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<dc:title>Switching hydrogen bonding to π-stacking: The thiophenol dimer and trimer</dc:title>
<dc:creator>Saragi, Rizalina Tama</dc:creator>
<dc:creator>Juanes San José, Marcos</dc:creator>
<dc:creator>Pérez Cuadrado, Cristobal</dc:creator>
<dc:creator>Pinacho Morante, Pablo</dc:creator>
<dc:creator>Tikhonov, Denis S.</dc:creator>
<dc:creator>Caminati, Walther</dc:creator>
<dc:creator>Schnell, Melanie</dc:creator>
<dc:creator>Lesarri Gómez, Alberto Eugenio</dc:creator>
<dc:subject>Hydrogen bondings</dc:subject>
<dc:subject>Enlaces de hidrógeno</dc:subject>
<dc:subject>Pi-stacking</dc:subject>
<dc:subject>Apilamiento</dc:subject>
<dc:subject>Thiophenol</dc:subject>
<dc:subject>Tiofeno</dc:subject>
<dc:description>Producción Científica</dc:description>
<dc:description>We used jet-cooled broadband rotational spectroscopy to explore the balance between π-stacking and hydrogen-bonding interactions in the self-aggregation of thiophenol. Two different isomers were detected for the thiophenol dimer, revealing dispersion-controlled π-stacked structures anchored by a long S–H···S sulfur hydrogen bond. The weak intermolecular forces allow for noticeable internal dynamics in the dimers, as tunneling splittings are observed for the global minimum. The large-amplitude motion is ascribed to a concerted inversion motion between the two rings, exchanging the roles of the proton donor and acceptor in the thiol groups. The determined torsional barrier of B2 = 250.3 cm–1 is consistent with theoretical predictions (290–502 cm–1) and the monomer barrier of 277.1(3) cm–1. For the thiophenol trimer, a symmetric top structure was assigned in the spectrum. The results highlight the relevance of substituent effects to modulate π-stacking geometries and the role of the sulfur-centered hydrogen bonds.</dc:description>
<dc:description>Ministerio de Ciencia e Innovación - Fondo Europeo de Desarrollo Regional (grant PGC2018-098561-BC22)</dc:description>
<dc:description>Deutsche Forschungsgemeinschaft (grant SCHN1280/4-2)</dc:description>
<dc:date>2021-07-30T08:07:33Z</dc:date>
<dc:date>2021-07-30T08:07:33Z</dc:date>
<dc:date>2021</dc:date>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/acceptedVersion</dc:type>
<dc:identifier>The Journal of Physical Chemistry Letters, 2021, vol. 12, n. 5. p. 1367-1373</dc:identifier>
<dc:identifier>1948-7185</dc:identifier>
<dc:identifier>https://uvadoc.uva.es/handle/10324/47827</dc:identifier>
<dc:identifier>10.1021/acs.jpclett.0c03797</dc:identifier>
<dc:language>eng</dc:language>
<dc:relation>https://pubs.acs.org/doi/10.1021/acs.jpclett.0c03797</dc:relation>
<dc:rights>Attribution-NonCommercial-NoDerivatives 4.0 Internacional</dc:rights>
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:rights>http://creativecommons.org/licenses/by-nc-nd/4.0/</dc:rights>
<dc:rights>© 2021 ACS Publications</dc:rights>
<dc:format>application/pdf</dc:format>
<dc:publisher>ACS Publications</dc:publisher>
<europeana:object>https://uvadoc.uva.es/bitstream/10324/47827/2/Switching-hydrogen-bonding.pdf.jpg</europeana:object>
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<europeana:type>TEXT</europeana:type>
<europeana:rights>http://creativecommons.org/licenses/by-nc-nd/4.0/</europeana:rights>
<europeana:dataProvider>UVaDOC. Repositorio Documental de la Universidad de Valladolid</europeana:dataProvider>
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