Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Setup and Characterization of a Single-Focused Beam Optical Trap for Lithium

Lars Heinen

Published Jan 1, 2017• 0 citations
OpenAlex

Abstract

Within the MOTREMI experiment at the Max-Plank-Institut für Kernphysik a new optical trap was constructed. A already installed magneto-optical trap cools 6Li atoms down to temperatures on the order of 100 μK. From the corresponding atoms an ultracold lithium gas is trapped inside the center of the main vacuum chamber. In the further course of the experiment, ionization measurements with a degenerate quantum gas will be carried out. In order to create theses gases, one needs to surpass the temperature limit of the magneto-optical trap. Traps using a high intensity, far red-detuned focused laser beam are able to achieve temperatures on the order of 100 nK. An intensity stabilization which is able to extend the lifetime of trapped gas was constructed in the scope of this thesis. With the use of two different photodiodes, every intensity level of the laser is covered. The high laser powers which are needed for the trap, can lead to thermal effects in the entire setup. Consequently, the properties of the laser and the optical elements the laser is passing through can change. Therefore, a quantitative analysis of these thermal effects has been carried out. Besides the shift and reduction of the focused laser beam, the thermal effect on the trap size was obtained.

Related papers

Umbau und Inbetriebnahme eines MOTReMi-Aufbaus für zukünftige Experimente mit ultrakaltem 6Li

C. Bogda

This thesis deals with the reconstruction of a MOTRe- Mi apparatus, which represents the combination of a magneto-optical trap (MOT) and a Reaction Microscope (ReMi). With this setup an ultracold degenerate Fermi gas consisting of 6Li atoms will be generated and studied in future. Primarily the Li atoms will be vaporized, precooled in a Zeeman Slower, trapped and stored with the MOT at typical temperatures of a few 100 μK. Within the scope of this thesis initially the parameters of the Zeeman Slower were optimized. For this purpose the magnetic field profiles of the single coils were measured and the ideal coil currents determined. The efficiency and other properties of the Zeeman Slower were calculated with a simulation programme. The focus of this thesis was on planning and reconstructing the laser system and the optical setup for the magneto-optical trap. This included among others the adaptation of the laser frequencies from 7Li to 6Li and the integration of an additional amplifier in order to achieve a higher output power. Using the frequency stabilization scheme of a frequency offset lock ([SEG+99]) it is now possible to tune the laser frequency over a large range at a constant laser power. This is required on the one hand for the later transfer of the atoms to a dipole trap and on the other hand for the imaging of the atom cloud by light absorption at high magnetic fields. Finally the vacuum chamber and the Reaction microscope was baked out and activated at a vacuum of about 7 · 10-10 mbar.

•Jan 1, 2015•0 citations

A Laser Cooled Lithium Beam Source for the Loading of a Magneto-Optical Trap in a Reaction Microscope

Dominik Globig

A new experiment is being built at the Max-Planck-Institut für Kernphysik (MPIK) within the PRIOC project (Precision studies on Ion Collisions) where a reaction microscope (Remi) and a magneto-optical trap (MOT) as target are combined to a so called MOTRemi. This setup will be implemented into the ion storage ring 'Testspeicherring' (TSR) of the MPIK. The world-wide unique combination of these three state-of-the-art technologies shall enable to perform kinematically complete studies of ion-atom collision with unprecedented detail and resolution. In this thesis, a two-dimensional magneto-optical trap (2D-MOT) was developed and tested as a source of slow lithium atoms for the loading of the target MOT. This method allows a very compact setup and oers a collimated beam and a ux of cold atoms comparable to the highest uxes achieved by using laser cooling. The temperature of the atomic beam was determined to be at the scale of a few Kelvin and, thus, it is already an adequate stand-alone target for momentum resolved experiments.

•Jan 1, 2011•0 citations

Implementation of an Optical Dipole Trap for Lithium Atoms

Pascal E. Blessing

Optical dipole traps are often used to provide an ultra-cold atom gas. Red detuned dipole traps are in principal rather easy to implement since they only consist of a focussed laser beam and without great complexity a potential minimum can be achieved. Bigger issues are the optimization of these traps as the intensity noise of the cw laser needs to be stabilized and thermal effects due to the high laser power traveling though the optical elements need to be minimized.

