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Bulletin of the American Physical Society

Towards microwave modulation in a wavelength-tuned magneto-optical trap

Aaron Allen, Stephen R. Segal, Evan A. Salim, Marika Meertens, Dana Anderson

Published Nov 13, 2009• 0 citations
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Abstract

Aaron Allen  ξ Physics REU 2009 JILA, National Institute of Standards and Technology and University of Colorado, and Department of Physics, University of Colorado-Boulder, Boulder, CO 80309, USA  Department of Physics and Astronomy, Clemson University, Clemson, SC 29634 ξ Department of Mathematical Sciences, Clemson University, Clemson, SC 29634 In this project, I present a new method for trapping Rubidium-87 atoms. The method proposed is microwave modulation of an external cavity diode laser. The modulation is designed so as to produce frequency sidebands for hyperfine pumping in addition to the main cooling frequency. It is designed for use in magneto-optical trapping. GENERAL MOTIVATION Doppler cooling of atoms is a central process in the field of atomic, molecular, and optical (AMO) physics. Doppler cooling is central to laser trapping, the formation of Bose-Einstein Condensates (BEC’s), the formation of Fermionic Condensates, advances in quantum computing, and proposed schemes in molecular trapping. Doppler cooling allows atoms to be slowed down many orders of magnitude below their room temperature velocity, which allows these atoms to be more easily controlled and studied. Doppler cooling can best be understood by its relationship to the thermodynamics of atoms. A collection of atoms at room temperature has an average velocity, v , that follows from its kinetic energy and the Maxwell-Boltzman distribution [1];

