TY - JOUR
T1 - Magnetic phase separation in [formula presented] by [formula presented] nuclear magnetic resonance
AU - Kuhns, P. L.
AU - Hoch, M. J.R.
AU - Moulton, W. G.
AU - Reyes, A. P.
AU - Wu, J.
AU - Leighton, C.
PY - 2003/1/1
Y1 - 2003/1/1
N2 - [Formula presented] NMR measurements on [Formula presented] reported here establish unequivocally, for the first time, the coexistence of ferromagnetic regions, spin-glass regions, and hole-poor low spin regions at all [Formula presented] values from 0.1 to 0.5. A zero external field NMR spectrum, which is assigned to the ferromagnetic regions, has a spectral shape that is nearly [Formula presented] independent at 1.9 K, as are the relaxation times, [Formula presented] and [Formula presented]. The integrated spectral area increases rapidly with [Formula presented] up to [Formula presented] and then decreases slightly for larger [Formula presented]. In a field of 9.97 T, a narrow NMR line is observed at 102 MHz, identical to that found in [Formula presented] samples in previous work. The integrated intensity of this spectrum decreases rapidly with increasing [Formula presented], and is ascribed to hole-poor low spin regions. Beneath this spectrum, a third broad line, with a peak at 100 MHz, is assigned to a spin- or cluster-glass-like phase.
AB - [Formula presented] NMR measurements on [Formula presented] reported here establish unequivocally, for the first time, the coexistence of ferromagnetic regions, spin-glass regions, and hole-poor low spin regions at all [Formula presented] values from 0.1 to 0.5. A zero external field NMR spectrum, which is assigned to the ferromagnetic regions, has a spectral shape that is nearly [Formula presented] independent at 1.9 K, as are the relaxation times, [Formula presented] and [Formula presented]. The integrated spectral area increases rapidly with [Formula presented] up to [Formula presented] and then decreases slightly for larger [Formula presented]. In a field of 9.97 T, a narrow NMR line is observed at 102 MHz, identical to that found in [Formula presented] samples in previous work. The integrated intensity of this spectrum decreases rapidly with increasing [Formula presented], and is ascribed to hole-poor low spin regions. Beneath this spectrum, a third broad line, with a peak at 100 MHz, is assigned to a spin- or cluster-glass-like phase.
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U2 - 10.1103/PhysRevLett.91.127202
DO - 10.1103/PhysRevLett.91.127202
M3 - Article
AN - SCOPUS:84861152919
SN - 0031-9007
VL - 91
JO - Physical Review Letters
JF - Physical Review Letters
IS - 12
ER -