Publications by authors named "Jian-xin Le"

Objective: To explore the clinical significance and surgical technique for revisionary submucous resection of nasal septum.

Methods: Thirty-two patients who had undergone nasal septal resection were evaluated rhinologically and the causes of unsuccessful septoplasty were analysed . Based on the location and extent of deviation, the status of residual cartilage and bone, and the age of the patients, one of three incisions was chosen during septal surgeries: (1) For 5 cases with anterior, 1 with inferior and 14 with superior deviation, a "U" shaped incision at the left side of anterior edge of septum cartilage was used.

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The critical slowing down of the kinetic Gaussian model on hierarchical lattices is studied by means of a real-space time-dependent renormalization-group transformation. The dynamic critical exponent z and the exponent Delta are calculated. For hierarchical lattices with reducible generators, both the dynamic critical exponent z and the exponent Delta are independent of the fractal dimension Df of the lattice, the number of branches m, and the number of bonds per branch b of the generator--i.

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Using the real-space renormalization-group transformation, we study the phase transitions of the Ashkin-Teller model including the antiferromagnetic interactions on a type of diamond hierarchical lattices, of which the number of bonds per branch of the generator is odd. The isotropic Ashkin-Teller model and the anisotropic one are, respectively, investigated. We find that the phase diagram, for the isotropic Ashkin-Teller model, consists of five phases, two of which are associated with the partially antiferromagnetic ordering of the system, while the phase diagram, for the anisotropic Ashkin-Teller model, contains 11 phases, six of which are related to the partially antiferromagnetic ordering of the system.

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The phase transitions of the anisotropic Ashkin-Teller model on a family of diamond-type hierarchical lattices is studied by means of the transfer-matrix method and the real-space renormalization-group transformation. We find that the phase diagram, for the ferromagnetic case, consists of five phases, i.e.

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