2018
DOI: 10.1021/acs.jpca.7b10083
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Vibrational Properties of Bulk Boric Acid 2A and 3T Polymorphs and Their Two-Dimensional Layers: Measurements and Density Functional Theory Calculations

Abstract: Boric acid (HBO) is being used effectively nowadays in traps/baits for the management of Aedes aegypti L. and Aedes albopictus Skuse species of mosquitoes, which are the main spreading vectors worldwide for diseases such as malaria, dengue, and zika. Previously, we published results on the structural, electronic, and optical properties of its molecular triclinic HBO-2A and trigonal HBO-3T polymorphs within the framework of density functional theory (DFT). Because of the renewed importance of these materials, t… Show more

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Cited by 11 publications
(17 citation statements)
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“…At ambient conditions, the Raman spectrum for fresh 1.2 B/SiO 2 contains peaks at 209, 500, and 882 cm –1 that match closely with vibrations observed in the Raman spectrum for boric acid (shown above the spectra for 1.2 B/SiO 2 in Figure ). The vibration at 209 cm –1 has been previously attributed to a lattice-translatory oscillation in boric acid, whereas the peaks at 500 and 882 cm –1 correspond to O–B–O bending and B–O stretching modes, respectively. , Upon dehydration of 1.2 B/SiO 2 at temperatures >100 °C, these features disappear, and instead a small feature at 807 cm –1 can be observed. This is very close to the feature at 808 cm –1 observed in B 2 O 3 (top spectrum in Figure ).…”
Section: Results and Discussionmentioning
confidence: 90%
“…At ambient conditions, the Raman spectrum for fresh 1.2 B/SiO 2 contains peaks at 209, 500, and 882 cm –1 that match closely with vibrations observed in the Raman spectrum for boric acid (shown above the spectra for 1.2 B/SiO 2 in Figure ). The vibration at 209 cm –1 has been previously attributed to a lattice-translatory oscillation in boric acid, whereas the peaks at 500 and 882 cm –1 correspond to O–B–O bending and B–O stretching modes, respectively. , Upon dehydration of 1.2 B/SiO 2 at temperatures >100 °C, these features disappear, and instead a small feature at 807 cm –1 can be observed. This is very close to the feature at 808 cm –1 observed in B 2 O 3 (top spectrum in Figure ).…”
Section: Results and Discussionmentioning
confidence: 90%
“…Calculated through density functional perturbation theory (DFPT), the phonon density of states enables a precise description of a thermodynamic state [161] enabling calculations of Gibbs free energy, enthalpy, entropy and zero-point energy. For example, a quite commonly performed comparison between experimental sublimation enthalpy and the calculated lattice energies requires the vibrational contribution, which is determined via phonon calculations [162,163].…”
Section: Lattice Dynamics and Phonons Calculationmentioning
confidence: 99%
“…Calculated through DFPT, the phonon density of states not only enables to obtain a precise description of a thermodynamic state [161] by calculating the Gibbs free energy, enthalpy, entropy, or zero-point energy but also the generation of vibrational spectra such as IR, Raman, and INS. All these calculations are usually characterized by a very good agreement with the experimental results [170,171] and in many cases they reveal the reason (e.g., molecular structure in itself, crystal packing) for spectral differences between two polymorphs [172].…”
Section: Vibrational Propertiesmentioning
confidence: 99%
“…Phonon dispersion and densities of states were also evaluated for each polymorph, as well as the temperaturedependent curves for their entropy, enthalpy, free energy, heat capacity, and Debye temperature. In particular, the calculations of Bezerra Da Silva et al 14 suggested a possible way to differentiate the 2A-and -3T crystals by Raman spectroscopy and heat capacity measurements. Following the steps of Bezerra Da Silva et al, 14 results of DFT calculations using a pure GGA functional incorporating an energy term describing dispersive noncovalent interactions will be presented here.…”
Section: Introductionmentioning
confidence: 99%