Loading…
Helium atom embedded in non‐ideal classical plasmas: Doubly excited singlet S states
The influence of the non‐ideality (NI) of the classical plasmas on the doubly excited singlet S states of the helium atom (He) embedded in the plasma has been investigated theoretically. A pseudopotential containing the Debye length and the non‐ideality parameter (NIP) as its characteristics is used...
Saved in:
Published in: | Contributions to plasma physics (1988) 2024-05, Vol.64 (4), p.n/a |
---|---|
Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | cdi_FETCH-LOGICAL-c3172-644938f5e748377a71f2766f0dfb1eb02d23b85c1e3c5e534688a296112c4f673 |
---|---|
cites | cdi_FETCH-LOGICAL-c3172-644938f5e748377a71f2766f0dfb1eb02d23b85c1e3c5e534688a296112c4f673 |
container_end_page | n/a |
container_issue | 4 |
container_start_page | |
container_title | Contributions to plasma physics (1988) |
container_volume | 64 |
creator | Das, Netai Ghoshal, Arijit Ho, Yew Kam |
description | The influence of the non‐ideality (NI) of the classical plasmas on the doubly excited singlet S states of the helium atom (He) embedded in the plasma has been investigated theoretically. A pseudopotential containing the Debye length and the non‐ideality parameter (NIP) as its characteristics is used to represent the screened interaction potentials in the plasma. Using a large wavefunction within the framework of the stabilization method, it has been possible to recognize six doubly excited singlet S states (five lying below the He+(2S) excitation threshold and one lying below the He+(3S) excitation threshold) for the plasma‐free case. The energies and the autoionization life‐times of those states are computed by fitting the density of states to the Lorentzian form. Convergence of the computed results is corroborated by increasing the number of terms in the employed wavefunction. For the plasma‐free case, these results are in excellent agreement with the established results in the literature. A comprehensive analysis has been made on changes induced on those doubly excited states by varying NI over a wide range. It has been observed that the energies of the states gradually approach the corresponding threshold energies with the increasing NI of the plasma, whereas the change in the life‐times (alternatively the widths of the states) of the states shows distinctive features depending on the angular momentum of an individual electron. |
doi_str_mv | 10.1002/ctpp.202300112 |
format | article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_3055403556</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>3055403556</sourcerecordid><originalsourceid>FETCH-LOGICAL-c3172-644938f5e748377a71f2766f0dfb1eb02d23b85c1e3c5e534688a296112c4f673</originalsourceid><addsrcrecordid>eNqFkMtKw0AUhgdRsFa3rgdcp565JnEn9VKhoGB1O0wmJzIlNzMJ2p2P4DP6JKZUdOnq_Iv_O4fzEXLKYMYA-Lnr23bGgQsAxvgemTDFWSTSRO-TCSRaRAwkPyRHIawBINWSTcjzAks_VNT2TUWxyjDPMae-pnVTf318-hxtSV1pQ_BuTO2YKhsu6FUzZOWG4rvz_QgEX7-U2NNHGnrbYzgmB4UtA578zCl5urlezRfR8v72bn65jJxgMY-0lKlICoWxTEQc25gVPNa6gLzIGGbAcy6yRDmGwilUQuoksTzV439OFjoWU3K229t2zeuAoTfrZujq8aQRoJQEoZQeW7Ndy3VNCB0Wpu18ZbuNYWC27szWnfl1NwLpDnjzJW7-aZv56uHhj_0GwoFy4Q</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>3055403556</pqid></control><display><type>article</type><title>Helium atom embedded in non‐ideal classical plasmas: Doubly excited singlet S states</title><source>Wiley-Blackwell Read & Publish Collection</source><creator>Das, Netai ; Ghoshal, Arijit ; Ho, Yew Kam</creator><creatorcontrib>Das, Netai ; Ghoshal, Arijit ; Ho, Yew Kam</creatorcontrib><description>The influence of the non‐ideality (NI) of the classical plasmas on the doubly excited singlet S states of the helium atom (He) embedded in the plasma has been investigated theoretically. A pseudopotential containing the Debye length and the non‐ideality parameter (NIP) as its characteristics is used to represent the screened interaction potentials in the plasma. Using a large wavefunction within the framework of the stabilization method, it has been possible to recognize six doubly excited singlet S states (five lying below the He+(2S) excitation threshold and one lying below the He+(3S) excitation threshold) for the plasma‐free case. The energies and the autoionization life‐times of those states are computed by fitting the density of states to the Lorentzian form. Convergence of the computed results is corroborated by increasing the number of terms in the employed wavefunction. For the plasma‐free case, these results are in excellent agreement with the established results in the literature. A comprehensive analysis has been made on changes induced on those doubly excited states by varying NI over a wide range. It has been observed that the energies of the states gradually approach the corresponding threshold energies with the increasing NI of the plasma, whereas the change in the life‐times (alternatively the widths of the states) of the states shows distinctive features depending on the angular momentum of an individual electron.