(*) The program committee selected a limited number of abstracts to receive special designation. These Invited Posters are designated with an asterisk (*) preceding the program number.
| 4PO1-1 to 4PO1-9 Abstracts | |
| *4PO1-1 | Quantum Disordered Slave Boson Theory of Underdoped Cuprates |
| *4PO1-2 | Superconductivity and ferromagnetism from effective mass reduction |
| 4PO1-3 | Extension of the Brinkman-Rice picture and metal-Mott-insulator transition |
| 4PO1-4 | Hole Pair Bose Condensation based on the SU(2) Slave-Boson Approach to the t-J Hamiltonian; Instability of the Normal State against Hole Pairing |
| 4PO1-5 | Spin and current correlations and excitations in the t-J model with two holes |
| 4PO1-6 | Momentum and doping dependence of the electron spectrum and (p, 0) feature in copper oxide materials |
| 4PO1-7 | Effect of the additional second neighbor hopping on the spin dynamics in the t-J model |
| 4PO1-8 | The Critical Temperature of Cuprate High Temperature Superconductors |
| 4PO1-9 | Possible theory of CuO-superconductivity: the chirality liquid and fictitious flux confinement |
| 4PO1-10 to 4PO1-19 Abstracts | |
| 4PO1-10 | Phase Diagram of the Quantum SO(5) Symmetry Model for High-Tc Superconductivity |
| 4PO1-11 | Magnetic-field-inducing first-order N to AF transition: a prediction by the SO(5) theory |
| 4PO1-12 | Three holes in the generalized Hubbard model |
| 4PO1-13 | Theory of the resonant neutron scattering in YBa2Cu3O7 |
| 4PO1-14 | Superconducting state in the underdoped high-Tc cuprates as a quantum spin liquid. Comparison with neutron scattering. |
| 4PO1-15 | Coherent potential approximation for d-wave superconductivity in disordered systems |
| 4PO1-16 | Influence of intersite Cu-O repulsion on hole binding and pairing correlations in the three-band Hubbard model |
| 4PO1-17 | Exact Magnetic Ground-State Properties in the One-Dimensional Attractive Hubbard Model |
| 4PO1-18 | Cutoff Dependence of a Configuration Interaction Approach to the Two Dimensional Hubbard Model |
| 4PO1-19 | Incommensurate modulation of spin magnetic susceptibility in single band Hubbard model |
| 4PO1-20 to 4PO1-29 Abstracts | |
| 4PO1-20 | Charge fluctuations in 2D Hubbard model |
| 4PO1-21 | Variational Monte Carlo Study of the Ground State of the Two-Dimensional d-p Model |
| 4PO1-22 | The Phase Diagram, BCS-Bose Condensation Crossover and Inhomogeneous Superconductivity in the Attractive Hubbard Model. |
| 4PO1-23 | Phase fluctuations and pseudogap properties in the presence of nonmagnetic impurities |
| 4PO1-24 | Characteristic Temperatures of Spin Gap Phenomenon in the Under-doped High Temperature Cuprate Superconductors |
| 4PO1-25 | Stripe Phase In the Presence of RVB Spin Liquid Background |
| 4PO1-26 | Stripe Structures and Superconductivity in Cuprates |
| *4PO1-27 | Hole Superconductivity From Kinetic Energy Gain |
| *4PO1-28 | Statistics of Coupled Hole Pairs in Superconducting Ceramics and the Bose-Einstein Condensation |
| 4PO1-29 | Zero-bias anomalies in the current-voltage relations in d-wave Josephson junctions |
| 4PO1-30 to 4PO1-39 Abstracts | |
| 4PO1-30 | Nuclear relaxation rate in (d + s)-wave superconductors |
| 4PO1-31 | Spectral functions of the Luttinger liquid in a magnetic field |
| 4PO1-32 | The seperated spin-charge Luttinger liquid in a magnetic field |
| 4PO1-33 | Inelastic scattering rates in d-wave superconductors |
| 4PO1-34 | Specific heat behavior near the Lifsitz point |
| 4PO1-35 | Orbital Distribution of Holes in Chain Cuprates |
| 4PO1-36 | Role of VHS on Tc of Doped Fullerenes |
| 4PO1-37 | The Hysteresis Effect of I-V Characteristics in YBaCuO Edge Junction |
| 4PO1-38 | Analysis of pressure effect on the superconducting transition temperature in high Tc cuprates |
| 4PO1-39 | Effect of nonzero interface resistance on perpendicular upper critical field in layered superconductors |
| 4PO1-40 to 4PO1-49 Abstracts | |
| 4PO1-40 | Models of paramagnetic centers with different valencies of Cu states in chains of YBa2Cu3O6+y |
