Диссертация (1102800), страница 15
Текст из файла (страница 15)
- P. 496–497.Millet P., Bastide B., Pashchenko V., Gnatchenko S., Gapon V., Ksari Y.,Stepanov a. Syntheses, crystal structures and magnetic properties offrancisite compounds Cu3Bi(SeO3)2O2X (X = Cl, Br and I) // J. Mater. Chem.- 2001. - V. 11, № 4. - P. 1152–1157.Nazarchuk E. V., Krivovichev S. V., Pankratova O.Y., Filatov S.K. Thermalexpansion of francisite, [Cu3BiO2](SeO3)2Cl, and its interpretation based onoxocentered copper-bismuth tetrahedra // Phys.
Chem. Miner. - 2000. - V.27, № 6. - P. 440–444.Becker R., Johnsson M. Crystal structure of Cu3Bi(TeO3)2O2Cl: A Kagome12528.29.30.31.32.33.34.35.36.37.38.39.lattice type compound // Solid State Sci. - 2005. - V. 7, № 4. - P. 375–380.Berdonosov P.S., Dolgikh V. a. Copper lanthanide selenite oxohalides withfrancisite structure: Synthesis and structural characteristics // Russ. J. Inorg.Chem. - 2008. - V. 53, № 9. - P. 1353–1358.Miller K.H., Stephens P.W., Martin C., Constable E., Lewis R.
a., Berger H.,Carr G.L., Tanner D.B. Infrared phonon anomaly and magnetic excitations insingle-crystal Cu3Bi(SeO3)2O2Cl // Phys. Rev. B. - 2012. - V. 86, № 17. - P.174104.Pregelj M., Zaharko O., Günther A., Loidl A., Tsurkan V., Guerrero S.Magnetic ground state and two-dimensional behavior in pseudo-kagomelayered system Cu3Bi(SeO3)2O2Br // Phys. Rev. B. - 2012. - V.
86, № 14. - P.144409.Deisenhofer J., Eremina R.M., Pimenov A., Gavrilova T., Berger H.,Johnsson M., Lemmens P., Krug von Nidda H. -a., Loidl A., Lee K.-S.,Whangbo M.-H. Structural and magnetic dimers in the spin-gapped systemCuTe2O5 // Phys. Rev. B. - 2006. - V. 74, № 17. - P. 174421.Rousochatzakis I., Richter J., Zinke R., Tsirlin A. a. Frustration andDzyaloshinsky-MoriyaanisotropyinthekagomefrancisitesCu3Bi(SeO3)2O2X (X = Br, Cl) // Phys.
Rev. B. - 2015. - V. 91, № 2. - P.24416.Harris a. B., Kallin C., Berlinsky a. J. Possible Néel orderings of theKagomé antiferromagnet // Phys. Rev. B. - 1992. - V. 45, № 6. - P. 2899–2919.Wang Z., Schmidt M., Goncharov Y., Tsurkan V., Krug von Nidda H.-A.,Loidl A., Deisenhofer J. Terahertz spectroscopy in the pseudo-Kagomesystem Cu3Bi(SeO3)2O2Br: Strongly Correlated Electrons // Phys.
Rev. B. 2012. - V. 86, № 17. - P. 174411.Birgeneau R.J. Phase Transitions and Magnetic Correlations in TwoDimensional Antiferromagnets // J. Appl. Phys. - 1970. - V. 41, № 3. - P.1303.Puche R.S., Norton M., White T.R., Glaunsingert W.S. Magnetic Propertiesof the Semiconducting Ln2Cu04 and Their Interpretation : Evidence PlanarCopper Antiferromagnets ” Lanthanide Cuprates for a New Series of // J.Solid State Chem.
- 1983. - V. 50. - P. 281–293.Seaman C.L., Ayoub N.Y., Bjørnholm T., Early E.A., Ghamaty S., LeeB.W., Markert J.T., Neumeier J.J., Tsai P.K., Maple M.B. Magnetic andsuperconductingpropertiesoftheelectron-dopedcompoundsLn2−xMxCuO4−y (Ln = Pr, Nd, Sm, Eu, Gd: M = Ce, Th) // Phys. CSupercond.
- 1989. - V. 159, № 4. - P. 391–403.Kovba M.L., Emelina a. L., Batuk M.M., Sorokin V. V. Thermodynamicproperties of nonsuperconducting Ln2CuO4 (Ln = Nd, Sm, Eu), Ho2Cu2O5and Ln2BaCuO5 (Ln = Nd, Sm, Eu, Ho, Yb) cuprates // Russ. J. Phys. Chem.A.
