Critical exponents of the ferromagnetic-paramagnetic phase transition of (formula presented) (formula presented)

The critical exponents of the second-order ferromagnetic-paramagnetic phase transition of (Formula presented) (Formula presented) compounds are obtained. The results (Formula presented) (Formula presented) and (Formula presented) are qualitatively different than those reported in the literature for...

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Autor principal: Mira, J.
Otros Autores: Rivas, J., Vázquez, M., García-Beneytez, J.M, Arcas, J., Sánchez, R.D, Señarís-Rodríguez, M.A
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 1999
Acceso en línea:Registro en Scopus
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Registro en la Biblioteca Digital
Aporte de:Registro referencial: Solicitar el recurso aquí
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100 1 |a Mira, J. 
245 1 0 |a Critical exponents of the ferromagnetic-paramagnetic phase transition of (formula presented) (formula presented) 
260 |c 1999 
506 |2 openaire  |e Política editorial 
504 |a von Helmolt, R., Wecker, J., Holzapfel, B., Schultz, L., Samwer, K., (1993) Phys. Rev. Lett., 71, p. 2331 
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504 |a Archibald, W., Goodenough, J.B., (1996) Phys. Rev. B, 53, p. 14 
504 |a Yamaguchi, S., Taniguchi, H., Takagi, H., Arima, T., Tokura, Y., (1995) J. Phys. Soc. Jpn., 64, p. 1885 
504 |a Golovanov, V., Mihaly, L., Moodenbaugh, A.R., (1996) Phys. Rev. B, 53, p. 8207 
504 |a Mahendiran, R., Raychaudhuri, A.K., (1996) Phys. Rev. B, 54, p. 16 
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504 |a Señarís-Rodríguez, M.A., Goodenough, J.B., (1995) J. Solid State Chem., 118, p. 323 
504 |a Itoh, M., Natori, I., Kubota, S., Motoya, K., (1994) J. Phys. Soc. Jpn., 63, p. 1486 
504 |a Señarís-Rodríguez, M.A., Goodenough, J.B., (1995) J. Solid State Chem., 116, p. 224 
504 |a Zhuang, M., Zhang, W., Ming, N., (1998) Phys. Rev. B, 57, p. 10 
504 |a Zhuang, M., Zhang, W., Hu, C., Ming, N., (1998), 57, p. 10; Potze, R.H., Sawatzky, G.A., Abbate, M., (1995) Phys. Rev. B, 51, p. 11 
504 |a (1996) Phys. Rev. B, 54, p. 5309 
504 |a (1997) Phys. Rev. B, 55, p. 4257 
504 |a Yamaguchi, S., Okimoto, Y., Tokura, Y., (1997), 55, pp. R8666; Banerjee, S.K., (1964) Phys. Lett., 12, p. 16 
504 |a Landau, L.D., (1937) Zh. Eksp. Teor. Fiz., 7, p. 19 
504 |a Lifshitz, E.M., (1941), 11, p. 269; Ginzburg, V.L., (1947), 17, p. 833; Vonsovskii, S.V., (1947) Izv. Akad. Nauk. SSSR, Ser. Fiz., 11, p. 485 
504 |a Bean, C.P., Rodbell, D.S., (1962) Phys. Rev., 126, p. 104 
504 |a Kellner, W.U., Fähnle, M., Kronmüller, H., Kaul, S.N., (1987) Phys. Status Solidi B, 144, p. 387 
504 |a See, for example, S. V. Vonsovskii, Magnetism (Wiley, New York, 1974), Vol. 2, Chap. 25; Fisher, M.E., Nickel, B.G., (1972) Phys. Rev. Lett., 29, p. 917 
504 |a Seeger, M., Kronmüller, H., Murugaraj, P., Maier, J., (1998) J. Magn. Magn. Mater., 183, p. 348 
504 |a Lofland, S.E., Bhagat, S.M., Ghosh, K., Greene, R.L., Karabashev, S.G., Shulyatev, D.A., Arsenov, A.A., Mukovskii, Y., (1997) Phys. Rev. B, 56, p. 13 
