Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence
Yields of atomic iodine I q+ ( q ≥ 2) fragments resulting from photoexcitation and photoionisation of the target cations CH x I + ( x = 0–3) have been measured in the photon-energy range 610 eV to 670 eV, which comprises the threshold for iodine 3d ionisation. The measured ion-yield spectra show two...
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creator | Schubert, Kaja Guda, Alexander A. Mertens, Karolin Schunck, Jan O. Schippers, Stefan Müller, Alfred Bari, Sadia Klumpp, Stephan Martins, Michael |
description | Yields of atomic iodine I
q+
(
q
≥ 2) fragments resulting from photoexcitation and photoionisation of the target cations CH
x
I
+
(
x
= 0–3) have been measured in the photon-energy range 610 eV to 670 eV, which comprises the threshold for iodine 3d ionisation. The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d
3/2,5/2
electrons into
ε
f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH
3
I
+
resembles the spectrum of IH
+
[Klumpp
et al.
,
Phys. Rev. A
, 2018,
97
, 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH
3
fragments both contain a single vacancy, only. For the molecular cations with higher number of vacancies in the valence molecular orbitals CH
x
I
+
(
x
= 0–2), a stronger hybridisation of the molecular orbitals occurs between the organic fragment and the iodine resulting in a change of bonding from a single σ bond in CH
3
I
+
to a triple bond including two π orbitals in CI
+
. This is reflected in the resonance energies of the observed absorption lines below the iodine 3d excitation threshold. |
doi_str_mv | 10.1039/C9CP04640B |
format | Article |
fullrecord | <record><control><sourceid>crossref</sourceid><recordid>TN_cdi_crossref_primary_10_1039_C9CP04640B</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1039_C9CP04640B</sourcerecordid><originalsourceid>FETCH-LOGICAL-c76B-139509160b20d53ce47d7afb24b13786a9451e5d27e6a41dbfb4054a742ba9c33</originalsourceid><addsrcrecordid>eNpFkLtOwzAYhS0EEqWw8AQeuSjwO77VA0MbAa1UCYbukW8hQSEOdhCw8Q68IU9CaRFM5xu-c4aD0DGBCwJUXRaquAcmGMx20IgwQTMFE7b7x1Lso4OUHgGAcEJHqJ2aFGI_NKHDqfd2iBrrAQ-1x01wTecxdWvqmqQ3zlBHn-rQOlyFtg2vTfewkYs5fsMLfI5P1nmF4evjk55iuy0l__ziO-sP0V6l2-SPfnOMVjfXq2KeLe9uF8V0mVkpZhmhioMiAkwOjlPrmXRSVyZnhlA5EVoxTjx3ufRCM-JMZRhwpiXLjVaW0jE6287aGFKKvir72Dzp-F4SKH9uKv9vot_taFl0</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence</title><source>Royal Society Of Chemistry Journals</source><source>Alma/SFX Local Collection</source><creator>Schubert, Kaja ; Guda, Alexander A. ; Mertens, Karolin ; Schunck, Jan O. ; Schippers, Stefan ; Müller, Alfred ; Bari, Sadia ; Klumpp, Stephan ; Martins, Michael</creator><creatorcontrib>Schubert, Kaja ; Guda, Alexander A. ; Mertens, Karolin ; Schunck, Jan O. ; Schippers, Stefan ; Müller, Alfred ; Bari, Sadia ; Klumpp, Stephan ; Martins, Michael</creatorcontrib><description>Yields of atomic iodine I
q+
(
q
≥ 2) fragments resulting from photoexcitation and photoionisation of the target cations CH
x
I
+
(
x
= 0–3) have been measured in the photon-energy range 610 eV to 670 eV, which comprises the threshold for iodine 3d ionisation. The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d
3/2,5/2
electrons into
ε
f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH
3
I
+
resembles the spectrum of IH
+
[Klumpp
et al.
