Vibrational Perturbations and Ligand–Layer Coupling in a Single Crystal of Au144(SC2H4Ph)60 Nanocluster
We have determined vibrational signatures and optical gap of the Au144(PET)60 (PET: phenylethylthiol, SC2H4Ph) nanocluster solvated in deuterated dichloromethane (DCM-D2, CD2Cl2) and in a single crystal. For crystals, solid-state 13C NMR and X-ray diffraction were also measured. A revised value of 2...
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Veröffentlicht in: | The journal of physical chemistry letters 2014-01, Vol.5 (2), p.387-392 |
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creator | Koivisto, Jaakko Salorinne, Kirsi Mustalahti, Satu Lahtinen, Tanja Malola, Sami Häkkinen, Hannu Pettersson, Mika |
description | We have determined vibrational signatures and optical gap of the Au144(PET)60 (PET: phenylethylthiol, SC2H4Ph) nanocluster solvated in deuterated dichloromethane (DCM-D2, CD2Cl2) and in a single crystal. For crystals, solid-state 13C NMR and X-ray diffraction were also measured. A revised value of 2200 cm–1 (0.27 eV) was obtained for the optical gap in both phases. The vibrational spectra of solvated AU144(PET)60 closely resembles that of neat PET, while the crystalline-state spectrum exhibits significant inhomogeneous spectral broadening, frequency shifts, intensity transfer between vibrational modes, and an increase in the overtone and combination transition intensities. Spectral broadening was also observed in the 13C NMR spectrum. Changes in the intensity are explained due to vibrational coupling of the normal modes induced by the crystal packing, and the vibrational broadening is caused by ligand-environment inhomogeneity in the crystal. This indicates a pseudocrystalline state where the cluster cores are arranged in periodic fashion, while the ligand-layer molecules between the cores form amorphous structures. |
doi_str_mv | 10.1021/jz4026003 |
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For crystals, solid-state 13C NMR and X-ray diffraction were also measured. A revised value of 2200 cm–1 (0.27 eV) was obtained for the optical gap in both phases. The vibrational spectra of solvated AU144(PET)60 closely resembles that of neat PET, while the crystalline-state spectrum exhibits significant inhomogeneous spectral broadening, frequency shifts, intensity transfer between vibrational modes, and an increase in the overtone and combination transition intensities. Spectral broadening was also observed in the 13C NMR spectrum. Changes in the intensity are explained due to vibrational coupling of the normal modes induced by the crystal packing, and the vibrational broadening is caused by ligand-environment inhomogeneity in the crystal. This indicates a pseudocrystalline state where the cluster cores are arranged in periodic fashion, while the ligand-layer molecules between the cores form amorphous structures.</description><identifier>ISSN: 1948-7185</identifier><identifier>EISSN: 1948-7185</identifier><identifier>DOI: 10.1021/jz4026003</identifier><identifier>PMID: 26270716</identifier><language>eng</language><publisher>United States: American Chemical Society</publisher><subject>Spectroscopy, Photochemistry, and Excited States</subject><ispartof>The journal of physical chemistry letters, 2014-01, Vol.5 (2), p.387-392</ispartof><rights>Copyright © 2014 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/jz4026003$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/jz4026003$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>315,781,785,27081,27929,27930,56743,56793</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/26270716$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Koivisto, Jaakko</creatorcontrib><creatorcontrib>Salorinne, Kirsi</creatorcontrib><creatorcontrib>Mustalahti, Satu</creatorcontrib><creatorcontrib>Lahtinen, Tanja</creatorcontrib><creatorcontrib>Malola, Sami</creatorcontrib><creatorcontrib>Häkkinen, Hannu</creatorcontrib><creatorcontrib>Pettersson, Mika</creatorcontrib><title>Vibrational Perturbations and Ligand–Layer Coupling in a Single Crystal of Au144(SC2H4Ph)60 Nanocluster</title><title>The journal of physical chemistry letters</title><addtitle>J. Phys. Chem. Lett</addtitle><description>We have determined vibrational signatures and optical gap of the Au144(PET)60 (PET: phenylethylthiol, SC2H4Ph) nanocluster solvated in deuterated dichloromethane (DCM-D2, CD2Cl2) and in a single crystal. For crystals, solid-state 13C NMR and X-ray diffraction were also measured. A revised value of 2200 cm–1 (0.27 eV) was obtained for the optical gap in both phases. The vibrational spectra of solvated AU144(PET)60 closely resembles that of neat PET, while the crystalline-state spectrum exhibits significant inhomogeneous spectral broadening, frequency shifts, intensity transfer between vibrational modes, and an increase in the overtone and combination transition intensities. Spectral broadening was also observed in the 13C NMR spectrum. Changes in the intensity are explained due to vibrational coupling of the normal modes induced by the crystal packing, and the vibrational broadening is caused by ligand-environment inhomogeneity in the crystal. This indicates a pseudocrystalline state where the cluster cores are arranged in periodic fashion, while the ligand-layer molecules between the cores form amorphous structures.