•Jan 1, 2016•0 citations

Tightly confined atoms in optical dipole traps

Matthias C. Schulz

This thesis reports on the design, setup, and operation of a new atom trap apparatus, which is developed to confine few rubidium atoms in ultrahigh vacuum by means of taylored and dynamically variable light potentials (dipole traps), thus making the atoms available for spectroscopy and controlled manipulations. To maintain low background pressure, atoms of a vapour cell are transferred into a cold atomic beam by laser cooling techniques, and accumulated by a magneto-optic trap (MOT) in a separate part of the vacuum system. The laser cooled atoms are then transferred into dipole traps made of focused far-off-resonant laser fields in single or crossed-beam geometry, which are superimposed with the center of the MOT. Gaussian as well as hollow Laguerre-Gaussian (LG01) beam profiles are used with red-detuned and blue-detuned light. Microfabricated dielectric phase objects allow the efficient and robust mode conversion of Gaussian into Laguerre-Gaussian laser beams. Trap geometries can easily be changed due to the highly flexible experimental setup. The dipole trap laser beams have powers up to several hundred milliwatts and are focused to around 10 m. At a detuning of several tens of nanometers from the atomic resonance, the resulting traps are a few millikelvin deep, and the trapped atoms exhibit motional frequencies near 30 kHz, trap light scattering rates of a few hundred photons per second per atom, and storage times of several seconds. The number of dipole-trapped atoms ranges from more than ten thousand to below ten. The dipole-trapped atoms are detected either by a photon counting system with efficient straylight discrimination, or by recapture into the MOT, which is imaged onto a sensitive photodiode and a CCD-camera. Due to the strong AC-Stark shift imposed by the high-intensity trapping light, energy-selective resonant excitation and detection of the stored atoms is possible. The measured energy distribution is consistent with a harmonic potential shape and allows for the determination of temperatures and heating rates. From initial measurements, the thermal energy is found to be about 10 % of the trap depth. Using a crossed-beam geometry with red-detuned laser light, efficient transfer of atoms between the beams is observed. Optimum transfer occurs when the two beams cross at a radial offset, which can qualitatively be understood when the particle energy and geometrical properties of the two-beam trapping potential are considered. Numerical simulations reproduce the general features of the measured transfer efficiency vs. radial beam offset. This experiment is a first step towards dynamically variable potentials. Atoms have been radially confined in a blue-detuned hollow beam, and their decay time has been determined. This configuration is currently extended to a three-dimensionally confining blue-detuned dipole trap. For advanced laser cooling, state manipulation and spectroscopy of trapped atoms, a system of two diode lasers has been set up which are phase-coherently locked with a difference frequency near 6.834 GHz, to drive Raman transitions between the hyperfine-split ground states of 87Rb atoms. Resonances of such a transition have been recorded in a buffer gas loaded rubidium vapour cell with linewidths below 100 Hz.

•Jan 1, 2002•7 citations

Optical Trapping of Li-6 for Studies of Transport in Strongly Interacting Fermions

Christopher K. Angyal

Ultracold gases provide a clean setup for investigating the many-body physics of stronglyinteracting fermions. Due to the universal nature of strongly interacting fermionic systems, an ultracold gas can serve as a quantum simulator for other strongly interacting systems of fermions such as neutron stars and high-Tc superconductors [1] [2]. A better understanding of such systems could potentially have great scientific and technological implications. In this thesis, I describe the construction of an apparatus that can be used for future experiments on ultracold atoms probing questions related to spin and heat transport in a strongly interacting gas of 6Li atoms. Multiple stages of cooling have been successfully completed on the way towards establishing a quantum degenerate ultracold gas of Li-6. To this end a magneto-optical trap (MOT) has been realized with a temperature on the order of ? 1mK, a compressed MOT (cMOT) has been realized with a temperature ? 600?K, and most recently a crossed optical-dipole trap (ODT) with a temperature ? 70?K. The foundations have also been laid for the final stage of atomic trapping in our apparatus, the multi-region trap, or "box trap"; in particular I will describe an optical setup that has been tested and is suitable for use in creating the hollow cylindrical walls or our box trap, which we like to call the "ring beam".

