2019
DOI: 10.1088/1367-2630/ab00bf
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Universality of miscible–immiscible phase separation dynamics in two-component Bose–Einstein condensates

Abstract: We investigate the non-equilibrium dynamics across the miscible-immiscible phase separation in a binary mixture of Bose-Einstein condensates. The excitation spectra reveal that the Landau critical velocity vanishes at the critical point, where the superfluidity spontaneously breaks down. We analytically extract the dynamical critical exponent z=2 and static correlation length critical exponent v=1/2 from the Landau critical velocity. Moreover, by simulating the real-time dynamics across the critical point,… Show more

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Cited by 13 publications
(11 citation statements)
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“…We considerer that the initial state of our system is configured, with two spinless soft core bosons and two one half spin fermions in the right side of the double well potential. This configuration is mainly due to the fact that we want to explore the conditions for which is generated the transmutation of bosons into fermions and vice versa, for which the two species are had under the same initial configuration and we varied the boson-boson λ BB , fermion-fermion λ FF and boson-fermion λ BF repulsive contact interaction terms The immiscible and miscible phases for our system is found by means of the probability of finding each species at a point x, at time t. Therefore, an overlap of the probability density of each species indicates that both wave functions occupy the same spatial regions [80].…”
Section: Bose-fermi Probabilitiesmentioning
confidence: 99%
“…We considerer that the initial state of our system is configured, with two spinless soft core bosons and two one half spin fermions in the right side of the double well potential. This configuration is mainly due to the fact that we want to explore the conditions for which is generated the transmutation of bosons into fermions and vice versa, for which the two species are had under the same initial configuration and we varied the boson-boson λ BB , fermion-fermion λ FF and boson-fermion λ BF repulsive contact interaction terms The immiscible and miscible phases for our system is found by means of the probability of finding each species at a point x, at time t. Therefore, an overlap of the probability density of each species indicates that both wave functions occupy the same spatial regions [80].…”
Section: Bose-fermi Probabilitiesmentioning
confidence: 99%
“…Due to the gapless excitations at the critical point, the adiabaticity breaks down when a system goes through a continuous phase transition. As a consequence, nontrivial excitations such as domains [4][5][6][7][8][9][10][11][12][13][14], vortices [15][16][17] and solitons [18][19][20] appear spontaneously and obey the wellkonwn Kibble-Zurek mechanism (KZM) [3,4,[21][22][23][24][25]. The KZM has been extensively studied in various systems, from the early universe [3,4], condensed matter systems [26][27][28], trapped ions [29][30][31][32][33], to ultracold atomic gases [5-15, 18-20, 34-37].…”
Section: Introductionmentioning
confidence: 99%
“…In the two-component BEC, a variety of dynamical properties have been observed and reported [24][25][26][27][28][29], and the tunable inter-component interaction has been realized experimentally by using the Feshbach resonance technology [30,31]. Especially, the quantized vortices have been created and studied [32][33][34][35][36][37][38][39].…”
Section: Introductionmentioning
confidence: 99%