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Chinese Physics Letters

Realization of Green MOT for Ytterbium Atoms

Zhao Peng-Yii, Xiong Zhuan-Xian, Yun Long, Lingxiang He, Baolong Lü

Published Aug 1, 2009• 12 citations
Publisher

Abstract

We report the experimental realization of a magneto-optical trap (MOT) of 174 Yb atoms operating on the 1 So− 3 P 1 intercombination transition at 555.8 nm. The green MOT is loaded by a Zeeman-slowed atomic beam. In order to increase the capture velocity of the MOT, we use the trapping laser beams consisting of five discrete frequency components obtained by modulating the laser light through an electro-optic modulator. The trapped atomic number of the 174 Yb isotope is about 6.2 × 10 5 , and the temperature of the cold atomic cloud is estimated to be about 100 μK. The success of the green MOT is an important step towards the goal of an ytterbium optical clock.

DOI
10.1088/0256-307x/26/8/083702

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We report the experimental realization of a magneto-optical trap (MOT) of 174 Yb atoms operating on the 1 So− 3 P 1 intercombination transition at 555.8 nm. The green MOT is loaded by a Zeeman-slowed atomic beam. In order to increase the capture velocity of the MOT, we use the trapping laser beams consisting of five discrete frequency components obtained by modulating the laser light through an electro-optic modulator. The trapped atomic number of the 174 Yb isotope is about 6.2 × 10 5 , and the temperature of the cold atomic cloud is estimated to be about 100 μK. The success of the green MOT is an important step towards the goal of an ytterbium optical clock.
We report the realization of ytterbium magneto-optical trap (MOT) operating on the dipole-allowed 1 S 0 — 1 P 1 transition at 398.9 nm. The MOT is loaded by a slowed atomic beam produced by a Zeeman slower. All seven stable isotopes of Yb atoms could be trapped separately at different laser detuning values. Over 10 7 174 Yb atoms are collected in the MOT, whereas the atom number of fermionic isotope 171 Yb is roughly 2.3 × 10 6 due to a lower abundance. Without the Zeeman slower, the trapped atom numbers are one order of magnitude lower. Both the even and odd isotopes are recognized as excellent candidates of optical clock transition, so the cooling and trapping of ytterbium atoms by the blue MOT is an important step for building an optical clock.
We report the magneto-optical trapping of ytterbium atoms using the 6s2 1S0-6s6p 3P1 intercombination transition. The magneto-optical trap is continuously loaded from an atomic beam decelerated by a Zeeman-tuned atomic-beam slower operated at the 6s2 1S0-6s6p 1P1 transition. Among seven stable isotopes of ytterbium, six isotopes of 170Yb, 171Yb, 172Yb, 173Yb, 174Yb, and 176Yb are successfully trapped. The number and density of the trapped atoms are about 108 and 1011 cm-3, respectively. The temperature of atoms is estimated to be about 20 μK from the time-of-flight measurement. The decay time of the trapped atoms after stopping the loading of atoms is about 3 s.
We report the magneto-optical trapping of ytterbium atoms using the ${6s}^{2}{}^{1}{S}_{0}\ensuremath{-}6s6p{}^{3}{P}_{1}$ intercombination transition. The magneto-optical trap is continuously loaded from an atomic beam decelerated by a Zeeman-tuned atomic-beam slower operated at the ${6s}^{2}{}^{1}{S}_{0}\ensuremath{-}6s6p{}^{1}{P}_{1}$ transition. Among seven stable isotopes of ytterbium, six isotopes of170Yb,\mathrm{of}{ }^{170}\mathrm{Y}\mathrm{b},of170Yb, 171Yb,{}^{171}\mathrm{Yb},171Yb, 172Yb,{}^{172}\mathrm{Yb},172Yb, 173Yb,{}^{173}\mathrm{Yb},173Yb, 174Yb,{}^{174}\mathrm{Yb},174Yb, and 176Yb{}^{176}\mathrm{Yb}176Yb are successfully trapped. The number and density of the trapped atoms are about 108{10}^{8}108 and ${10}^{11} {\mathrm{cm}}^{\ensuremath{-}3},$ respectively. The temperature of atoms is estimated to be about $20 \ensuremath{\mu}\mathrm{K}$ from the time-of-flight measurement. The decay time of the trapped atoms after stopping the loading of atoms is about 3 s.
We demonstrate a method to enhance the atom loading rate of a ytterbium (Yb) magneto-optic trap (MOT) operating on the 556 nm 1S0 → 3P1 intercombination transition (narrow linewidth Γg = 2π × 182 kHz). Following traditional Zeeman slowing of an atomic beam near the 399 nm 1S0 → 1P1 transition (broad linewidth Γp = 2π × 29 MHz), two laser beams in a crossed-beam geometry, frequency tuned near the same transition, provide additional slowing immediately prior to the MOT. Using this technique, we observe an improvement by a factor of 6 in the atom loading rate of a narrow-line Yb MOT. The relative simplicity and generality of this approach make it readily adoptable to other experiments involving narrow-line MOTs. We also present a numerical simulation of this two-stage slowing process, which shows good agreement with the observed dependence on experimental parameters, and use it to assess potential improvements to the method.
We present an experimental setup to laser cool and trap a large number of ytterbium atoms. Our design uses an oven with an array of micro-tubes for efficient collimation of the atomic beam, and we implement a magneto-optical trap of 174Yb on the 1S0 → 1P1 transition at 399 nm. Despite the absence of a Zeeman slower, we obtain a loading of 4 × 109 at./s. We trap up to N = 109 at., where light-assisted collisions become the dominant loss mechanism. We precisely characterize our atomic beam, the loading rate of the magneto-optical trap, and several loss mechanisms relevant for trapping a large number of atoms.
We demonstrate launching of laser-cooled Yb atoms in a cold atomic fountain. Atoms in a collimated thermal beam are first cooled and captured in a magneto-optical trap (MOT) operating on the strongly allowed ${{}^{1}S}_{0}\ensuremath{\rightarrow}{{}^{1}P}_{1}$ transition at 399 nm (blue line). They are then transferred to a MOT on the weakly allowed ${{}^{1}S}_{0}\ensuremath{\rightarrow}{{}^{3}P}_{1}$ transition at 556 nm (green line). Cold atoms from the green MOT are launched against gravity at a velocity of around 2.5 m/s using a pair of green beams. We trap more than 107{10}^{7}107 atoms in the blue MOT and transfer up to 7070%70 into the green MOT. The temperature for the odd isotope 171Yb^{171}\mathrm{Yb}171Yb is  1mK~1 \mathrm{mK} 1mK in the blue MOT, and reduces by a factor of 40 in the green MOT.