Organic Superconductors—New Benchmarks

Recent advances in the design and synthesis of organic synthetic metals have yielded materials that have the highest superconducting transition temperatures (Tc ≈ 13 kelvin) reported for these systems. These materials have crystal structures consisting of alternating layers of organic donor molecules and inorganic anions. Organic superconductors have various electronic and magnetic properties and crystal structures that are similar to those of the inorganic copper oxide superconductors (which have high Tc values); these similarities include highly anisotropic conductivities, critical fields, and short coherence lengths. The largest number of organic superconductors, including those with the highest Tc values, are charge-transfer salts derived from the electron donor molecule BEDT-TTF or ET [bis(ethylenedithio)-tetrathiafulvalene]. The synthesis and crystal structures of these salts are discussed; their electrical, magnetic, and band electronic structure properties and their many similarities to the copper oxide superconductors are treated as well.

[1]  Alan J. Heeger,et al.  Superconducting fluctuations and the Peierls instability in an organic solid , 1993 .

[2]  D. Murphy,et al.  Superconductivity at 18 K in potassium-doped C60 , 1991, Nature.

[3]  D. L. Overmyer,et al.  Strain index, lattice softness and superconductivity of organic donor-molecule salts: Crystal and electronic structures of three isostructural salts k-(BEDT- TTF)2Cu[N(CN)2]X (X=Cl, Br, I) , 1991 .

[4]  Wang,et al.  Specific heat in zero and applied magnetic fields of the organic superconductor alpha -di , 1990, Physical review. B, Condensed matter.

[5]  Wang,et al.  Unusual behavior in the upper critical magnetic fields of the ambient-pressure organic superconductor kappa -(BEDT-TTF)2Cu , 1990, Physical review. B, Condensed matter.

[6]  Takehiko Mori,et al.  A new ambient-pressure organic superonductor, κ-(BEDT-TTF)2Ag(CN)2H2O (TC=5.0 K) , 1990 .

[7]  Takahashi,et al.  Superconductivity in beta -di , 1990, Physical review. B, Condensed matter.

[8]  J. M. Williams,et al.  From semiconductor-semiconductor transition (42 K) to the highest-Tc organic superconductor, κ-(ET)2Cu[N(CN)2]Cl (Tc = 12.5 K) , 1990 .

[9]  W. Kwok,et al.  Synthesis of the new highest Tc ambient-pressure organic superconductor, .kappa.-(BEDT-TTF)2Cu[N(CN)2]Br, by five different routes , 1990 .

[10]  Kurt Vandervoort,et al.  A new ambient-pressure organic superconductor, κ-(ET)2Cu[N(CN)2]Br, with the highest transition temperature yet observed (inductive onset Tc=11.6 K, resistive onset = 12.5 K) , 1990 .

[11]  R. Thorn,et al.  Temperature dependence of conductivity of κ(BEDTTTF)2Cu(SCN)2; Resolution into two components; Small polaron , 1990 .

[12]  J. Howard,et al.  Crystal structure and physical properties of a metallic charge‐transfer salt: (BEDT‐TTF)2Ag(CN)2.H2O , 1990 .

[13]  W. Kwok,et al.  The first ambient pressure organic superconductor containing oxygen in the donor molecule, βm-(BEDO-TTF)3Cu2(NCS)3, Tc = 1.06 K , 1990 .

[14]  K. Kikuchi,et al.  Structural and Electronic Properties of K-Phase Organic Donor Salts: κ-(DMET)2AuBr2 and κ-(BEDT-TTF)4Hg3Cl8 , 1990 .

[15]  H. Kusuhara,et al.  Tensile stress effect on transport properties of (BEDTTTF)2Cu(NCS)2 , 1990 .

[16]  M. Beno,et al.  Ubiquitous Superconductivity Near 4K in Salts of the BEDT-TTF/I System: Is There a Common Source? , 1990 .

