Loading…

Geometric phase effects in the ultracold D + HD $ \rightarrow $ D + HD and D + HD $\leftrightarrow $ H + D 2 reactions

The results of accurate quantum reactive scattering calculations for the D + HD(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $), D + HD(v = 4, j = 0) $\to $ H + D2($v^{\prime} $, $j^{\prime} $) and H + D2(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $) reactions are presented for...

Full description

Saved in:
Bibliographic Details
Published in:New journal of physics 2016-12, Vol.18 (12), p.123020
Main Authors: Kendrick, B K, Hazra, Jisha, Balakrishnan, N
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-c1153-65a426bfb7a68d780232077898cbefd3dafb074d09750606d9cc6ffcdddc76c53
cites cdi_FETCH-LOGICAL-c1153-65a426bfb7a68d780232077898cbefd3dafb074d09750606d9cc6ffcdddc76c53
container_end_page
container_issue 12
container_start_page 123020
container_title New journal of physics
container_volume 18
creator Kendrick, B K
Hazra, Jisha
Balakrishnan, N
description The results of accurate quantum reactive scattering calculations for the D + HD(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $), D + HD(v = 4, j = 0) $\to $ H + D2($v^{\prime} $, $j^{\prime} $) and H + D2(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $) reactions are presented for collision energies between $1\,\mu {\rm{K}}$ and $100\,{\rm{K}}$. The ab initio BKMP2 PES for the ground electronic state of H3 is used and all values of total angular momentum between $J=0-4$ are included. The general vector potential approach is used to include the geometric phase. The rotationally resolved, vibrationally resolved, and total reaction rate coefficients are reported as a function of collision energy. Rotationally resolved differential cross sections are also reported as a function of collision energy and scattering angle. Large geometric phase effects appear in the ultracold reaction rate coefficients which result in a significant enhancement or suppression of the rate coefficient (up to 3 orders of magnitude) relative to calculations which ignore the geometric phase. The results are interpreted using a new quantum interference mechanism which is unique to ultracold collisions. Significant effects of the geometric phase also appear in the rotationally resolved differential cross sections which lead to a very different oscillatory structure in both energy and scattering angle. Several shape resonances occur in the 1–$10\,{\rm{K}}$ energy range and the geometric phase is shown to significantly alter the predicted resonance spectrum. The geometric phase effects and ultracold rate coefficients depend sensitively on the nuclear spin. Furthermore, experimentalists may be able to control the reaction by the selection of a particular nuclear spin state.
doi_str_mv 10.1088/1367-2630/aa4fd2
format article
fullrecord <record><control><sourceid>crossref_osti_</sourceid><recordid>TN_cdi_osti_scitechconnect_1336493</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1088_1367_2630_aa4fd2</sourcerecordid><originalsourceid>FETCH-LOGICAL-c1153-65a426bfb7a68d780232077898cbefd3dafb074d09750606d9cc6ffcdddc76c53</originalsourceid><addsrcrecordid>eNpVkE1LAzEQhoMoWKt3j0G8ydp87CbZo7TaCgUveiuE7CRxV7a7JYmK_94tW_w4zcw7DwPzIHRJyS0lSs0oFzJjgpOZMbm37AhNfqLjP_0pOovxjRBKFWMT9LF0_dal0ADe1SY67Lx3kCJuOpxqh9_bFAz0rcULfINXC3yNN6F5rZMJof8cpkNsul9i0zqf_kGrYbPADAdnIDV9F8_RiTdtdBeHOkUvD_fP81W2flo-zu_WGVBa8EwUJmei8pU0QlmpCOOMSKlKBZXzllvjKyJzS0pZEEGELQGE92CtBSmg4FN0Nd7tY2p0hCY5qKHvuuFHTTkXeckHiIwQhD7G4LzehWZrwpemRO_l6r09vbenR7n8Gzm2aY0</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Geometric phase effects in the ultracold D + HD $ \rightarrow $ D + HD and D + HD $\leftrightarrow $ H + D 2 reactions</title><source>Publicly Available Content (ProQuest)</source><creator>Kendrick, B K ; Hazra, Jisha ; Balakrishnan, N</creator><creatorcontrib>Kendrick, B K ; Hazra, Jisha ; Balakrishnan, N ; Los Alamos National Lab. (LANL), Los Alamos, NM (United States)</creatorcontrib><description>The results of accurate quantum reactive scattering calculations for the D + HD(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $), D + HD(v = 4, j = 0) $\to $ H + D2($v^{\prime} $, $j^{\prime} $) and H + D2(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $) reactions are presented for collision energies between $1\,\mu {\rm{K}}$ and $100\,{\rm{K}}$. The ab initio BKMP2 PES for the ground electronic state of H3 is used and all values of total angular momentum between $J=0-4$ are included. The general vector potential approach is used to include the geometric phase. The rotationally resolved, vibrationally resolved, and total reaction rate coefficients are reported as a function of collision energy. Rotationally resolved differential cross sections