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Experimental studies on a dark magneto-optical trap for 85Rb

Laura Russell, Rajesh Kumar, Vibhuti Bhushan Tiwari, Síle Nic Chormaic

Published Jun 25, 2013• 0 citations
OpenAlex

Abstract

This work is concerned with density enhancements in a laser-cooled sample of 85Rb using a dark magneto-optical trap (MOT). The density of atoms in a standard MOT is limited to approximately ~1011 atoms/cm3 due to radiation pressure and collisions. The dark MOT (DMOT) circumvents problems associated with radiation pressure in the atom cloud. To create a DMOT, a donut-shaped repump beam is projected on to the cloud of 85Rb. The dark region in the center of the donut is attenuated by ~10^(-4) compared to the bright outer ring. Atoms which encounter this dark region in the repump beam are scattered to the lower hyperfine ground level, F = 2, otherwise known as the dark hyperfine level. Additionally, a depump beam is used to force more atoms into F = 2. Results using free-space spectroscopy are presented to demonstrate the effect of the donut-shaped repump beam and the depump beam on the population distribution of the atoms in the hyperfine ground states. A tapered optical fiber is used to measure the quality of the DMOT via a parameter, p, and a strong population transfer from the bright, F = 3, to the dark, F = 2, hyperfine ground level is demonstrated. The tapered fiber, with a waist of ~ 1 micron, is made from commercially-available optical fiber and is used to detect fluorescence from the cold 85Rb coupled into the fiber guided modes. This work lays the foundation for optical nanofiber absorption spectroscopy with a small number of atoms in an optically-dense system.

