On the Influence of the Magnetic Ordering on Thermodynamic and Electrical Properties in the Hubbard Model

1983 ◽  
Vol 120 (2) ◽  
pp. 621-629 ◽  
Author(s):  
W. Schumacher
2021 ◽  
Vol 7 (7) ◽  
pp. 93
Author(s):  
Samia Benmansour ◽  
Carlos J. Gómez-García

Here, we review the different series of (super)conducting and magnetic radical salts prepared with organic donors of the tetrathiafulvalene (TTF) family and oxalato-based metal complexes (ox = oxalate = C2O42−). Although most of these radical salts have been prepared with the donor bis(ethylenedithio)tetrathiafulvalene (BEDT-TTF = ET), we also include all the salts prepared with other TTF-type donors such as tetrathiafulvalene (TTF), tetramethyl-tetrathiafulvalene (TM-TTF), bis(ethylenediseleno)tetrathiafulvalene (BEST), bis(ethylenedithio)tetraselenafulvalene (BETS) and 4,5bis((2S)-2-hydroxypropylthio)-4’,5’-(ethylenedithio)tetrathiafulvalene (DMPET). Most of the oxalate-based complexes are monomers of the type [MIII(C2O4)3]3−, [Ge(C2O4)3]2− or [Cu(C2O4)2]2−, but we also include the reported salts with [Fe2(C2O4)5]4− dimers, [MII(H2O)2[MIII(C2O4)3]2]4− trimers and homo- or heterometallic extended 2D layers such as [MIIMIII(C2O4)3]− and [MII2(C2O4)3]2−. We will present the different structural families and their magnetic properties (such as diamagnetism, paramagnetism, antiferromagnetism, ferromagnetism and even long-range magnetic ordering) that coexist with interesting electrical properties (such as semiconductivity, metallic conductivity and even superconductivity). We will focus on the electrical and magnetic properties of the so-called Day series formulated as β”-(BEDT-TTF)4[A+MIII(C2O4)3]·G, which represents the largest family of paramagnetic metals and superconductors reported to date, with more than fifty reported examples.


1972 ◽  
Vol 27 (6) ◽  
pp. 889-893 ◽  
Author(s):  
Rainer Jelitto

Abstract We have calculated the ground state energy of the Hubbard model in the approximation of Hubbard's first paper1 . For the neutral model with nearest neighbour interaction the energy resulting from the selfconsistent paramagnetic solution is compared with those ones following from the (ferromagnetic) Hartree-Fock and an (antiferromagnetic) single particle theory. The energy of the latter one turns out to be the best approximation of the true ground state energy of the model for all values of the coupling constant V0 , but the energy derived from Hubbard's approximation, in spite of the absence of magnetic ordering, is a reasonable approximation at least for sufficiently large values of V0.


1988 ◽  
Vol 153-155 ◽  
pp. 1277-1278 ◽  
Author(s):  
Marc Gabay ◽  
Sebastian Doniach ◽  
Masahiko Inui

2008 ◽  
Vol 59 (11) ◽  
Author(s):  
Emil Burzo ◽  
Istvan Balasz ◽  
Mihaela Albu

The Y0.67Ca0.33Mn1-yAlyO3 system with y � 0.2, crystallizes in an orthorhombic type structure having Pnma space group. The La1-xPbxMnO3 perovskites with 0.24 � x 0.40 have a rhombohedral structure of R 3c�type. The Y0.67Ca0.33Mn1-yAlyO3 samples show a mictomagnetic type behaviour. The analysis of charge compensation mechanism suggests that the number of oxygen vacancies increases with Al content. A semiconducting type behaviour was also shown. The contributions of double exchange mechanism to magnetic ordering in La1-xPbxMnO3 increase as the lead content is higher. A nearly ferromagnetic type ordering was shown for the sample with x=0.4. The number of Mn4+ ions fits well with the Pb2+ ones, suggesting that the change in Mn valence state is the dominant mechanism for charge compensation. A transition from metallic to semiconducting type behaviour is shown at temperatures by@130 K lower than the Curie points. Magnetoresistivities up to @ 50 % were determined in fields of 60�70 kOe.


2013 ◽  
Vol 763 ◽  
pp. 17-22
Author(s):  
Zeng Hua Cai ◽  
Ling Zhang ◽  
Jing Huang ◽  
Chun Lan Ma

The structural and electronic properties of fully-relaxed thin-film SrTcO3 are investigated using first-principles method. In contrast to the insulating property of the bulk SrTcO3, the thin-film SrTcO3 with a thickness of 8.06 Å is found to be nearly metallic with a very small band gap of 0.17 eV. Its band structure meets the demands of being thermoelectric material. Moreover, thin-film SrTcO3 is found to retain its bulk high magnetic ordering temperature(TN) property, which suggests that it is applicable in high ambient temperatures. Comparison of the electronic/magnetic property of thin-film and bulk SrTcO3 is performed to explore the origins of their different electrical properties.


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