Laboratory of Physical Chemistry, ETH Zurich, Vladimir-Prelog-Weg 2, 8057 Zurich, Switzerland.
Laboratoire Aimé Cotton, CNRS, Univ Paris-Sud 11, ENS-Cachan, Campus d'Orsay Batiment 505, 91405 Orsay, France.
Phys Rev Lett. 2014 Nov 7;113(19):193001. doi: 10.1103/PhysRevLett.113.193001. Epub 2014 Nov 4.
We observe the direct excitation of pairs of Cs atoms from the ground state to molecular states correlating asymptotically to nsn'f asymptotes. The molecular resonances are interpreted as originating from the dipole-quadrupole interaction between the nsn'f pair states and close-by npnp asymptotes (22≤n≤32). This interpretation is supported by Stark spectroscopy of the pair states and a detailed modeling of the interaction potentials. The dipole-quadrupole interaction mixes electronic states of opposite parity and, thus, requires a coupling between electronic and nuclear motion to conserve the total parity of the system. This non-Born-Oppenheimer coupling is facilitated by the near-degeneracy of even- and odd-L partial waves in the atom-atom scattering which have opposite parity.
我们观察到从基态直接激发 Cs 原子对到渐近关联到 nsn'f 渐近线的分子态。分子共振被解释为源于 nsn'f 对态与附近 npnp 渐近线(22≤n≤32)之间的偶极-四极相互作用。这种解释得到了对态的 Stark 光谱和相互作用势的详细建模的支持。偶极-四极相互作用混合了相反宇称的电子态,因此需要电子和核运动之间的耦合来守恒系统的总宇称。这种非玻恩-奥本海默耦合是由原子-原子散射中偶极和奇极 L 部分波的近简并性促进的,它们具有相反的宇称。