Weak vibrational coupling in a large van der Waals complex: fluorescence spectroscopy of perylene/naphthalene

Fluorescence excitation and dispersed fluorescence spectra are reported for 1:1 and 2:1 complexes of naphthalene with perylene under supersonic jet conditions. Confirming preliminary results, the fluorescence spectra of the 1:1 complex following excitation of an ag (in-plane) mode at 353 cm−1 and it...

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Veröffentlicht in:The Journal of chemical physics 1988-10, Vol.89 (8), p.4586-4599
Hauptverfasser: MOTYKA, A. L, WITTMEYER, S. A, BABBITT, R. J, TOPP, M. R
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WITTMEYER, S. A
BABBITT, R. J
TOPP, M. R
description Fluorescence excitation and dispersed fluorescence spectra are reported for 1:1 and 2:1 complexes of naphthalene with perylene under supersonic jet conditions. Confirming preliminary results, the fluorescence spectra of the 1:1 complex following excitation of an ag (in-plane) mode at 353 cm−1 and its first overtone show unusually weak vibrational coupling. Although excitation of combination levels of 3531 with out-of-plane modes at 74, 79, and 93 cm−1 gives rise to emission which is predominantly ‘‘relaxed,’’ the residual ‘‘unrelaxed’’ component indicates a significant degree of mode-selective vibrational coupling. It is notable that the vibrational coupling for 3532 excitation (i.e., at ≈700 cm−1) is substantially less extensive than for excitation into the 3531 combination bands nearly 300 cm−1 lower in energy. A similar comparison has been made between a second ag mode, at 550 cm−1, and a perturbed b3g (out-of-plane) mode, at 540 cm−1. In this case, the data indicate a difference in coupling, which is less obvious than for the 353 cm−1 case, but still indicates a significant dynamic difference in the picosecond domain. Higher-energy excitation is seen to give rise to a large amount of spectral broadening, to ≈700 cm−1, yet without any appreciable shift. This indicates that a single equilibrium conformation is present. Comparison with data for uncomplexed perylene and for other perylene complexes at a similar excitation energy (1300–1400 cm−1) suggests that the broadening is due to vibrational coupling involving combinations and overtones of Franck–Condon active low-frequency modes in perylene/naphthalene. Fluorescence excitation data for 2:1 complexes show that the three-band combination of the 1:1 complex at 74–93 cm−1 is replaced by a single, strongly Franck–Condon active mode at 62 cm−1. The corresponding ground state frequency is about 56 cm−1 and, overall, this mode shows harmonic behavior. Like the 1:1 complex, the fluorescence spectrum following excitation into v=2 of the out-of-plane mode, at ≈125 cm−1, shows little evidence of vibrational coupling. At and above 353 cm−1, perylene/(naphthalene)2 shows extensive vibrational coupling, since no structure persists in the fluorescence spectra. A comparison has been made between the naphthalene and some other 1:1 complexes of perylene. At 353 cm−1, the Ar1 complex shows less vibrational coupling than perylene/naphthalene, although the presence even of an argon dimer generates a greater degree of coupl
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L ; WITTMEYER, S. A ; BABBITT, R. J ; TOPP, M. R</creator><creatorcontrib>MOTYKA, A. L ; WITTMEYER, S. A ; BABBITT, R. J ; TOPP, M. R</creatorcontrib><description>Fluorescence excitation and dispersed fluorescence spectra are reported for 1:1 and 2:1 complexes of naphthalene with perylene under supersonic jet conditions. Confirming preliminary results, the fluorescence spectra of the 1:1 complex following excitation of an ag (in-plane) mode at 353 cm−1 and its first overtone show unusually weak vibrational coupling. Although excitation of combination levels of 3531 with out-of-plane modes at 74, 79, and 93 cm−1 gives rise to emission which is predominantly ‘‘relaxed,’’ the residual ‘‘unrelaxed’’ component indicates a significant degree of mode-selective vibrational coupling. It is notable that the vibrational coupling for 3532 excitation (i.e., at ≈700 cm−1) is substantially less extensive than for excitation into the 3531 combination bands nearly 300 cm−1 lower in