𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Order and disorder operators of the Baxter model

✍ Scribed by B Berg


Publisher
Elsevier Science
Year
1979
Tongue
English
Weight
89 KB
Volume
122
Category
Article
ISSN
0003-4916

No coin nor oath required. For personal study only.

✦ Synopsis


We complete the construction of order and disorder operators of the Baxter model along the lines of a previous paper.


πŸ“œ SIMILAR VOLUMES


Comment on β€œan order-disorder model for
✍ L. Guttman πŸ“‚ Article πŸ“… 1965 πŸ› Elsevier Science βš– 280 KB

or orientation. This lattice invariant shear can occur by slip or twinning. If the lattice invariant shear occurs by slip it is not clear whether it occurs in the parent lattice, product lattice, or at an intermediate stage. The presence of sessile inherited dislocations would certainly inhibit latt

Protein folding and the order/disorder p
✍ Prakash Kulkarni; Krithika Rajagopalan; David Yeater; Robert H. Getzenberg πŸ“‚ Article πŸ“… 2011 πŸ› John Wiley and Sons 🌐 English βš– 172 KB

## Abstract Most proteins encoded by the nuclear genome are synthesized in the cytoplasm and fold into precise 3D structures. During synthesis, the nascent polypeptide begins to fold as it traverses the large subunit of the ribosome and is assisted by molecular chaperones in attaining its precise f

Spin waves, vortices, fermions, and dual
✍ Michael C Ogilvie πŸ“‚ Article πŸ“… 1981 πŸ› Elsevier Science 🌐 English βš– 890 KB

Field-theoretic methods are applied to a number of two-dimensional lattice models with Abelian symmetry groups. It is shown, using a vortex + spin-wave decomposition. that the Z, Villain models are related to a class of continuum field theories with analogous duality properties. Fermion operators f

3-State Potts Model and Automorphisms of
✍ Masahiko Miyamoto πŸ“‚ Article πŸ“… 2001 πŸ› Elsevier Science 🌐 English βš– 167 KB

We study the fusion rules of a vertex operator algebra W 0 , which is a VOA ‫ޒ‬ over the real number field ‫ޒ‬ and has a positive definite invariant bilinear form, Ε½ . q and such that its complexification ‫ރ‬W 0 is a direct sum of the 3-state Potts ‫ޒ‬ 4 4 Ε½ . Ε½ . model L , 0 and its module L , 3 .