Topology and many-body physics in synthetic lattices
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1 Topology and many-body physics in synthetic lattices Alessio Celi Synthetic dimensions workshop, Zurich 20-23/11/17
2 Synthetic Hofstadter strips as minimal quantum Hall experimental systems Alessio Celi Synthetic dimensions workshop, Zurich 20-23/11/17
3 Plan Synthetic lattice (Extradimension) Synthetic strip as minimal integer quantum Hall systems Edge states in narrow strips Topological response in narrow strips
4 Plan Synthetic lattice (Extradimension) Synthetic strip as minimal integer quantum Hall systems Edge states in narrow strips Topological response in narrow strips Dimerized interacting ladder Meissner/Vortex phase (in analogy to type II superconductors) Effect of the dimerization: Reverse of chiral current (single particle) Commensurate-Incommensurate transition (strong interactions)
5 Plan Synthetic lattice (Extradimension) Synthetic strip as minimal integer quantum Hall systems Edge states in narrow strips Topological response in narrow strips Dimerized interacting ladder Meissner/Vortex phase (in analogy to type II superconductors) Effect of the dimerization: Reverse of chiral current (single particle) Commensurate-Incommensurate transition (strong interactions) Interacting flux ladder from ion chains and a puzzle
6 Plan Synthetic lattice (Extradimension) Synthetic strip as minimal integer quantum Hall systems Edge states in narrow strips Topological response in narrow strips Dimerized interacting ladder Meissner/Vortex phase (in analogy to type II superconductors) Effect of the dimerization: Reverse of chiral current (single particle) Commensurate-Incommensurate transition (strong interactions) Interacting flux ladder from ion chains and a puzzle Prospects and philosophical view
7 Simulating an extra dimension [Boada,AC,Latorre,Lewenstein, PRL 108, (2012)] In optical lattices 1D-3D Hubbard model by tuning optical potential And > 3D? In a lattice Dimensionality Connectivity Atoms in D+1-lattice = coherently coupled atomic states in D-lattices Not only spin states Momentum states Trap modes Not only atoms Cold molecules, Photonic crystal, Ring resonators
8 Synthetic dim. Synthetic gauge fields in synthetic dimension [AC et al PRL 112, (2014)] X= n a 1d-lattice loaded e.g. with 87 Rb (F=1, m=-1,0,1) + Raman dressing J Constant magnetic flux! J Exp[i n] Minimal instance of a quantum Hall system!
9 Synthetic dim. Synthetic gauge fields in synthetic dimension [AC et al PRL 112, (2014)] X= n a 1d-lattice loaded e.g. with 87 Rb (F=1, m=-1,0,1) + Raman dressing J Constant magnetic flux! J Exp[i n] Sharp Boundaries Edge currents (hard to get in real 2d lattice) signal of Topological nature of quantum Hall (bulk-boundary correspondence)
10 Synthetic gauge fields in synthetic dimension [AC et al PRL 112, (2014)] Spectrum "Genuine" Edge states for small J /J: -live in the gap, -have linear dispersion -have well defined spin
11 Synthetic gauge fields in synthetic dimension [AC et al PRL 112, (2014)] Spectrum Experimental Realizations: I) Bosons: NIST Spielman group 87 Rb [Science (2015)] "Genuine" Edge states for small J /J: -live in the gap, -have linear dispersion -have well defined spin
![Synthetic gauge fields in synthetic dimension [AC et al PRL 112, 043001 (2014)] Spectrum Experimental Realizations: I) Bosons: NIST Spielman group 87 Rb [Science](/docs-images/89/99397536/images/12-0.jpg "(2015)] II) Fermions: LENS Fallani group 173 Yb [Science (2015)] \"Genuine\" Edge states for small J /J: -live in the gap, -have linear dispersion -have well defined")
12 Synthetic gauge fields in synthetic dimension [AC et al PRL 112, (2014)] Spectrum Experimental Realizations: I) Bosons: NIST Spielman group 87 Rb [Science (2015)] II) Fermions: LENS Fallani group 173 Yb [Science (2015)] "Genuine" Edge states for small J /J: -live in the gap, -have linear dispersion -have well defined spin
13 Synthetic gauge fields in synthetic dimension [AC et al PRL 112, (2014)] Spectrum Experimental Realizations: I) Bosons: NIST Spielman group 87 Rb [Science (2015)] II) Fermions: LENS Fallani group 173 Yb [Science (2015)] Also with clock states (ladder) LENS: Livi et al. PRL 117, (2016) JILA: Kolkowitz et al. Nature (2017) "Genuine" Edge states for small J /J: -live in the gap, -have linear dispersion -have well defined spin
14 Topology in narrow strips Narrow Hofstadter strips have edge states What about the bulk?
15 Topology in narrow strips Narrow Hofstadter strips have edge states What about the bulk? How big should it be to display topological properties? Is there some reminiscence of open/closed boundary correspondence? Is Chern number defined? / Can we measure it?
