TY - JOUR
T1 - Dynamical Signatures of Quasiparticle Interactions in Quantum Spin Chains
AU - Keselman, Anna
AU - Balents, Leon
AU - Starykh, Oleg A.
N1 - Funding Information: We would like to thank R. Coldea and L. Motrunich for inspiring remarks and questions, J. S. Caux for pointing out Ref. , and M. Kohno for discussions of Ref. . This research is funded in part by the Gordon and Betty Moore Foundation through Grant No. GBMF8690 to UCSB to support the work of A. K. Use was made of the computational facilities administered by the Center for Scientific Computing at the CNSI and MRL (an NSF MRSEC; DMR-1720256) and purchased through NSF CNS-1725797. This work was supported by the NSF CMMT program under Grant No. DMR-1818533 (L. B.) and DMR-1928919 (O. A. S.). We benefitted from the facilities of the KITP, NSF Grant No. PHY-1748958. Publisher Copyright: © 2020 American Physical Society.
PY - 2020/10/27
Y1 - 2020/10/27
N2 - We study the transverse dynamical susceptibility of an antiferromagnetic spin-1/2 chain in the presence of a longitudinal Zeeman field. In the low magnetization regime in the gapless phase, we show that the marginally irrelevant backscattering interaction between the spinons creates a nonzero gap between two branches of excitations at small momentum. We further demonstrate how this gap varies upon introducing a second neighbor antiferromagnetic interaction, vanishing in the limit of a noninteracting "spinon gas."In the high magnetization regime, as the Zeeman field approaches the saturation value, we uncover the appearance of two-magnon bound states in the transverse susceptibility. This bound state feature generalizes the one arising from string states in the Bethe ansatz solution of the integrable case. Our results are based on numerically accurate, unbiased matrix-product-state techniques as well as analytic approximations.
AB - We study the transverse dynamical susceptibility of an antiferromagnetic spin-1/2 chain in the presence of a longitudinal Zeeman field. In the low magnetization regime in the gapless phase, we show that the marginally irrelevant backscattering interaction between the spinons creates a nonzero gap between two branches of excitations at small momentum. We further demonstrate how this gap varies upon introducing a second neighbor antiferromagnetic interaction, vanishing in the limit of a noninteracting "spinon gas."In the high magnetization regime, as the Zeeman field approaches the saturation value, we uncover the appearance of two-magnon bound states in the transverse susceptibility. This bound state feature generalizes the one arising from string states in the Bethe ansatz solution of the integrable case. Our results are based on numerically accurate, unbiased matrix-product-state techniques as well as analytic approximations.
UR - https://www.scopus.com/pages/publications/85094907368
U2 - 10.1103/PhysRevLett.125.187201
DO - 10.1103/PhysRevLett.125.187201
M3 - Article
C2 - 33196249
SN - 0031-9007
VL - 125
JO - Physical Review Letters
JF - Physical Review Letters
IS - 18
M1 - 187201
ER -