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The effect of counter ions on the far-infrared spectra of tris(triphenylphosphinegold)oxonium dimer saltsElectronic supplementary information (ESI) available: Containing a comparison between the crystallographic and DFT-optimized Au6O2 core, optimized structures for the [[(Ph3PAu)3O]BF4]2 and [[(Ph3PAu)3O]MnO4]2 species, and a comparison between the theoretical spectra for the [(PPh3Au)3O]− and ([(PPh3Au)3O]−)2 species. See DOI: 10.1039/c5ra11599j
Two tris(triphenylphosphinegold)oxonium dimer salts [{{Au(PPh 3 )} 3 (μ 3 −O)} 2 ] 2+ (X − ) 2 (X = BF − 4 , MnO − 4 ) were investigated via synchrotron-based far-infrared vibrational spectroscopy and density functional theory modelled at the M06/LANL2DZ level of theory. The 50-800 cm −1 region of b...
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creator | Bennett, Trystan Falcinella, Alexander J White, Reuben J Adnan, Rohul H Golovko, Vladimir Andersson, Gunther G Metha, Gregory F |
description | Two tris(triphenylphosphinegold)oxonium dimer salts [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(X
−
)
2
(X = BF
−
4
, MnO
−
4
) were investigated
via
synchrotron-based far-infrared vibrational spectroscopy and density functional theory modelled at the M06/LANL2DZ level of theory. The 50-800 cm
−1
region of both oxonium salts is presented, with the spectrum for [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
found to possess a large feature at 330.3 cm
−1
, attributable to counter-ion vibrational modes, which is only predicted upon explicit inclusion of counter-ions in the calculation. A feature around 107 cm
−1
observed for the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
infrared spectrum is assigned to 21 distinct vibrational modes arising from Au-Au bond stretching and other motions of the Au core. The same feature is predicted to be present within the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
spectrum but is masked by experimental noise. In the 50-400 cm
−1
region, the relative intensities of predicted vibrational modes is found to depend heavily on the presence and nature of the counter-ions, while within the 400-800 cm
−1
region, little dependence of the theoretical spectra on the type of counter-ion is predicted. Finally, the dimerization energies of both [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
and [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
are calculated to be 3.06 eV and 3.20 eV, respectively, when the counter-ions are explicitly included within the calculation, and just 1.10 eV in their absence.
The far-infrared spectra of two tris(triphenylphosphinegold)oxonium dimer salts in the 50-800 cm
−1
region were recorded using synchrotron-based IR radiation, and comprehensively assigned utilising density functional theory calculations. |
doi_str_mv | 10.1039/c5ra11599j |
format | article |
fullrecord | <record><control><sourceid>rsc</sourceid><recordid>TN_cdi_rsc_primary_c5ra11599j</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>c5ra11599j</sourcerecordid><originalsourceid>FETCH-rsc_primary_c5ra11599j3</originalsourceid><addsrcrecordid>eNqFUU1rGzEQ3RYCDU0uuRemtzXEzn7YC84tTWziQ7AhvoVgJtpZr4xWEpI2ifsLeu6f6v_IL8nYCQ5taSOQBt68ee8xiqKjNOmlST48EQOHaToYDlcfo_0s6RfdLCmGn6JD71cJn2KQZkW6_-HXvCagqiIRwFQgTKsDOZBGezAaAncrdF2pK4eOSvCWmQ433OCkj_mxNem1srXxtpaalkaVHfNotGwbKGXDah5V8CO1mWRYgG-tVdSQDujWwNrGNRjYE-LR9aQDeI9S4Z2iUzg3TJJa6iUgp2sssisT7yg8EL0EFG7tAypllg45ggDUJVyM511jg2zkd4591hbTjOcdHcMb6oNrRWgdeeAIW62bm3hW57OztpNPb7-N-7fZVu03-EpPN_hmFZL88Zbwz3B82TVIgWq3vJ1ZPGPVF9GnHz-3QvEfYGdn1INrIriYTk7h718-iPYqVJ4OX-vn6Mt4ND-_7DovFtbJhje9eKPn7_e__q-_sGWVPwPmhM7q</addsrcrecordid><sourcetype>Enrichment Source</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>The effect of counter ions on the far-infrared spectra of tris(triphenylphosphinegold)oxonium dimer saltsElectronic supplementary information (ESI) available: Containing a comparison between the crystallographic and DFT-optimized Au6O2 core, optimized structures for the [[(Ph3PAu)3O]BF4]2 and [[(Ph3PAu)3O]MnO4]2 species, and a comparison between the theoretical spectra for the [(PPh3Au)3O]− and ([(PPh3Au)3O]−)2 species. See DOI: 10.1039/c5ra11599j</title><source>Royal Society of Chemistry</source><creator>Bennett, Trystan ; Falcinella, Alexander J ; White, Reuben J ; Adnan, Rohul H ; Golovko, Vladimir ; Andersson, Gunther G ; Metha, Gregory F</creator><creatorcontrib>Bennett, Trystan ; Falcinella, Alexander J ; White, Reuben J ; Adnan, Rohul H ; Golovko, Vladimir ; Andersson, Gunther G ; Metha, Gregory F</creatorcontrib><description>Two tris(triphenylphosphinegold)oxonium dimer salts [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(X
