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The energy-conserving dynamics of quantum-classical systems based on quantum trajectories

机译:基于量子轨迹的量子古典系统的节能动力学

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The method, described in the paper, incorporates ideas of the Bohmian formulation of quantum mechanics into a trajectory approach designed for systems comprised of light (quantum) and heavy (nearly classical) particles. The goal is to treat all degrees of freedom on the same footing but, for practical reasons, to include the quantum-mechanical effects into dynamics for just the light particles. The total wavefunction, taken as a product of slow and fast components representing the heavy and light particles respectively is represented in terms of trajectories. The fast component depends on the trajectory-guided configurations of the heavy particles. The initial conditions for the trajectories are defined by the full-dimensional initial wavefunction according to Bohm's prescription of associating the trajectory momentum with the gradient of the wavefunction phase. The time-dependent Schrödinger equation is solved for the quantum degrees of freedom using an ensemble of the quantum trajectories (or other time-propagation method) for each guiding trajectory of the classical subspace. Neglect of the quantum force acting on the heavy particles allows decoupling of the quantum calculations associated with different guiding trajectories. The approach allows reconstruction of the full-dimensional wavefunction and conserves the total wavefunction energy as illustrated for the vibrationally non-adiabatic model.View full textDownload full textKeywordsquantum dynamics, approximate trajectories, quantum/classicalRelated var addthis_config = { ui_cobrand: "Taylor & Francis Online", services_compact: "citeulike,netvibes,twitter,technorati,delicious,linkedin,facebook,stumbleupon,digg,google,more", pubid: "ra-4dff56cd6bb1830b" }; Add to shortlist Link Permalink http://dx.doi.org/10.1080/00268976.2012.675449
机译:本文中描述的方法将量子力学的玻姆公式的构想纳入了为由轻(量子)和重(几乎是经典)粒子组成的系统设计的轨迹方法。目标是在相同的立足点上对待所有自由度,但出于实际原因,将量子力学效应仅包含在轻粒子的动力学中。总波函数是分别表示重粒子和轻粒子的慢速分量和快速分量的乘积,以轨迹表示。快速成分取决于重粒子的轨迹引导配置。轨迹的初始条件由全尺寸的初始波函数定义,这是根据将轨迹动量与波函数相位的梯度相关联的Bohm处方进行的。对于经典子空间的每个引导轨迹,使用量子轨迹的集合(或其他时间传播方法)来求解与时间相关的Schrödinger方程的量子自由度。忽略作用在重粒子上的量子力可以使与不同引导轨迹相关的量子计算解耦。该方法允许重建完整的波函数并节省总的波函数能量,如振动非绝热模型所示。查看全文下载全文关键字量子动力学,近似轨迹,量子/经典相关变量var addthis_config = {ui_cobrand:“ Taylor&Francis Online ”,services_compact:“ citeulike,网络振动,微博,technorati,美味,linkedin,facebook,stumbleupon,digg,google,更多”,发布号:“ ra-4dff56cd6bb1830b”};添加到候选列表链接永久链接http://dx.doi.org/10.1080/00268976.2012.675449

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