are also reported as a function of collision energy and scattering angle. Large geometric phase effects appear in the ultracold reaction rate coefficients which result in a significant enhancement or suppression of the rate coefficient (up to 3 orders of magnitude) relative to calculations which ignore the geometric phase. The results are interpreted using a new quantum interference mechanism which is unique to ultracold collisions. Significant effects of the geometric phase also appear in the rotationally resolved differential cross sections which lead to a very different oscillatory structure in both energy and scattering angle. Several shape resonances occur in the 1–$10\,{\rm{K}}$ energy range and the geometric phase is shown to significantly alter the predicted resonance spectrum. The geometric phase effects and ultracold rate coefficients depend sensitively on the nuclear spin. Furthermore, experimentalists may be able to control the reaction by the selection of a particular nuclear spin state.</description><identifier>ISSN: 1367-2630</identifier><identifier>EISSN: 1367-2630</identifier><identifier>DOI: 10.1088/1367-2630/aa4fd2</identifier><language>eng</language><publisher>United Kingdom: IOP Publishing</publisher><subject>ATOMIC AND MOLECULAR PHYSICS ; Inorganic and Physical Chemistry ; Ultracold chemistry, cold molecules, geometric phase</subject><ispartof>New journal of physics, 2016-12, Vol.18 (12), p.123020</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1153-65a426bfb7a68d780232077898cbefd3dafb074d09750606d9cc6ffcdddc76c53</citedby><cites>FETCH-LOGICAL-c1153-65a426bfb7a68d780232077898cbefd3dafb074d09750606d9cc6ffcdddc76c53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/1336493$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Kendrick, B K</creatorcontrib><creatorcontrib>Hazra, Jisha</creatorcontrib><creatorcontrib>Balakrishnan, N</creatorcontrib><creatorcontrib>Los Alamos National Lab. (LANL), Los Alamos, NM (United States)</creatorcontrib><title>Geometric phase effects in the ultracold D + HD $ \rightarrow $ D + HD and D + HD $\leftrightarrow $ H + D 2 reactions</title><title>New journal of physics</title><description>The results of accurate quantum reactive scattering calculations for the D + HD(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $), D + HD(v = 4, j = 0) $\to $ H + D2($v^{\prime} $, $j^{\prime} $) and H + D2(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $) reactions are presented for collision energies between $1\,\mu {\rm{K}}$ and $100\,{\rm{K}}$. The ab initio BKMP2 PES for the ground electronic state of H3 is used and all values of total angular momentum between $J=0-4$ are included. The general vector potential approach is used to include the geometric phase. The rotationally resolved, vibrationally resolved, and total reaction rate coefficients are reported as a function of collision energy. Rotationally resolved differential cross sections are also reported as a function of collision energy and scattering angle. Large geometric phase effects appear in the ultracold reaction rate coefficients which result in a significant enhancement or suppression of the rate coefficient (up to 3 orders of magnitude) relative to calculations which ignore the geometric phase. The results are interpreted using a new quantum interference mechanism which is unique to ultracold collisions. Significant effects of the geometric phase also appear in the rotationally resolved differential cross sections which lead to a very different oscillatory structure in both energy and scattering angle. Several shape resonances occur in the 1–$10\,{\rm{K}}$ energy range and the geometric phase is shown to significantly alter the predicted resonance spectrum. The geometric phase effects and ultracold rate coefficients depend sensitively on the nuclear spin. Furthermore, experimentalists may be able to control the reaction by the selection of a particular nuclear spin state.</description><subject>ATOMIC AND MOLECULAR PHYSICS</subject><subject>Inorganic and Physical Chemistry</subject><subject>Ultracold chemistry, cold molecules, geometric phase</subject><issn>1367-2630</issn><issn>1367-2630</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNpVkE1LAzEQhoMoWKt3j0G8ydp87CbZo7TaCgUveiuE7CRxV7a7JYmK_94tW_w4zcw7DwPzIHRJyS0lSs0oFzJjgpOZMbm37AhNfqLjP_0pOovxjRBKFWMT9LF0_dal0ADe1SY67Lx3kCJuOpxqh9_bFAz0rcULfINXC3yNN6F5rZMJof8cpkNsul9i0zqf_kGrYbPADAdnIDV9F8_RiTdtdBeHOkUvD_fP81W2flo-zu_WGVBa8EwUJmei8pU0QlmpCOOMSKlKBZXzllvjKyJzS0pZEEGELQGE92CtBSmg4FN0Nd7tY2p0hCY5qKHvuuFHTTkXeckHiIwQhD7G4LzehWZrwpemRO_l6r09vbenR7n8Gzm2aY0</recordid><startdate>20161215</startdate><enddate>20161215</enddate><creator>Kendrick, B K</creator><creator>Hazra, Jisha</creator><creator>Balakrishnan, N</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>20161215</creationdate><title>Geometric