[17]  W. Kwok,et al.  A new ambient-pressure organic superconductor: (BEDT-TTF)2(NH4)Hg(SCN)4 , 1990 .

[18]  C. Lenoir,et al.  Some properties of the organic superconductor kappa -(BEDT TTF)2Cu(SCN)2 under pressure , 1990 .

[19]  M. Whangbo,et al.  Molecular identities in first-principles self-consistent-field band electronic structures of the organic superconducting salts. Beta. -(BEDT-TTF) sub 2 X (X sup minus = I sub 3 sup minus , AuI sub 2 sup minus , IBr sub 2 sup minus ) , 1990 .

[20]  S. Kagoshima,et al.  The Physics and Chemistry of Organic Superconductors , 1990 .

[21]  P. Nigrey,et al.  Similarities and differences in the structural and electronic properties of. kappa. -phase organic conducting and superconducting salts , 1989 .

[22]  Wang,et al.  Specific heat in high magnetic field of kappa -di , 1989, Physical review. B, Condensed matter.

[23]  D. L. Overmyer,et al.  Anomalous pressure dependence of the superconducting transition temperature of (ET)4Hg2.89Br8 , 1989 .

[24]  W. Kwok,et al.  Crystal growth and phase selectivity of organic superconductors [.beta.-(ET)2I3 (Tc = 1.5 K) and .kappa.-(ET)2Cu(NCS)2 (Tc = 10.4 K)] on graphite electrodes , 1989 .

[25]  R. Friend,et al.  Pressure dependence of the transport properties of the molecular superconductor, κ-(BEDT TTF)2Cu(NCS)2 , 1989 .

[26]  L. Brossard,et al.  Pressure induced superconductivity in molecular TTF(Pd(dmit) 2)2 , 1989 .

[27]  Liu,et al.  Magnetic measurements of the upper critical field of YBa2Cu3O7- delta single crystals. , 1989, Physical review letters.

[28]  D. L. Overmyer,et al.  (MDT-TTF)2 AuI2: An ambient pressure organic superconductor (Tc = 4.5 K) based on an unsymmetrical electron donor , 1989 .

[29]  K. Hass Electronic Structure of Copper-Oxide Superconductors , 1989 .

[30]  G. Papavassiliou,et al.  Low temperature measurements of the electrical conductivities of some charge transfer salts with the asymmetric donors MDT-TTF, EDT-TTF and EDT-DSDTF. (MDT-TTF)2AuI2, a new superconductor (Tc=3.5 K at ambient pressure) , 1988 .

[31]  M. Beno,et al.  Characterization of the electrocrystallization products of the mixed-donor system ET:MET (1:1) / I3 / TCE: How to get crystals with the ordered ß∗-(ET) 2I3 structure and a Tc of 4.6 K without applied pressure , 1988 .

[32]  W. Kwok,et al.  How well do we understand the synthesis of (ET) 2I3 by electrocrystallization? ESR and X-ray identification of (ET) 2I3 crystals which are mixtures of phases and observation of high-Tc states of (ET) 2I3, ranging from 2.5–6.9 K , 1988 .

[33]  K. Yamaji Mechanism of superconductivity in TTF-analog complexes , 1988 .

[34]  L. Bulaevskii Organic layered superconductors , 1988 .

[35]  E. Fanghänel,et al.  Synthesis, Reactions, and Selected Physico-Chemical Properties of 1,3- and 1,2-tetrachalcogenafulvalenes , 1988 .

[36]  T. Emge,et al.  Rational design of synthetic metal superconductors , 1988 .

[37]  Kazuya Saito,et al.  Polymorphism and electrical conductivity of the organic superconductor (DMET)2AuBr2 , 1988 .

[38]  E. Conwell Highly conducting quasi-one-dimensional organic crystals , 1988 .

[39]  Kazuya Saito,et al.  Superconductivity in (DMET)2AuCl2 and (DMET)2AuI2 , 1987 .

