2015
DOI: 10.1088/1367-2630/17/12/125002
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The Harper–Hofstadter Hamiltonian and conical diffraction in photonic lattices with grating assisted tunneling

Abstract: We propose the realization of a grating assisted tunneling scheme for tunable synthetic magnetic fields in optically induced one-and two-dimensional dielectric photonic lattices. As a signature of the synthetic magnetic fields, we demonstrate conical diffraction patterns in particular realization of these lattices, which possess Dirac points in k-space. We compare the light propagation in these realistic (continuous) systems with the evolution in discrete models representing the Harper-Hofstadter Hamiltonian, … Show more

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Cited by 15 publications
(12 citation statements)
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“…In this issue, there are a number of important contributions, including theoretical analyses that apply to both condensed matter and photonic systems. For example, there are new proposed designs to achieve optical topological protection: Ma and Shvets [26] discuss an analogue of the valley hall effect in photonics; Jacobs et al [27] propose using tellegen metamaterial systems to break Lorentz reciprocity to realize Chern insulators; and Dubcek et al [28] present a novel design to realize the Harper-Hofstadter (i.e., integer quantum-Hall-like) Hamiltonian in waveguide arrays. In the realm of Floquet topological systems, Nathan and Rudner [29] show new theoretical insights by looking at the spectra of instantaneous Hamiltonians and relating their properties to the overall topology of the stroboscopic Floquet Hamiltonian; Sommer and Simon [30] cast their experimental effort on resonator-based realizations of fractional quantum Hall systems in terms of Floquet theory; Tauber and Delplace [31] use transfer matrices to gain new analytical insight into the Floquet problem.…”
Section: Topological Phases With Photonic Materialsmentioning
confidence: 99%
“…In this issue, there are a number of important contributions, including theoretical analyses that apply to both condensed matter and photonic systems. For example, there are new proposed designs to achieve optical topological protection: Ma and Shvets [26] discuss an analogue of the valley hall effect in photonics; Jacobs et al [27] propose using tellegen metamaterial systems to break Lorentz reciprocity to realize Chern insulators; and Dubcek et al [28] present a novel design to realize the Harper-Hofstadter (i.e., integer quantum-Hall-like) Hamiltonian in waveguide arrays. In the realm of Floquet topological systems, Nathan and Rudner [29] show new theoretical insights by looking at the spectra of instantaneous Hamiltonians and relating their properties to the overall topology of the stroboscopic Floquet Hamiltonian; Sommer and Simon [30] cast their experimental effort on resonator-based realizations of fractional quantum Hall systems in terms of Floquet theory; Tauber and Delplace [31] use transfer matrices to gain new analytical insight into the Floquet problem.…”
Section: Topological Phases With Photonic Materialsmentioning
confidence: 99%
“…We estimate the effective hopping amplitude to be = K E 0.012 R . This is obtained by comparing the expansion of the initially localized single particle Gaussian wave packet in the total potential (13), with the expansion in the discrete lattice (14), and adjusting K until the two patterns coincide; this method was adopted from [48].…”
Section: Laser Assisted Tunneling In a Tonks-girardeau Gasmentioning
confidence: 99%
“…These modes appear at the lattice’s edges with intensive localization of vibrational energy, when carefully designing the dynamical lattice to obey the BDI symmetry, and, hence, enjoying non-vanishing winding numbers of ±1 [44]. The second key example in this work is enabling the QVHE in a staggered square AIM with well-defined Dirac cones at high-symmetry points, inspired from similar photonic square lattices with alternating negative/positive coupling [52,53]. While acoustic-based square crystals may exhibit the QVHE by means of tilted (or tipped-over) Dirac cones away from high-symmetry points [5961], a realization of the QVHE in square mechanical lattices remains, to our knowledge, an uncharted territory.…”
Section: Introductionmentioning
confidence: 99%