2017
DOI: 10.1103/physreva.95.042701
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Investigation of Feshbach resonances in ultracold K40 spin mixtures

Abstract: Magnetically tunable Feshbach resonances are an indispensable tool for experiments with atomic quantum gases. We report on 37 thus far unpublished Feshbach resonances and four further probable Feshbach resonances in spin mixtures of ultracold fermionic 40K with temperatures well below 100 nK. In particular, we locate a broad resonance at B = 389.7G with a magnetic width of 26.7 G. Here 1 G = 10−4 T. Furthermore, by exciting low-energy spin waves, we demonstrate a means to precisely determine the zero crossing … Show more

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Cited by 10 publications
(8 citation statements)
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“…The magnetic field (or in alternative the light shift) inducing the Feshbach resonance has to be then tuned spatially on the lattice spacing scale such to provide the desired V -shape interaction profile. In alternative, at the price of doubling the number of Dirac points, we can consider two spin states of fermionic atoms with Feshbach resonance like potassium [126] loaded in a spin-independent π-flux square lattice and perceiving the same laser-induced tunneling term. The interactions are now on site.…”
Section: Experimental Realization and Detection Of Unruh Effectmentioning
confidence: 99%
“…The magnetic field (or in alternative the light shift) inducing the Feshbach resonance has to be then tuned spatially on the lattice spacing scale such to provide the desired V -shape interaction profile. In alternative, at the price of doubling the number of Dirac points, we can consider two spin states of fermionic atoms with Feshbach resonance like potassium [126] loaded in a spin-independent π-flux square lattice and perceiving the same laser-induced tunneling term. The interactions are now on site.…”
Section: Experimental Realization and Detection Of Unruh Effectmentioning
confidence: 99%
“…To demonstrate the feasibility of our protocol, we prepare the two-state spin-mixture in both the strongly and weakly interacting regimes. [29,30] We apply a variable number N p of resonant RF π-pulses (square shaped in time domain) during each measurement cycle prior to the time of flight imaging (TOF). We define the total measurement cycle duration T t as (T π + T f ) × N p , where T f is the separation between the neighboring π-pulses, as depicted in Fig.…”
Section: Results and Analysismentioning
confidence: 99%
“…Large-spin ( f > 1 2 ) [1][2][3][4] and multi-component [5][6][7][8][9] cold Fermi atoms provide a good simulation platform for studying many-body physics. The former system usually satisfies the SP(N) or SU(N) symmetries, while the latter can be mapped into more general pseudo-spin models with lower symmetries by precisely controlling interaction parameters, atomic species, and particle numbers.…”
Section: Introductionmentioning
confidence: 99%