16 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Pragmatic approach: measure transverse displacement to a force after a Bloch oscillation, Laughlin pump argument
17 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Pragmatic approach: measure transverse displacement to a force after a Bloch oscillation, Laughlin pump argument - Large (periodic) system, a lowest band state well localized in y and spread in x - Apply a force along x Brillouin sketch
18 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Pragmatic approach: measure transverse displacement to a force after a Bloch oscillation, Laughlin pump argument - Large (periodic) system, a lowest band state well localized in y and spread in x - Apply a force along x Brillouin sketch of semiclassical dynamics
19 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Pragmatic approach: measure transverse displacement to a force after a Bloch oscillation, Laughlin pump argument - Large (periodic) system, a lowest band state well localized in y and spread in x - Apply a force along x - After a Bloch oscillation observe the displacement Brillouin sketch of semiclassical dynamics Displacement in y due to anomalous velocity!
20 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Pragmatic approach: measure transverse displacement to a force after a Bloch oscillation, Laughlin pump argument In formulae: semiclassical approach Wave packet: State easy to prepare if the coupling
21 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Pragmatic approach: measure transverse displacement to a force after a Bloch oscillation, Laughlin pump argument In formulae: semiclassical approach Wave packet: State easy to prepare if the coupling Applicable also to strips until we don t reach the boundary
22 Measuring Chern numbers in (narrow) Scheme: Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017)
23 Measuring Chern numbers in (narrow) Scheme: Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Results:
24 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Why does it work? Perturbative argument as for the edge states: Gap linear in Hybridization spin states (spreading in ) quadratic in Quadratic degradation of the measurement
25 Measuring Chern numbers in (narrow) Scheme: Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Results:
26 Measuring Chern numbers in (narrow) Hofstadter strips, S.Mugel,.AC, SciPost 3, 012, (2017) Higher possible for Ex: Better than Fukui-Hatsugai-Suzuki algorithm J. Phys. Soc. Jpn. (2005) Robust to disorder (< gap) and typical harmonic confinement Interactions? Gap small (although may hold thought adiabatic argument, see later)
27 Synthetic lattices in interaction Interesting route to interaction -> Fractional QH effect?! -> many-body localization?! No heating expected Peculiarity: Interactions are naturally long range in the synthetic dimension Quasi 1D approach to 2D interesting both theoretically & practically
28 Synthetic lattices in interaction Interesting route to interaction -> Fractional QH effect?! -> many-body localization?! No heating expected Peculiarity: Interactions are naturally long range in the synthetic dimension Quasi 1D approach to 2D interesting both theoretically & practically Many studies: Meissner-vortex and commensurable incommensurable transitions, Fractional pumping, Laughlin like states, pseudo Majorana Here: effect of dimerization on synthetic Hofstadter ladder
29 Meissner/Vortex phase in flux ladder No interactions: real = synthetic ladder Weak interleg (Raman) coupling: Strong interleg (Raman) coupling: 2 minima, 1 minimum, [Orignac,Giamarchi, PRB 2001] Analogous to type II, also in presence interactions Real ladder experiment [Atala et, Nature Phys. 2014]
30 Meissner/Vortex phase in flux ladder No interactions: real = synthetic ladder Weak interleg (Raman) coupling: 2 minima, Observables Strong interleg (Raman) coupling: 1 minimum, [Orignac,Giamarchi, PRB 2001] Analogous to type II, also in presence interactions Real ladder experiment [Atala et, Nature Phys. 2014]
31 Meissner/Vortex phase in flux ladder No interactions: real = synthetic ladder Weak interleg (Raman) coupling: 2 minima, Observables Strong interleg (Raman) coupling: 1 minimum, [Orignac,Giamarchi, PRB 2001] Analogous to type II, also in presence interactions Real ladder experiment [Atala et, Nature Phys. 2014]
32 Meissner/Vortex phase in flux ladder U Effect of interactions: suppress vortex phase Real ladder: vortex phase survives in the hard-core limit for more phases at Synthetic ladder: vortex phase disappears in the hard-core limit large see [Petrescu, Le Hur,PRL 2013] [Piraud et al, PRB 2015] more phases at.
