Multi-layer S=1/2 Heisenberg antiferromagnet

Physics – Condensed Matter – Strongly Correlated Electrons

Scientific paper

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

13 pages plus 8 figures

Scientific paper

10.1103/PhysRevB.59.387

The multi-layer $S={1\over 2}$ square lattice Heisenberg antiferromagnet with up to 6 layers is studied via various series expansions. For the systems with an odd number of coupled planes, the ground-state energy, staggered magnetization, and triplet excitation spectra are calculated via two different Ising expansions. The systems are found to have long range N\'eel order and gapless excitations for all ratios of interlayer to intralayer couplings, as for the single-layer system. For the systems with an even number of coupled planes, there is a second order transition point separating the gapless Ne\'el phase and gapped quantum disordered spin liquid phase, and the critical points are located via expansions in the interlayer exchange coupling. This transition point is found to vary about inversely as the number of layers. The triplet excitation spectra are also computed, and at the critical point the normalized spectra appear to follow a universal function, independent of number of layers.

No associations

LandOfFree

Say what you really think

Search LandOfFree.com for scientists and scientific papers. Rate them and share your experience with other people.

Rating

Multi-layer S=1/2 Heisenberg antiferromagnet does not yet have a rating. At this time, there are no reviews or comments for this scientific paper.

If you have personal experience with Multi-layer S=1/2 Heisenberg antiferromagnet, we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Multi-layer S=1/2 Heisenberg antiferromagnet will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFWR-SCP-O-589081

  Search
All data on this website is collected from public sources. Our data reflects the most accurate information available at the time of publication.