Abstract
Polar molecules offer a new platform for quantum simulation of systems with long-range interactions, based on the electrostatic interaction between their electric dipole moments. Here, we report the development of coherent quantum state control using microwave fields in 40Ca19F and 87Rb133Cs molecules, a crucial ingredient for many quantum simulation applications. We perform Ramsey interferometry measurements with fringe spacings of ∼1 kHz and investigate the dephasing time of a superposition of N = 0 and N = 1 rotational states when the molecules are confined. For both molecules, we show that a judicious choice of molecular hyperfine states minimises the impact of spatially varying transition-frequency shifts across the trap. For magnetically trapped 40Ca19F we use a magnetically insensitive transition and observe a coherence time of 0.61(3) ms. For optically trapped 87Rb133Cs we exploit an avoided crossing in the AC Stark shifts and observe a maximum coherence time of 0.75(6) ms.
Highlights
In this paper we explore the potential of ultracold molecules for quantum simulation
We motivate our study of rotational coherence by illustrating how the rotational degrees of freedom can be used to encode models of quantum magnetism
The typical energy scale associated with vibrations is 50 K or more; the ultracold molecules we consider are in a single vibrational state, and we focus on the rotational degree of freedom
Summary
Jesús Aldegunde , Jordi Mur-Petit , Dieter Jaksch4,5 , Jeremy M Hutson , B E Sauer , M R Tarbutt and Simon L Cornish. Kingdom 2 Centre for Cold Matter, Blackett Laboratory, Imperial College London, Prince Consort Road, London SW7 2AZ, United Kingdom 3 Departamento de Quimica Fisica, Universidad de Salamanca, E-37008, Salamanca, Spain. Any further distribution of 8 Authors to whom any correspondence should be addressed
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