07.12.2012 Views

th  - 1988 - 51st ENC Conference

th  - 1988 - 51st ENC Conference

th  - 1988 - 51st ENC Conference

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

• . r<br />

T[-~-UE ~ t~ve 8:00! 63,65Cu NQR STUDIES OF HIGH T OXIDE SUPERCONDUCTORS:<br />

W. W. Warren, Jr.*, R. E. Walstedt, G. F. Brennert, R. F c. Bell, R. J. Cava, G. P. Espinosa,<br />

and J. P. Remeika, AT&T Bell Laboratories, Murray Hill, NJ 07974<br />

Nuclear quadrupole resonance provides a local, site selective probe which has proven highly<br />

informative for studies of oxide superconductors. In <strong>th</strong>is talk I will review our investigations<br />

using <strong>th</strong>e 6~,6SCu resonances in <strong>th</strong>e 90 K superconductor YBa2Cu3OT_8" The crystal structure<br />

of YBa2Cu307 contains two inequivalent Cu sites (Cu-O ".chains" and "planes") whose NQR<br />

lines fall at roughly 22 MI-Iz and 31.5 MHz. Al<strong>th</strong>ough electron band <strong>th</strong>eory calculations imply<br />

similar electronic structure at <strong>th</strong>e two sites, spin-lattice relaxation time measurements reveal<br />

strikingly different behavior in bo<strong>th</strong> <strong>th</strong>e normal and superconducting states. In <strong>th</strong>e normal<br />

states, <strong>th</strong>e 22 MHz sites relax by an enhanced Korringa process <strong>th</strong>at exhibits <strong>th</strong>e usual roughly<br />

linear temperature dependence for <strong>th</strong>e relaxation rate. At 31 MHz, in contrast, <strong>th</strong>e rate<br />

increases only slightly wi<strong>th</strong> increasing temperature. Below To, spin-lattice relaxation reflects<br />

<strong>th</strong>e excitation spectrum of unpaired electrons ("quasiparticles"). Again, <strong>th</strong>e relaxation<br />

behavior is dramatically different for <strong>th</strong>e two sites. An exponential representation of <strong>th</strong>e<br />

relaxation rate yields a value 2A / kT c -- 2.4 for <strong>th</strong>e 22 MI-Iz sites (A is <strong>th</strong>e superconducting<br />

energy gap) while for 31.5 MHz, <strong>th</strong>e corresponding value is 2A / kT c -- 8.3. Reduced oxygen<br />

content (8 = 0.3) leads to relaxation at <strong>th</strong>e 31.5 MHz sites reduced by a factor - 1/1500 but<br />

only a modest 30 ~o effect at 22 MHz. This indicates <strong>th</strong>at <strong>th</strong>e former sites carry almost no<br />

conduction electron density and, by implication, do not participate in <strong>th</strong>e 60 K<br />

superconductivity observed in <strong>th</strong>is phase. The effects of extrinsic paramagnetic moments, <strong>th</strong>e<br />

assignment of <strong>th</strong>e NQR lines to <strong>th</strong>e respective Cu sites, and <strong>th</strong>e implications of <strong>th</strong>ese results of<br />

models of superconductivity will be discussed.<br />

45

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!