Nonlocal spatial correlations in an interacting atomic gas

We report measurements of the nonlocal two-body spatial correlation function <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"> <a:mrow> <a:msup> <a:mi>g</a:mi> <a:mrow> <a:mo>(</a:mo> <a:mn>2</a:mn> <a:mo>)</a:mo> </a:mrow> </a:msup> <a:mrow> <a:mo>(</a:mo> <a:mi>R</a:mi> <a:mo>)</a:mo> </a:mrow> </a:mrow> </a:math> in an ultracold Bose gas with strong interactions using photoassociation of ultra-long-range Rydberg molecules (ULRRMs) as a spatially selective probe. This technique provides access to <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"> <b:mrow> <b:msup> <b:mi>g</b:mi> <b:mrow> <b:mo>(</b:mo> <b:mn>2</b:mn> <b:mo>)</b:mo> </b:mrow> </b:msup> <b:mrow> <b:mo>(</b:mo> <b:mi>R</b:mi> <b:mo>)</b:mo> </b:mrow> </b:mrow> </b:math> on length scales from 60 to 180 nm, bridging the gap between short-range and long-range correlation measurements. The large <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"> <c:mi>s</c:mi> </c:math> -wave scattering length of <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"> <d:mmultiscripts> <d:mi>Sr</d:mi> <d:mprescripts/> <d:none/> <d:mn>86</d:mn> </d:mmultiscripts> </d:math> ( <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"> <e:mrow> <e:mi>a</e:mi> <e:mo>=</e:mo> <e:mn>811</e:mn> <e:mspace width="0.16em"/> <e:msub> <e:mi>a</e:mi> <e:mn>0</e:mn> </e:msub> </e:mrow> </e:math> ) enables exploration of the universal regime where <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"> <g:mrow> <g:msup> <g:mi>g</g:mi> <g:mrow> <g:mo>(</g:mo> <g:mn>2</g:mn> <g:mo>)</g:mo> </g:mrow> </g:msup> <g:mrow> <g:mo>(</g:mo> <g:mi>R</g:mi> <g:mo>)</g:mo> </g:mrow> </g:mrow> </g:math> is governed solely by two-body interactions. Comparison with a weakly interacting isotope, <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"> <h:mmultiscripts> <h:mi>Sr</h:mi> <h:mprescripts/> <h:none/> <h:mn>84</h:mn> </h:mmultiscripts> </h:math> , highlights interaction-induced suppression of pair correlations. The measured correlation functions agree quantitatively with calculations based on the two-body reduced density matrix, without adjustable parameters. Our results establish Rydberg molecular photoassociation as a powerful tool for probing nonlocal correlations in strongly interacting quantum gases.

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Journal
Physical review. A/Physical review, A
Published
2026-01-13
DOI
https://doi.org/10.1103/2q22-grqy
Primary Topic
Cold Atom Physics and Bose-Einstein Condensates
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article
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article

Nonlocal spatial correlations in an interacting atomic gas

Ang Li, S. Yoshida, Anonymous, S. K. Kanungo et al.
Physical review. A/Physical review, A
Cold Atom Physics and Bose-Einstein Condensates
article

Nonlocal spatial correlations in an interacting atomic gas

Ang Li, S. Yoshida, Anonymous, S. K. Kanungo, Y. Lu, T. C. Killian, F. B. Dunning
article en

Abstract

We report measurements of the nonlocal two-body spatial correlation function <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"> <a:mrow> <a:msup> <a:mi>g</a:mi> <a:mrow> <a:mo>(</a:mo> <a:mn>2</a:mn> <a:mo>)</a:mo> </a:mrow> </a:msup> <a:mrow> <a:mo>(</a:mo> <a:mi>R</a:mi> <a:mo>)</a:mo> </a:mrow> </a:mrow> </a:math> in an ultracold Bose gas with strong interactions using photoassociation of ultra-long-range Rydberg molecules (ULRRMs) as a spatially selective probe. This technique provides access to <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"> <b:mrow> <b:msup> <b:mi>g</b:mi> <b:mrow> <b:mo>(</b:mo> <b:mn>2</b:mn> <b:mo>)</b:mo> </b:mrow> </b:msup> <b:mrow> <b:mo>(</b:mo> <b:mi>R</b:mi> <b:mo>)</b:mo> </b:mrow> </b:mrow> </b:math> on length scales from 60 to 180 nm, bridging the gap between short-range and long-range correlation measurements. The large <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"> <c:mi>s</c:mi> </c:math> -wave scattering length of <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"> <d:mmultiscripts> <d:mi>Sr</d:mi> <d:mprescripts/> <d:none/> <d:mn>86</d:mn> </d:mmultiscripts> </d:math> ( <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"> <e:mrow> <e:mi>a</e:mi> <e:mo>=</e:mo> <e:mn>811</e:mn> <e:mspace width="0.16em"/> <e:msub> <e:mi>a</e:mi> <e:mn>0</e:mn> </e:msub> </e:mrow> </e:math> ) enables exploration of the universal regime where <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"> <g:mrow> <g:msup> <g:mi>g</g:mi> <g:mrow> <g:mo>(</g:mo> <g:mn>2</g:mn> <g:mo>)</g:mo> </g:mrow> </g:msup> <g:mrow> <g:mo>(</g:mo> <g:mi>R</g:mi> <g:mo>)</g:mo> </g:mrow> </g:mrow> </g:math> is governed solely by two-body interactions. Comparison with a weakly interacting isotope, <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"> <h:mmultiscripts> <h:mi>Sr</h:mi> <h:mprescripts/> <h:none/> <h:mn>84</h:mn> </h:mmultiscripts> </h:math> , highlights interaction-induced suppression of pair correlations. The measured correlation functions agree quantitatively with calculations based on the two-body reduced density matrix, without adjustable parameters. Our results establish Rydberg molecular photoassociation as a powerful tool for probing nonlocal correlations in strongly interacting quantum gases.

Physical review. A/Physical review, AVol. 113(2)
TU Wien (AT), Rice University (US)
Openalex Percentile: Top 86%
Cold Atom Physics and Bose-Einstein Condensates
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