,
Phys. Rev. A
, 2018,
97
, 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH
3
fragments both contain a single vacancy, only. For the molecular cations with higher number of vacancies in the valence molecular orbitals CH
x
I
+
(
x
= 0–2), a stronger hybridisation of the molecular orbitals occurs between the organic fragment and the iodine resulting in a change of bonding from a single σ bond in CH
3
I
+
to a triple bond including two π orbitals in CI
+
. This is reflected in the resonance energies of the observed absorption lines below the iodine 3d excitation threshold.</description><identifier>ISSN: 1463-9076</identifier><identifier>EISSN: 1463-9084</identifier><identifier>DOI: 10.1039/C9CP04640B</identifier><language>eng</language><ispartof>Physical chemistry chemical physics : PCCP, 2019-11, Vol.21 (45), p.25415-25424</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c76B-139509160b20d53ce47d7afb24b13786a9451e5d27e6a41dbfb4054a742ba9c33</citedby><cites>FETCH-LOGICAL-c76B-139509160b20d53ce47d7afb24b13786a9451e5d27e6a41dbfb4054a742ba9c33</cites><orcidid>0000-0002-0146-6318 ; 0000-0002-3222-8195 ; 0000-0003-3945-191X ; 0000-0003-3985-2051 ; 0000-0002-6941-4987 ; 0000-0002-6166-7138 ; 0000-0002-0030-6929 ; 0000-0002-1228-5029</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Schubert, Kaja</creatorcontrib><creatorcontrib>Guda, Alexander A.</creatorcontrib><creatorcontrib>Mertens, Karolin</creatorcontrib><creatorcontrib>Schunck, Jan O.</creatorcontrib><creatorcontrib>Schippers, Stefan</creatorcontrib><creatorcontrib>Müller, Alfred</creatorcontrib><creatorcontrib>Bari, Sadia</creatorcontrib><creatorcontrib>Klumpp, Stephan</creatorcontrib><creatorcontrib>Martins, Michael</creatorcontrib><title>Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence</title><title>Physical chemistry chemical physics : PCCP</title><description>Yields of atomic iodine I
q+
(
q
≥ 2) fragments resulting from photoexcitation and photoionisation of the target cations CH
x
I
+
(
x
= 0–3) have been measured in the photon-energy range 610 eV to 670 eV, which comprises the threshold for iodine 3d ionisation. The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d
3/2,5/2
electrons into
ε
f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH
3
I
+
resembles the spectrum of IH
+
[Klumpp
et al.
,
Phys. Rev. A
, 2018,
97
, 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH
3
fragments both contain a single vacancy, only. For the molecular cations with higher number of vacancies in the valence molecular orbitals CH
x
I
+
(
x
= 0–2), a stronger hybridisation of the molecular orbitals occurs between the organic fragment and the iodine resulting in a change of bonding from a single σ bond in CH
3
I
+
to a triple bond including two π orbitals in CI
+
. This is reflected in the resonance energies of the observed absorption lines below the iodine 3d excitation threshold.</description><issn>1463-9076</issn><issn>1463-9084</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNpFkLtOwzAYhS0EEqWw8AQeuSjwO77VA0MbAa1UCYbukW8hQSEOdhCw8Q68IU9CaRFM5xu-c4aD0DGBCwJUXRaquAcmGMx20IgwQTMFE7b7x1Lso4OUHgGAcEJHqJ2aFGI_NKHDqfd2iBrrAQ-1x01wTecxdWvqmqQ3zlBHn-rQOlyFtg2vTfewkYs5fsMLfI5P1nmF4evjk55iuy0l__ziO-sP0V6l2-SPfnOMVjfXq2KeLe9uF8V0mVkpZhmhioMiAkwOjlPrmXRSVyZnhlA5EVoxTjx3ufRCM-JMZRhwpiXLjVaW0jE6287aGFKKvir72Dzp-F4SKH9uKv9vot_taFl0</recordid><startdate>20191120</startdate><enddate>20191120</enddate><creator>Schubert, Kaja</creator><creator>Guda, Alexander A.</creator><creator>Mertens, Karolin</creator><creator>Schunck, Jan O.