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•Jan 1, 1995•0 citations
This work is concerned with density enhancements in a laser-cooled sample of 85Rb using a dark magneto-optical trap (MOT). The density of atoms in a standard MOT is limited to approximately ~1011 atoms/cm3 due to radiation pressure and collisions. The dark MOT (DMOT) circumvents problems associated with radiation pressure in the atom cloud. To create a DMOT, a donut-shaped repump beam is projected on to the cloud of 85Rb. The dark region in the center of the donut is attenuated by ~10^(-4) compared to the bright outer ring. Atoms which encounter this dark region in the repump beam are scattered to the lower hyperfine ground level, F = 2, otherwise known as the dark hyperfine level. Additionally, a depump beam is used to force more atoms into F = 2. Results using free-space spectroscopy are presented to demonstrate the effect of the donut-shaped repump beam and the depump beam on the population distribution of the atoms in the hyperfine ground states. A tapered optical fiber is used to measure the quality of the DMOT via a parameter, p, and a strong population transfer from the bright, F = 3, to the dark, F = 2, hyperfine ground level is demonstrated. The tapered fiber, with a waist of ~ 1 micron, is made from commercially-available optical fiber and is used to detect fluorescence from the cold 85Rb coupled into the fiber guided modes. This work lays the foundation for optical nanofiber absorption spectroscopy with a small number of atoms in an optically-dense system.
Spectral characteristics of rubidium atoms confined in a dark magneto-optical trap (DMOT) are measured, including probe absorption spectra and atom density as a function of the cooling and repumping laser frequencies. The trap can capture and cool more than 2.5 × 10 8 rubidium atoms, confining them in a hyperfine state weakly perturbed by the laser beams used to form the trap. The optical density of the trapped atomic cloud approaches 9. A qualitative model of the DMOT operation is presented, based on the experimental results obtained.
In this paper, ultracold atoms and molecules in a dark magneto-optical trap (MOT) are studied via depumping the cesium cold atoms into the dark hyperfine ground state. The collision rate is reduced to 0.45 s −1 and the density of the atoms is increased to 5.6 × 10 11 cm −3 when the fractional population of the atoms in the bright hyperfine ground state is as low as 0.15. The vibrational spectra of the ultracold cesium molecules are also studied in a standard MOT and in a dark MOT separately. The experimental results are analyzed by using the perturbative quantum approach.
In this paper,ultracold atoms and molecules in a dark magneto-optical trap(MOT) are studied via depumping the cesium cold atoms into the dark hyperfine ground state.The collision rate is reduced to 0.45s-1 and the density of the atoms is increased to 5.6×1011cm-3 when the fractional population of the atoms in the bright hyperfine ground state is as low as 0.15.The vibrational spectra of the ultracold cesium molecules are also studied in a standard MOT and in a dark MOT separately.The experimental results are analyzed by using the perturbative quantum approach.
We have performed release-recapture temperature measurements of laser-cooled 85Rb atoms using an optical nanofibre (ONF) in a magneto-optical trap (MOT). The effects of changing the cooling laser light-shift parameter on the temperature of the cold atoms and spring constant of the trap are studied. By varying the cold atom number density near the ONF, the onset of the multiple scattering regime is observed without the need for an estimation of the atom cloud size. Moreover, this sensitive ONF assisted release-recapture technique is easily able to detect any optical misalignment of the cooling laser beams in the MOT. Keywords: laser cooling, optical nanofiber, rubidium, release-recapture, temperature
ENGLISH ABSTRACT: A Magneto Optical Trap (MOT) is a configuration formed by three orthogonal pairs of counterpropagating circularly polarized laser beams and a magnetic field gradient. A MOT is used to cool, capture and trap large numbers of atoms in vacuum at very low temperature in K range. In this thesis the development of an experimental setup for realising a MOT of 87Rb atoms is presented. The atomic structure of Rb and the theoretical background of laser cooling and magneto optical trapping was reviewed. The influence of rubidium background pressure in the vacuum system, the laser beam size and the power and frequency on the number of the trapped atoms were studied in literature. The trapping and repumping lasers were characterised experimentally. Six circularly polarised trapping beams with equal power were formed and properly aligned to intersect at the center of the trapping cell. Two optical setups were designed and exploited to investigate and optimise the trapping beam polarisation. The repumping laser beam was successfully aligned and colinearly combined into all the trapping beams. Three different experimental setups for saturated absorption spectroscopy were developed. Saturated absorption spectra showing the hyperfine structure of both 85Rb and 87Rb isotopes were measured and are discussed. Using two saturated absorption spectroscopy setups, the frequencies of both lasers were successfully locked to the trapping and repumping transitions of 87Rb respectively. A rectangular trapping cell was designed and attached to the vacuum system. A pressure of about 10­¯7 mbar was achieved. The magnetic field coils were characterised and affixed on both sides of the cell in an anti-Helmholtz configuration. Setups for imaging and quantification of the 87Rb atoms in the MOT were designed. Finally, the procedures for demonstrating a MOT are presented. In conclusion, the current status of the project is reported, with recommendations for the future work.
A detailed experimental and theoretical investigation of a magneto-optical trap for caesium atoms is presented. Particular emphasis has been placed on achieving high spatial number densities and low temperatures. Optimizing both of these together enables efficient evaporative cooling from a conservative trap, a procedure which has recently led to the first observations of Bose-Einstein condensation in a dilute atomic vapour. The behaviour of a magneto-optical trap is nominally determined by four independent parameters: the detuning and intensity of the light field, the magnetic field gradient and the number of trapped atoms. A model is presented which incorporates previous treatments into a single description of the trap that encompasses a wide range of its behaviour. This model was tested quantitatively by measuring the temperature of the cloud and its spatial distribution as a function of the four parameters. The maximum density was found to be limited both by the reabsorption of photons scattered within the cloud and by a reduction of the confining force at small light shifts. The nonlinear variation with position of the restoring force was found to be significant in limiting the number of atoms confined to a high density. A maximum density in phase space (defined as the number of atoms in a box with sides of dimension one thermal de Broglie wavelength) of (1.5 ± 0.5) x 10-5 was observed, with a spatial density of 1.5 x 1011 atoms per cm3. Cold collision losses from a caesium magneto-optical trap have been studied with the purpose of assessing their influence on spatial densities. In contrast to previous measurements of similar quantities, these measurements did not require the use of an ultra-low (< 10-10 Torr) background vapour pressure. The dependence of the cold collision loss coefficient β on the trapping intensity was measured to permit identification of the different cold collision processes. The largest loss rates observed were those due to hyperfine structure-changing collisions, with a coefficient β = (2±1) x 10-10cm3s-1. A study is presented of a modified magneto-optical trap in which a fraction of the population is shelved into a hyperfine level that does not interact with the trapping light. In this so-called "dark" magneto-optical trap, improved densities of nearly 1012cm-3 have been previously reported for sodium. The application of the technique to caesium is not straightforward due to the larger excited state hyperfine splittings. A simple theory for caesium is presented and its main predictions verified by measurements of density, number and temperature. A density of nearly 1012cm,-3 was indeed obtained but at a temperature substantially higher than in the conventional magneto-optical trap.