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$T^{-3}$-shift in a short-baseline atomic interferometer-gravimeter

D. N. Kapusta, A. E. Bonert, A. N. Goncharov, V. I. Yudin, K. N. Adamov, A. V. Taichenachev, M. Yu. Basalaev, M. D. Radchenko, O. N. Prudnikov

Abstract

This paper presents the first experimental observation and investigation of a lineshape-asymmetry-caused shift (LACS) in a short-baseline atomic interferometer-gravimeter. It is shown that this shift scales inversely with the cube of the free evolution time, $\propto T^{-3}$, and can lead to a noticeable systematic error in the measured value of the gravitational acceleration g at the level of 0.1-1 mGal ($T\approx$ milliseconds). The obtained results are in good agreement with our previous theoretical studies and highlight the importance of accounting for LACS in high-precision absolute measurements of g in compact atomic gravimeters.

$T^{-3}$-shift in a short-baseline atomic interferometer-gravimeter

Abstract

This paper presents the first experimental observation and investigation of a lineshape-asymmetry-caused shift (LACS) in a short-baseline atomic interferometer-gravimeter. It is shown that this shift scales inversely with the cube of the free evolution time, , and can lead to a noticeable systematic error in the measured value of the gravitational acceleration g at the level of 0.1-1 mGal ( milliseconds). The obtained results are in good agreement with our previous theoretical studies and highlight the importance of accounting for LACS in high-precision absolute measurements of g in compact atomic gravimeters.
Paper Structure (1 equation, 3 figures)

This paper contains 1 equation, 3 figures.

Figures (3)

  • Figure 1: (Color online) Chirping of the Raman beam frequency: (a) interferometric sequence (blue curve) and frequency chirp scheme (orange curve); (b) typical resonance corresponding to the two-photon transition $|F=1, m_F=0\rangle \rightarrow |F=2, m_F=0\rangle$.
  • Figure 2: (Color online) Observation of the LACS shift in an atomic interferometer-gravimeter: (a) typical interference signal (red curve, blue curve — fit based on the theoretical model Yudin_2025) obtained for $T=110~\mu$s without averaging (each point represents a single experimental cycle); (b) fragment of the central interference fringe (red curve, blue — fit) and the corresponding lock-in amplifier output signal (orange curve) fitted with a straight line (black dashed-dotted line) over its linear region (highlighted in pink); (c–g) plots of the LACS shift $\Delta_{LACS}$ versus Raman beam detuning $\delta_D$ for different free-evolution intervals $T$.
  • Figure 3: (Color online) Plot of the proportionality coefficient $\beta$ as a function of the free-evolution time $T$.