Abstract

The present work emphasizes the value of periodic density functional theory (DFT) calculations in the assessment of the vibrational spectra of molecular crystals. Periodic calculations provide a nearly one-to-one match between the calculated and observed bands in the inelastic neutron scattering (INS) spectrum of crystalline 4-phenylbenzaldehyde, thus validating their assignment and correcting previous reports based on single molecule calculations. The calculations allow the unambiguous assignment of the phenyl torsional mode at ca. 118–128 cm−1, from which a phenyl torsional barrier of ca. 4000 cm−1 is derived, and the identification of the collective mode involving the antitranslational motion of CH···O bonded pairs, a hallmark vibrational mode of systems where C-H···O contacts are an important feature.

Highlights

  • The use of periodic density functional calculations to address the vibrational spectra of molecular crystals is becoming increasingly popular [1,2,3,4,5,6,7,8,9,10,11,12]

  • The present work is a simple exercise that illustrates the capabilities of periodic density functional theory (DFT) as an aid in the vibrational assignment of organic crystals

  • Despite being more resource intensive than its discrete counterparts, the effort of running periodic DFT calculations pays off by delivering accurate estimated spectra, which can be used as a direct guide for assignments

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Summary

Introduction

The use of periodic density functional calculations (periodic DFT) to address the vibrational spectra of molecular crystals is becoming increasingly popular [1,2,3,4,5,6,7,8,9,10,11,12]. The periodic DFT approach, originally developed to deal with extended inorganic systems, was found to be highly efficient in predicting the vibrational spectra of molecular crystals [13]. Periodic methods—available through programs such as VASP [14], CRYSTAL [15,16] and CASTEP [17]—are often used to assist vibrational assignments of infrared and inelastic neutron scattering (INS) spectra of molecular crystals [1,2,6,7,8,9,18].

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