energy. A similar comparison has been made between a second ag mode, at 550 cm−1, and a perturbed b3g (out-of-plane) mode, at 540 cm−1. In this case, the data indicate a difference in coupling, which is less obvious than for the 353 cm−1 case, but still indicates a significant dynamic difference in the picosecond domain. Higher-energy excitation is seen to give rise to a large amount of spectral broadening, to ≈700 cm−1, yet without any appreciable shift. This indicates that a single equilibrium conformation is present. Comparison with data for uncomplexed perylene and for other perylene complexes at a similar excitation energy (1300–1400 cm−1) suggests that the broadening is due to vibrational coupling involving combinations and overtones of Franck–Condon active low-frequency modes in perylene/naphthalene. Fluorescence excitation data for 2:1 complexes show that the three-band combination of the 1:1 complex at 74–93 cm−1 is replaced by a single, strongly Franck–Condon active mode at 62 cm−1. The corresponding ground state frequency is about 56 cm−1 and, overall, this mode shows harmonic behavior. Like the 1:1 complex, the fluorescence spectrum following excitation into v=2 of the out-of-plane mode, at ≈125 cm−1, shows little evidence of vibrational coupling. At and above 353 cm−1, perylene/(naphthalene)2 shows extensive vibrational coupling, since no structure persists in the fluorescence spectra. A comparison has been made between the naphthalene and some other 1:1 complexes of perylene. At 353 cm−1, the Ar1 complex shows less vibrational coupling than perylene/naphthalene, although the presence even of an argon dimer generates a greater degree of coupling. The benzene complex shows extensive IVR at this energy, by comparison with the weakly coupled naphthalene case. Further, while the naphthalene/perylene out-of-plane modes show predominantly resonant Franck–Condon emission profiles, up to excitation energies of 170 and 124 cm−1 for the 1:1 and 2:1 complexes, respectively, perylene/benzene shows extensive IVR even for 70 cm−1 excitation. These data strongly indicate that intermolecular modes, especially weakly hindered internal rotation, are responsible for the pronounced differences in the degree of vibrational coupling.</description><identifier>ISSN: 0021-9606</identifier><identifier>EISSN: 1089-7690</identifier><identifier>DOI: 10.1063/1.454799</identifier><identifier>CODEN: JCPSA6</identifier><language>eng</language><publisher>Woodbury, NY: American Institute of Physics</publisher><subject>Atomic and molecular physics ; Exact sciences and technology ; Fluorescence and phosphorescence; radiationless transitions, quenching (intersystem crossing, internal conversion) ; Molecular properties and interactions with photons ; Physics</subject><ispartof>The Journal of chemical physics, 1988-10, Vol.89 (8), p.4586-4599</ispartof><rights>1989 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c169t-fe3f0f4745f07f5176281ea1ccad3b8005ae1ec21cc2031bb9e1360075c6b75c3</citedby><cites>FETCH-LOGICAL-c169t-fe3f0f4745f07f5176281ea1ccad3b8005ae1ec21cc2031bb9e1360075c6b75c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=7247993$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>MOTYKA, A. L</creatorcontrib><creatorcontrib>WITTMEYER, S. A</creatorcontrib><creatorcontrib>BABBITT, R. J</creatorcontrib><creatorcontrib>TOPP, M. R</creatorcontrib><title>Weak vibrational coupling in a large van der Waals complex: fluorescence spectroscopy of perylene/naphthalene</title><title>The Journal of chemical physics</title><description>Fluorescence excitation and dispersed fluorescence spectra are reported for 1:1 and 2:1 complexes of naphthalene with perylene under supersonic jet conditions. Confirming preliminary results, the fluorescence spectra of the 1:1 complex following excitation of an ag (in-plane) mode at 353 cm−1 and its first overtone show unusually weak vibrational coupling. Although excitation of combination levels of 3531 with out-of-plane modes at 74, 79, and 93 cm−1 gives rise to emission which is predominantly ‘‘relaxed,’’ the residual ‘‘unrelaxed’’ component indicates a significant degree of mode-selective vibrational coupling. It is notable that the vibrational coupling for 3532 excitation (i.e., at ≈700 cm−1) is substantially less extensive than for excitation into the 3531 combination bands nearly 300 cm−1 lower in energy. A similar comparison has been made between a second ag mode, at 550 cm−1, and a perturbed b3g (out-of-plane) mode, at 540 cm−1. In this case, the data indicate a difference in coupling, which is less obvious than for the 353 cm−1 case, but still indicates a significant dynamic difference in the picosecond domain. Higher-energy excitation is seen to give rise to a large amount of spectral broadening, to ≈700 cm−1, yet without any appreciable shift. This indicates that a single equilibrium conformation is present. Comparison with data for uncomplexed perylene and for other perylene complexes at a similar excitation energy (1300–1400 cm−1) suggests that the broadening is due to vibrational coupling involving combinations and overtones of Franck–Condon active low-frequency modes in perylene/naphthalene. Fluorescence excitation data for 2:1 complexes show that the three-band combination of the 1:1 complex at 74–93 cm−1 is replaced by a single, strongly Franck–Condon active mode at 62 cm−1. The corresponding ground state frequency is about 56 cm−1 and, overall, this mode shows harmonic behavior. Like the 1:1 complex, the fluorescence spectrum following excitation into v=2 of the out-of-plane mode, at ≈125 cm−1, shows little evidence of vibrational coupling. At and above 353 cm−1, perylene/(naphthalene)2 shows extensive vibrational coupling, since no structure persists in the fluorescence spectra. A comparison has been made between the naphthalene and some other 1:1 complexes of perylene. At 353 cm−1, the Ar1 complex shows less vibrational coupling than perylene/naphthalene, although the presence even of an argon dimer generates a greater degree of coupling. The benzene complex shows extensive IVR at this energy, by comparison with the weakly coupled naphthalene case. Further, while the naphthalene/perylene out-of-plane modes show predominantly resonant Franck–Condon emission profiles, up to excitation energies of 170 and 124 cm−1 for the 1:1 and 2:1 complexes, respectively, perylene/benzene shows extensive IVR even for 70 cm−1 excitation. These data strongly indicate that intermolecular modes, especially weakly hindered internal rotation, are responsible for the pronounced differences in the degree of vibrational coupling.</description><subject>Atomic and molecular physics</subject><subject>Exact sciences and technology</subject><subject>Fluorescence and phosphorescence; radiationless transitions, quenching (intersystem crossing, internal conversion)</subject><subject>Molecular properties and interactions with photons</subject><subject>Physics</subject><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1988</creationdate><recordtype>article</recordtype><recordid>eNo9kE1LAzEQhoMoWKvgT8jBg5dtZ_Yj2_UmxS8oeFF6XGbTSbuaZkOyLfbfu6XiZWZ4eXgZHiFuESYIKpviJC_ysqrOxAhhViWlquBcjABSTCoF6lJcxfgFAFim-Uhsl0zfct82gfq2c2Sl7nbetm4tWydJWgprlntycsVBLolsHIitt_zzII3ddYGjZqdZRs-6D13UnT_IzkjP4WDZ8dSR3_QbOt7X4sIMDXzzt8fi8_npY_6aLN5f3uaPi0SjqvrEcGbA5GVeGChNgaVKZ8iEWtMqa2YABTGyTocghQybpmLMFEBZaNUMIxuL-1OvHh6KgU3tQ7ulcKgR6qOmGuuTpgG9O6GeoiZrAjndxn9-kHSksl8Aw2iI</recordid><startdate>19881015</startdate><enddate>19881015</enddate><creator>MOTYKA, A. L</creator><creator>WITTMEYER, S. A</creator><creator>BABBITT, R. J</creator><creator>TOPP, M. R</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19881015</creationdate><title>Weak vibrational coupling in a large van der Waals complex: fluorescence spectroscopy of perylene/naphthalene</title><author>MOTYKA, A. L ; WITTMEYER, S. A ; BABBITT, R. J ; TOPP, M. R</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c169t-fe3f0f4745f07f5176281ea1ccad3b8005ae1ec21cc2031bb9e1360075c6b75c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1988</creationdate><topic>Atomic and molecular physics</topic><topic>Exact sciences and technology</topic><topic>Fluorescence and phosphorescence; radiationless transitions, quenching (intersystem crossing, internal conversion)</topic><topic>Molecular properties and interactions with