%0 Journal Article %1 WOS:000083443400005 %A de Lima, JP %A Goncalves, LL %C PO BOX 211, 1000 AE AMSTERDAM, NETHERLANDS %D 1999 %I ELSEVIER SCIENCE BV %J JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS %K model; superlattices} {XY %N 3 %P 135-148 %R 10.1016/S0304-8853(99)00446-1 %T The XY model on the one-dimensional superlattice: static properties %V 206 %X The XY model (s = 1/2) on the one-dimensional alternating superlattice (closed chain) is solved exactly by using a generalized Jordan-Wigner transformation and the Green function method. Closed expressions are obtained for the excitation spectrum, the internal energy, the specific heat, the average magnetization per site, the static susceptibility, X-zz, and the two-spin correlation function in the field direction at arbitrary temperature. At T = 0, it is shown that the system presents multiple second-order phase transitions induced by the transverse field, which are associated to the zero energy mode with wave number equal to 0 or pi. It is also shown that the average magnetization as a function of the held presents, alternately, regions of plateaux (disordered phases) and regions of variable magnetization (ordered phases). The static correlation function presents an oscillating behavior in the ordered phase and its period goes to infinity at the critical point. (C) 1999 Elsevier Science B.V. All rights reserved.The XY model (s = 1/2) on the one-dimensional alternating superlattice (closed chain) is solved exactly by using a generalized Jordan-Wigner transformation and the Green function method. Closed expressions are obtained for the excitation spectrum, the internal energy, the specific heat, the average magnetization per site, the static susceptibility, chi(zz), and the two-spin correlation function in the field direction at arbitrary temperature. At T = 0, it is shown that the system presents multiple second-order phase transitions induced by the transverse field, which are associated to the zero energy mode with wave number equal to 0 or pi. It is also shown that the average magnetization as a function of the held presents, alternately, regions of plateaux (disordered phases) and regions of variable magnetization (ordered phases). The static correlation function presents an oscillating behavior in the ordered phase and its period goes to infinity at the critical point. (C) 1999 Elsevier Science B.V. All rights reserved.

@article{WOS:000083443400005, abstract = {The XY model (s = 1/2) on the one-dimensional alternating superlattice (closed chain) is solved exactly by using a generalized Jordan-Wigner transformation and the Green function method. Closed expressions are obtained for the excitation spectrum, the internal energy, the specific heat, the average magnetization per site, the static susceptibility, X-zz, and the two-spin correlation function in the field direction at arbitrary temperature. At T = 0, it is shown that the system presents multiple second-order phase transitions induced by the transverse field, which are associated to the zero energy mode with wave number equal to 0 or pi. It is also shown that the average magnetization as a function of the held presents, alternately, regions of plateaux (disordered phases) and regions of variable magnetization (ordered phases). The static correlation function presents an oscillating behavior in the ordered phase and its period goes to infinity at the critical point. (C) 1999 Elsevier Science B.V. All rights reserved.The XY model (s = 1/2) on the one-dimensional alternating superlattice (closed chain) is solved exactly by using a generalized Jordan-Wigner transformation and the Green function method. Closed expressions are obtained for the excitation spectrum, the internal energy, the specific heat, the average magnetization per site, the static susceptibility, chi(zz), and the two-spin correlation function in the field direction at arbitrary temperature. At T = 0, it is shown that the system presents multiple second-order phase transitions induced by the transverse field, which are associated to the zero energy mode with wave number equal to 0 or pi. It is also shown that the average magnetization as a function of the held presents, alternately, regions of plateaux (disordered phases) and regions of variable magnetization (ordered phases). The static correlation function presents an oscillating behavior in the ordered phase and its period goes to infinity at the critical point. (C) 1999 Elsevier Science B.V. All rights reserved.}, added-at = {2022-05-23T20:00:14.000+0200}, address = {PO BOX 211, 1000 AE AMSTERDAM, NETHERLANDS}, author = {de Lima, JP and Goncalves, LL}, biburl = {https://www.bibsonomy.org/bibtex/2b2e8d9ed15ef9f7a0107520c6426e7aa/ppgfis_ufc_br}, doi = {10.1016/S0304-8853(99)00446-1}, interhash = {8703d757fecb08ccee7030fa8a6eb8ca}, intrahash = {b2e8d9ed15ef9f7a0107520c6426e7aa}, issn = {0304-8853}, journal = {JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS}, keywords = {model; superlattices} {XY}, number = 3, pages = {135-148}, publisher = {ELSEVIER SCIENCE BV}, pubstate = {published}, timestamp = {2022-05-23T20:00:14.000+0200}, title = {The XY model on the one-dimensional superlattice: static properties}, tppubtype = {article}, volume = 206, year = 1999 }