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Optik & Photonik

Specialized Fiber Collimators

Anja Krischke, Michael Schulz, Christian Knothe, Ulrich Oechsner

Published May 1, 2014• 0 citations
Publisher

Abstract

Abstract The general interest in the investigation of ultra‐cold atoms and their distinct features has been constantly growing over the last few decades [1]. Whereas in the beginning, the process of cooling down presented the major challenge, now the extraordinary features of these ultra‐cold systems — for example Bose‐Einstein‐Condensates‐motivate researchers world‐wide to look closer than ever.

DOI
10.1002/opph.201400044

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Abstract The general interest in the investigation of ultra‐cold atoms and their distinct features has been constantly growing over the last few decades [1]. Whereas in the beginning, the process of cooling down presented the major challenge, now the extraordinary features of these ultra‐cold systems — for example Bose‐Einstein‐Condensates‐motivate researchers world‐wide to look closer than ever.
Abstract Over the last two decades, the interest in the investigation of atoms at ultralow temperatures has increased substantially, as is reflected in the number of Nobel prizes awarded during this time. The major focus has shifted from primarily cooling down atoms as close as possible to absolute zero and towards the experimental investigation of these already cooled atoms. Fiber‐optical components designed for the accomplishment of these goals assist researchers all over the world in concentrating their experimental effort on their endeavours with ultra‐cold atoms.
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Ultra-cold atoms have become indispensable in quantum sensing, quantum computing, and quantum communication applications, as well as in fundamental sciences. In quantum sensing, they enable precision measurements with outstanding sensitivities that can be of great benefit in navigation, geodesy, and fundamental physics applications. The sensitivity of the atom interferometers used herefore typically scales with the square of the interrogation time. Therefore, in atom interferometric measurements, one seeks ensembles that feature a particularly low internal kinetic energy and can thus be detected after a long time-of-flight. The lowest values are achieved using Bose-Einstein condensates in conjunction with delta-kick collimation, a technique for the collimation of the atomic wave function. Bose-Einstein condensation can be achieved using a multi-stage laser cooling scheme, followed by evaporative cooling, which finally brings the temperature down to the critical temperature, typically in the nanokelvin regime. In addition to the low thermal spread, microgravity enables particularly long observation times, as it avoids limitations of the interrogation time due to vacuum chamber constraints, which are present when falling freely under the influence of gravity. Additionally, microgravity enables measurements that are not possible under normal gravity conditions, such as buoyancy-free miscibility studies, truly uniform potentials, and advanced cold atom quantum memories, which are projected to feature unprecedented time-bandwidth products. For the preparation of a Bose-Einstein condensate, two techniques are widely used in science, namely magnetic traps and optical dipole traps. For microgravity missions, magnetic traps on atom chips have been used in nearly all setups so far due to their particularly low SWAP budget and high cold atom flux. In contrast, ground-based experiments often prefer optical traps due to their higher versatility, full optical access, and the absence of surfaces in proximity to the atoms, which is fundamental for precision measurements. Additionally, optical traps enable the manipulation of intra- and inter-species scattering lengths using Feshbach resonances. Compared to atom chip traps, they also feature an intrinsically better symmetry of the trapping potential, in theory leading to fewer aberrations in matter-wave optics. The latter could enable the generation of ensembles in the yet unreached femtokelvin regime using delta-kick collimation with fewer perturbations. This thesis is about the realization of a 1064nm optical dipole trap set up for the microgravity environment of the Bremen Drop Tower. It aims to highlight the advantages of optical traps in conjunction with microgravity and prepare optical trapping technology for use in future microgravity and space missions. The thesis describes the experimental setup, the direct loading process, the characterization of the optical potential, and the optimization and investigation of the evaporative cooling in the optical dipole trap. For the evaporation process, the influence of gravity is comprehensively investigated through analytical calculations and microgravity tests. Bose-Einstein condensation is demonstrated, proving the achievement of condensation through absorption imaging of the spatial distribution, tests on the free evolution of the ensemble, and investigation of the phase-space densities achieved. Up to (74 ± 4)% condensation of an ensemble featuring (30 000 ± 13 000) atoms at a kinetic temperature of (37 ± 3) nK is demonstrated. The evaporation shows high efficiency down to a 3 s evaporation time, while a critical phase-space density can be achieved within (1.29 ± 0.07) s using an even faster evaporation ramp. This opens the door to fundamental physics experiments on Bose-Einstein condensates in microgravity, as well as applications pursuing atomic ensembles with exceptionally low expansion velocities.