Instituto de Física Fundamental, CSIC, Serrano 123, 28006 Madrid, Spain.
J Chem Phys. 2010 Jun 28;132(24):244303. doi: 10.1063/1.3445773.
The Ar(3) system has been studied between T=0 K and T=40 K by means of a path-integral Monte Carlo (PIMC) method. The behavior of the average energy in terms of the temperature has been explained by comparison with results obtained with the thermal averaged rovibrational spectra estimated via: (i) a quantum mechanical method based on distributed Gaussian functions for the interparticle distances and (ii) an analytical model which precisely accounts for the participation of the dissociative continua Ar(2)+Ar and Ar+Ar+Ar. Beyond T approximately 20 K, the system explores floppier configurations than the rigid equilateral geometry, as linear and Ar-Ar(2)-like arrangements, and fragmentates around T approximately 40 K. A careful investigation of the specific heat in terms of a confining radius in the PIMC calculation seems to discard a proper phase transition as in larger clusters, in apparent contradiction with previous reports of precise values for a liquid-gas transition. The onset of this noticeable change in the dynamics of the trimer occurs, however, at a remarkably low value of the temperature in comparison with Ar(n) systems formed with more Ar atoms. Quantum mechanical effects are found of relevance at T<or=15 K, with both energies and radial distributions obtained with a quantum PIMC deviating from the corresponding classical results, thus precluding exclusively classical approaches for a precise description of the system at this low temperature range.
采用路径积分蒙特卡罗(PIMC)方法研究了 T=0 K 到 T=40 K 之间的 Ar(3) 体系。通过比较与以下两种方法得到的结果,解释了平均能量随温度的变化行为:(i)基于粒子间距离分布高斯函数的量子力学方法,以及(ii)精确考虑了离解连续体 Ar(2)+Ar 和 Ar+Ar+Ar 参与的分析模型。在 T 约 20 K 以上,体系探索了比刚性等边几何更松软的构型,如线性和 Ar-Ar(2)-样排列,并在 T 约 40 K 时碎裂。通过在 PIMC 计算中考虑约束半径对比热的仔细研究,似乎排除了在较大簇中存在的适当相变,这与先前关于液体-气体转变的精确值的报告明显矛盾。然而,与形成更多 Ar 原子的 Ar(n)体系相比,这种三聚体动力学明显变化的起始温度非常低。在 T<15 K 时,量子力学效应被发现是相关的,与相应的经典结果相比,能量和径向分布都可以通过量子 PIMC 得到,因此,在这个低温范围内,完全排除了经典方法对体系的精确描述。