Abstract

We report accurate calculations of tonsorial elements of α-Diisopropylammonium bromide (α-DIPAB) molecular ferroelectric crystal. In particular, elastic, piezoelectric and dielectric tensors were calculated using Vienna ab initio simulation package (VASP) within the framework of density functional (DFT) theory. The determination of above parameters allows an accurate description of the energy landscape for modeling of realistic devices at finite temperatures. We determine the major physical tensors in energy expansion of total energy per volume of un-deformed crystal to provide experimentalists with valuable information for designing and fabrication of pyroelectric detectors, capacitors, piezoelectric ferroelectric memories, display devices, electro-optic devices, and ultrasound transducers based on α-DIPAB. The spontaneous polarization P_s was calculated using Berry phase approach and found to be 22.64 μC⁄〖cm〗^2 in agreement with reported theoretical value. The dynamical Born effective charge tensor is reported for all atoms in the unit cell of α-DIPAB to get a deeper insight into the bonding network. The neighboring layers of DIPA molecules were found to be strongly crenelated due to the strong short-ranged electrostatic repulsion between Br sites in the DIPAB crystal structure. The organization of species in DIPA molecular layer as well as in the bromine “stitching” layer is essential for accurate calculation of DIPAB elastic properties. Having understood the actual network bonding in α-DIPAB, we calculated the components of the elastic moduli tensor. Our results indicate that a Young’s modulus of 10-180 GPa and a shear modulus of 4-26 GPa were found. Thus, α-DIPAB phase has a great potential to be a terrific candidate for flexible electronic device applications. The value of the principle component of electronic contribution to the static dielectric tensor of α-DIPAB is found to be ≈ 2.5, i.e. 50% smaller than that in typical perovskite-based ferroelectrics. Therefore, α-DIPAB is anticipated to exhibit creative materials' innovations. It offers highly customized features for specific applications, including insulation on polymer thick film conductive inks in the manufacture of membrane switches and flex circuits. Furthermore, clamped-ion piezoelectric tensor is calculated. Our results indicate a reasonable piezoelectric response of this polar crystal making it a low cost attractive candidate for piezoelectric applications.

Highlights

  • Ferroelectric materials and in particular perovskites [1, 2] are widely investigated experimentally and theoretically due to their prospective opto-electronic and piezoelectric device applications [3]

  • The spontaneous polarization (Ps) of α-diisopropylammonium bromide (DIPAB) crystal is defined as the difference between the polarization of the polar ferroelectric phase and the paraelectric centrosymmetric phase (P = 0)

  • We considered two different DIPAB polymorphs formed experimentally during recrystallization from aqueous solution, one is the ferroelectric phase labeled P21 (α) 1-F (α-DIPAB) and the other is the paraelectric structure mimicking P21/m (β)

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Summary

INTRODUCTION

Ferroelectric materials and in particular perovskites [1, 2] are widely investigated experimentally and theoretically due to their prospective opto-electronic and piezoelectric device applications [3]. We obtained the basic physical quantities describing the dielectric behavior of α-DIPAB including spontaneous polarization, dynamical Born effective charges, static dielectric, clamped-ion piezoelectric, and elastic stiffness tensors. This information can be used for modeling of potential DIPAB-based devices both ordered and disordered [21, 22]. The main motivation of the present work is to report accurate parameterization of the vector components of the “gradient” vector A and tonsorial elements of “Hessian matrix” B of polar α-DIPAB crystal Such parameterization is backbone of the correct depiction of the energy background for fabrication of convincing optoelectronic and piezoelectric devices at finite temperatures for large scale and massive production. Conclude the findings and results of this work in section Summary And Conclusions

COMPUTATIONAL METHODS
H16 Br N P21
RESULTS AND DISCUSSION
DATA AVAILABILITY STATEMENT
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