Triana Johan F, Peláez Daniel, Sanz-Vicario José Luis
Grupo de Fı́sica Atómica y Molecular, Instituto de Fı́sica, Universidad de Antioquia , AA1226 Medellı́n, Colombia.
Laboratoire de Physique des Lasers, Atomes et Molécules (PhLAM), Unité Mixte de Recherche (UMR) 8523, Université Lille 1 , Bât. P5, 59650 Villeneuve d'Ascq Cedex, France.
J Phys Chem A. 2018 Mar 1;122(8):2266-2278. doi: 10.1021/acs.jpca.7b11833. Epub 2018 Feb 16.
The quantum photodynamics of a simple diatomic molecule with a permanent dipole immersed within an optical cavity containing a quantized radiation field is studied in detail. The chosen molecule under study, lithium fluoride (LiF), is characterized by the presence of an avoided crossing between the two lowest Σ potential energy curves (covalent-ionic diabatic crossing). Without field, after prompt excitation from the ground state 1 Σ, the excited nuclear wave packet moves back and forth in the upper 2 Σ state, but in the proximity of the avoided crossing, the nonadiabatic coupling transfers part of the nuclear wave packet to the lower 1 Σ state, which eventually leads to dissociation. The quantized field of a cavity also induces an additional light crossing in the modified dressed potential energy curves with similar transfer properties. To understand the entangled photonic-nuclear dynamics, we solve the time-dependent Schrödinger equation by using the multiconfigurational time-dependent Hartree method (MCTDH). The single mode quantized field of the cavity is represented in the coordinate space instead of in the Fock space, which allows us to deal with the field as an additional vibrational mode within the MCTDH procedure on equal footing. We prepare the cavity with different quantum states of light, namely, Fock states, coherent states, and squeezed coherent states. Our results reveal pure quantum light effects on the molecular photodynamics and the dissociation yields of LiF, which are quite different from the light-undressed case and which cannot be described in general by a semiclassical approach using classical electromagnetic fields.
详细研究了一个具有永久偶极矩的简单双原子分子,浸没在包含量子化辐射场的光学腔内时的量子光动力学。所研究的选定分子是氟化锂(LiF),其特征在于两个最低Σ势能曲线之间存在一个避免交叉(共价 - 离子非绝热交叉)。在无场情况下,从基态1Σ迅速激发后,激发的核波包在较高的2Σ态中来来回回移动,但在避免交叉附近,非绝热耦合将部分核波包转移到较低的1Σ态,最终导致解离。腔的量子化场也会在具有类似转移特性的修正缀饰势能曲线中诱导额外的光交叉。为了理解纠缠的光子 - 核动力学,我们使用多组态含时哈特里方法(MCTDH)求解含时薛定谔方程。腔的单模量子化场在坐标空间而非福克空间中表示,这使我们能够在MCTDH过程中把场当作一个额外的振动模式同等对待。我们用不同的光量子态,即福克态、相干态和压缩相干态来制备腔。我们的结果揭示了纯量子光对LiF分子光动力学和解离产率的影响,这与无光缀饰情况有很大不同,并且一般不能用使用经典电磁场的半经典方法来描述。