[40]  D. Schweitzer,et al.  A stable superconducting state at 8 K and ambient pressure in $$\alpha _t - (BEDT - TTF^ \star )_2 I_3 ^1 $$ , 1987 .

[41]  Kazuya Saito,et al.  On Ambient-Pressure Superconductivity in Organic Conductors: Electrical Properties of (DMET)2I3, (DMET)2I2Br and (DMET)2IBr2 , 1987 .

[42]  Takehiko Mori,et al.  Superconductivity in (BEDT-TTF)3Cl22H2O , 1987 .

[43]  Kazuya Saito,et al.  Superconductivity and the possibility of semiconductor-metal transition in (DMET)2AuBr2 , 1987 .

[44]  J. Ferraro,et al.  Introduction to Synthetic Electrical Conductors , 1987 .

[45]  Ruvalds Plasmons and high-temperature superconductivity in alloys of copper oxides. , 1987, Physical review. B, Condensed matter.

[46]  T. Emge,et al.  Importance of Intermolecular Hydrogen—Hydrogen And Hydrogen-anion Contacts For The Lattice Softness, The Electron-phonon Coupling, And The Superconducting Transition Temperatures, T c , of Organic Conducting Salts β-(et) 2 x (x- = Ibr 2 -, aui2”, I 3 ) , 1987 .

[47]  T. Emge,et al.  Effect of anion ordering on the H―anion interactions and band electronic structure of (TMTSF)2BF4 at 20 K , 1986 .

[48]  T. Emge,et al.  A neutron diffraction study of the extent of disorder in the low temperature (20 K) structure of β-(BEDT-TTF)2I2Br , 1986 .

[49]  H. H. Wang,et al.  Effect of structural disorder on organic superconductors: a neutron diffraction body of "high-Tc" .beta.*-(bis(ethylenedithio)tetrathiafulvalene)2 triiodide at 4.5 K and 1.5 kbar. , 1986, Journal of the American Chemical Society.

[50]  Wang,et al.  Measurement of the energy gap in an organic superconductor: Evidence for extremely strong coupling. , 1986, Physical review letters.

[51]  J. F. Kwak,et al.  Simple recipe for formation or recovery at ambient pressure of the 8K superconducting state of β-(BEDT-TTF)2I3 , 1986 .

[52]  Dwaine O. Cowan,et al.  The Organic Solid State. , 1986 .

[53]  Wang,et al.  Neutron-diffraction evidence for ordering in the high-Tc phase of beta -di , 1986, Physical review. B, Condensed matter.

[54]  Wang,et al.  Shear-induced superconductivity in beta -di , 1986, Physical review. B, Condensed matter.

[55]  M. Firestone,et al.  Crystal and band electronic structures of an organic salt with the first three-dimensional radical-cation donor network, (BEDT-TTF)Ag4(CN)5 , 1985 .

[56]  T. Emge,et al.  Organic superconductors: structural aspects and design of new materials , 1985 .

[57]  M. Firestone,et al.  Ambient-pressure superconductivity at the highest temperature (5 K) observed in an organic system: β-(BEDT-TTF)2AuI2 , 1985 .

[58]  T. Emge,et al.  A test of superconductivity vs. molecular disorder in (BEDT-TTF)2X synthetic metals: synthesis, structure (298, 120 K), and microwave/ESR conductivity of (BEDT-TTF)2I2Br , 1985 .

[59]  M. Tokumoto,et al.  Superconductivity with the Onset at 8 K in the Organic Conductor β-(BEDT–TTF) 2 I 3 under Pressure , 1985 .

[60]  G. Crabtree,et al.  Inductive And Resistive Studies Of The Ambient Pressure Organic Superconductor β-(BEDT-TTF)2I3 , 1985 .

[61]  V. P. Kaminskii,et al.  Crystal Structures of Organic Metals and Superconductors of (BEDT-TTP)-I System , 1985 .

