Interferometry using magnetic sensitive states

Abstract

Atomic interferometry is a very sensitive technique in precision measurements. In this PhD work we explore ways to improve certain aspects of atomic interferometry. We show that there are some advantages on using magnetic sensitive states. We introduce the required infrastructures to implement Ramsey type interferometry on particular transitions. Using a Magneto Optical Trap (MOT) which is the main prerequisite, the atoms are trapped and cooled. The trapping procedure with the MOT requires ingredients such as lasers, the homogeneous and inhomogeneous magnetic elds, the chamber containing the sample, the vacuum system and the detection part (see Chapter 2). At the beginning of my PhD, this facility for trapping the rubidium atoms was available. Later on we upgraded the vacuum system. During this PhD work we could further cool down the trapped sample thanks to the optical molasses technique. We maintain the atoms at temperatures typically below some tenths of micro Kelvin. The coherent manipulation of the atoms is the signi cant part of this thesis since we aim to do atomic interferometry. Using radiations in microwave domain, it is feasible to couple any two states and do the Rabi oscillations between the hyper ne and Zeeman levels. My rst work as a PhD student was to contribute in the Dual Isotope MOT (DIMOT) experiment (see Chapter 3). The idea was to trap both isotopes of rubidium simultaneously by using only single laser and an Electro-Optical Modulator (EOM). This work introduces huge simpli cations on the optical part and is extendable to trap more isotopes at the same time. The experiment has the optical and RF parts and my contribution was to complete the RF part. Starting all the atoms at the particular initial point for the interferometry takes us some considerable time to be sure that we correctly transfer the atomic population into the desired state (see the discussion in Chapter 4). From that point we focused on two transitions to use the Ramsey type interferometer. Each of these two transitions have an optimum operating point in order to be far from the magnetic eld uctuations since the interferometers are quite sensitive to the eld perturbations sensed from the environment. At the end we aim to combine these two transitions of interest to make a dual interferometer (see Chapter 6). The idea is to obtain the minimum magnetic sensitivity at a tunable magnetic eld by changing the fraction of atoms in each interferometer. The dual interferometer may be useful in applications where low magnetic sensitivity is required at a particular magnetic eld.