504 |a Caciuffo, R., Mira, J., Rivas, J., Radaelli, P.G., Carsughi, F., Fiorani, D., Goodenough, J.B., M. A. Señarís-Rodríguez (unpublished); Menyuk, N., Raccah, P.M., Dwight, K., (1968) Phys. Rev., 166, p. 510 
504 |a (Formula presented) presents a distorted perovskite structure. The introduction of the larger size (Formula presented) cations progressively reduces the rhombohedral distortion present in the parent (Formula presented) For more details see, for example, Ref. 12, and references therein; Stanley, H.E., (1967) Phys. Rev., 158, p. 546 
504 |a Abbate, M., (1993) Phys. Rev. B, 47, p. 16 
504 |a Munakata, F., Takahashi, H., Akimune, Y., Shichi, Y., Tanimura, M., Inoue, Y., Itti, R., Koyama, Y., (1997) Phys. Rev. B, 56, p. 979 
504 |a Mira, J., Rivas, J., Sánchez, R.D., Señarís-Rodríguez, M.A., Fiorani, D., Rinaldi, D., Caciuffo, R., (1997) J. Appl. Phys., 81, p. 5753 
504 |a Gayathri, N., Raychaudhuri, A.K., Tiwary, S.K., Gundakaram, R., Arulraj, A., Rao, C.N.R., (1997) Phys. Rev. B, 56, p. 1345 
504 |a Poon, S.J., Durand, J., (1977) Phys. Rev. B, 16, p. 316 
504 |a Müller-Krumbhaar, H., (1976) J. Phys. C, 9, p. 345 
520 3 |a The critical exponents of the second-order ferromagnetic-paramagnetic phase transition of (Formula presented) (Formula presented) compounds are obtained. The results (Formula presented) (Formula presented) and (Formula presented) are qualitatively different than those reported in the literature for parent manganites, and are taken as the indication of the absence of long-range interactions below the Curie point. Electronic phase segregation in hole-rich ferromagnetic and hole-poor (Formula presented)-like regions is supposed to explain the observations. The hole-poor regions would dilute the magnetic lattice and prevent the occurrence of long-range order. Also, a spin transition of the (Formula presented) ions at (Formula presented) or the hole-poor regions (acting equivalently to missed spin clusters in amorphous ferromagnets) could be the reason for the high β value in the framework of a Heisenberg model. © 1999 The American Physical Society.  |l eng 
593 |a Departamento de Física Aplicada, Universidade de Santiago, E-15706 Santiago de Compostela, Spain 
593 |a Instituto de Magnetismo Aplicado (UCM/RENFE) and Instituto de Ciencia de Materiales (CSIC), P.O. Box 155, Las Rozas, 28230, Madrid, Spain 
593 |a Departamento de Física, Universidad de Buenos Aires, Buenos Aires, 1428, Argentina 
593 |a Departamento de Qímica Fundamental e Industrial, Universidade de A Coruña, E-15008 A Coruña, Spain 
700 1 |a Rivas, J. 
700 1 |a Vázquez, M. 
700 1 |a García-Beneytez, J.M. 
700 1 |a Arcas, J. 
700 1 |a Sánchez, R.D. 
700 1 |a Señarís-Rodríguez, M.A. 
773 0 |d 1999  |g v. 59  |h pp. 123-126  |k n. 1  |p Phys. Rev. B Condens. Matter Mater. Phys.  |x 10980121  |t Physical Review B - Condensed Matter and Materials Physics 
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856 4 0 |u https://doi.org/10.1103/PhysRevB.59.123  |y DOI 
856 4 0 |u https://hdl.handle.net/20.500.12110/paper_10980121_v59_n1_p123_Mira  |y Handle 
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