Defining under and over-doping as bond order phenomena in the pair plaid model

[1]  H. Takagi,et al.  Nodal Quasiparticles and Antinodal Charge Ordering in Ca2-xNaxCuO2Cl2 , 2005, Science.

[2]  K. Kudo,et al.  Magnetic-field effects on the in-plane electrical resistivity in single-crystal La2?xBaxCuO4 and La1.6?xNd0.4SrxCuO4 around x=1/8: Implication for the field-induced stripe order , 2004, cond-mat/0405088.

[3]  H. Takagi,et al.  A ‘checkerboard’ electronic crystal state in lightly hole-doped Ca2-xNaxCuO2Cl2 , 2004, Nature.

[4]  H. Oesterreicher Origin of Superconductivity and Construction of Doping Curves for Cuprates on an Elasticity-Exchange Competition Model , 2004 .

[5]  H. Oesterreicher Knight Shift Data and Superconducting Tc Modeling Based on an Effective Hole Model , 2003 .

[6]  M. Vojta Superconducting charge-ordered states in cuprates , 2002, cond-mat/0204284.

[7]  A. Bishop,et al.  Spin and charge order around vortices and impurities in high-T(c) superconductors. , 2002, Physical review letters.

[8]  E. Demler,et al.  Competing orders in a magnetic field: Spin and charge order in the cuprate superconductors , 2001, cond-mat/0112343.

[9]  Y. Tokunaga,et al.  Unusual magnetic and superconducting characteristics in multilayered high-Tc cuprates: 63Cu NMR study , 2001 .

[10]  H. Oesterreicher Unifying Chemical and Physical Principles for Oxide Superconductivity Based on an Anionic Charge Order Model , 2001 .

[11]  V. Anderson Sources of quantum protection in high-T(c) superconductivity , 2000, Science.

[12]  J. Zaanen,et al.  Self-Organized One Dimensionality , 1999, Science.

[13]  Z. Shen,et al.  Is This Why Tc Is So Low? , 1999, Science.

[14]  R. Snyder,et al.  Structures of High‐Temperature Cuprate Superconductors , 1995 .

[15]  S. Uchida,et al.  Evidence for stripe correlations of spins and holes in copper oxide superconductors , 1995, Nature.

[16]  J. Tarascon,et al.  Superconductivity at 40 K in the Oxygen-Defect Perovskites La2-xSrxCuO4-y , 1987, Science.