2016
DOI: 10.1038/nphys3622
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Topological Thouless pumping of ultracold fermions

Abstract: An electron gas in a one-dimensional periodic potential can be transported even in the absence of a voltage bias if the potential is slowly and periodically modulated in time. Remarkably, the transferred charge per cycle is sensitive only to the topology of the path in parameter space. Although this so-called Thouless charge pump was first proposed more than thirty years ago 1 , it has not yet been realized. Here we report the demonstration of topological Thouless pumping using ultracold fermionic atoms in a d… Show more

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Cited by 598 publications
(583 citation statements)
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“…However, while the existence of such edge states is linked to the non-trivial global topological properties of bulk bands, a direct measurement of the Berry curvature itself has so far not been realized. In ultracold atoms, instead, there has been much progress in this direction, for example, with experiments exploiting the effects of Berry curvature on particle transport to extract, in 2D systems, the Chern number 19 and topological phase diagrams 20 , and, in 1D systems, both the quantized 'Thouless pumping' of atoms in a filled band 23,24 and the un-quantized 'geometrical pumping' of a Bose-Einstein condensate 25 .…”
mentioning
confidence: 99%
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“…However, while the existence of such edge states is linked to the non-trivial global topological properties of bulk bands, a direct measurement of the Berry curvature itself has so far not been realized. In ultracold atoms, instead, there has been much progress in this direction, for example, with experiments exploiting the effects of Berry curvature on particle transport to extract, in 2D systems, the Chern number 19 and topological phase diagrams 20 , and, in 1D systems, both the quantized 'Thouless pumping' of atoms in a filled band 23,24 and the un-quantized 'geometrical pumping' of a Bose-Einstein condensate 25 .…”
mentioning
confidence: 99%
“…By preparing a wavepacket with a narrow spectral width and a well-defined centre-of-mass momentum Q, we realize a geometrical charge pump by slowly ramping the phase amplitude, ϕ, in time. Due to this pumping, the wavepacket moves along the 1D 'photonic mesh lattice' , with an anomalous velocity contribution 1,[23][24][25] lengths are used to simulate light evolution on a 1 + 1D lattice spanned by a discrete time m and position n. b, The light evolution in the fibre loops is mapped onto a lattice, where a round trip in the short loop stands for the motion from northeast to southwest, while the propagation from northwest to southeast is equivalent to a round trip through the long loop. c, Measurement of the intensity distribution of short-loop pulses for a single lattice site excitation in the absence of any modulation.…”
mentioning
confidence: 99%
“…[27] Also a recent experiment on cold atoms has realized this model experimentally. [28] Now we consider the 2D parameter space of Q 1 − Q 2 , and rotate the parameter set Q = (Q 1 , Q 2 ) on this plane as sketched in Figure 3. For simplicity, we consider the case with…”
Section: Geometry and Topology In Quantum Physicsmentioning
confidence: 99%
“…Due to the fact that the polarization as a function of the parameters of the Hamiltonian is not single valued, the polarization in such a process changes by a "polarization quantum." A recent related study [17] realized quantized adiabatic charge pumping [18], also in the RM model.…”
Section: Introductionmentioning
confidence: 99%