33 Meissner/Vortex phase in flux ladder U Effect of interactions: suppress vortex phase Real ladder: vortex phase survives in the hard-core limit for more phases at Synthetic ladder: vortex phase disappears in the hard-core limit large see [Petrescu, Le Hur,PRL 2013] [Piraud et al, PRB 2015] more phases at. Idea: enhance vortex phase by dimerizing the lattice ( easy exp. handle)
34 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress Effect of dimerization: new handle
35 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress Effect of dimerization: new handle No interactions: 4 bands Bands deform & mix Minima separate: dimerization enhances vortex phase!
36 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress Effect of dimerization: new handle No interactions: Reverse of chiral current Current behavior confirms vortex enhancement!
37 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress U Effect of dimerization: new handle Interactions: 3 states per rung
38 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress U Effect of dimerization: new handle Interactions: 3 states per rung 9 states per plaquette 1 n=0, 4 n=1, 4 n=2 Spectrum plaquette
39 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress Interactions: U Effect of dimerization: new handle 3 states per rung 9 states per plaquette 1 n=0, 4 n=1, 4 n=2 Spectrum plaquette Plaquette in n=2 Plaquette in n=1 Band insulator Imprinted vortex
40 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress DMRG calculations confirm perturbative expectations Ex. Phase diagram through calculation of currents and structure factors
41 Vortex Nesting and Melting in synthetic ladders, E. Tirrito, R. Citro, M. Lewenstein, AC in progress Ex. Imprinted vortex Melted vortex Meissner charge density wave Meissner Similar to attractive interleg interaction, [Orignac et al, PRB 96, (2017)] Evidence of commensurate-incommensurate transition
42 Further steps No hard-core boson limit: bosons different fermions Study the accessible experimental parameters Search for visible Laughlin-like states in such regimes cf. [Calvanese et al, PRX 7, (2017)],[Petrescu et al, PRB 96, (2017)] Toy model for many-body localization?
43 Alternative route to synthetic interacting ladders long range interactions!
44 Alternative route to synthetic interacting ladders long range interactions! How? E.g. ion analogue simulation
45 Alternative route to synthetic interacting ladders long range interactions! Driven Dicke model with fluxes seems robust to photon heating! Special instance: Triangle! [T. Grass,AC,G. Pagano,M. Lewenstein, arxiv: ] Deviation from the effective spin model are suppressed also for strong driving in presence of fluxes! Topological protection?
46 Summary Synthetic edge state in synthetic Hofstadter strips Bulk topology in synthetic Hofstadter strips Effect of dimerization in synthetic Hofstadter ladder w/o interactions Synthetic fluxes in driven ion chain
47 A bit of philosophy Synthetic lattices: practical tool for reshaping degrees of freedom in experimentally convenient way Same Hamiltonian = Same model Useful approach for questioning conventions, ease detection, suggest new models
48 A bit of philosophy Synthetic lattices: practical tool for reshaping degrees of freedom in experimentally convenient way Same Hamiltonian = Same model Useful approach for questioning conventions, ease detection, suggest new models Pushing it further Same time evolution = Same model Synthetic lattices naturally combine with the Floquet approach Realization of quantum simulation paradigm
49 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein
50 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass
51 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass G. Juzeliunas P. Massignan J. Ruseckas N. Goldman I.B. Spielman
52 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass G. Juzeliunas P. Massignan J. Ruseckas N. Goldman I.B. Spielman J. Rodriguez-Laguna
53 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass G. Juzeliunas P. Massignan J. Ruseckas N. Goldman I.B. Spielman J. Rodriguez-Laguna C. Muschik R.W. Chhajlany
54 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass G. Juzeliunas P. Massignan J. Rodriguez-Laguna J. Ruseckas N. Goldman I.B. Spielman C. Muschik R.W. Chhajlany S. Mugel J. Asboth C. Lobo
55 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass G. Juzeliunas P. Massignan J. Rodriguez-Laguna J. Ruseckas N. Goldman I.B. Spielman C. Muschik R.W. Chhajlany S. Mugel J. Asboth C. Lobo A. Dauphin L. Tarruell
56 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass G. Juzeliunas P. Massignan J. Rodriguez-Laguna J. Ruseckas N. Goldman I.B. Spielman C. Muschik R.W. Chhajlany S. Mugel J. Asboth C. Lobo A. Dauphin L. Tarruell E. Tirrito R. Citro
57 Extradimensional collaborators J.I. Latorre O. Boada M. Lewenstein T. Grass G. Juzeliunas P. Massignan J. Rodriguez-Laguna J. Ruseckas N. Goldman I.B. Spielman C. Muschik R.W. Chhajlany S. Mugel J. Asboth C. Lobo A. Dauphin L. Tarruell E. Tirrito R. Citro.
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