Abstract:(1974, Vol. IV) 1.486 (6) C(I 2)---<2 (13) 1.517 (6) C(12)---C(14)1.526 (6)110.9 Symmetry codes: (i) x, 1 + y, ½,½-z;(iv) x-l,Y,Z. CAMERON (Pearce & Watkin, 1993). Software used to prepare material for publication: CRYSTALS.HRP wishes to thank the CCDC and the University Chemical Laboratories, Cambridge, for the use of X-ray diffraction and computing facilities.Lists of structure factors, anisotropic displacement parameters, Hatom coordinates and complete geometry have been deposited with the IUCr (Referen… Show more
“…Initially, the closely related bromine analog, diisopropylammonium bromide (DPB), had seemed to be a good candidate to exhibit polar properties in the room temperature phase, however, further research indicated that the phase situation and a rich polymorphism of DPB appeared to be quite complicated. Two polymorphs of DPB are known at room temperature: monoclinic P2 1 6 and orthorhombic P2 1 2 1 2 1 . 7 The crystal structure of the latter polymorph (abbreviated in this paper as O) was presented as a private communications by G. J. Reiss.…”
mentioning
confidence: 99%
“…7 The monoclinic polymorph was obtained accidentally during the reaction of BrRe(CO) 5 and lithium diisopropylamide. 6 It undergoes an irreversible PT below room temperature to the monoclinic phase (P2 1 /n). 8 In turn, O presented in this paper was obtained during the reaction of HBr and diisopropylamine and did not disclose any PTs below room temperature.…”
mentioning
confidence: 99%
“…The second polymorph is isomorphic to the crystal of DPB obtained as reported in ref. 6. The key difference between polymorph O and M(II) is the mutual orientation of the neighboring hydrogen bonded chains.…”
A room-temperature ferroelectric, diisopropylammonium bromide (DPB), with dielectric constant e # 12 000 and a clear hysteresis loop at T c = 425 K is reported. At 417 K DPB undergoes the irreversible phase transition from nonpolar orthorhombic P2 1 2 1 2 1 to the ferroelectric monoclinic phase (P2 1 ) and subsequently, at 425 K, to the paraelectric prototype phase (P2 1 /m). The molecular mechanism of the paraelectric-ferroelectric transition is ascribed to the 'order-disorder' behaviour of the diisopropylammonium cations.
“…Initially, the closely related bromine analog, diisopropylammonium bromide (DPB), had seemed to be a good candidate to exhibit polar properties in the room temperature phase, however, further research indicated that the phase situation and a rich polymorphism of DPB appeared to be quite complicated. Two polymorphs of DPB are known at room temperature: monoclinic P2 1 6 and orthorhombic P2 1 2 1 2 1 . 7 The crystal structure of the latter polymorph (abbreviated in this paper as O) was presented as a private communications by G. J. Reiss.…”
mentioning
confidence: 99%
“…7 The monoclinic polymorph was obtained accidentally during the reaction of BrRe(CO) 5 and lithium diisopropylamide. 6 It undergoes an irreversible PT below room temperature to the monoclinic phase (P2 1 /n). 8 In turn, O presented in this paper was obtained during the reaction of HBr and diisopropylamine and did not disclose any PTs below room temperature.…”
mentioning
confidence: 99%
“…The second polymorph is isomorphic to the crystal of DPB obtained as reported in ref. 6. The key difference between polymorph O and M(II) is the mutual orientation of the neighboring hydrogen bonded chains.…”
A room-temperature ferroelectric, diisopropylammonium bromide (DPB), with dielectric constant e # 12 000 and a clear hysteresis loop at T c = 425 K is reported. At 417 K DPB undergoes the irreversible phase transition from nonpolar orthorhombic P2 1 2 1 2 1 to the ferroelectric monoclinic phase (P2 1 ) and subsequently, at 425 K, to the paraelectric prototype phase (P2 1 /m). The molecular mechanism of the paraelectric-ferroelectric transition is ascribed to the 'order-disorder' behaviour of the diisopropylammonium cations.
“…Generally, the structural chemistry of simple dipH salts dates back in the ninetys of the last century [18]. The dipH halogenides and some other directly related salt structures, which were characterized, all feature hydrogen bonded chains [19][20][21][22][23][24][25][26][27].…”
“…It has been reported that diisopropylammonium bromide (DIPAB) crystallizes into a room-temperature ferroelectric phase branded as P2 1 (α-DIPAB) and a high temperature paraelectric phase categorized as P2 1/m (β) [7]. X-ray diffraction (XRD) structural characterization indicates that P2 1 (α-DIPAB) belongs to polar point group C 2 [8] illustrated schematically in Figure 1A. In contrast, at high temperature P2 1/m (β) has a crystal structure with a non-polar point group D 2 shown schematically in Figure 1B.…”
We report accurate calculations of tonsorial elements of α-Diisopropylammonium bromide (α-DIPAB) molecular ferroelectric crystal. In particular, elastic, piezoelectric and dielectric tensors were computed using density functional theory (DFT)-based Vienna ab initio simulation package (VASP). 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 devices 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. Furthermore, we calculate dynamical Born effective charge tensor to get a deeper insight into the bonding network and lattice dynamic of α-DIPAB crystal. 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 50-150 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 could be potential candidate as insulating layer of polymer thick films. Alsaad et al.
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