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arXiv:2012.11544 · Physical Review A

Interorbital interactions in an SU(2)⊗SU(6) -symmetric Fermi-Fermi mixture

B. Abeln, Koen Sponselee, M. Diem, Nejira Pintul, K. Sengstock, C. Becker

Published Mar 18, 2021• 17 citations
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Abstract

We characterize interisotope interorbital interactions between atoms in the $^{1}S_{0}$ ground state and the $^{3}P_{0}$ metastable state in interacting Fermi-Fermi mixtures of $^{171}\mathrm{Yb}$ and $^{173}\mathrm{Yb}$. We perform high-precision clock spectroscopy to measure interaction-induced energy shifts in a deep three-dimensional optical lattice and determine the corresponding scattering lengths. We find the elastic interaction of the interisotope mixtures $^{173}\mathrm{Yb}_{\mathrm{e}}\text{\ensuremath{-}}^{171}\mathrm{Yb}_{\mathrm{g}}$ and $^{173}\mathrm{Yb}_{\mathrm{g}}\text{\ensuremath{-}}^{171}\mathrm{Yb}_{\mathrm{e}}$ to be weakly attractive and very similar, while the corresponding two-body decay coefficients differ by more than two orders of magnitude. By comparing different spin mixtures we experimentally demonstrate the $\mathrm{SU}(2)\ensuremath{\bigotimes}\mathrm{SU}(6)$ symmetry of the elastic interactions. Furthermore, we measure the interorbital spin-exchange interaction in $^{171}\mathrm{Yb}$ and confirm its previously observed antiferromagnetic nature.

