectively. The resonance width of a few low-lying resonance states is determined using the stabilization method under different plasma conditions. Ionization potential depression is noted for both the bound and resonance states of the plasma-embedded ions. It is evident that the width (or the lifetime) of the considered resonance states originating from different dominant configurations follows different patterns w.r.t. the plasma screening length.

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来源期刊
Contributions to Plasma Physics
Contributions to Plasma Physics 物理-物理:流体与等离子体
CiteScore
2.90
自引率
12.50%
发文量
110
审稿时长
4-8 weeks
期刊介绍: Aims and Scope of Contributions to Plasma Physics: Basic physics of low-temperature plasmas; Strongly correlated non-ideal plasmas; Dusty Plasmas; Plasma discharges - microplasmas, reactive, and atmospheric pressure plasmas; Plasma diagnostics; Plasma-surface interaction; Plasma technology; Plasma medicine.
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