phase effects in the ultracold D + HD $ \rightarrow $ D + HD and D + HD $\leftrightarrow $ H + D 2 reactions</title><author>Kendrick, B K ; Hazra, Jisha ; Balakrishnan, N</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1153-65a426bfb7a68d780232077898cbefd3dafb074d09750606d9cc6ffcdddc76c53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>ATOMIC AND MOLECULAR PHYSICS</topic><topic>Inorganic and Physical Chemistry</topic><topic>Ultracold chemistry, cold molecules, geometric phase</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kendrick, B K</creatorcontrib><creatorcontrib>Hazra, Jisha</creatorcontrib><creatorcontrib>Balakrishnan, N</creatorcontrib><creatorcontrib>Los Alamos National Lab. (LANL), Los Alamos, NM (United States)</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>New journal of physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kendrick, B K</au><au>Hazra, Jisha</au><au>Balakrishnan, N</au><aucorp>Los Alamos National Lab. (LANL), Los Alamos, NM (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Geometric phase effects in the ultracold D + HD $ \rightarrow $ D + HD and D + HD $\leftrightarrow $ H + D 2 reactions</atitle><jtitle>New journal of physics</jtitle><date>2016-12-15</date><risdate>2016</risdate><volume>18</volume><issue>12</issue><spage>123020</spage><pages>123020-</pages><issn>1367-2630</issn><eissn>1367-2630</eissn><abstract>The results of accurate quantum reactive scattering calculations for the D + HD(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $), D + HD(v = 4, j = 0) $\to $ H + D2($v^{\prime} $, $j^{\prime} $) and H + D2(v = 4, j = 0) $\to $ D + HD($v^{\prime} $, $j^{\prime} $) reactions are presented for collision energies between $1\,\mu {\rm{K}}$ and $100\,{\rm{K}}$. The ab initio BKMP2 PES for the ground electronic state of H3 is used and all values of total angular momentum between $J=0-4$ are included. The general vector potential approach is used to include the geometric phase. The rotationally resolved, vibrationally resolved, and total reaction rate coefficients are reported as a function of collision energy. Rotationally resolved differential cross sections are also reported as a function of collision energy and scattering angle. Large geometric phase effects appear in the ultracold reaction rate coefficients which result in a significant enhancement or suppression of the rate coefficient (up to 3 orders of magnitude) relative to calculations which ignore the geometric phase. The results are interpreted using a new quantum interference mechanism which is unique to ultracold collisions. Significant effects of the geometric phase also appear in the rotationally resolved differential cross sections which lead to a very different oscillatory structure in both energy and scattering angle. Several shape resonances occur in the 1–$10\,{\rm{K}}$ energy range and the geometric phase is shown to significantly alter the predicted resonance spectrum. The geometric phase effects and ultracold rate coefficients depend sensitively on the nuclear spin. Furthermore, experimentalists may be able to control the reaction by the selection of a particular nuclear spin state.</abstract><cop>United Kingdom</cop><pub>IOP Publishing</pub><doi>10.1088/1367-2630/aa4fd2</doi></addata></record>
fulltext fulltext
identifier ISSN: 1367-2630
ispartof New journal of physics, 2016-12, Vol.18 (12), p.123020
issn 1367-2630
1367-2630
language eng
recordid cdi_osti_scitechconnect_1336493
source Publicly Available Content (ProQuest)
subjects ATOMIC AND MOLECULAR PHYSICS
Inorganic and Physical Chemistry
Ultracold chemistry, cold molecules, geometric phase
title Geometric phase effects in the ultracold D + HD $ \rightarrow $ D + HD and D + HD $\leftrightarrow $ H + D 2 reactions
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-29T01%3A00%3A19IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-crossref_osti_&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Geometric%20phase%20effects%20in%20the%20ultracold%20D%20+%20HD%20$%20%5Crightarrow%20$%20D%20+%20HD%20and%20D%20+%20HD%20$%5Cleftrightarrow%20$%20H%20+%20D%202%20reactions&rft.jtitle=New%20journal%20of%20physics&rft.au=Kendrick,%20B%20K&rft.aucorp=Los%20Alamos%20National%20Lab.%20(LANL),%20Los%20Alamos,%20NM%20(United%20States)&rft.date=2016-12-15&rft.volume=18&rft.issue=12&rft.spage=123020&rft.pages=123020-&rft.issn=1367-2630&rft.eissn=1367-2630&rft_id=info:doi/10.1088/1367-2630/aa4fd2&rft_dat=%3Ccrossref_osti_%3E10_1088_1367_2630_aa4fd2%3C/crossref_osti_%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c1153-65a426bfb7a68d780232077898cbefd3dafb074d09750606d9cc6ffcdddc76c53%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true