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Intro Lieb-Robinson Long-range Applications Conclusions Supersonic propagation in long-range lattice models Michael Kastner GGI Florence, 29 May 2014 based on: D. Mtivier, R. Bachelard, and M. K., PRL (in press) J. Eisert, M. van den

Intro Lieb-Robinson Long-range Applications Conclusions Supersonic propagation in long-range lattice models Michael Kastner GGI Florence, 29 May 2014 based on: D. Métivier, R. Bachelard, and M. K., PRL (in press) J. Eisert, M. van den Worm, S. R. Manmana, and M. K., PRL 111 , 260401 (2013) R. Bachelard, M. K., PRL 110 , 170603 (2013) Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Stellenbosch Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Propagation in spatially extended systems Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Propagation in spatially extended systems Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Propagation in spatially extended systems Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Propagation in spatially extended systems Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Velocity of propagation In (some) condensed matter systems: propagation velocity is group velocity ∂ω ( k ) obtained from quasi-particle dispersion ∂ k = ⇒ General behaviour??? Lieb-Robinson bound Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Velocity of propagation In (some) condensed matter systems: propagation velocity is group velocity ∂ω ( k ) obtained from quasi-particle dispersion ∂ k = ⇒ General behaviour??? Lieb-Robinson bound Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Velocity of propagation In (some) condensed matter systems: propagation velocity is group velocity ∂ω ( k ) obtained from quasi-particle dispersion ∂ k = ⇒ General behaviour??? Lieb-Robinson bound Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Velocity of propagation In (some) condensed matter systems: propagation velocity is group velocity ∂ω ( k ) obtained from quasi-particle dispersion ∂ k = ⇒ General behaviour??? Lieb-Robinson bound Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Spatio-temporal evolution Relativistic theory: ∃ finite maximum propagation speed Nonrelativistic quantum lattice systems, finite local dimension, finite-range interactions: ∃ finite group velocity, with exponentially small effects outside an effective light cone Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Spatio-temporal evolution Relativistic theory: ∃ finite maximum propagation speed Nonrelativistic quantum lattice systems, finite local dimension, finite-range interactions: ∃ finite group velocity, with exponentially small effects outside an effective light cone Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Lieb-Robinson bound Commun. Math. Phys. 28 , 251 (1972) � [ O A ( t ) , O B ( 0 )] � � C � O A � � O B � min ( | A | , | B | ) e ( v | t |− d ( A , B )) /ξ ∃ finite group velocity, with exponentially small effects outside an effective light cone physical relevance: transmission of information, growth of entanglement, clustering of correlations, Lieb-Schultz-Mattis in D > 1, finite-size errors of simulations. . . very general result restrictions: finite local dimension ← − relax! finite interaction range Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Lieb-Robinson bound Commun. Math. Phys. 28 , 251 (1972) � [ O A ( t ) , O B ( 0 )] � � C � O A � � O B � min ( | A | , | B | ) e ( v | t |− d ( A , B )) /ξ ∃ finite group velocity, with exponentially small effects outside an effective light cone physical relevance: transmission of information, growth of entanglement, clustering of correlations, Lieb-Schultz-Mattis in D > 1, finite-size errors of simulations. . . very general result restrictions: finite local dimension ← − relax! finite interaction range Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Lieb-Robinson bound Commun. Math. Phys. 28 , 251 (1972) � [ O A ( t ) , O B ( 0 )] � � C � O A � � O B � min ( | A | , | B | ) e ( v | t |− d ( A , B )) /ξ ∃ finite group velocity, with exponentially small effects outside an effective light cone physical relevance: transmission of information, growth of entanglement, clustering of correlations, Lieb-Schultz-Mattis in D > 1, finite-size errors of simulations. . . very general result restrictions: finite local dimension ← − relax! finite interaction range Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Lieb-Robinson bound Commun. Math. Phys. 28 , 251 (1972) � [ O A ( t ) , O B ( 0 )] � � C � O A � � O B � min ( | A | , | B | ) e ( v | t |− d ( A , B )) /ξ ∃ finite group velocity, with exponentially small effects outside an effective light cone physical relevance: transmission of information, growth of entanglement, clustering of correlations, Lieb-Schultz-Mattis in D > 1, finite-size errors of simulations. . . very general result restrictions: finite local dimension ← − relax! finite interaction range Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Lieb-Robinson bound Commun. Math. Phys. 28 , 251 (1972) � [ O A ( t ) , O B ( 0 )] � � C � O A � � O B � min ( | A | , | B | ) e ( v | t |− d ( A , B )) /ξ ∃ finite group velocity, with exponentially small effects outside an effective light cone physical relevance: transmission of information, growth of entanglement, clustering of correlations, Lieb-Schultz-Mattis in D > 1, finite-size errors of simulations. . . very general result restrictions: finite local dimension ← − relax! finite interaction range Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Lieb-Robinson bound Commun. Math. Phys. 28 , 251 (1972) � [ O A ( t ) , O B ( 0 )] � � C � O A � � O B � min ( | A | , | B | ) e ( v | t |− d ( A , B )) /ξ ∃ finite group velocity, with exponentially small effects outside an effective light cone physical relevance: transmission of information, growth of entanglement, clustering of correlations, Lieb-Schultz-Mattis in D > 1, finite-size errors of simulations. . . very general result restrictions: finite local dimension ← − relax! finite interaction range Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Long-range lattice models Short-range: finite-range (e.g. nearest-neighbour) or exponentially decaying ( ∝ e − cr with c > 0) Long-range: power law decaying, ∝ 1 / r α with α � 0 Realisations of long-range many-body systems: Dipolar materials Free Electron Laser Rydberg atoms Cavity QED Crystals of trapped ions: 1 / r α Propagation in long-range lattice models??? Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Long-range lattice models Short-range: finite-range (e.g. nearest-neighbour) or exponentially decaying ( ∝ e − cr with c > 0) Long-range: power law decaying, ∝ 1 / r α with α � 0 Realisations of long-range many-body systems: Dipolar materials Free Electron Laser Rydberg atoms Cavity QED Crystals of trapped ions: 1 / r α Propagation in long-range lattice models??? Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Long-range lattice models Short-range: finite-range (e.g. nearest-neighbour) or exponentially decaying ( ∝ e − cr with c > 0) Long-range: power law decaying, ∝ 1 / r α with α � 0 Realisations of long-range many-body systems: Dipolar materials Free Electron Laser Rydberg atoms Cavity QED Crystals of trapped ions: 1 / r α Propagation in long-range lattice models??? Michael Kastner Supersonic propagation in long-range lattice models
Intro Lieb-Robinson Long-range Applications Conclusions Propagation in long-range lattice models 120 5 ln( Q pq ln( Q pq ij ) ij ) 100 20 4 0 80 10 −2 3 60 t t −4 0 2 40 −6 −10 1 −8 20 −10 −20 −100 −50 0 50 100 −100 −50 0 50 100 i − j i − j short-range long-range Absence of a finite propagation velocity! General predictions? Long-range Lieb-Robinson bounds? Michael Kastner Supersonic propagation in long-range lattice models

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