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Understanding how strongly correlated two-dimensional (2D) systems can give rise to unconventional superconductivity with high critical temperatures is one of the major unsolved problems in condensed matter physics.
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Measurements performed at interaction strengths of up to ln ( k F a 2 D ) = 1.1 {\rm ln}(k_{\rm F}a_{\rm 2D})=1.1 show the same qualitative behaviour [ 19 ] , but we currently do not have a quantitatively accurate temperature determination for our homogenous system at these interaction strengths
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