- 2011. - V. 85, № 9. - P. 1533–1539.Denisova L.T., Chumilina L.G., Denisov V.M. Heat capacity of Ln2CuO412640.41.42.43.44.45.46.47.48.49.50.51.(Ln = La-Gd) cuprates // Phys. Solid State. - 2014. - V. 56, № 9. - P. 1928–1931.Sobolev V.L., Huang H.L., Vitebskii I.M., Knigavko A.N., Pashkevich Y.G.Spin-reorientation phase transition in Nd2CuO4 in an external magnetic field:Unusual manifestations of magnetoelastic coupling // Phys. Rev. B / ed.Intergovernmental Panel on Climate Change.
Cambridge: CambridgeUniversity Press, - 1993. - V. 48, № 5. - P. 3417–3422.Butera A., Tovar M., Oseroff S.B., Fisk Z. In-plane magnetization anisotropyin Gd2CuO4 single crystals // Phys. Rev. B. - 1995. - V. 52, № 18. - P.13444–13449.Search H., Journals C., Contact A., Iopscience M., Address I.P. MagneticField-Induced Weak Ferromagnetic Order in Y , Cu04 . - V. 651.Rouco A., Obradors X., Tovar M., Pérez F., Chateigner D., Bordet P.Magnetic phase diagram of Y2CuO4: Weak ferromagnetism andmetamagnetic transition // Phys. Rev. B. - 1994.
- V. 50, № 14. - P. 9924–9936.Oseroff S.B., Rao D., Wright F., Vier D.C., Schultz S., Thompson J.D., FiskZ., Cheong S.-W., Hundley M.F., Tovar M. Complex magnetic properties ofthe rare-earth copper oxides, R2CuO4 , observed via measurements of the dcand ac magnetization, EPR, microwave magnetoabsorption, and specific heat// Phys. Rev. B. - 1990. - V.
41, № 4. - P. 1934–1948.Tovar M., Obradors X., Pérez F., Oseroff S.B., Duro R.J., Rivas J.,Chateigner D., Bordet P., Chenavas J. Weak ferromagnetism and spin-glasslike behavior in the rare-earth cuprates R2CuO4 (R=Tb, Dy, Ho, Er, Tm, andY) // Phys. Rev. B. - 1992. - V. 45, № 9. - P. 4729–4737.Thompson J.D., Cheong S.-W., Brown S.E., Fisk Z., Oseroff S.B., Tovar M.,Vier D.C., Schultz S. Magnetic properties of Gd2CuO4 crystals // Phys. Rev.B.
- 1989. - V. 39, № 10. - P. 6660–6666.Matsuda M., Yamada K., Kakurai K., Kadowaki H., Thurston T.R., EndohY., Hidaka Y., Birgeneau R.J., Kastner M.A., Gehring P.M., Moudden A.H.,Shirane G. Three-dimensional magnetic structures and rare-earth magneticordering in Nd2CuO4 and Pr2CuO4 // Phys. Rev. B. - 1990. - V. 42, № 16. - P.10098–10107.Skanthakumar S., Lynn J.W., Peng J.L., Li Z.Y. Antiferromagnetic order ofCu in Sm2CuO4 // J. Appl.
Phys. - 1991. - V. 69, № 8. - P. 4866–4868.Park C. Observation of noncollinear magnetic structure for the Cu spins inNd2CuO4-type systems // Phys. Rev. B. - 1993. - V. 47, № 10. - P. 6173–6176.Chattopadhyay T., Brown P.J., Roessli B., Stepanov A.A., Barilo S.N.,Zhigunov D.I. Magnetic ordering of Cu in Gd2CuO4 // Phys. Rev. B. - 1992. V. 46, № 9. - P. 5731–5734.Takikawa Y., Ebisu S., Nagata S.
Van Vleck paramagnetism of the trivalentEu ions // J. Phys. Chem. Solids. Elsevier, - 2010. - V. 71, № 11. - P. 1592–1598.12752.53.54.55.56.57.58.59.60.61.62.63.64.65.66.67.Dunlap B.D., Shenoy G.K. Crystal-field analysis for the susceptibility oflanthanide compounds of the form Cs2NaRCl6 // Phys. Rev. B. - 1975.
