2018
DOI: 10.1103/physreva.97.043415
|View full text |Cite
|
Sign up to set email alerts
|

Mobile bound states of Rydberg excitations in a lattice

Abstract: Spin lattice models play central role in the studies of quantum magnetism and non-equilibrium dynamics of spin excitations -magnons. We show that a spin lattice with strong nearest-neighbor interactions and tunable long-range hopping of excitations can be realized by a regular array of laser driven atoms, with an excited Rydberg state representing the spin-up state and a Rydbergdressed ground state corresponding to the spin-down state. We find exotic interaction-bound states of magnons that propagate in the la… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
18
0

Year Published

2019
2019
2024
2024

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 18 publications
(19 citation statements)
references
References 66 publications
(92 reference statements)
1
18
0
Order By: Relevance
“…7(b) corresponds to the interaction-induced bound states of two excitations. These bound states are identical to the magnon bound states in spin models [54,69] or the particle-bound states in Hubbard models [58][59][60][61][62]. They are characterized by exponentially decaying φ K (r) with the maximum at r = 1, showing that it is more likely to find the excitations at adjacent sites.…”
Section: Bound and Scattering Statesmentioning
confidence: 67%
See 2 more Smart Citations
“…7(b) corresponds to the interaction-induced bound states of two excitations. These bound states are identical to the magnon bound states in spin models [54,69] or the particle-bound states in Hubbard models [58][59][60][61][62]. They are characterized by exponentially decaying φ K (r) with the maximum at r = 1, showing that it is more likely to find the excitations at adjacent sites.…”
Section: Bound and Scattering Statesmentioning
confidence: 67%
“…At any instant, we have |ψ (t ) = i< j c i j (t )|i j , with i< j |c i j (t )| 2 = 1, and the time-dependent probability amplitudes c i j (t ) are obtained by solving the corresponding Schrödinger equations. We use the scaled two-body distribution i j (t ) = |c i j (t As for the case for the single excitation, the energy spectrum ofĤ t plays an important role in determining the dynamics of the two initially localized excitations [51,57,69]. To obtain the two-excitation spectrum, we introduce the center of mass R = (i + j)a/2 and the relative r = ( j − i)a coordinates.…”
Section: Two Excitationsmentioning
confidence: 99%
See 1 more Smart Citation
“…For excitons separated by more than one site, the state evolution is governed byĤ ′ eff . Unlike spin systems reported earlier [23,46], the long-range interaction U ij can be tuned much larger than the exchange rate J ij here, which results in a highly anisotropic XXZ model and permits the existence of high-order bound states. If the NNN interaction U i,i+2 is sufficiently larger than the NN hopping rate J i,i+1 , excitons separated by one lattice site also forms bound state and exhibits correlated motion.…”
mentioning
confidence: 82%
“…When this is the case, the denominator the integrals in Eq. (12) can be simplified to (4β cos(q) − α) 2 /(4β). We can then evaluate the NNN integrals without using contour integration, but find these solutions do not obey the bound state solution.…”
Section: Appendix D Next-nearest-neighbour Bound State Solutionmentioning
confidence: 99%