−
)
2
(X = BF
−
4
, MnO
−
4
) were investigated
via
synchrotron-based far-infrared vibrational spectroscopy and density functional theory modelled at the M06/LANL2DZ level of theory. The 50-800 cm
−1
region of both oxonium salts is presented, with the spectrum for [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
found to possess a large feature at 330.3 cm
−1
, attributable to counter-ion vibrational modes, which is only predicted upon explicit inclusion of counter-ions in the calculation. A feature around 107 cm
−1
observed for the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
infrared spectrum is assigned to 21 distinct vibrational modes arising from Au-Au bond stretching and other motions of the Au core. The same feature is predicted to be present within the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
spectrum but is masked by experimental noise. In the 50-400 cm
−1
region, the relative intensities of predicted vibrational modes is found to depend heavily on the presence and nature of the counter-ions, while within the 400-800 cm
−1
region, little dependence of the theoretical spectra on the type of counter-ion is predicted. Finally, the dimerization energies of both [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
and [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
are calculated to be 3.06 eV and 3.20 eV, respectively, when the counter-ions are explicitly included within the calculation, and just 1.10 eV in their absence.
The far-infrared spectra of two tris(triphenylphosphinegold)oxonium dimer salts in the 50-800 cm
−1
region were recorded using synchrotron-based IR radiation, and comprehensively assigned utilising density functional theory calculations.</description><identifier>EISSN: 2046-2069</identifier><identifier>DOI: 10.1039/c5ra11599j</identifier><language>eng</language><creationdate>2015-09</creationdate><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Bennett, Trystan</creatorcontrib><creatorcontrib>Falcinella, Alexander J</creatorcontrib><creatorcontrib>White, Reuben J</creatorcontrib><creatorcontrib>Adnan, Rohul H</creatorcontrib><creatorcontrib>Golovko, Vladimir</creatorcontrib><creatorcontrib>Andersson, Gunther G</creatorcontrib><creatorcontrib>Metha, Gregory F</creatorcontrib><title>The effect of counter ions on the far-infrared spectra of tris(triphenylphosphinegold)oxonium dimer saltsElectronic supplementary information (ESI) available: Containing a comparison between the crystallographic and DFT-optimized Au6O2 core, optimized structures for the [[(Ph3PAu)3O]BF4]2 and [[(Ph3PAu)3O]MnO4]2 species, and a comparison between the theoretical spectra for the [(PPh3Au)3O]− and ([(PPh3Au)3O]−)2 species. See DOI: 10.1039/c5ra11599j</title><description>Two tris(triphenylphosphinegold)oxonium dimer salts [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(X
−
)
2
(X = BF
−
4
, MnO
−
4
) were investigated
via
synchrotron-based far-infrared vibrational spectroscopy and density functional theory modelled at the M06/LANL2DZ level of theory. The 50-800 cm
−1
region of both oxonium salts is presented, with the spectrum for [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
found to possess a large feature at 330.3 cm
−1
, attributable to counter-ion vibrational modes, which is only predicted upon explicit inclusion of counter-ions in the calculation. A feature around 107 cm
−1
observed for the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
infrared spectrum is assigned to 21 distinct vibrational modes arising from Au-Au bond stretching and other motions of the Au core. The same feature is predicted to be present within the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
spectrum but is masked by experimental noise. In the 50-400 cm
−1
region, the relative intensities of predicted vibrational modes is found to depend heavily on the presence and nature of the counter-ions, while within the 400-800 cm
−1
region, little dependence of the theoretical spectra on the type of counter-ion is predicted. Finally, the dimerization energies of both [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
and [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
are calculated to be 3.06 eV and 3.20 eV, respectively, when the counter-ions are explicitly included within the calculation, and just 1.10 eV in their absence.