DOI
10.1103/physreva.103.033315

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We characterize interisotope interorbital interactions between atoms in the 1S0^{1}S_{0}1S0​ ground state and the 3P0^{3}P_{0}3P0​ metastable state in interacting Fermi-Fermi mixtures of 171Yb^{171}\mathrm{Yb}171Yb and 173Yb^{173}\mathrm{Yb}173Yb. We perform high-precision clock spectroscopy to measure interaction-induced energy shifts in a deep three-dimensional optical lattice and determine the corresponding scattering lengths. We find the elastic interaction of the interisotope mixtures 173Ybe\ensuremath-171Ybg^{173}\mathrm{Yb}_{\mathrm{e}}\text{\ensuremath{-}}^{171}\mathrm{Yb}_{\mathrm{g}}173Ybe​\ensuremath-171Ybg​ and 173Ybg\ensuremath-171Ybe^{173}\mathrm{Yb}_{\mathrm{g}}\text{\ensuremath{-}}^{171}\mathrm{Yb}_{\mathrm{e}}173Ybg​\ensuremath-171Ybe​ to be weakly attractive and very similar, while the corresponding two-body decay coefficients differ by more than two orders of magnitude. By comparing different spin mixtures we experimentally demonstrate the SU(2)\ensuremath⨂SU(6)\mathrm{SU}(2)\ensuremath{\bigotimes}\mathrm{SU}(6)SU(2)\ensuremath⨂SU(6) symmetry of the elastic interactions. Furthermore, we measure the interorbital spin-exchange interaction in 171Yb^{171}\mathrm{Yb}171Yb and confirm its previously observed antiferromagnetic nature.
We report on the investigation of the scattering properties between the ground state 1S0^{1}S_{0}1S0​ and the metastable state 3P0^{3}P_{0}3P0​ of the fermionic isotope of 171Yb^{171}\mathrm{Yb}171Yb. We measure the sss-wave scattering lengths in the two-orbital collision channels as aeg+=225(13)a0{a}_{eg}^{+}=225(13){a}_{0}aeg+​=225(13)a0​ and ${a}_{eg}^{\ensuremath{-}}=355(6){a}_{0}$, using clock transition spectroscopy in a three-dimensional optical lattice. The results show that the interorbital spin-exchange interaction is antiferromagnetic, indicating that 171Yb^{171}\mathrm{Yb}171Yb is a promising isotope for the quantum simulation of the Kondo effect with the two-orbital system.
We report the realization of a novel degenerate Fermi mixture with an $\mathrm{SU}(2)\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(6)$ symmetry in a cold atomic gas. We successfully cool the mixture of the two fermionic isotopes of ytterbium 171Yb^{171}\mathrm{Yb}171Yb with the nuclear spin I=1/2I=1/2I=1/2 and 173Yb^{173}\mathrm{Yb}173Yb with I=5/2I=5/2I=5/2 below the Fermi temperature TF{T}_{F}TF​ as 0.46TF0.46{T}_{F}0.46TF​ for 171Yb^{171}\mathrm{Yb}171Yb and 0.54TF0.54{T}_{F}0.54TF​ for 173Yb^{173}\mathrm{Yb}173Yb. The same scattering lengths for different spin components make this mixture featured with the novel $\mathrm{SU}(2)\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(6)$ symmetry. The nuclear spin components are separately imaged by exploiting an optical Stern-Gerlach effect. In addition, the mixture is loaded into a 3D optical lattice to implement the $\mathrm{SU}(2)\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(6)$ Hubbard model. This mixture will open the door to the study of novel quantum phases such as a spinor Bardeen-Cooper-Schrieffer-like fermionic superfluid.
We report on the experimental observation of a novel interorbital Feshbach resonance in ultracold (173)Yb atoms. This opens up the possibility of tuning the interactions between the (1)S(0) and (3)P(0) metastable state, both possessing zero total electronic angular momentum. The resonance is observed at experimentally accessible magnetic field strengths and occurs universally for all hyperfine state combinations. We characterize the resonance in the bulk via interorbital cross thermalization as well as in a three-dimensional lattice using high-resolution clock-line spectroscopy. Our measurements are well described by a generalized two-channel model of the orbital-exchange interactions.
Abstract We studied the behavior of mixtures of 173Yb (with symmetry up to SU(6)) and 171Yb (up to SU(2)) fermionic isotopes loaded in one-dimensional (1D) optical lattices. To do so, we solved the Schrödinger equation describing different systems using a diffusion Monte Carlo technique. We considered continuous Hamiltonians in which the interactions between atoms of different species (isotopes and/or spins) were modeled by contact potentials with parameters derived from their experimental scattering lengths. This implies that we can find both attractive and repulsive interactions between fermion pairs in the same cluster. The strength of those interactions can be changed by varying the transverse confinement, leading to different cluster behaviors. Only balanced clusters, i.e. with the same number of 173Yb and 171Yb atoms were considered. We found that the standard state for these clusters is a metallic-like one with different populations of 173Yb–171Yb molecule-like pairs in each optical lattice potential well. However, for big enough clusters, insulator-like states are also possible.
We report on the observation of the spin-exchange dynamics of 171Yb^{171}\mathrm{Yb}171Yb atoms in the ground state 1S0{}^{1}{S}_{0}1S0​ and in the metastable state 3P0{}^{3}{P}_{0}3P0​. We implement the mixed-dimensional two-orbital system using near-resonant and magic-wavelength optical lattices, where the 1S0{}^{1}{S}_{0}1S0​ and 3P0{}^{3}{P}_{0}3P0​ atoms are itinerant in a one-dimensional tube and localized in three dimensions, respectively. By exploiting an optical Stern-Gerlach method, we observe the spin depolarization of the 1S0{}^{1}{S}_{0}1S0​ atoms induced by the spin-exchange interaction with the 3P0{}^{3}{P}_{0}3P0​ atom. Our work could pave the way to the quantum simulation of the Kondo effect.
We present experimental results on the inelastic and elastic interspecies interactions between ytterbium (Yb) in the metastable 3P2{}^{3}P{}_{2}3P2​ state loaded into a deep optical lattice and spin polarized lithium (Li) in its ground state. Focusing on the mJ=0{m}_{J}=0mJ​=0 magnetic sublevel of Yb(3P2\mathrm{Yb}({}^{3}P{}_{2}Yb(3P2​), bias magnetic fields between 20 and 800G800\phantom{\rule{0.28em}{0ex}}\mathrm{G}800G are investigated and significantly enhanced inelastic collision rates with high magnetic fields are found. In addition, by direct spectroscopy of the Yb Mott insulator immersed in the Li Fermi gas an upper boundary of the background scattering length of the $\mathrm{Yb}({}^{3}P{}_{2},{m}_{J}=0)\ensuremath{-}\mathrm{Li}{(}^{2}{S}_{1/2},F=1/2,{m}_{F}=+1/2$) system is estimated, revealing the absence of useful Feshbach resonances. These observations are qualitatively consistent with the theoretical calculations.