Abrams Jerry B, Rosso Lula, Tuckerman Mark E
Department of Chemistry, New York University, New York, New York 10003, USA.
J Chem Phys. 2006 Aug 21;125(7):074115. doi: 10.1063/1.2232082.
A new molecular dynamics method for calculating free energies associated with transformations of the thermodynamic state or chemical composition of a system (also known as alchemical transformations) is presented. The new method extends the adiabatic dynamics approach recently introduced by Rosso et al. [J. Chem. Phys. 116, 4389 (2002)] and is based on the use of an additional degree of freedom, lambda, that is used as a switching parameter between the potential energy functions that characterize the two states. In the new method, the coupling parameter lambda is introduced as a fictitious dynamical variable in the Hamiltonian, and a system of switching functions is employed that leads to a barrier in the lambda free energy profile between the relevant thermodynamic end points. The presence of such a barrier, therefore, enhances sampling in the end point (lambda = 0 and lambda = 1) regions which are most important for computing relevant free energy differences. In order to ensure efficient barrier crossing, a high temperature T(lambda) is assigned to lambda and a fictitious mass m(lambda) is introduced as a means of creating an adiabatic separation between lambda and the rest of the system. Under these conditions, it is shown that the lambda free energy profile can be directly computed from the adiabatic probability distribution function of lambda without any postprocessing or unbiasing of the output data. The new method is illustrated on two model problems and in the calculation of the solvation free energy of amino acid side-chain analogs in TIP3P water. Comparisons to previous work using thermodynamic integration and free energy perturbation show that the new lambda adiabatic free energy dynamics method results in very precise free energy calculations using significantly shorter trajectories.
提出了一种新的分子动力学方法,用于计算与系统热力学状态或化学成分转变(也称为炼金术转变)相关的自由能。这种新方法扩展了Rosso等人最近提出的绝热动力学方法[《化学物理杂志》116, 4389 (2002)],它基于使用一个额外的自由度λ,该自由度用作表征两种状态的势能函数之间的切换参数。在新方法中,耦合参数λ作为哈密顿量中的一个虚拟动力学变量被引入,并且采用了一组切换函数,这导致在相关热力学端点之间的λ自由能分布中出现一个势垒。因此,这种势垒的存在增强了对端点(λ = 0和λ = 1)区域的采样,这些区域对于计算相关的自由能差最为重要。为了确保有效地跨越势垒,为λ赋予一个高温T(λ),并引入一个虚拟质量m(λ),作为在λ与系统其余部分之间创建绝热分离的一种手段。在这些条件下,结果表明可以直接从λ的绝热概率分布函数计算λ自由能分布,而无需对输出数据进行任何后处理或去偏。在两个模型问题以及在计算TIP3P水中氨基酸侧链类似物的溶剂化自由能中展示了这种新方法。与先前使用热力学积分和自由能微扰的工作进行比较表明,新的λ绝热自由能动力学方法使用明显更短的轨迹就能得到非常精确的自由能计算结果。