2021
DOI: 10.1103/physrevresearch.3.043062
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Quantum to classical walk transitions tuned by spontaneous emissions

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Cited by 8 publications
(30 citation statements)
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“…This is the so-called quantum resonant regime of the kicked rotor [24][25][26]. In this regime the evolution well approximates an ideal quantum walk as suggested in [27] and subsequently realised in [19][20][21], in particular for kick strengths of the order k ≈ 1.5, for which the kicks dominantly couple nearest-neighbor momentum states. There is another important difference to ideal quantum walks: the kicked-rotor dynamics for both internal states would be completely symmetric in momentum space if the parity symmetry was not broken.…”
Section: The Experimental Setupmentioning
confidence: 67%
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“…This is the so-called quantum resonant regime of the kicked rotor [24][25][26]. In this regime the evolution well approximates an ideal quantum walk as suggested in [27] and subsequently realised in [19][20][21], in particular for kick strengths of the order k ≈ 1.5, for which the kicks dominantly couple nearest-neighbor momentum states. There is another important difference to ideal quantum walks: the kicked-rotor dynamics for both internal states would be completely symmetric in momentum space if the parity symmetry was not broken.…”
Section: The Experimental Setupmentioning
confidence: 67%
“…We are looking at a one-dimensional DTQW [8] in the following, as it was realised in [19][20][21] using a rubidium Bose-Einstein condensate. The Hilbert space for this system is given by H = H C ⊗ H P , where H C is the two-state coin space, spanned by the orthonormal basis {|0 C , |1 C }(corresponding to the two ground state hyperfine levels of rubidium) and H P represents the infinite walker's space spanned by {|n ; n ∈ Z} (corresponding to the center-of-mass momentum of the rubidium Bose-Einstein condensate).…”
Section: The Experimental Setupmentioning
confidence: 99%
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“…Even if the atom would return to the initial ground-state level, it receives a recoil changing its quasimomentum (see below after Eq. ( 7)) and hence its response to the kicking pulses [18,19]. This implies that it will be effectively lost from the signal, and only potentially contributing to an incoherent background [14,20].…”
Section: Theoretical Backgroundmentioning
confidence: 99%