</creator><creator>Schippers, Stefan</creator><creator>Müller, Alfred</creator><creator>Bari, Sadia</creator><creator>Klumpp, Stephan</creator><creator>Martins, Michael</creator><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-0146-6318</orcidid><orcidid>https://orcid.org/0000-0002-3222-8195</orcidid><orcidid>https://orcid.org/0000-0003-3945-191X</orcidid><orcidid>https://orcid.org/0000-0003-3985-2051</orcidid><orcidid>https://orcid.org/0000-0002-6941-4987</orcidid><orcidid>https://orcid.org/0000-0002-6166-7138</orcidid><orcidid>https://orcid.org/0000-0002-0030-6929</orcidid><orcidid>https://orcid.org/0000-0002-1228-5029</orcidid></search><sort><creationdate>20191120</creationdate><title>Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence</title><author>Schubert, Kaja ; Guda, Alexander A. ; Mertens, Karolin ; Schunck, Jan O. ; Schippers, Stefan ; Müller, Alfred ; Bari, Sadia ; Klumpp, Stephan ; Martins, Michael</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c76B-139509160b20d53ce47d7afb24b13786a9451e5d27e6a41dbfb4054a742ba9c33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schubert, Kaja</creatorcontrib><creatorcontrib>Guda, Alexander A.</creatorcontrib><creatorcontrib>Mertens, Karolin</creatorcontrib><creatorcontrib>Schunck, Jan O.</creatorcontrib><creatorcontrib>Schippers, Stefan</creatorcontrib><creatorcontrib>Müller, Alfred</creatorcontrib><creatorcontrib>Bari, Sadia</creatorcontrib><creatorcontrib>Klumpp, Stephan</creatorcontrib><creatorcontrib>Martins, Michael</creatorcontrib><collection>CrossRef</collection><jtitle>Physical chemistry chemical physics : PCCP</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schubert, Kaja</au><au>Guda, Alexander A.</au><au>Mertens, Karolin</au><au>Schunck, Jan O.</au><au>Schippers, Stefan</au><au>Müller, Alfred</au><au>Bari, Sadia</au><au>Klumpp, Stephan</au><au>Martins, Michael</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence</atitle><jtitle>Physical chemistry chemical physics : PCCP</jtitle><date>2019-11-20</date><risdate>2019</risdate><volume>21</volume><issue>45</issue><spage>25415</spage><epage>25424</epage><pages>25415-25424</pages><issn>1463-9076</issn><eissn>1463-9084</eissn><abstract>Yields of atomic iodine I
q+
(
q
≥ 2) fragments resulting from photoexcitation and photoionisation of the target cations CH
x
I
+
(
x
= 0–3) have been measured in the photon-energy range 610 eV to 670 eV, which comprises the threshold for iodine 3d ionisation. The measured ion-yield spectra show two strong and broad resonance features due to the excitation of the 3d
3/2,5/2
electrons into
ε
f states similar to atomic iodine. In the 3d pre-edge range, electrons are excited into molecular orbitals consisting of iodine, carbon, and hydrogen atomic orbitals. These transitions have been identified by comparison with literature data and by simulations using time-dependent density functional theory (TDDFT) with the KMLYP functional. The ion-yield spectrum for CH
3
I
+
resembles the spectrum of IH
+
[Klumpp
et al.
,
Phys. Rev. A
, 2018,
97
, 033401] because the highest occupied molecular orbitals (HOMO) of the H and CH
3
fragments both contain a single vacancy, only. For the molecular cations with higher number of vacancies in the valence molecular orbitals CH
x
I
+
(
x
= 0–2), a stronger hybridisation of the molecular orbitals occurs between the organic fragment and the iodine resulting in a change of bonding from a single σ bond in CH
3
I
+
to a triple bond including two π orbitals in CI
+
. This is reflected in the resonance energies of the observed absorption lines below the iodine 3d excitation threshold.</abstract><doi>10.1039/C9CP04640B</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0002-0146-6318</orcidid><orcidid>https://orcid.org/0000-0002-3222-8195</orcidid><orcidid>https://orcid.org/0000-0003-3945-191X</orcidid><orcidid>https://orcid.org/0000-0003-3985-2051</orcidid><orcidid>https://orcid.org/0000-0002-6941-4987</orcidid><orcidid>https://orcid.org/0000-0002-6166-7138</orcidid><orcidid>https://orcid.org/0000-0002-0030-6929</orcidid><orcidid>https://orcid.org/0000-0002-1228-5029</orcidid></addata></record> |
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source | Royal Society Of Chemistry Journals; Alma/SFX Local Collection |
title | Absorption spectra at the iodine 3d ionisation threshold following the CH x I + ( x = 0–3) cation sequence |
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