Abstract
We have studied magnetic excitations in the spin-Peierls phase of by inelastic neutron scattering. There is a dispersive mode which is gapped throughout the Brillouin zone. This mode is separated by an unexpected second gap of , from a continuum of magnetic excitations. The first gap (or “triplet gap”) and its associated dispersive mode are due to the breaking of a singlet dimer into a delocalized triplet. We propose that the second gap (or “solitonic gap”) and the continuum correspond to dissociation of that triplet into two unbound spin- solitons that are separated by a dimerized region of arbitrary length.
- Received 1 March 1996
DOI:https://doi.org/10.1103/PhysRevLett.78.1560
©1997 American Physical Society