S. Mondal, A. N. Sil, S. Dutta, S. Nandi, T. K. Mukhopadhyay, J. K. Saha
{"title":"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","authors":"S. Mondal, A. N. Sil, S. Dutta, S. Nandi, T. K. Mukhopadhyay, J. K. 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. 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 <i>w.r.t.</i> the plasma screening length.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 10","pages":""},"PeriodicalIF":1.3000,"publicationDate":"2024-08-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Bound and resonance states of highly charged H- and He-like ions under weakly coupled plasma environment\",\"authors\":\"S. Mondal, A. N. Sil, S. Dutta, S. Nandi, T. K. Mukhopadhyay, J. K. 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. 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 <i>w.r.t.</i> the plasma screening length.</p>\",\"PeriodicalId\":10700,\"journal\":{\"name\":\"Contributions to Plasma Physics\",\"volume\":\"64 10\",\"pages\":\"\"},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2024-08-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Contributions to Plasma Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/ctpp.202400041\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, FLUIDS & PLASMAS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Contributions to Plasma Physics","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/ctpp.202400041","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
Bound and resonance states of highly charged H- and He-like ions under weakly coupled plasma environment
The position of bound () states as well as doubly excited resonance , () states of symmetry has been determined for highly charged He-like ions (, , , , , and Ar16+) along with their respective one-electron thresholds (, , and ) 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.