2022
DOI: 10.3390/ma15144858
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A DFT-Based Quantitative and Geometric Analysis of the Effect of Pressure on Boron Arsenate

Abstract: Boron arsenate, BAsO4, is a β-cristobalite-like crystal which has been reported to exhibit the rather unusual property of negative linear compressibility behaviour at elevated pressures, that is expanding rather than shrinking in a linear dimension when subjected to pressure. This work proposes a ‘geometry—deformation mechanism’-based mathematical model to aid the discernment of the manner how this anomalous pressure behaviour is achieved. The model makes use of data obtained from DFT simulations over an exten… Show more

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Cited by 5 publications
(9 citation statements)
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References 61 publications
(101 reference statements)
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“…As explained by Grima‐Cornish et al, [ 54 ] given these parameters, one may calculate the height of the AsO 4 and BO 4 tetrahedra, h a and h b respectively as h a = 2 l a cos ( θ a 2 ) h b = 2 l b cos ( θ b 2 ) and the dimensions of 2D projected squares, in terms of the lengths of the diagonals, which correspond to the lengths of the edges lying in the (001) plane, i.e., d a (for the square related to the AsO 4 tetrahedron) and d b (for the square related to the BO 4 tetrahedron) and the 2D angle between them, θ 2d , as follows d a = 2 l a sin ( θ a 2 ) d b = 2 l b sin ( θ b 2 ) θ 2 d = cos 1 ( cos ( θ a 2 ) cos ( θ b 2 ) + cos ( θ 3 d ) sin ( θ a 2 ) sin ( θ b 2 ) ) …”
Section: Methodsmentioning
confidence: 82%
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“…As explained by Grima‐Cornish et al, [ 54 ] given these parameters, one may calculate the height of the AsO 4 and BO 4 tetrahedra, h a and h b respectively as h a = 2 l a cos ( θ a 2 ) h b = 2 l b cos ( θ b 2 ) and the dimensions of 2D projected squares, in terms of the lengths of the diagonals, which correspond to the lengths of the edges lying in the (001) plane, i.e., d a (for the square related to the AsO 4 tetrahedron) and d b (for the square related to the BO 4 tetrahedron) and the 2D angle between them, θ 2d , as follows d a = 2 l a sin ( θ a 2 ) d b = 2 l b sin ( θ b 2 ) θ 2 d = cos 1 ( cos ( θ a 2 ) cos ( θ b 2 ) + cos ( θ 3 d ) sin ( θ a 2 ) sin ( θ b 2 ) ) …”
Section: Methodsmentioning
confidence: 82%
“…The same work [ 54 ] further explains that when this material is subjected to a pressure change (increase), there are two main types of deformation that are crucial to imparting on this material its observed compressibility properties, namely: 1) A deformation of the tetrahedra themselves, due to changes in OX bond lengths and OXO bond angles, where the tetrahedra are observed to become elongated with an increase in pressure within the pressure range from c. 5 to c. 50 GPa, while retaining their characteristic tetragonal disphenoidal shape (i.e., the length d gets shorter and their height increases). This feature gives rise to the observed negative linear compressibility (NLC) characteristics in the c direction at elevated pressures within the range of c. 5 to c. 50 GPa (range predicted by the simulations) and occurs since over this pressure range, changes in the OXO bond angles are more pronounced than changes in the OX bond lengths.…”
Section: Introductionmentioning
confidence: 98%
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