[62]  G. Crabtree,et al.  Band electronic structures of the ambient pressure organic superconductors β-(ET)2X (X=I3−, IBr2−) , 1985 .

[63]  Beno,et al.  Novel structural modulation in the ambient-pressure sulfur-based organic superconductor β-(BEDT-TTF)2I3: Origin and effects on its electrical conductivity , 1985 .

[64]  V. Petříček,et al.  Novel structural modulation in the first ambient-pressure sulfur-based organic superconductor (BEDT-TTF)2I3 , 1985 .

[65]  T. Emge,et al.  Neutron and x-ray diffraction evidence for a structural phase transition in the sulfur-based ambient-pressure organic superconductor bis(ethylenedithio) tetrathiafulvalene triiodide , 1984 .

[66]  F. Behroozi,et al.  Ambient-pressure superconductivity at 2.7 K and higher temperatures in derivatives of (BEDT-TTF)2IBr2: synthesis, structure, and detection of superconductivity , 1984 .

[67]  G. Ball,et al.  Neutron-diffraction evidence for structural phase transitions in the organic conductors bis-tetramethyltetraselenafulvalenium salts [(TMTSF) 2 X, X=ClO - 4 and BF - 4 ] , 1984 .

[68]  F. Wudl From organic metals to superconductors: managing conduction electrons in organic solids , 1984 .

[69]  E. Sackmann,et al.  On defects in different phases of two-dimensional lipid bilayers , 1983 .

[70]  J. Fabre,et al.  X-ray evidence of a structural phase transition in di-tetramethyltetraselenafulvalenium perchlorate [(TMTSF)2ClO4], pristine and slightly doped , 1983 .

[71]  S. Wolf,et al.  Metal-insulator transitions and superconductivity in ditetramethyltetraselenafulvalenium fluorosulfonate [(TMTSF)2FSO3] , 1983 .

[72]  S. Parkin,et al.  Superconductivity in a new family of organic conductors , 1983 .

[73]  K. Bechgaard,et al.  Observation of a magnetic state in the organic superconductor (TMTSF) 2ClO4 : influence of the cooling rate , 1982 .

[74]  C. S. Jacobsen,et al.  Zero-Pressure Organic Superconductor: Di-(Tetramethyltetraselenafulvalenium)-Perchlorate [ ( TMTSF ) 2 Cl O 4 ] , 1981 .

[75]  J. Carbotte,et al.  Effect of changes in. cap alpha. ²(. cap omega. )F(. cap omega. ) on the zero-temperature energy gap of a superconductor , 1980 .

[76]  R. Hoffmann,et al.  The band structure of the tetracyanoplatinate chain , 1978 .

[77]  John P. Ferraris,et al.  Electron transfer in a new highly conducting donor-acceptor complex , 1973 .

[78]  W. L. Mcmillan TRANSITION TEMPERATURE OF STRONG-COUPLED SUPERCONDUCTORS. , 1968 .

[79]  A R Plummer,et al.  Introduction to Solid State Physics , 1967 .

[80]  J. Hubbard,et al.  Electron correlations in narrow energy bands III. An improved solution , 1964, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[81]  W. Mahler,et al.  7,7,8,8-TETRACYANOQUINODIMETHANE AND ITS ELECTRICALLY CONDUCTING ANION-RADICAL DERIVATIVES , 1960 .

[82]  L. Cooper,et al.  Theory of superconductivity , 1957 .

[83]  H. Fröhlich On the theory of superconductivity: the one-dimensional case , 1954, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[84]  N F Mott,et al.  The Basis of the Electron Theory of Metals, with Special Reference to the Transition Metals , 1949 .

[85]  W. C. Moore,et al.  ORGANIC AMALGAMS: SUBSTANCES WITH METALLIC PROPERTIES COMPOSED IN PART OF NON-METALLIC ELEMENTS.2 , 1911 .