Effect of Strong Correlation on Metal-Insulator Transition of DCNQI-Cu Salts:Rigorous Treatment of the Local Constraint

Electronic properties originated from the strong correlation have been examined for both metallic and insulating states in organic conductor, DCNQI-Cu salt by use of a periodic Anderson model with electron-phonon interaction. The local constraint imposed on the d -electron in the Cu atom is taken into account in terms of a method of the slave-boson. Compared with the previous mean-field calculation which corresponds to the global constraint, we have found novel aspects that the transition temperature is suppressed and that the magnetic susceptibility of the insulating state exhibits the temperature dependence of the Curie law. These results are in favor of the explanation of the experimental results.

[1]  Miyazaki,et al.  First-principles theoretical study of metallic states of DCNQI-(Cu,Ag,Li) systems. , 1996, Physical review. B, Condensed matter.

[2]  Y. Shimazu,et al.  Effects of pressure and magnetic field on metal-insulator transition of partially deuterated (DM-DCNQI-d3[1,1;1])2Cu around reentrant metallic region , 1996 .

[3]  Ogawa,et al.  Electronic properties of strongly correlated states in dicyanoquinonediimine-Cu organic conductors. , 1996, Physical review. B, Condensed matter.

[4]  Hasegawa,et al.  Electronic structure of the quasi-one-dimensional organic conductors DCNQI (N,N'-dicyanoquinonediimine)-Cu salts. , 1995, Physical review. B, Condensed matter.

[5]  H. Sawa,et al.  (DCNQI)2Cu: Variety of Magnetism Arising from pπ-d Interactions , 1995 .

[6]  Miyazaki,et al.  First-principles theoretical study of metallic states of DCNQI-(Cu,Ag) systems: Simplicity and variety in complex systems. , 1995, Physical review letters.

[7]  Ogawa,et al.  Theory of the metal-insulator transition in dicyanoquinonediimine salt mixed-valence organic conductors. , 1995, Physical review. B, Condensed matter.

[8]  Aoki,et al.  Coexistence of one- and three-dimensional Fermi surfaces and heavy cyclotron mass in the molecular conductor (DMe-DCNQI)2Cu. , 1994, Physical review. B, Condensed matter.

[9]  T. Ogawa,et al.  Peierls Transition of Strongly Correlated DCNQI-Cu Salts , 1994 .

[10]  H. Sawa,et al.  Magnetic Study of Metal-Insulator-Metal Transitions in (DMe-DCNQI-α,α'-d2)2Cu , 1994 .

[11]  T. Osada,et al.  Resistance enhancement by magnetic field in the regime of the metal-insulator-metal re-entrance transition of the alloy of pristine and fully deuterated (2,5-dimethyldicyanoquinonediimine)2Cu salts , 1993 .

[12]  Y. Ono,et al.  Strongly Correlated Electrons in Mixed-Valence Conductors DCNQI-Cu Salts , 1993 .

[13]  M. Nakano,et al.  Metal-insulator transition in DCNQI-Cu , 1993 .

[14]  H. Maeda,et al.  XANES study and valence states in (R1,R2-DCNQI)2Cu , 1993 .

[15]  H. Sawa,et al.  Giant Metal-Insulator-Metal Transition Induced by Selective Deuteration of the Molecular Conductor, (DMe-DCNQI)2Cu (DMe-DCNQI = 2,5-dimethyl-N,N′-dicyanoquinonediimine) , 1993 .

[16]  Miyamoto,et al.  Mixed valency of Cu, electron-mass enhancement, and three-dimensional arrangement of magnetic sites in the organic conductors (R1,R2-N,N'-dicyanoquinonediimine)2Cu (where R1,R2=CH3,CH3O,Cl,Br). , 1993, Physical review. B, Condensed matter.

[17]  H. Fukuyama (DCNQI)2Cu: A Luttinger-Peierls System , 1992 .

[18]  H. Fukuyama,et al.  Mean-Field Theory of Mixed-Valence Conductors (R1,R2-DCNQI)2 Cu , 1992 .

[19]  Kobayashi,et al.  Copper valence fluctuation in the organic conductor (dimethyl-N,N'-dicyanoquinonediimine)2Cu studied by x-ray photoemission spectroscopy. , 1992, Physical review. B, Condensed matter.

[20]  H. Kobayashi,et al.  Thermal and magnetic properties in organic metals (DMe-DCNQI)2Cu, (DMeO-DCNQI)2Cu and (DMe1-xMeBrx-DCNQI)2Cu: Enhancement of density of states , 1992 .

[21]  Y. Ono,et al.  Electronic State of the Anderson Lattice over the Whole Temperature Range , 1991 .

[22]  A. Kobayashi,et al.  Magnetic susceptibilities of (DMe-DCNQI)2Cu and (DBr-DCNQI)2Cu , 1990 .

[23]  Y. Ono,et al.  Critical study of strongly correlated systems: A unified description of the incoherent and coherent regimes , 1989 .

[24]  Reizo Kato,et al.  Crystal and electronic structures of conductive anion-radical salts, (2,5-R1R2-DCNQI)2Cu (DCNQI = N,N'-dicyanoquinonediimine; R1, R2 = CH3, CH3O, Cl, Br) , 1989 .

[25]  R. Moret Structural instabilities in molecular conductors: Silver and copper salts of dicyanoquinonediimine, (DCNQI)2X (X = Ag or Cu) , 1988 .

[26]  Takehiko Mori,et al.  Anomalous magnetic properties of (DMDCNQI)2Cu , 1988 .

[27]  Biao Jin,et al.  Critical Study of the Anderson Impurity and the Anderson Lattice , 1988 .

[28]  P. Erk,et al.  The pressure-temperature phase diagram of the organic conductor (2,5 DM-DCNQI)2Cu , 1988 .

[29]  H. Inokuchi,et al.  The organic π-electron metal system with interaction through mixed-valence metal cation: Electronic and structural properties of radical salts of dicyano-quinodiimine, (DMe-DCNQI)2Cu and (MeCl-DCNQI)2Cu , 1987 .

[30]  Gerhard Klebe,et al.  A Radical Anion Salt of 2,5‐Dimethyl‐N,N′‐dicyanoquinonediimine with Extremely High Electrical Conductivity , 1986 .

[31]  Piers Coleman,et al.  New approach to the mixed-valence problem , 1984 .