•May 1, 2023•0 citations

A versatile apparatus for fermionic lithium quantum gases based on an interference-filter laser system

Benjamin Gänger, Jan Phieler, Benjamin Nagler +1 more

We report on the design and construction of a versatile setup for experiments with ultracold lithium (Li) gases. We discuss our methods to prepare an atomic beam and laser cool it in a Zeeman slower and a subsequent magneto-optical trap, which rely on established methods. We focus on our laser system based on a stable interference-filter-stabilized, linear-extended-cavity diode laser, so far unreported for lithium wavelengths. Moreover, we describe our optical setup to combine various laser frequencies for cooling, manipulation, and detection of Li atoms. We characterize the performance of our system preparing degenerate samples of Li atoms via forced evaporation in a hybrid crossed-beam optical-dipole trap plus confining magnetic trap. Our apparatus allows one to produce quantum gases of N ≈ 105…106 fermionic lithium-6 atoms at nanokelvin temperatures in cycle times below 10 s. Our optical system is particularly suited to study the dynamics of fermionic superfluids in engineered optical potentials.

Review of Scientific Instruments•Sep 1, 2018•16 citations
Within the MOTREMI experiment at the Max-Plank-Institut für Kernphysik a new optical trap was constructed. A already installed magneto-optical trap cools 6Li atoms down to temperatures on the order of 100 μK. From the corresponding atoms an ultracold lithium gas is trapped inside the center of the main vacuum chamber. In the further course of the experiment, ionization measurements with a degenerate quantum gas will be carried out. In order to create theses gases, one needs to surpass the temperature limit of the magneto-optical trap. Traps using a high intensity, far red-detuned focused laser beam are able to achieve temperatures on the order of 100 nK. An intensity stabilization which is able to extend the lifetime of trapped gas was constructed in the scope of this thesis. With the use of two different photodiodes, every intensity level of the laser is covered. The high laser powers which are needed for the trap, can lead to thermal effects in the entire setup. Consequently, the properties of the laser and the optical elements the laser is passing through can change. Therefore, a quantitative analysis of these thermal effects has been carried out. Besides the shift and reduction of the focused laser beam, the thermal effect on the trap size was obtained.
This thesis deals with the reconstruction of a MOTRe- Mi apparatus, which represents the combination of a magneto-optical trap (MOT) and a Reaction Microscope (ReMi). With this setup an ultracold degenerate Fermi gas consisting of 6Li atoms will be generated and studied in future. Primarily the Li atoms will be vaporized, precooled in a Zeeman Slower, trapped and stored with the MOT at typical temperatures of a few 100 μK. Within the scope of this thesis initially the parameters of the Zeeman Slower were optimized. For this purpose the magnetic field profiles of the single coils were measured and the ideal coil currents determined. The efficiency and other properties of the Zeeman Slower were calculated with a simulation programme. The focus of this thesis was on planning and reconstructing the laser system and the optical setup for the magneto-optical trap. This included among others the adaptation of the laser frequencies from 7Li to 6Li and the integration of an additional amplifier in order to achieve a higher output power. Using the frequency stabilization scheme of a frequency offset lock ([SEG+99]) it is now possible to tune the laser frequency over a large range at a constant laser power. This is required on the one hand for the later transfer of the atoms to a dipole trap and on the other hand for the imaging of the atom cloud by light absorption at high magnetic fields. Finally the vacuum chamber and the Reaction microscope was baked out and activated at a vacuum of about 7 · 10-10 mbar.
A new experiment is being built at the Max-Planck-Institut für Kernphysik (MPIK) within the PRIOC project (Precision studies on Ion Collisions) where a reaction microscope (Remi) and a magneto-optical trap (MOT) as target are combined to a so called MOTRemi. This setup will be implemented into the ion storage ring 'Testspeicherring' (TSR) of the MPIK. The world-wide unique combination of these three state-of-the-art technologies shall enable to perform kinematically complete studies of ion-atom collision with unprecedented detail and resolution. In this thesis, a two-dimensional magneto-optical trap (2D-MOT) was developed and tested as a source of slow lithium atoms for the loading of the target MOT. This method allows a very compact setup and oers a collimated beam and a ux of cold atoms comparable to the highest uxes achieved by using laser cooling. The temperature of the atomic beam was determined to be at the scale of a few Kelvin and, thus, it is already an adequate stand-alone target for momentum resolved experiments.
