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Test of universality of free fall with Bragg atom interferometer

Zhong-Kun Hu, Min-Kang Zhou, Xiao‐Chun Duan, Xiao-Bing Deng, Lushuai Cao

Published May 1, 2018• 0 citations
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Progress towards a test of the universality of free fall using a 6^66Li/7^77Li atom interferometer
Testing the Universality of Free Fall at 10−10{10^{ - 10}}10−10 level by Comparing the Atoms in Different Hyperfine States with Bragg Diffraction
We have performed a precision atomic interferometry experiment on testing the universality of free fall (UFF) considering atoms' spin degree of freedom. Our experiment employs the Bragg atom interferometer with 87^{87}87Rb atoms either in hyperfine state $\left| {F = 1,{m_F} = 0} \right\rangle $ or $\left| {F = 2,{m_F} = 0} \right\rangle ,andthewavepacketsinthesetwostatesarediffractedinonepairofBraggbeamsalternatively,whichcanhelpsuppressthecommon−modesystematicerrors.WehaveobtainedanE, and the wave packets in these two states are diffracted in one pair of Bragg beams alternatively, which can help suppress the common-mode systematic errors. We have obtained an E,andthewavepacketsinthesetwostatesarediffractedinonepairofBraggbeamsalternatively,whichcanhelpsuppressthecommon−modesystematicerrors.WehaveobtainedanE\rm{\ddot{o}}tvtvtv\rm{\ddot{o}}$s ratio η=(0.9±2.7)×10−10η= \left( { 0.9 \pm 2.7} \right) \times {10^{ - 10}}η=(0.9±2.7)×10−10, and set a new record on the precision with a nearly 5 times improvement. Our experiment gives stronger restrictions on the possible UFF breaking mechanism.
We perform a precision atom interferometry experiment to test the universality of free fall. Our experiment employs the Bragg atom interferometer with 87Rb atoms either in hyperfine state F = 1 , m F = 0 or F = 2 , m F = 0 , and the wave packets in these two states are diffracted by one pair of Bragg beams alternatively, which is helpful for suppressing common-mode systematic errors. We obtain an Eötvös ratio η 1 − 2 = 0.9 ± 2.7 × 10 − 10 , and set a new record on the precision with improvement of nearly 5 times. This measurement also provides constraint on the difference of the diagonal terms of the mass-energy operator.