Ndiaye Mamadou, Boukheddaden Kamel
Université Paris-Saclay, UVSQ, CNRS, GEMaC, 45 Avenue des Etats Unis, 78035 Versailles, France.
Département de Physique, Université Cheikh Anta Diop de Dakar, FST, BP 5005, Fann, Dakar, Senegal.
Phys Chem Chem Phys. 2022 Jun 1;24(21):12870-12889. doi: 10.1039/d2cp01285e.
Spin transition materials are known to exhibit a rich variety of behaviors under several stimuli, among which pressure leads to major changes in their electronic and elastic properties. From an experimental point of view, thermal spin transitions under isotropic pressure showed transformations from (i) hysteretic to continuous transformations where the hysteresis width vanishes beyond some threshold pressure value; this is the conventional case. In several other cases very pathological and unexpected behaviours emerged, like (ii) persistent hysteresis under pressure; (iii) non-uniform behavior of the thermal hysteresis width which first increases with pressure and then decreases and vanishes at higher pressures; (iv) furthermore, double step transitions induced by pressure are also often obtained, where the pressure triggers the appearance of a plateau during the thermal transition, leading to two-step transitions, and finally (v) other non-conventional re-entrant transitions, where the thermal hysteresis vanishes at some pressure and then reappears at higher pressure values are also observed. In the present theoretical study, we investigate this problem with an electro-elastic description of the spin-crossover phenomenon by solving the Hamiltonian using a Monte Carlo technique. The pressure effect is here introduced directly in the lattice parameters, the elastic constants and ligand field energy. By considering spin state-dependent compressibility, we demonstrate that a large panel of experimental observations can be qualitatively described with this model. Among them, we quote (i) the conventional pressure effect decreasing the hysteresis width, (ii) the unconventional cases with pressure causing a non-monotonous behavior of the hysteresis width, (iii) re-entrant, as well as (iv) double step transitions accompanied with various types of spin state self-organization in the plateau regions.
自旋转变材料在多种刺激下表现出丰富多样的行为,其中压力会导致其电子和弹性性质发生重大变化。从实验角度来看,各向同性压力下的热自旋转变呈现出从(i)滞后转变为连续转变的过程,其中滞后宽度在超过某个阈值压力值时消失;这是常规情况。在其他一些情况下,出现了非常反常和意想不到的行为,比如(ii)压力下的持续滞后;(iii)热滞后宽度的非均匀行为,即先随压力增加,然后减小并在更高压力下消失;(iv)此外,还经常观察到压力诱导的双步转变,其中压力在热转变过程中触发一个平台的出现,导致两步转变,最后(v)还观察到其他非常规的再入转变,即热滞后在某个压力下消失,然后在更高压力值时再次出现。在本理论研究中,我们通过使用蒙特卡罗技术求解哈密顿量,以自旋交叉现象的电弹性描述来研究这个问题。这里将压力效应直接引入晶格参数、弹性常数和配体场能量中。通过考虑自旋态依赖的压缩性,我们证明该模型可以定性地描述大量的实验观测结果。其中包括(i)传统的压力效应使滞后宽度减小,(ii)压力导致滞后宽度呈现非单调行为的非常规情况,(iii)再入转变,以及(iv)在平台区域伴有各种类型自旋态自组织的双步转变。