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Aaron Allen  ξ Physics REU 2009 JILA, National Institute of Standards and Technology and University of Colorado, and Department of Physics, University of Colorado-Boulder, Boulder, CO 80309, USA  Department of Physics and Astronomy, Clemson University, Clemson, SC 29634 ξ Department of Mathematical Sciences, Clemson University, Clemson, SC 29634 In this project, I present a new method for trapping Rubidium-87 atoms. The method proposed is microwave modulation of an external cavity diode laser. The modulation is designed so as to produce frequency sidebands for hyperfine pumping in addition to the main cooling frequency. It is designed for use in magneto-optical trapping. GENERAL MOTIVATION Doppler cooling of atoms is a central process in the field of atomic, molecular, and optical (AMO) physics. Doppler cooling is central to laser trapping, the formation of Bose-Einstein Condensates (BEC’s), the formation of Fermionic Condensates, advances in quantum computing, and proposed schemes in molecular trapping. Doppler cooling allows atoms to be slowed down many orders of magnitude below their room temperature velocity, which allows these atoms to be more easily controlled and studied. Doppler cooling can best be understood by its relationship to the thermodynamics of atoms. A collection of atoms at room temperature has an average velocity, v , that follows from its kinetic energy and the Maxwell-Boltzman distribution [1];
The advent of the laser opened the way to the development of powerful new methods for manipulating and cooling atoms which were exploited in the realization of Bose–Einstein condensation in alkali atom vapours. To set the stage we describe a typical experiment, which is shown schematically in Fig. 4.1. A beam of sodium atoms emerges from an oven at a temperature of about 600 K, corresponding to a speed of about 800 m s –1 , and is then passed through a so-called Zeeman slower, in which the velocity of the atoms is reduced to about 30 m s –1 , corresponding to a temperature of about 1 K. In the Zeeman slower, a laser beam propagates in the direction opposite that of the atomic beam, and the radiation force produced by absorption of photons retards the atoms. Due to the Doppler effect, the frequency of the atomic transition in the laboratory frame is not generally constant, since the atomic velocity varies. However, by applying an inhomogeneous magnetic field designed so that the Doppler and Zeeman effects cancel, the frequency of the transition in the rest frame of the atom may be held fixed. On emerging from the Zeeman slower the atoms are slow enough to be captured by a magneto-optical trap (MOT), where they are further cooled by interactions with laser light to temperatures of order 100 μK. Another way of compensating for the changing Doppler shift is to increase the laser frequency in time, which is referred to as ‘chirping’. In other experiments the MOT is filled by transferring atoms from a second MOT where atoms are captured directly from the vapour.
We have laser cooled an atomic beam of rubidium with diode lasers and have used these slow atoms to load a magneto-optical trap. The cooling is performed with the frequency-chirp method,1,2 in which the laser's frequency is ramped linearly (by the injection currant) to maintain resonance with the decelerating atoms. Two synchronously chirped lasers are required to prevent optical hyperfine pumping of the ground state. The chirp typically covers 500 MHz in 10 ms. At the end of each ramp, the resulting velocity distribution is measured with a pulsed probe laser. By varying the end point of the chirp, we are able to obtain slow atoms with average velocities ranging from 200 to −50 m/s. The widths of the velocity distributions are measured to be approximately 40 m/s. This relatively large width results from the inherent linewidth (~30 MHz) of the free-running diode lasers used for both cooling and probing.
Research interest in designing sources of cold atoms has significantly increased during the past ten years with the development of suitable laser sources for magneto-optical trapping and the further mastering of evaporative cooling in order to achieve Bose-Einstein condensation. The magneto-optical trap is now viewed as a standard research facility worldwide and has opened up many new exciting research directions in atomic physics. One area of interest is that of combining spherical microcavities with cold atomic sources in order to achieve efficient photon exchange between the cavity and atom for further understandings of cavity quantum electrodynamics. This could eventually lead to atom entanglement via photon exchange which would have implications for quantum logic design. However, initial attempts to achieve such interactions have been hindered by inadequate control and manipulation of the cold atom source. Here, we present work on designing and building an ultra-stable source of magneto-optically cooled rubidium atoms with a temperature in the tens of microKelvin range. We discuss the different cooling mechanisms involved in the process and present a suitable experimental arrangement including details on the ultra-high vacuum chamber, the laser systems being used and the source of rubidium vapour. Finally, we discuss some future direction for the research including the diffraction of atoms from gratings and micron-sized objects and the parameter control of the cloud of atoms.
Magneto optical traps brilliantly combine semi-classical optics with modern physics. By carefully controlling the polarization and frequency of laser beams, it is possible to trap and cool atoms down to the millikelvin range at a relatively low cost. This has opened previously inaccessible physical domains to enterprising physicists all around the world, and is responsible for some of the most interesting experiments being conducted in AMO sciences today. We attempted to employ magneto optical trapping techniques to generate a sample of Rubidium 87 atoms for use in the development of multidimensional Fourier transform spectroscopy with comb lasers. My work entailed the construction and characterization of two external cavity diode lasers (ECDLs), as well as the assembly of a MOT system, which is as of 04/07/2015 not operational. Future work will focus on debugging the system.
The advent of the laser opened the way to the development of powerful methods for producing and manipulating cold atomic gases. To set the stage we describe a typical experiment, which is shown schematically in Fig. 4.1. A beam of sodium atoms emerges from an oven at a temperature of about 600 K, corresponding to a speed of about 800 m s −1 , and is then passed through a so-called Zeeman slower, in which the velocity of the atoms is reduced to about 30 m s −1 , corresponding to a temperature of about 1 K. In the Zeeman slower, a laser beam propagates in the direction opposite that of the atomic beam, and the radiation force produced by absorption of photons retards the atoms. Due to the Doppler effect, the frequency of the atomic transition in the laboratory frame is not generally constant, since the atomic velocity varies. However, by applying an inhomogeneous magnetic field designed so that the Doppler and Zeeman effects cancel, the frequency of the transition in the rest frame of the atom may be held fixed. On emerging from the Zeeman slower the atoms are slow enough to be captured by a magneto-optical trap (MOT), where they are further cooled by interactions with laser light to temperatures of order 100 μK. Another way of compensating for the changing Doppler shift is to increase the laser frequency in time, which is referred to as ‘chirping’.
The theory of cooling neutral atoms to microkelvin temperatures using a magneto optical trap will be presented. The system that is discussed uses a stabilized grating tuned diode laser that is controlled using feedback from a saturation absorption spectrophotometer to produce narrow band continuously tunable IR light for trapping rubidium atoms. A description of the design and construction of each of the components used to create the magneto optical trap will also be discussed. In the final section a description of an exceptionally accurate atomic clock that is used to measure the natural resonance frequency of laser cooled cesium atoms is also presented.