Sznajd J
Institute for Low Temperature and Structure Research, Polish Academy of Sciences, Wrocław, Poland.
Phys Rev E. 2016 Dec;94(6-1):062134. doi: 10.1103/PhysRevE.94.062134. Epub 2016 Dec 22.
The linear perturbation renormalization group (LPRG) is used to study the phase transition of the weakly coupled Ising chains with intrachain (J) and interchain nearest-neighbor (J_{1}) and next-nearest-neighbor (J_{2}) interactions forming the triangular and rectangular lattices in a field. The phase diagrams with the frustration point at J_{2}=-J_{1}/2 for a rectangular lattice and J_{2}=-J_{1} for a triangular lattice have been found. The LPRG calculations support the idea that the phase transition is always continuous except for the frustration point and is accompanied by a divergence of the specific heat. For the antiferromagnetic chains, the external field does not change substantially the shape of the phase diagram. The critical temperature is suppressed to zero according to the power law when approaching the frustration point with an exponent dependent on the value of the field.
线性微扰重整化群(LPRG)用于研究弱耦合伊辛链的相变,该链具有链内相互作用(J)以及链间最近邻相互作用(J₁)和次近邻相互作用(J₂),它们在磁场中形成三角晶格和矩形晶格。已经得到了矩形晶格在J₂ = -J₁/2以及三角晶格在J₂ = -J₁处存在失配点的相图。LPRG计算支持这样一种观点,即除了失配点外,相变总是连续的,并且伴随着比热的发散。对于反铁磁链,外场基本上不会改变相图的形状。当接近失配点时,临界温度根据幂律被抑制到零,其指数取决于场的值。