The far-infrared spectra of two tris(triphenylphosphinegold)oxonium dimer salts in the 50-800 cm
−1
region were recorded using synchrotron-based IR radiation, and comprehensively assigned utilising density functional theory calculations.</description><issn>2046-2069</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNqFUU1rGzEQ3RYCDU0uuRemtzXEzn7YC84tTWziQ7AhvoVgJtpZr4xWEpI2ifsLeu6f6v_IL8nYCQ5taSOQBt68ee8xiqKjNOmlST48EQOHaToYDlcfo_0s6RfdLCmGn6JD71cJn2KQZkW6_-HXvCagqiIRwFQgTKsDOZBGezAaAncrdF2pK4eOSvCWmQ433OCkj_mxNem1srXxtpaalkaVHfNotGwbKGXDah5V8CO1mWRYgG-tVdSQDujWwNrGNRjYE-LR9aQDeI9S4Z2iUzg3TJJa6iUgp2sssisT7yg8EL0EFG7tAypllg45ggDUJVyM511jg2zkd4591hbTjOcdHcMb6oNrRWgdeeAIW62bm3hW57OztpNPb7-N-7fZVu03-EpPN_hmFZL88Zbwz3B82TVIgWq3vJ1ZPGPVF9GnHz-3QvEfYGdn1INrIriYTk7h718-iPYqVJ4OX-vn6Mt4ND-_7DovFtbJhje9eKPn7_e__q-_sGWVPwPmhM7q</recordid><startdate>20150902</startdate><enddate>20150902</enddate><creator>Bennett, Trystan</creator><creator>Falcinella, Alexander J</creator><creator>White, Reuben J</creator><creator>Adnan, Rohul H</creator><creator>Golovko, Vladimir</creator><creator>Andersson, Gunther G</creator><creator>Metha, Gregory F</creator><scope/></search><sort><creationdate>20150902</creationdate><title>The effect of counter ions on the far-infrared spectra of tris(triphenylphosphinegold)oxonium dimer saltsElectronic supplementary information (ESI) available: Containing a comparison between the crystallographic and DFT-optimized Au6O2 core, optimized structures for the [[(Ph3PAu)3O]BF4]2 and [[(Ph3PAu)3O]MnO4]2 species, and a comparison between the theoretical spectra for the [(PPh3Au)3O]− and ([(PPh3Au)3O]−)2 species. See DOI: 10.1039/c5ra11599j</title><author>Bennett, Trystan ; Falcinella, Alexander J ; White, Reuben J ; Adnan, Rohul H ; Golovko, Vladimir ; Andersson, Gunther G ; Metha, Gregory F</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-rsc_primary_c5ra11599j3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bennett, Trystan</creatorcontrib><creatorcontrib>Falcinella, Alexander J</creatorcontrib><creatorcontrib>White, Reuben J</creatorcontrib><creatorcontrib>Adnan, Rohul H</creatorcontrib><creatorcontrib>Golovko, Vladimir</creatorcontrib><creatorcontrib>Andersson, Gunther G</creatorcontrib><creatorcontrib>Metha, Gregory F</creatorcontrib></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bennett, Trystan</au><au>Falcinella, Alexander J</au><au>White, Reuben J</au><au>Adnan, Rohul H</au><au>Golovko, Vladimir</au><au>Andersson, Gunther G</au><au>Metha, Gregory F</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The effect of counter ions on the far-infrared spectra of tris(triphenylphosphinegold)oxonium dimer saltsElectronic supplementary information (ESI) available: Containing a comparison between the crystallographic and DFT-optimized Au6O2 core, optimized structures for the [[(Ph3PAu)3O]BF4]2 and [[(Ph3PAu)3O]MnO4]2 species, and a comparison between the theoretical spectra for the [(PPh3Au)3O]− and ([(PPh3Au)3O]−)2 species. See DOI: 10.1039/c5ra11599j</atitle><date>2015-09-02</date><risdate>2015</risdate><volume>5</volume><issue>91</issue><spage>74499</spage><epage>7455</epage><pages>74499-7455</pages><eissn>2046-2069</eissn><abstract>Two tris(triphenylphosphinegold)oxonium dimer salts [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(X
−
)
2
(X = BF
−
4
, MnO
−
4
) were investigated
via
