Magnetic order and electronic phase diagrams of electron-doped copper oxide materials

G. M. Luke(Columbia University), L. P. Le(Columbia University), B. J. Sternlieb(Columbia University), Y. J. Uemura(Columbia University), J. H. Brewer(University of British Columbia), R. Kadono(Columbia University), R. F. Kiefl(University of British Columbia), S. R. Kreitzman(University of British Columbia), T. M. Riseman(Columbia University), C. E. Stronach(Virginia State University), Mike Davis(Virginia State University), S. Uchida(The University of Tokyo), H. Takagi(Columbia University), Y. Tokura(Columbia University), Y. Hidaka(NTT (Japan)), T. Murakami(NTT (Japan)), J. Gopalakrishnan(DuPont (United States)), A.W. Sleight(Experimental Station), M.A. Subramanian(DuPont (United States)), Edward A. Early(University of California San Diego), J. T. Markert(Applied Physical Sciences (United States)), M. B. Maple(Columbia University), C.L. Seaman(Columbia University)
Physical review. B, Condensed matter
November 1, 1990
Cited by 188

Abstract

We report muon spin relaxation and rotation measurements on sintered ceramic samples of ${\mathrm{Nd}}_{2\mathrm{\ensuremath{-}}\mathit{x}}$${\mathrm{Ce}}_{\mathit{x}}$${\mathrm{CuO}}_{4\mathrm{\ensuremath{-}}\mathit{y}}$ and a large single crystal of ${\mathrm{Nd}}_{2}$${\mathrm{CuO}}_{4\mathrm{\ensuremath{-}}\mathit{y}}$. We find an electronic phase diagram that is quite similar to that of hole-doped superconductors such as ${\mathrm{La}}_{2\mathrm{\ensuremath{-}}\mathit{x}}$${\mathrm{Sr}}_{\mathit{x}}$${\mathrm{CuO}}_{4\mathrm{\ensuremath{-}}\mathit{y}}$, although the doping of electrons into the system is less efficient in destroying the static moments on the copper ions. Static magnetic order appears in ${\mathrm{Nd}}_{2}$${\mathrm{CuO}}_{4\mathrm{\ensuremath{-}}\mathit{y}}$ below about 250 K; two spin reorientations are seen at T=75 and 35 K, providing information about the muon site in this material.


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