* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download pptx - Harvard Condensed Matter Theory group
Renormalization group wikipedia , lookup
Basil Hiley wikipedia , lookup
Bell test experiments wikipedia , lookup
Probability amplitude wikipedia , lookup
Quantum chromodynamics wikipedia , lookup
Matter wave wikipedia , lookup
Bohr–Einstein debates wikipedia , lookup
Renormalization wikipedia , lookup
Measurement in quantum mechanics wikipedia , lookup
Double-slit experiment wikipedia , lookup
Quantum decoherence wikipedia , lookup
Identical particles wikipedia , lookup
Wave–particle duality wikipedia , lookup
Copenhagen interpretation wikipedia , lookup
Particle in a box wikipedia , lookup
Scalar field theory wikipedia , lookup
Spin (physics) wikipedia , lookup
Quantum electrodynamics wikipedia , lookup
Hydrogen atom wikipedia , lookup
Quantum dot wikipedia , lookup
Delayed choice quantum eraser wikipedia , lookup
Quantum field theory wikipedia , lookup
Many-worlds interpretation wikipedia , lookup
Coherent states wikipedia , lookup
Quantum fiction wikipedia , lookup
Orchestrated objective reduction wikipedia , lookup
Path integral formulation wikipedia , lookup
Molecular Hamiltonian wikipedia , lookup
Density matrix wikipedia , lookup
Quantum computing wikipedia , lookup
Quantum entanglement wikipedia , lookup
Theoretical and experimental justification for the Schrödinger equation wikipedia , lookup
Bell's theorem wikipedia , lookup
Interpretations of quantum mechanics wikipedia , lookup
Relativistic quantum mechanics wikipedia , lookup
History of quantum field theory wikipedia , lookup
Quantum machine learning wikipedia , lookup
Quantum teleportation wikipedia , lookup
EPR paradox wikipedia , lookup
Quantum key distribution wikipedia , lookup
Hidden variable theory wikipedia , lookup
Quantum group wikipedia , lookup
Quantum state wikipedia , lookup
Canonical quantization wikipedia , lookup
Exploring Topological Phases With Quantum Walks Takuya Kitagawa, Erez Berg, Mark Rudner Eugene Demler Harvard University Also collaboration with A. White’s group, Univ. of Queensland PRA 82:33429 and arXiv:1010.6126 (PRA in press) Harvard-MIT $$ NSF, AFOSR MURI, DARPA, ARO Topological states of electron systems Robust against disorder and perturbations Geometrical character of ground states Realizations with cold atoms: Jaksch et al., Sorensen et al., Lewenstein et al., Das Sarma et al., Spielman et al., Mueller et al., Dalibard et al., Duan et al., and many others Can dynamics possess topological properties ? One can use dynamics to make stroboscopic implementations of static topological Hamiltonians Dynamics can possess its own unique topological characterization Focus of this talk on Quantum Walk Outline Discreet time quantum walk From quantum walk to topological Hamiltonians Edge states as signatures of topological Hamiltonians. Experimental demonstration with photons Topological properties unique to dynamics Experimental demonstration with photons Discreet time quantum walk Definition of 1D discrete Quantum Walk 1D lattice, particle starts at the origin Spin rotation Spindependent Translation Analogue of classical random walk. Introduced in quantum information: Q Search, Q computations PRL 104:100503 (2010) Also Schmitz et al., PRL 103:90504 (2009) PRL 104:50502 (2010) From discreet time quantum walks to Topological Hamiltonians Discrete quantum walk Spin rotation around y axis Translation One step Evolution operator Effective Hamiltonian of Quantum Walk Interpret evolution operator of one step as resulting from Hamiltonian. Stroboscopic implementation of Heff Spin-orbit coupling in effective Hamiltonian From Quantum Walk to Spin-orbit Hamiltonian in 1d k-dependent “Zeeman” field Winding Number Z on the plane defines the topology! Winding number takes integer values. Can we have topologically distinct quantum walks? Split-step DTQW Split-step DTQW Phase Diagram Symmetries of the effective Hamiltonian Chiral symmetry Particle-Hole symmetry For this DTQW, Time-reversal symmetry For this DTQW, Topological Hamiltonians in 1D Schnyder et al., PRB (2008) Kitaev (2009) Detection of Topological phases: localized states at domain boundaries Phase boundary of distinct topological phases has bound states Topologically distinct, Bulks are insulators so the “gap” has to close near the boundary a localized state is expected Split-step DTQW with site dependent rotations Apply site-dependent spin rotation for Split-step DTQW with site dependent rotations: Boundary State Experimental demonstration of topological quantum walk with photons A. White et al., Univ. Queensland Quantum Hall like states: 2D topological phase with non-zero Chern number Chern Number This is the number that characterizes the topology of the Integer Quantum Hall type states Chern number is quantized to integers 2D triangular lattice, spin 1/2 “One step” consists of three unitary and translation operations in three directions Phase Diagram Topological Hamiltonians in 2D Schnyder et al., PRB (2008) Kitaev (2009) Combining different degrees of freedom one can also perform quantum walk in d=4,5,… What we discussed so far Split time quantum walks provide stroboscopic implementation of different types of single particle Hamiltonians By changing parameters of the quantum walk protocol we can obtain effective Hamiltonians which correspond to different topological classes Related theoretical work N. Lindner et al., arXiv:1008.1792 Topological properties unique to dynamics Topological properties of evolution operator Time dependent periodic Hamiltonian Floquet operator Floquet operator Uk(T) gives a map from a circle to the space of unitary matrices. It is characterized by the topological invariant This can be understood as energy winding. This is unique to periodic dynamics. Energy defined up to 2p/T Example of topologically non-trivial evolution operator and relation to Thouless topological pumping Spin ½ particle in 1d lattice. Spin down particles do not move. Spin up particles move by one lattice site per period group velocity n1 describes average displacement per period. Quantization of n1 describes topological pumping of particles. This is another way to understand Thouless quantized pumping Experimental demonstration of topological quantum walk with photons A. White et al., Univ. Queensland Topological properties of evolution operator Dynamics in the space of m-bands for a d-dimensional system Floquet operator is a mxm matrix which depends on d-dimensional k New topological invariants Example: d=3 Summary Harvard-MIT Quantum walks allow to explore a wide range of topological phenomena. From realizing known topological Hamiltonians to studying topological properties unique to dynamics. First evidence for topological Hamiltonian with “artificial matter” Topological Hamiltonians in 1D Schnyder et al., PRB (2008) Kitaev (2009)