synchrotron-based far-infrared vibrational spectroscopy and density functional theory modelled at the M06/LANL2DZ level of theory. The 50-800 cm
−1
region of both oxonium salts is presented, with the spectrum for [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
found to possess a large feature at 330.3 cm
−1
, attributable to counter-ion vibrational modes, which is only predicted upon explicit inclusion of counter-ions in the calculation. A feature around 107 cm
−1
observed for the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
infrared spectrum is assigned to 21 distinct vibrational modes arising from Au-Au bond stretching and other motions of the Au core. The same feature is predicted to be present within the [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
spectrum but is masked by experimental noise. In the 50-400 cm
−1
region, the relative intensities of predicted vibrational modes is found to depend heavily on the presence and nature of the counter-ions, while within the 400-800 cm
−1
region, little dependence of the theoretical spectra on the type of counter-ion is predicted. Finally, the dimerization energies of both [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(BF
−
4
)
2
and [{{Au(PPh
3
)}
3
(μ
3
−O)}
2
]
2+
(MnO
−
4
)
2
are calculated to be 3.06 eV and 3.20 eV, respectively, when the counter-ions are explicitly included within the calculation, and just 1.10 eV in their absence.
The far-infrared spectra of two tris(triphenylphosphinegold)oxonium dimer salts in the 50-800 cm
−1
region were recorded using synchrotron-based IR radiation, and comprehensively assigned utilising density functional theory calculations.</abstract><doi>10.1039/c5ra11599j</doi><tpages>7</tpages></addata></record> |
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source | Royal Society of Chemistry |
title | The effect of counter ions on the far-infrared spectra of tris(triphenylphosphinegold)oxonium dimer saltsElectronic supplementary information (ESI) available: Containing a comparison between the crystallographic and DFT-optimized Au6O2 core, optimized structures for the [[(Ph3PAu)3O]BF4]2 and [[(Ph3PAu)3O]MnO4]2 species, and a comparison between the theoretical spectra for the [(PPh3Au)3O]− and ([(PPh3Au)3O]−)2 species. See DOI: 10.1039/c5ra11599j |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-25T20%3A21%3A43IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-rsc&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=The%20effect%20of%20counter%20ions%20on%20the%20far-infrared%20spectra%20of%20tris(triphenylphosphinegold)oxonium%20dimer%20saltsElectronic%20supplementary%20information%20(ESI)%20available:%20Containing%20a%20comparison%20between%20the%20crystallographic%20and%20DFT-optimized%20Au6O2%20core,%20optimized%20structures%20for%20the%20%5B%5B(Ph3PAu)3O%5DBF4%5D2%20and%20%5B%5B(Ph3PAu)3O%5DMnO4%5D2%20species,%20and%20a%20comparison%20between%20the%20theoretical%20spectra%20for%20the%20%5B(PPh3Au)3O%5D%E2%88%92%20and%20(%5B(PPh3Au)3O%5D%E2%88%92)2%20species.%20See%20DOI:%2010.1039/c5ra11599j&rft.au=Bennett,%20Trystan&rft.date=2015-09-02&rft.volume=5&rft.issue=91&rft.spage=74499&rft.epage=7455&rft.pages=74499-7455&rft.eissn=2046-2069&rft_id=info:doi/10.1039/c5ra11599j&rft_dat=%3Crsc%3Ec5ra11599j%3C/rsc%3E%3Cgrp_id%3Ecdi_FETCH-rsc_primary_c5ra11599j3%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 |