Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2745
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dc.contributor.authorSathyamurthy, N.-
dc.date.accessioned2020-12-07T08:37:03Z-
dc.date.available2020-12-07T08:37:03Z-
dc.date.issued2015-
dc.identifier.citationMolecular Physics, 113(19)en_US
dc.identifier.other10.1080/00268976.2015.1060365-
dc.identifier.urihttps://www.tandfonline.com/doi/full/10.1080/00268976.2015.1060365-
dc.identifier.urihttp://hdl.handle.net/123456789/2745-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractThe O–H⋅⋅⋅N hydrogen-bonded dimer of serotonin is shown to be more stable than the stacked dimer in its ground electronic state, by using the Møller–Plesset second-order perturbation theory (MP2) and the 6–31g** basis set. The vertical excitation energy for the lowest π → π* transition for the monomer as well as the dimer is predicted by time-dependent density functional theory. The experimentally observed red shift of excitation wavelength on oligomerisation is explained in terms of the change in the HOMO–LUMO energy gap due to complex formation. The impact of dimer formation on the proton magnetic resonance spectrum of serotonin monomer is also examined.en_US
dc.language.isoen_USen_US
dc.publisherTaylor and Francis Ltd.en_US
dc.subjectserotonin dimeren_US
dc.subjectconformer stabilityen_US
dc.subjecthydrogen bond and stackingen_US
dc.subjectabsorption maximaen_US
dc.titleRelative stabilities and the spectral signatures of stacked and hydrogen-bonded dimers of serotoninen_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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