Quantum Many-Body Scars and Space-Time Crystalline Order from Magnon Condensation
APA
Iadecola, T. (2019). Quantum Many-Body Scars and Space-Time Crystalline Order from Magnon Condensation. Perimeter Institute. https://pirsa.org/19040131
MLA
Iadecola, Thomas. Quantum Many-Body Scars and Space-Time Crystalline Order from Magnon Condensation. Perimeter Institute, Apr. 30, 2019, https://pirsa.org/19040131
BibTex
@misc{ pirsa_PIRSA:19040131, doi = {10.48660/19040131}, url = {https://pirsa.org/19040131}, author = {Iadecola, Thomas}, keywords = {Condensed Matter}, language = {en}, title = {Quantum Many-Body Scars and Space-Time Crystalline Order from Magnon Condensation}, publisher = {Perimeter Institute}, year = {2019}, month = {apr}, note = {PIRSA:19040131 see, \url{https://pirsa.org}} }
We study the eigenstate properties of a nonintegrable spin chain that was recently realized experimentally in a Rydberg-atom quantum simulator. In the experiment, long-lived coherent many-body oscillations were observed only when the system was initialized in a particular product state. This pronounced coherence has been attributed to the presence of special "scarred" eigenstates with nearly equally-spaced energies and putative nonergodic properties despite their finite energy density. In this paper we uncover a surprising connection between these scarred eigenstates and low-lying quasiparticle excitations of the spin chain. In particular, we show that these eigenstates can be accurately captured by a set of variational states containing a macroscopic number of magnons with momentum π. This leads to an interpretation of the scarred eigenstates as finite-energy-density condensates of weakly interacting π-magnons. One natural consequence of this interpretation is that the scarred eigenstates possess long-range order in both space and time, providing a rare example of the spontaneous breaking of continuous time-translation symmetry. We verify numerically the presence of this space-time crystalline order and explain how it is consistent with established no-go theorems precluding its existence in ground states and at thermal equilibrium.