</description><subject>Spectroscopy, Photochemistry, and Excited States</subject><issn>1948-7185</issn><issn>1948-7185</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNpNkLFOwzAURS0EoqUw8APIC1IZAs-O4yRjFQFFiqBSgTWyk5eSKk2KHQ9l4h_4Q76EQAtiuvdJ593hEHLK4JIBZ1fLNwFcAvh7ZMhiEXkhi4L9f31AjqxdAsgYovCQDLjkIYRMDkn1XGmjuqptVE1naDpn9M9pqWoKmlaLPj7fP1K1QUOT1q3rqlnQqqGKzvtWI03Mxnb9d1vSiWNCjOcJn4rZy4UEeq-aNq-d7dAck4NS1RZPdjkiTzfXj8nUSx9u75JJ6inOeefFUpdaAxalzv0AdJiD7JPFWPA4ViyIlOZc-iJE6UuEnAmFEQKqHEXgh_6IjLe7a9O-OrRdtqpsjnWtGmydzVgIwhdBFEOPnu1Qp1dYZGtTrZTZZL96euB8C6jcZsvWmd5SvwDZt_bsT7v_BQHhcXs</recordid><startdate>20140116</startdate><enddate>20140116</enddate><creator>Koivisto, Jaakko</creator><creator>Salorinne, Kirsi</creator><creator>Mustalahti, Satu</creator><creator>Lahtinen, Tanja</creator><creator>Malola, Sami</creator><creator>Häkkinen, Hannu</creator><creator>Pettersson, Mika</creator><general>American Chemical Society</general><scope>NPM</scope><scope>7X8</scope></search><sort><creationdate>20140116</creationdate><title>Vibrational Perturbations and Ligand–Layer Coupling in a Single Crystal of Au144(SC2H4Ph)60 Nanocluster</title><author>Koivisto, Jaakko ; Salorinne, Kirsi ; Mustalahti, Satu ; Lahtinen, Tanja ; Malola, Sami ; Häkkinen, Hannu ; Pettersson, Mika</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a222t-96bfbb0edfbc350b7c0635019ed299a158ab226347e636e0c14ae8e0eace45373</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Spectroscopy, Photochemistry, and Excited States</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Koivisto, Jaakko</creatorcontrib><creatorcontrib>Salorinne, Kirsi</creatorcontrib><creatorcontrib>Mustalahti, Satu</creatorcontrib><creatorcontrib>Lahtinen, Tanja</creatorcontrib><creatorcontrib>Malola, Sami</creatorcontrib><creatorcontrib>Häkkinen, Hannu</creatorcontrib><creatorcontrib>Pettersson, Mika</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>The journal of physical chemistry letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Koivisto, Jaakko</au><au>Salorinne, Kirsi</au><au>Mustalahti, Satu</au><au>Lahtinen, Tanja</au><au>Malola, Sami</au><au>Häkkinen, Hannu</au><au>Pettersson, Mika</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Vibrational Perturbations and Ligand–Layer Coupling in a Single Crystal of Au144(SC2H4Ph)60 Nanocluster</atitle><jtitle>The journal of physical chemistry letters</jtitle><addtitle>J. Phys. Chem. Lett</addtitle><date>2014-01-16</date><risdate>2014</risdate><volume>5</volume><issue>2</issue><spage>387</spage><epage>392</epage><pages>387-392</pages><issn>1948-7185</issn><eissn>1948-7185</eissn><abstract>We have determined vibrational signatures and optical gap of the Au144(PET)60 (PET: phenylethylthiol, SC2H4Ph) nanocluster solvated in deuterated dichloromethane (DCM-D2, CD2Cl2) and in a single crystal. For crystals, solid-state 13C NMR and X-ray diffraction were also measured. A revised value of 2200 cm–1 (0.27 eV) was obtained for the optical gap in both phases. The vibrational spectra of solvated AU144(PET)60 closely resembles that of neat PET, while the crystalline-state spectrum exhibits significant inhomogeneous spectral broadening, frequency shifts, intensity transfer between vibrational modes, and an increase in the overtone and combination transition intensities. Spectral broadening was also observed in the 13C NMR spectrum. Changes in the intensity are explained due to vibrational coupling of the normal modes induced by the crystal packing, and the vibrational broadening is caused by ligand-environment inhomogeneity in the crystal. This indicates a pseudocrystalline state where the cluster cores are arranged in periodic fashion, while the ligand-layer molecules between the cores form amorphous structures.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>26270716</pmid><doi>10.1021/jz4026003</doi><tpages>6</tpages></addata></record> |
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title | Vibrational Perturbations and Ligand–Layer Coupling in a Single Crystal of Au144(SC2H4Ph)60 Nanocluster |
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