This thesis reports on the design, setup, and operation of a new atom trap apparatus, which is developed to confine few rubidium atoms in ultrahigh vacuum by means of taylored and dynamically variable light potentials (dipole traps), thus making the atoms available for spectroscopy and controlled manipulations. To maintain low background pressure, atoms of a vapour cell are transferred into a cold atomic beam by laser cooling techniques, and accumulated by a magneto-optic trap (MOT) in a separate part of the vacuum system. The laser cooled atoms are then transferred into dipole traps made of focused far-off-resonant laser fields in single or crossed-beam geometry, which are superimposed with the center of the MOT. Gaussian as well as hollow Laguerre-Gaussian (LG01) beam profiles are used with red-detuned and blue-detuned light. Microfabricated dielectric phase objects allow the efficient and robust mode conversion of Gaussian into Laguerre-Gaussian laser beams. Trap geometries can easily be changed due to the highly flexible experimental setup. The dipole trap laser beams have powers up to several hundred milliwatts and are focused to around 10 m. At a detuning of several tens of nanometers from the atomic resonance, the resulting traps are a few millikelvin deep, and the trapped atoms exhibit motional frequencies near 30 kHz, trap light scattering rates of a few hundred photons per second per atom, and storage times of several seconds. The number of dipole-trapped atoms ranges from more than ten thousand to below ten. The dipole-trapped atoms are detected either by a photon counting system with efficient straylight discrimination, or by recapture into the MOT, which is imaged onto a sensitive photodiode and a CCD-camera. Due to the strong AC-Stark shift imposed by the high-intensity trapping light, energy-selective resonant excitation and detection of the stored atoms is possible. The measured energy distribution is consistent with a harmonic potential shape and allows for the determination of temperatures and heating rates. From initial measurements, the thermal energy is found to be about 10 % of the trap depth. Using a crossed-beam geometry with red-detuned laser light, efficient transfer of atoms between the beams is observed. Optimum transfer occurs when the two beams cross at a radial offset, which can qualitatively be understood when the particle energy and geometrical properties of the two-beam trapping potential are considered. Numerical simulations reproduce the general features of the measured transfer efficiency vs. radial beam offset. This experiment is a first step towards dynamically variable potentials. Atoms have been radially confined in a blue-detuned hollow beam, and their decay time has been determined. This configuration is currently extended to a three-dimensionally confining blue-detuned dipole trap. For advanced laser cooling, state manipulation and spectroscopy of trapped atoms, a system of two diode lasers has been set up which are phase-coherently locked with a difference frequency near 6.834 GHz, to drive Raman transitions between the hyperfine-split ground states of 87Rb atoms. Resonances of such a transition have been recorded in a buffer gas loaded rubidium vapour cell with linewidths below 100 Hz.
Ultracold gases provide a clean setup for investigating the many-body physics of stronglyinteracting fermions. Due to the universal nature of strongly interacting fermionic systems, an ultracold gas can serve as a quantum simulator for other strongly interacting systems of fermions such as neutron stars and high-Tc superconductors [1] [2]. A better understanding of such systems could potentially have great scientific and technological implications. In this thesis, I describe the construction of an apparatus that can be used for future experiments on ultracold atoms probing questions related to spin and heat transport in a strongly interacting gas of 6Li atoms. Multiple stages of cooling have been successfully completed on the way towards establishing a quantum degenerate ultracold gas of Li-6. To this end a magneto-optical trap (MOT) has been realized with a temperature on the order of ? 1mK, a compressed MOT (cMOT) has been realized with a temperature ? 600?K, and most recently a crossed optical-dipole trap (ODT) with a temperature ? 70?K. The foundations have also been laid for the final stage of atomic trapping in our apparatus, the multi-region trap, or "box trap"; in particular I will describe an optical setup that has been tested and is suitable for use in creating the hollow cylindrical walls or our box trap, which we like to call the "ring beam".
We report on the design and construction of a versatile setup for experiments with ultracold lithium (Li) gases. We discuss our methods to prepare an atomic beam and laser cool it in a Zeeman slower and a subsequent magneto-optical trap, which rely on established methods. We focus on our laser system based on a stable interference-filter-stabilized, linear-extended-cavity diode laser, so far unreported for lithium wavelengths. Moreover, we describe our optical setup to combine various laser frequencies for cooling, manipulation, and detection of Li atoms. We characterize the performance of our system preparing degenerate samples of Li atoms via forced evaporation in a hybrid crossed-beam optical-dipole trap plus confining magnetic trap. Our apparatus allows one to produce quantum gases of N ≈ 105…106 fermionic lithium-6 atoms at nanokelvin temperatures in cycle times below 10 s. Our optical system is particularly suited to study the dynamics of fermionic superfluids in engineered optical potentials.