2016
DOI: 10.1038/srep38258
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Shortcut to adiabatic control of soliton matter waves by tunable interaction

Abstract: We propose a method for shortcut to adiabatic control of soliton matter waves in harmonic traps. The tunable interaction controlled by Feshbach resonance is inversely designed to achieve fast and high-fidelity compression of soliton matter waves as compared to the conventional adiabatic compression. These results pave the way to control the nonlinear dynamics for matter waves and optical solitons by using shortcuts to adiabaticity.

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Cited by 27 publications
(45 citation statements)
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References 37 publications
(71 reference statements)
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“…Therefore we aim to employ a STA which will suppress these excitations and ensure the final state has a large overlap with the one that would have been created in a fully adiabatic process. Such a technique was recently developed in [25] and we briefly review it in this section.…”
Section: Shortcuts To Adiabaticity For Soliton Matter Wavesmentioning
confidence: 99%
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“…Therefore we aim to employ a STA which will suppress these excitations and ensure the final state has a large overlap with the one that would have been created in a fully adiabatic process. Such a technique was recently developed in [25] and we briefly review it in this section.…”
Section: Shortcuts To Adiabaticity For Soliton Matter Wavesmentioning
confidence: 99%
“…Techniques such as quantum transitionless driving (or counter-diabatic driving), fastfoward algorithms, and inverse engineering have been shown to yield states with high fidelity in finite time, see the recent reviews [18,19]. While these approaches have often centered around non-interacting systems, STAs have also been explored in interacting, nonlinear, and other systems [20][21][22][23][24][25]. Remarkably, STAs have fundamental implications on quantum speed limits (QSL) [26][27][28][29][30], time-energy uncertainty relations (or energy cost) [31][32][33][34][35][36][37][38], and the quantification of the third law of thermodynamics in the context of quantum refrigerators [39,40], which results in intriguing practical applications in heat engines [41][42][43][44][45][46][47].…”
Section: Introductionmentioning
confidence: 99%
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“…whereˆˆ † a a , i i are the creation and annihilation operators at site i, ω is the common resonant frequency of both modes, and U(t), J(t) are the strengths of the nonlinearity and coherent coupling, respectively, which are assumed to be controllable functions of time. Note that, although the coupling rate is a well-known control parameter, the nonlinearity can also be varied in time experimentally [56,57] and it has been exploited in the design of STAs [45,58,59]. As we shall latter explain, the desired transfer cannot be achieved with constant controls.…”
Section: Weakly Populated Bjjsmentioning
confidence: 99%
“…These techniques offer some opportunities to achieve a nonlinearity management through the use of time-dependent and/or nonuniform fields. Utilizing this nonlinearity management concept, several nonlinear wave patterns and effects, such as, non-autonomous bright solitons [13] as well as dark-bright solitons [14], Bloch oscillations [15], and rogue waves [16] have been observed in BECs.…”
Section: Introductionmentioning
confidence: 99%