The real frequency response at high energy is a hard-core problem of condensed matter
physics.
On the other hand, 1D integrable models due to their exact solvability provide
reliable reference points for studying quantum and thermodynamic correlations.
Although the low energy fractional excitations are often well understood,
exploring quantum dynamics in these systems remains challenging in
the gapless regime, especially at intermediate and high energies.
References and talks
In quantum spin systems, a single spin's flip proporgates through coupling with
neighboring spins, wihch is called a "magnon" excitation.
In a ferromagnet, there exists an effective attraction between magnons, which
leads to bound states of magnons, denoted as "string states" by H. Bethe.
In one-dimensional antiferromagnet, there are thermdynamically large number of
flipped spins, hence the string states become an essentially many-body
problem.
An n-string states means that n magnons form a bound state, and they further
collide with other magnons in the scattering states.
Furthermore, the interaction among magnons in antiferromaggnet is repulsive,
hence, string states do not appear at the ground state but
show up as excited states, which can be detected through spin
spectroscopy measurements.
Bethe string states and dynamics spin responses
Based on the algebraic Bethe ansatz formalism, we study spin dynamics in the
antiferromagnetic spin-1/2 XXZ chain with the Ising anisotropy via the form-factor
formulae [Ref. 1] .
The dynamic spin structure factors (DSF) are calculated and contributions from
various excitations at different energy scales are identified under
the guidance of sum rules.
In particular, string states - complex magnon bound states merged in the sea of
scattering states of unbound magons are of particular interest.
The S+-(q,\omega) spectra separate into low, intermediate and high energy branches.
The low energy branches are dominated by fractional excitations, reflecting
antiferromagnetic quantum fluctuations.
In contrast, the two-string and three-string states govern the quantum spin
dynamics at intermediate and high energies close to the quantum criticality,
which are multi-particle inter-band excitations based on the commensurate
Neel ordered background.
Experimental realization and identification of string states in condensed-matter
systems remains a challenge up to date.
We have collaborated with A. Loidl's group providing theory support to their ESR
measurement on the dynamic spin structure measurement on the 1D XXZ chain SrCo2V2O8
[Ref 2.] .
The bound states (strings) and fractional magnetic excitations (psinons and antipsinons)
are observed in the field-induced critical regime, which are precisely described by
the Bethe ansatz.
Experiment detection of the (many-body) string states
For a non-technical report, please see
UC San Diego Physicists Apply Pencil, Paper and Sociology to Breakthrough Research .
arXiv:1702.01854.
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Last modified: Oct 16, 2018.