photons</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>MOTYKA, A. L</creatorcontrib><creatorcontrib>WITTMEYER, S. A</creatorcontrib><creatorcontrib>BABBITT, R. J</creatorcontrib><creatorcontrib>TOPP, M. R</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>MOTYKA, A. L</au><au>WITTMEYER, S. A</au><au>BABBITT, R. J</au><au>TOPP, M. R</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Weak vibrational coupling in a large van der Waals complex: fluorescence spectroscopy of perylene/naphthalene</atitle><jtitle>The Journal of chemical physics</jtitle><date>1988-10-15</date><risdate>1988</risdate><volume>89</volume><issue>8</issue><spage>4586</spage><epage>4599</epage><pages>4586-4599</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><coden>JCPSA6</coden><abstract>Fluorescence excitation and dispersed fluorescence spectra are reported for 1:1 and 2:1 complexes of naphthalene with perylene under supersonic jet conditions. Confirming preliminary results, the fluorescence spectra of the 1:1 complex following excitation of an ag (in-plane) mode at 353 cm−1 and its first overtone show unusually weak vibrational coupling. Although excitation of combination levels of 3531 with out-of-plane modes at 74, 79, and 93 cm−1 gives rise to emission which is predominantly ‘‘relaxed,’’ the residual ‘‘unrelaxed’’ component indicates a significant degree of mode-selective vibrational coupling. It is notable that the vibrational coupling for 3532 excitation (i.e., at ≈700 cm−1) is substantially less extensive than for excitation into the 3531 combination bands nearly 300 cm−1 lower in energy. A similar comparison has been made between a second ag mode, at 550 cm−1, and a perturbed b3g (out-of-plane) mode, at 540 cm−1. In this case, the data indicate a difference in coupling, which is less obvious than for the 353 cm−1 case, but still indicates a significant dynamic difference in the picosecond domain. Higher-energy excitation is seen to give rise to a large amount of spectral broadening, to ≈700 cm−1, yet without any appreciable shift. This indicates that a single equilibrium conformation is present. Comparison with data for uncomplexed perylene and for other perylene complexes at a similar excitation energy (1300–1400 cm−1) suggests that the broadening is due to vibrational coupling involving combinations and overtones of Franck–Condon active low-frequency modes in perylene/naphthalene. Fluorescence excitation data for 2:1 complexes show that the three-band combination of the 1:1 complex at 74–93 cm−1 is replaced by a single, strongly Franck–Condon active mode at 62 cm−1. The corresponding ground state frequency is about 56 cm−1 and, overall, this mode shows harmonic behavior. Like the 1:1 complex, the fluorescence spectrum following excitation into v=2 of the out-of-plane mode, at ≈125 cm−1, shows little evidence of vibrational coupling. At and above 353 cm−1, perylene/(naphthalene)2 shows extensive vibrational coupling, since no structure persists in the fluorescence spectra. A comparison has been made between the naphthalene and some other 1:1 complexes of perylene. At 353 cm−1, the Ar1 complex shows less vibrational coupling than perylene/naphthalene, although the presence even of an argon dimer generates a greater degree of coupling. The benzene complex shows extensive IVR at this energy, by comparison with the weakly coupled naphthalene case. Further, while the naphthalene/perylene out-of-plane modes show predominantly resonant Franck–Condon emission profiles, up to excitation energies of 170 and 124 cm−1 for the 1:1 and 2:1 complexes, respectively, perylene/benzene shows extensive IVR even for 70 cm−1 excitation. These data strongly indicate that intermolecular modes, especially weakly hindered internal rotation, are responsible for the pronounced differences in the degree of vibrational coupling.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.454799</doi><tpages>14</tpages></addata></record>
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Exact sciences and technology
Fluorescence and phosphorescence
radiationless transitions, quenching (intersystem crossing, internal conversion)
Molecular properties and interactions with photons
Physics
title Weak vibrational coupling in a large van der Waals complex: fluorescence spectroscopy of perylene/naphthalene
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