</description><identifier>ISSN: 0863-1042</identifier><identifier>EISSN: 1521-3986</identifier><identifier>DOI: 10.1002/ctpp.202300112</identifier><language>eng</language><publisher>Weinheim: WILEY‐VCH Verlag GmbH & Co. KGaA</publisher><subject>Angular momentum ; Autoionization ; Computation ; Debye length ; doubly excited states ; Excitation ; Helium ; helium atom ; Helium atoms ; non‐ideal plasma ; Plasma ; Plasmas (physics) ; resonance ; stabilization method ; Wave functions</subject><ispartof>Contributions to plasma physics (1988), 2024-05, Vol.64 (4), p.n/a</ispartof><rights>2024 Wiley‐VCH GmbH.</rights><rights>2024 Wiley‐VCH GmbH</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3172-644938f5e748377a71f2766f0dfb1eb02d23b85c1e3c5e534688a296112c4f673</citedby><cites>FETCH-LOGICAL-c3172-644938f5e748377a71f2766f0dfb1eb02d23b85c1e3c5e534688a296112c4f673</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids></links><search><creatorcontrib>Das, Netai</creatorcontrib><creatorcontrib>Ghoshal, Arijit</creatorcontrib><creatorcontrib>Ho, Yew Kam</creatorcontrib><title>Helium atom embedded in non‐ideal classical plasmas: Doubly excited singlet S states</title><title>Contributions to plasma physics (1988)</title><description>The influence of the non‐ideality (NI) of the classical plasmas on the doubly excited singlet S states of the helium atom (He) embedded in the plasma has been investigated theoretically. A pseudopotential containing the Debye length and the non‐ideality parameter (NIP) as its characteristics is used to represent the screened interaction potentials in the plasma. Using a large wavefunction within the framework of the stabilization method, it has been possible to recognize six doubly excited singlet S states (five lying below the He+(2S) excitation threshold and one lying below the He+(3S) excitation threshold) for the plasma‐free case. The energies and the autoionization life‐times of those states are computed by fitting the density of states to the Lorentzian form. Convergence of the computed results is corroborated by increasing the number of terms in the employed wavefunction. For the plasma‐free case, these results are in excellent agreement with the established results in the literature. A comprehensive analysis has been made on changes induced on those doubly excited states by varying NI over a wide range. It has been observed that the energies of the states gradually approach the corresponding threshold energies with the increasing NI of the plasma, whereas the change in the life‐times (alternatively the widths of the states) of the states shows distinctive features depending on the angular momentum of an individual electron.</description><subject>Angular momentum</subject><subject>Autoionization</subject><subject>Computation</subject><subject>Debye length</subject><subject>doubly excited states</subject><subject>Excitation</subject><subject>Helium</subject><subject>helium atom</subject><subject>Helium atoms</subject><subject>non‐ideal plasma</subject><subject>Plasma</subject><subject>Plasmas (physics)</subject><subject>resonance</subject><subject>stabilization method</subject><subject>Wave functions</subject><issn>0863-1042</issn><issn>1521-3986</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNqFkMtKw0AUhgdRsFa3rgdcp565JnEn9VKhoGB1O0wmJzIlNzMJ2p2P4DP6JKZUdOnq_Iv_O4fzEXLKYMYA-Lnr23bGgQsAxvgemTDFWSTSRO-TCSRaRAwkPyRHIawBINWSTcjzAks_VNT2TUWxyjDPMae-pnVTf318-hxtSV1pQ_BuTO2YKhsu6FUzZOWG4rvz_QgEX7-U2NNHGnrbYzgmB4UtA578zCl5urlezRfR8v72bn65jJxgMY-0lKlICoWxTEQc25gVPNa6gLzIGGbAcy6yRDmGwilUQuoksTzV439OFjoWU3K229t2zeuAoTfrZujq8aQRoJQEoZQeW7Ndy3VNCB0Wpu18ZbuNYWC27szWnfl1NwLpDnjzJW7-aZv56uHhj_0GwoFy4Q</recordid><startdate>202405</startdate><enddate>202405</enddate><creator>Das, Netai</creator><creator>Ghoshal, Arijit</creator><creator>Ho, Yew Kam</creator><general>WILEY‐VCH Verlag GmbH & Co. KGaA</general><general>Wiley Subscription Services, Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>202405</creationdate><title>Helium atom embedded in non‐ideal classical plasmas: Doubly excited singlet S states</title><author>Das, Netai ; Ghoshal, Arijit ; Ho, Yew Kam</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3172-644938f5e748377a71f2766f0dfb1eb02d23b85c1e3c5e534688a296112c4f673</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Angular momentum</topic><topic>Autoionization</topic><topic>Computation</topic><topic>Debye length</topic><topic>doubly excited states</topic><topic>Excitation</topic><topic>Helium</topic><topic>helium atom</topic><topic>Helium atoms</topic><topic>non‐ideal plasma</topic><topic>Plasma</topic><topic>Plasmas (physics)</topic><topic>resonance</topic><topic>stabilization method</topic><topic>Wave functions</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Das, Netai</creatorcontrib><creatorcontrib>Ghoshal, Arijit</creatorcontrib><creatorcontrib>Ho, Yew Kam</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Contributions to plasma physics (1988)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Das, Netai</au><au>Ghoshal, Arijit</au><au>Ho, Yew Kam</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Helium atom embedded in non‐ideal classical plasmas: Doubly excited singlet S states</atitle><jtitle>Contributions to plasma physics (1988)</jtitle><date>2024-05</date><risdate>2024</risdate><volume>64</volume><issue>4</issue><epage>n/a</epage><issn>0863-1042</issn><eissn>1521-3986</eissn><abstract>The influence of the non‐ideality (NI) of the classical plasmas on the doubly excited singlet S states of the helium atom (He) embedded in the plasma has been investigated theoretically. A pseudopotential containing the Debye length and the non‐ideality parameter (NIP) as its characteristics is used to represent the screened interaction potentials in the plasma. Using a large wavefunction within the framework of the stabilization method, it has been possible to recognize six doubly excited singlet S states (five lying below the He+(2S) excitation threshold and one lying below the He+(3S) excitation threshold) for the plasma‐free case. The energies and the autoionization life‐times of those states are computed by fitting the density of states to the Lorentzian form. Convergence of the computed results is corroborated by increasing the number of terms in the employed wavefunction. For the plasma‐free case, these results are in excellent agreement with the established results in the literature. A comprehensive analysis has been made on changes induced on those doubly excited states by varying NI over a wide range. It has been observed that the energies of the states gradually approach the corresponding threshold energies with the increasing NI of the plasma, whereas the change in the life‐times (alternatively the widths of the states) of the states shows distinctive features depending on the angular momentum of an individual electron.</abstract><cop>Weinheim</cop><pub>WILEY‐VCH Verlag GmbH & Co. KGaA</pub><doi>10.1002/ctpp.202300112</doi><tpages>10</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0863-1042 |
ispartof | Contributions to plasma physics (1988), 2024-05, Vol.64 (4), p.n/a |
issn | 0863-1042 1521-3986 |
language | eng |
recordid | cdi_proquest_journals_3055403556 |
source | Wiley-Blackwell Read & Publish Collection |
subjects | Angular momentum Autoionization Computation Debye length doubly excited states Excitation Helium helium atom Helium atoms non‐ideal plasma Plasma Plasmas (physics) resonance stabilization method Wave functions |
title | Helium atom embedded in non‐ideal classical plasmas: Doubly excited singlet S states |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-03T02%3A58%3A19IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Helium%20atom%20embedded%20in%20non%E2%80%90ideal%20classical%20plasmas:%20Doubly%20excited%20singlet%20S%20states&rft.jtitle=Contributions%20to%20plasma%20physics%20(1988)&rft.au=Das,%20Netai&rft.date=2024-05&rft.volume=64&rft.issue=4&rft.epage=n/a&rft.issn=0863-1042&rft.eissn=1521-3986&rft_id=info:doi/10.1002/ctpp.202300112&rft_dat=%3Cproquest_cross%3E3055403556%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c3172-644938f5e748377a71f2766f0dfb1eb02d23b85c1e3c5e534688a296112c4f673%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=3055403556&rft_id=info:pmid/&rfr_iscdi=true |