| Foreword | p. 1 |
| Special Features of the Superconducting State | p. 2 |
| Magnetization M(H) | p. 2 |
| Specific Heat | p. 3 |
| The Energy Gap | p. 4 |
| The London Penetration Depth, The Coherence Length | p. 5 |
| Superconductivity and Magnetism | p. 5 |
| Heavy-Electron Superconductors | p. 7 |
| Organic Superconductors | p. 14 |
| High-T[subscript c] Superconductors | p. 18 |
| Prelude to High-T[subscript c] superconductors: Superconducting ternary oxides | p. 18 |
| SrTiO[subscript 3] | p. 18 |
| LiTi[subscipt 2]O[subscript 4] | p. 19 |
| [actual symbol not reproducible] | p. 19 |
| High-T[subscript c] superconductors: The great step forward | p. 21 |
| [actual symbol not reproducible] | p. 21 |
| [actual symbol not reproducible] | p. 26 |
| Bi-based Cu-oxides | p. 31 |
| Tl-based compounds | p. 32 |
| General basic issues | p. 32 |
| Concluding Remarks | p. 33 |
| Reprinted Articles | p. 35 |
| Other References | p. 38 |
| Reprinted Articles | p. 49 |
| Superconductivity in a synthetic organic conductor (TMTSF)[subscript 2]PF[subscript 6] | p. 201 |
| Zero-Pressure Organic Superconductor: Di-(Tetramethyltetraselenafulvalenium)-Perchlorate [(TMTSF)[subscript 2]ClO[subscript 4]] | p. 205 |
| Superconductivity in a New Family of Organic Conductors | p. 209 |
| Normal-pressure superconductivity in an organic metal (BEDT-TTF)[subscript 2]I[subscript 3] [bis(ethylene dithiolo) tetrathiofulvalene triiodide] | p. 213 |
| A New Ambient Pressure Organic Superconductor (BEDT-TTF)[subscript 2]Cu(NCS)[subscript 2] with T[subscript c] above 10 | p. 218 |
| One-dimensional correlations in organic superconductors: magnetism and superconductivity | p. 223 |
| Organic Conductors and Superconductors in High Magnetic Fields | p. 254 |
| High-Temperature superconductivity in the [actual symbol not reproducible] system | p. 257 |
| Superconductivity in the [actual symbol not reproducible] System | p. 259 |
| Possible High T[subscript c] Superconductivity in the Ba-La-Cu-O System | p. 267 |
| High-T[subscript c] Superconductivity of La-Ba-Cu Oxides. II. -Specification of the Superconducting Phase | p. 272 |
| Superconductivity Produced by Electron Doping in CuO[subscript 2]-Layered Compounds | p. 274 |
| The Resonating Valence Bond State in La[subscript 2]CuO[subscript 4] and Superconductivity | p. 278 |
| Superconductivity at 93 K in a New Mixed-Phase Y-Ba-Cu-O Compound System at Ambient Pressure | p. 281 |
| Flux Trapping and Superconductive Glass State in [actual symbol not reproducible] | p. 284 |
| Thermally Activated Dissipation in [actual symbol not reproducible] | p. 288 |
| SQUID Picovoltometry of [actual symbol not reproducible] Single Crystals: Evidence for a Finite-Temperature Phase Transition in the High-Field Vortex State | p. 292 |
| High-Resolution Photoemission Study of the Low-Energy Excitations Reflecting the Superconducting State of Bi-Sr-Ca-Cu-O Single Crystal | p. 296 |
| Superconductivity in the Bi-Sr-Cu-O System | p. 300 |
| A New High-T[subscript c] Oxide Superconductor without a Rare Earth Element | p. 303 |
| Superconductivity in the rare-earth-free Tl-Ba-Cu-O system above liquid nitrogen temperature | p. 305 |
| Bulk Superconductivity at 125 K in [actual symbol not reproducible] | p. 309 |
| Superconducting Ground State of Noninteracting Particles Obeying Fractional Statistics | p. 313 |
| Author Index | p. 317 |
| Subject Index | p. 319 |
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