- V.12, № 7. - P. 2716–2724.Wakeshima M., Harada D., Hinatsu Y., Masaki N. Magnetic Properties ofOrdered Perovskites Ba2LnIrO6 (Ln=Sm, Eu, Gd, and Yb) // J. Solid StateChem. - 1999. - V. 147, № 2. - P. 618–623.Sasaki Y., Doi Y., Hinatsu Y. Magnetic and calorimetric studies of doubleperovskites Ba2LnReO6 (Ln = Y, Nd, Sm, Lu) // J.
Mater. Chem. - 2002. - V.12, № 8. - P. 2361–2366.Bain G.A., Berry J.F. Diamagnetic Corrections and Pascal’s Constants // J.Chem. Educ. American Chemical Society, - 2008. - V. 85, № 4. - P. 532.Banks M.G., Kremer R.K., Hoch C., Simon A., Ouladdiaf B., Broto J.M.,Rakoto H., Lee C., Whangbo M.H. Magnetic ordering in the frustratedHeisenberg chain system cupric chloride CuCl2 // Phys. Rev. B Condens.Matter. - 2009. - V.
80, № 2. - P. 1–15.Giannozzi P. et al. QUANTUM ESPRESSO: a modular and open-sourcesoftware project for quantum simulations of materials. // J. Phys. Condens.Matter. IOP Publishing, - 2009. - V. 21, № 39. - P. 395502.Perdew J.P., Burke K., Ernzerhof M. Generalized Gradient ApproximationMade Simple // Phys. Rev. Lett. - 1996. - V. 77, № 18. - P. 3865–3868.Streltsov S. V., Khomskii D.I.
Theoretical prediction of Jahn-Tellerdistortions and orbital ordering in Cs2CuCl2Br2 // Phys. Rev. B. - 2012. - V.86, № 3. - P. 35109.Streltsov S., Petrova M., Morozov V., Romanenko G., Anisimov V., LukzenN. Interplay between lattice, orbital, and magnetic degrees of freedom in thechain-polymer Cu(II) breathing crystals // Phys.
Rev. B. - 2013. - V. 87, № 2.- P. 24425.Kohn W., Sham L.J. Self-Consistent Equations Including Exchange andCorrelation Effects // Phys. Rev. - 1965. - V. 140, № 4A. - P. A1133–A1138.Anderson P.W. Antiferromagnetism. Theory of Suyerexchange // Phys. Rev.- 1950. - V. 79, № 1934.Andersen O.K., Saha-Dasgupta T. Muffin-tin orbitals of arbitrary order //Phys. Rev. B - Condens.
Matter Mater. Phys. - 2000. - V. 62, № 24. - P. 219–222.Geertsma W., Khomskii D. Influence of side groups on 90 degreessuperexchange: A modification of the Goodenough-Kanamori-Andersonrules. // Phys. Rev. B. Condens. Matter. - 1996. - V.
54, № 5. - P. 3011–3014.Goodenough J.B. Magnetism and the Chemical Bond. Interscien. New York,- 1963.Nath R., Ranjith K.M., Sichelschmidt J., Baenitz M., Skourski Y., Alet F.,Rousochatzakis I., Tsirlin A.A. Hindered magnetic order from mixeddimensionalities in CuP2O6 // Phys. Rev. B - Condens. Matter Mater. Phys. 2014. - V. 89, № 1. - P. 014407.Moriya T. Anisotropic Superexchange Interaction and Weak Ferromagnetism12868.69.70.// Phys. Rev. - 1960. - V. 120, № 1.
- P. 91–98.Meyer C., Ruck B.J., Zhong J., Granville S., Preston A.R.H., WilliamsG.V.M., Trodahl H.J. Near-zero-moment ferromagnetism in thesemiconductor SmN // Phys. Rev. B - Condens. Matter Mater. Phys. - 2008. V. 78, № 17. - P. 174406.Popova M.N., Klimin S.A., Chukalina E.P., Malkin B.Z., Levitin R.Z., MillB. V., Antic-Fidancev E. High-resolution spectral study of Er3+ crystal-fieldlevels and magnetic ordering in (ErxY1-x)2BaNiO5 chain compounds // Phys.Rev.
B. - 2003. - V. 68, № 15. - P. 155103.Popova E.A., Klimin S.A., Popova M.N., Klingeler R., Tristan N., BüchnerB., Vasiliev A.N. Magnetic properties of quasi-one-dimensionalantiferromagnets (Y1−xNdx)2BaNiO5 (x=1, 0.15) // J. Magn. Magn. Mater. 2013. - V. 331. - P. 133–139.129.
![](https://s.studizba.com/z.php?f=/templates/si/i/noavatar.png&w=100&h=100&t=1"){kind=avatar}