| 4PO1-41 | Pressure-induced charge distribution effect on the superconducting critical temperature of HgBa2Ca2Cu3O8+d |
| 4PO1-42 | Fixed Number and Quantum Size Effects in Nanoscale Superconductors |
| *4PO1-43 | Zeeman Coupling between the Magnetic Field and the Internal Motion of d-Wave Cooper Pairs: Microscopic Derivation |
| 4PO1-44 | Effect of Ba-Doping on Zone-Boundary Phonons in La2CuO4 |
| 4PO1-45 | Phenomenological Model of High-Tc Superconductivity: a MCS model |
| *4PO1-46 | Vortex State of a dx2-y2 & dxy-Wave Superconductor with Zeeman Coupling |
| 4PO1-47 | The electronic specific heat in the pairing pseudogap regime |
| 4PO1-48 | Anisotropy and temperature dependence of the scattering rate in overdoped cuprates |
| 4PO1-49 | Transmission of the Infinite Frequencies by Using High-Tc Superconductors |
| 4PO1-50 to 4PO1-59 Abstracts | |
| 4PO1-52 | The variation of the transition temperature of high Tc superconductors by electric field effect |
| 4PO1-53 | Magnetic Field Induced Singlet to Triplet phase Transition in Organic Superconductors |
| 4PO1-54 | Explanation for the Isotope Effect of the High-Tc Cuprates |
| 4PO1-55 | s- and d-wave solutions of the Eliashberg equations with finite bandwidth. |
| 4PO1-56 | Possible non-adiabatic behavior of the electron-phonon system in YBCO and other HTSC compounds. |
| 4PO1-57 | Upper Limit of Transition Temperatures of Strong-Coupled Superconductors |
| 4PO1-58 | Solution of real-axis Eliashberg equations with different pair symmetries and tunneling density of states. |
| 4PO1-59 | Quantum Chaos in the Conductance of a Mesoscopic System |
| 4PO1-60 to 4PO1-69 Abstracts | |
| 4PO1-60 | Electronegativities of some Cuprate and Non-Cuprate Superconductors |
| 4PO1-61 | A Universal Correction Function in the Measurement of Anisotropic Resistivity in High Tc Supercoductors |
| 4PO1-62 | A new theoretical approach of the gravitational shielding: Podkletnov's effect |
| 4PO1-63 | Self-consistent description of simplified pseudospin-electron model |
| 4PO1-64 | All High-temperature Cuprate Superconductors are p-type |
| 4PO1-65 | The Possibility of bi-'exciton' pairing in singlet and in triplet states in cuprate superconductors |
| 4PO1-66 | The Enhancement of the Special Theory of Relativity by Using the Superconductivity |
| 4PO1-67 | On the Universal Quantum Corrections of the Conductance of Metal-Superconductor Wires and Andreev Interferometers |
| 4PO1-68 | U(1) gauge symmetry breaking by a Berry phase in a crystal with a doubly degenerate electronic band |
| 4PO1-69 | Coherent Pairing State and High Tc Superconductivity |
| 4PO1-70 to 4PO1-79 Abstracts | |
| 4PO1-70 | New phase induced by a magnetic field in Bi2212 superconductors |
| 4PO1-71 | Anomalous Signatures of Superconductivity Near Room-Temperature: A New Explanation? |
| *4PO1-72 | U(1)xSU(2) Gauge Field Theory of Transport and Magnetic Relaxation in Underdoped High Tc Cuprates |
| 4PO1-73 | Boson FQHE state in cuprate oxide induced by large //c zero-point oscillation |
| 4PO1-74 | Is the Quantum Melting of a Polaron Wigner Crystal an Insulator-to-Superconductor Transition? |
| 4PO1-75 | Quasi-One-Dimensional Band in the t-J Model |
| 4PO1-76 | "Is electron fracton interaction for superconductivity possible for quasicrystals?" |
| 4PO1-77 | A Theory for Doping in High -Temperature Superconductors |
| 4PO1-78 | Onset of Stripe Dynamics in Cuprates and Nickelates |
| 4PO1-79 | Impact Evidence for the Compressive Deformation Origin of Low- and High-Tc Superconductivity |
| 4PO1-80 to 4PO1-85 Abstracts | |
| 4PO1-80 | Universality of Dislocation Mechanisms in Electrical, Magnetic, Dielectric and Mechanical Properties of Solids |
| 4PO1-81 | Simple Lattice Model for Twinning Plane Superconductivity in YBa2Cu3O7-d |
| 4PO1-82 | Study of magnetic properties within an imperfect nested Fermi surface |
| 4PO1-83 | Superconductivity as a Bose-Einstein Condensation? |
| 4PO1-84 | Impurity spin dynamics in two-dimensional antiferromagnets and superconductors |
| 4PO1-85 | Collective excitations in unconventional superfluids and superconductors |