2001
DOI: 10.1002/1521-3951(200101)223:2<423::aid-pssb423>3.0.co;2-5
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Structural Phase Transitions of Ga2Se3 and GaSe under High Pressure

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Cited by 16 publications
(17 citation statements)
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“…Figure 2 shows the evolution of the intralayer first neighbour Se−In distance, as obtained from XAS experiments under pressure [9]. This distance follows a monotonous compression up to 7.1 GPa, that can be accounted for by a Murnaghan-type equation of state: Se-In Distance (Å) P (GPa) 13] it is possible to deduce the bulk modulus corresponding to the "a" parameter of the hexagonal cell, that turns out to be 44 GPa for InSe [7,14] and (61 ± 4) GPa for GaSe [15], with B′ 0 fixed to 5. It is then clear that the In−Se (Ga −Se) bond-length and the a-axis do not shrink at the same rate.…”
Section: Experimental and Calculation Methodsmentioning
confidence: 99%
“…Figure 2 shows the evolution of the intralayer first neighbour Se−In distance, as obtained from XAS experiments under pressure [9]. This distance follows a monotonous compression up to 7.1 GPa, that can be accounted for by a Murnaghan-type equation of state: Se-In Distance (Å) P (GPa) 13] it is possible to deduce the bulk modulus corresponding to the "a" parameter of the hexagonal cell, that turns out to be 44 GPa for InSe [7,14] and (61 ± 4) GPa for GaSe [15], with B′ 0 fixed to 5. It is then clear that the In−Se (Ga −Se) bond-length and the a-axis do not shrink at the same rate.…”
Section: Experimental and Calculation Methodsmentioning
confidence: 99%
“…According to the literature data, phase transitions in the 10-30 GPa pressure range are rather typical for A III B VI layered compounds [1,3,36,[39][40][41]. Nevertheless, the crystal structures of the new high-pressure A III B VI phases have not been experimentally refined so far.…”
Section: B the New High-pressure Phase Of Bsmentioning
confidence: 99%
“…The combined analysis of XRD and XAS results in DAC for other III-VI layered compounds (GaS, GaSe. GaTe) [32][33][34][35][36] showed that this behavior can result in an unexpected effect: the thickness of the layer can actually increase under pressure, as shown in Figure 3b [37]. This behavior is very relevant to the discussion of the reliability of deformation potential models that were proposed to give quantitative account of the extremely non-linear pressure dependence of the bandgap in III-VI semiconductors, as we will discuss in Section 3.…”
Section: Crystal Structure Eos and Pressure-temperature Phase Diagrmentioning
confidence: 80%
“…These authors reported complex behavior including (i) a nonlinear pressure dependence of the direct bangap, exhibiting a low-pressure interval with negative pressure coefficient and then increasing with pressure after a minimum, as shown in Figure 5b; (ii) a large negative pressure coefficient for the indirect gap of GaS; and (iii) a progressive widening and disappearing of the exciton peak, as shown in Figure 5a. Concerning ε-GaSe, Panfilov et al [50] suggested that nonlinear behavior was the result of a phase transition to a different polytype occurring at 0.6 GPa, a hypothesis that was not supported by later XRD experiments [32,34]. badgap of 2 eV at RT [46].…”
Section: Optical Measurements and Ab-initio Band Structure Calculationsmentioning
confidence: 98%