Atom Interferometry with Rb Blue Transitions.

We demonstrate a novel scheme for Raman-pulse and Bragg-pulse atom interferometry based on the 5S-6P blue transitions of ^{87}Rb that provides an increase by a factor ∼2 of the interferometer phase due to accelerations with respect to the commonly used infrared transition at 780 nm. A narrow-linewidth laser system generating more than 1 W of light in the 420-422 nm range was developed for this purpose. Used as a cold-atom gravity gradiometer, our Raman interferometer attains a stability to differential acceleration measurements of 1×10^{-8}  g at 1 s and 2×10^{-10}  g after 2000 s of integration time. When operated on first-order Bragg transitions, the interferometer shows a stability of 6×10^{-8}  g at 1 s, averaging to 1×10^{-9}  g after 2000 s of integration time. The instrument sensitivity, currently limited by the noise due to spontaneous emission, can be further improved by increasing the laser power and the detuning from the atomic resonance. The present scheme is attractive for high-precision experiments as, in particular, for the determination of the Newtonian gravitational constant.

[1]  G. Tino,et al.  New apparatus design for high-precision measurement of G with atom interferometry , 2021, The European Physical Journal D.

[2]  Zhibin Yao,et al.  Determination of the fine-structure constant with an accuracy of 81 parts per trillion , 2020, Nature.

[3]  G. Tino Testing gravity with cold atom interferometry: results and prospects , 2020, Quantum Science and Technology.

[4]  Philippe Bouyer,et al.  Taking atom interferometric quantum sensors from the laboratory to real-world applications , 2019, Nature Reviews Physics.

[5]  Achim Peters,et al.  AEDGE: Atomic Experiment for Dark Matter and Gravity Exploration in Space , 2019, Experimental Astronomy.

[6]  S. Capozziello,et al.  SAGE: A proposal for a space atomic gravity explorer , 2019, The European Physical Journal D.

[7]  Chenghui Yu,et al.  Measurement of the fine-structure constant as a test of the Standard Model , 2018, Science.

[8]  L. Cacciapuoti,et al.  Measuring the gravitational acceleration with matter-wave velocimetry , 2018, The European Physical Journal D.

[9]  A. Bhardwaj,et al.  In situ click chemistry generation of cyclooxygenase-2 inhibitors , 2017, Nature Communications.

[10]  G. Rosi A proposed atom interferometry determination of G at 10−5 using a cold atomic fountain , 2017, 1702.01608.

[11]  Hong-Wei Song,et al.  Extracting the differential phase in dual atom interferometers by modulating magnetic fields , 2016, 1602.08569.

[12]  M. Kasevich,et al.  Quantum superposition at the half-metre scale , 2015, Nature.

[13]  F. Sorrentino,et al.  Measuring the Newtonian constant of gravitation G with an atomic interferometer , 2014, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[14]  F. Sorrentino,et al.  Precision measurement of the Newtonian gravitational constant using cold atoms , 2014, Nature.

[15]  A. Clairon,et al.  Limits to the sensitivity of a low noise compact atomic gravimeter , 2008, 0801.1270.

[16]  J. H. Müller,et al.  Two-photon ionization of cold rubidium atoms with a near resonant intermediate state , 2004 .

[17]  T. Gustavson,et al.  Rotation sensing with a dual atom-interferometer Sagnac gyroscope , 2000 .

[18]  Harold Metcalf,et al.  Laser Cooling and Trapping , 1999, Peking University-World Scientific Advanced Physics Series.

[19]  A. Peters,et al.  Measurement of gravitational acceleration by dropping atoms , 1999, Nature.

[20]  A. Peters,et al.  High-precision gravity measurements using atom interferometry , 1998 .

[21]  B. Muzykantskii,et al.  ON QUANTUM NOISE , 1995 .