Probing lambda-gravity with Bose-Einstein condensates

We propose a precise test of two fundamental gravitational constants using a detector concept that exploits the dynamics of quantum phononic excitations in a trapped Bose-Einstein condensate (BEC), operable at the scale of tabletop experiments. In this setup, the sensitivity is enhanced by approximately 2 orders of magnitude through the use of a tritter operation, which mixes phononic excitations with the BEC's ground state. The BEC exhibits unique sensitivity to the two key components of the gravitational potential in <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"> <a:mi mathvariant="normal">Λ</a:mi> </a:math> -gravity: the Newtonian <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"> <c:mrow> <c:mi>G</c:mi> <c:mi>M</c:mi> <c:mo>/</c:mo> <c:mi>r</c:mi> </c:mrow> </c:math> term and the cosmological constant <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"> <d:mrow> <d:mi mathvariant="normal">Λ</d:mi> <d:msup> <d:mi>r</d:mi> <d:mn>2</d:mn> </d:msup> </d:mrow> </d:math> , both entering the most general function following from a Gurzadyan's theorem. Using state-of-the-art experimental design, we predict that the gravitational constant <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"> <f:mi>G</f:mi> </f:math> could be measured with an accuracy up to <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"> <g:mrow> <g:msup> <g:mn>10</g:mn> <g:mrow> <g:mo>−</g:mo> <g:mn>17</g:mn> </g:mrow> </g:msup> <g:mspace width="0.16em"/> <g:mi mathvariant="normal">N</g:mi> </g:mrow> <g:mo> </g:mo> <g:mrow> <g:msup> <g:mrow> <g:mi mathvariant="normal">m</g:mi> </g:mrow> <g:mn>2</g:mn> </g:msup> <g:msup> <g:mrow> <g:mo>/</g:mo> <g:mi>kg</g:mi> </g:mrow> <g:mn>2</g:mn> </g:msup> </g:mrow> </g:math> , representing an improvement by 2 orders of magnitude over current measurements. Moreover, this experiment aims to establish the best Earth-based upper limit on <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"> <k:mi mathvariant="normal">Λ</k:mi> </k:math> at <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mo>&lt;</m:mo> <m:msup> <m:mn>10</m:mn> <m:mrow> <m:mo>−</m:mo> <m:mn>31</m:mn> </m:mrow> </m:msup> </m:mrow> <m:mo> </m:mo> <m:msup> <m:mrow> <m:mi mathvariant="normal">m</m:mi> </m:mrow> <m:mrow> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> </m:math> , marking the first laboratory-based probe of the cosmological constant. Additionally, the setup allows for the measurement of the distance-dependent behavior of each term in the gravitational potential, providing a means to test modified gravity theories.

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Journal
Physical Review Research
Published
2025-09-22
DOI
https://doi.org/10.1103/7x8h-t1l9
Citations
1
Primary Topic
Quantum Electrodynamics and Casimir Effect
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article
Field-Weighted Citation Impact
1.25
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article

Probing lambda-gravity with Bose-Einstein condensates

Ivette Fuentes, A. Belyaev, Vahe Gurzadyan, Hector A. Fernandez-Melendez
1 citations
Physical Review Research
Quantum Electrodynamics and Casimir Effect
1.25
article

Probing lambda-gravity with Bose-Einstein condensates

Ivette Fuentes, A. Belyaev, Vahe Gurzadyan, Hector A. Fernandez-Melendez
article en
1 citations

Abstract

We propose a precise test of two fundamental gravitational constants using a detector concept that exploits the dynamics of quantum phononic excitations in a trapped Bose-Einstein condensate (BEC), operable at the scale of tabletop experiments. In this setup, the sensitivity is enhanced by approximately 2 orders of magnitude through the use of a tritter operation, which mixes phononic excitations with the BEC's ground state. The BEC exhibits unique sensitivity to the two key components of the gravitational potential in <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"> <a:mi mathvariant="normal">Λ</a:mi> </a:math> -gravity: the Newtonian <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"> <c:mrow> <c:mi>G</c:mi> <c:mi>M</c:mi> <c:mo>/</c:mo> <c:mi>r</c:mi> </c:mrow> </c:math> term and the cosmological constant <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"> <d:mrow> <d:mi mathvariant="normal">Λ</d:mi> <d:msup> <d:mi>r</d:mi> <d:mn>2</d:mn> </d:msup> </d:mrow> </d:math> , both entering the most general function following from a Gurzadyan's theorem. Using state-of-the-art experimental design, we predict that the gravitational constant <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"> <f:mi>G</f:mi> </f:math> could be measured with an accuracy up to <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"> <g:mrow> <g:msup> <g:mn>10</g:mn> <g:mrow> <g:mo>−</g:mo> <g:mn>17</g:mn> </g:mrow> </g:msup> <g:mspace width="0.16em"/> <g:mi mathvariant="normal">N</g:mi> </g:mrow> <g:mo> </g:mo> <g:mrow> <g:msup> <g:mrow> <g:mi mathvariant="normal">m</g:mi> </g:mrow> <g:mn>2</g:mn> </g:msup> <g:msup> <g:mrow> <g:mo>/</g:mo> <g:mi>kg</g:mi> </g:mrow> <g:mn>2</g:mn> </g:msup> </g:mrow> </g:math> , representing an improvement by 2 orders of magnitude over current measurements. Moreover, this experiment aims to establish the best Earth-based upper limit on <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"> <k:mi mathvariant="normal">Λ</k:mi> </k:math> at <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"> <m:mrow> <m:mo>&lt;</m:mo> <m:msup> <m:mn>10</m:mn> <m:mrow> <m:mo>−</m:mo> <m:mn>31</m:mn> </m:mrow> </m:msup> </m:mrow> <m:mo> </m:mo> <m:msup> <m:mrow> <m:mi mathvariant="normal">m</m:mi> </m:mrow> <m:mrow> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> </m:math> , marking the first laboratory-based probe of the cosmological constant. Additionally, the setup allows for the measurement of the distance-dependent behavior of each term in the gravitational potential, providing a means to test modified gravity theories.

Physical Review ResearchVol. 7(4)
Rutherford Appleton Laboratory (GB), A. Alikhanyan National Laboratory (AM), Yerevan State University (AM), University of Oxford (GB), University of Southampton (GB)
Openalex Percentile: Top 15%
Quantum Electrodynamics and Casimir Effect
1.25
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