Abstract:A one-dimensional quantum charge pump transfers a quantized charge in each pumping cycle. This quantization is topologically robust being analogous to the quantum Hall effect. The charge transferred in a fraction of the pumping period is instead generally unquantized. We show, however, that with specific symmetries in parameter space the charge transferred at well-defined fractions of the pumping period is quantized as integer fractions of the Chern number. We illustrate this in a one-dimensional Harper-Hofsta… Show more
“…In addition, the finite temperature effects do not interfere with the particle transport progression for temperatures smaller than the energy gap [33]. This requires the temperature of the order of 0.08E R /k B ∼ 20 nk (k B is the Boltzmann constant), which has been achieved in current experiments with, e.g., 40 K atoms. So we can conclude that the required Hamiltonian with tunable parameters and the adiabatic condition are able to be realized under realistic circumstances.…”
Section: A Two Experimental Setupsmentioning
confidence: 98%
“…The shift of the Wannier center encodes the adiabatic particle transport (the variation of polarization) as [33,39,40]…”
Section: B Experimental Measurement Methodsmentioning
confidence: 99%
“…This is an analog of the adiabatic charge pumping proposed by Thouless [32]; however, the parametric driving in our case does not form a closed cycle but only a half one. The topological pumping in cold atom systems and photonic quasi-crystals has been discussed in the contexts of SSH model [33][34][35] and 1D quasi-periodic Harper model [36][37][38][39][40], where the pumping particle is shown to be quantized one over one period and can be fractional over a fraction of one period [40].…”
We propose a scheme to mimic and directly measure the fractional particle number in a generalized Su-Schrieffer-Heeger model with ultracold fermions in one-dimensional optical lattices. We show that the fractional particle number in this model can be simulated in the momentum-time parameter space in terms of Berry curvature without a spatial domain wall. In this simulation, a hopping modulation is adiabatically tuned to form a kink-type configuration and the induced current plays the role of an analogous soliton distributing in the time domain, such that the mimicked fractional particle number is expressed by the particle transport. Two feasible experimental setups of optical lattices for realizing the required Su-Schrieffer-Heeger Hamiltonian with tunable parameters and time-varying hopping modulation are presented. We also show practical methods for measuring the particle transport in the proposed cold atom systems by numerically calculating the shift of the Wannier center and the center of mass of an atomic cloud.
“…In addition, the finite temperature effects do not interfere with the particle transport progression for temperatures smaller than the energy gap [33]. This requires the temperature of the order of 0.08E R /k B ∼ 20 nk (k B is the Boltzmann constant), which has been achieved in current experiments with, e.g., 40 K atoms. So we can conclude that the required Hamiltonian with tunable parameters and the adiabatic condition are able to be realized under realistic circumstances.…”
Section: A Two Experimental Setupsmentioning
confidence: 98%
“…The shift of the Wannier center encodes the adiabatic particle transport (the variation of polarization) as [33,39,40]…”
Section: B Experimental Measurement Methodsmentioning
confidence: 99%
“…This is an analog of the adiabatic charge pumping proposed by Thouless [32]; however, the parametric driving in our case does not form a closed cycle but only a half one. The topological pumping in cold atom systems and photonic quasi-crystals has been discussed in the contexts of SSH model [33][34][35] and 1D quasi-periodic Harper model [36][37][38][39][40], where the pumping particle is shown to be quantized one over one period and can be fractional over a fraction of one period [40].…”
We propose a scheme to mimic and directly measure the fractional particle number in a generalized Su-Schrieffer-Heeger model with ultracold fermions in one-dimensional optical lattices. We show that the fractional particle number in this model can be simulated in the momentum-time parameter space in terms of Berry curvature without a spatial domain wall. In this simulation, a hopping modulation is adiabatically tuned to form a kink-type configuration and the induced current plays the role of an analogous soliton distributing in the time domain, such that the mimicked fractional particle number is expressed by the particle transport. Two feasible experimental setups of optical lattices for realizing the required Su-Schrieffer-Heeger Hamiltonian with tunable parameters and time-varying hopping modulation are presented. We also show practical methods for measuring the particle transport in the proposed cold atom systems by numerically calculating the shift of the Wannier center and the center of mass of an atomic cloud.
“…The same topological invariant was also used to classify the integer quantum Hall effect [3]. There have been continuous interest in the topological charge pumping [4,5,6,7,8,9,10].…”
Abstract. Based on the Floquet scattering theory, we analytically investigate the topological spin pumping for an exactly solvable model. Floquet spin Chern numbers are introduced to characterize the periodically time-dependent system. The topological spin pumping remains robust both in the presence and in the absence of the timereversal symmetry, as long as the pumping frequency is smaller than the band gap, where the electron transport involves only the Floquet evanescent modes in the pump. For the pumping frequency greater than the band gap, where the propagating modes in the pump participate in the electron transport, the spin pumping rate decays rapidly, marking the end of the topological pumping regime.
“…In particular, the sum of the Chern numbers of all the filled bands below the Fermi surface determines the number of pumped charges over one adiabatic cycle in a one-dimensional (1D) periodic lattice. To date various quantum pumps have been proposed to study topological phases and topological phase transitions [3][4][5][6][7][8][9][10][11][12]. Thouless's concept, which can be deemed as a dynamical version of the integer quantum Hall effect, is directly simulated this year in two cold-atom experiments [13,14].…”
Thouless's quantum adiabatic pumping is of fundamental interest to condensed-matter physics.It originally considered a zero-temperature equilibrium state uniformly occupying all the bands below a Fermi surface. In the light of recent direct simulations of Thouless's concept in cold-atom systems, this work investigates the dynamics of quantum adiabatic pumping subject to dephasing, for rather general initial states with nonuniform populations and possibly interband coherence. Using a theory based on pure-dephasing Lindblad evolution, we find that the pumping is contributed by two parts of different nature, a dephasing-modified geometric part weighted by initial Bloch state populations, and an interband-coherence-induced part compromised by dephasing, both of them being independent of the pumping time scale. The overall pumping reflects an interplay of the band topology, initial state populations, initial state coherence, and dephasing. Theoretical results are carefully checked in a Chern insulator model coupled to a pure-dephasing environment, providing a useful starting point to understand and coherently control quantum adiabatic pumping in general situations.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.