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In the Ca doped systems, a sharp increase of the relaxation rate
() was observed as the temperature approached from
the paramagnetic side (Fig.41). The
increase of the relaxation rate probably reflects the critical slowing
down of the moments, as has been observed typically in spin glass systems
[7]. In the Ca doped x=4.5% sample, the temperature dependence
of suggests a glass temperature K, which was below the
temperature of our SQUID magnetometer.
Figure 43:
LF-SR spectra in the Ca doped x=9.5% sample at 50 mK. The solid
line on the zero-field (ZF) data is the fit with a dynamical Gaussian
Kubo-Toyabe function. The broken line is the Kubo-Toyabe function in
static case.
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In order to investigate field fluctuations in the charge doped system,
we performed longitudinal field measurements. The results
are shown in Fig. 43. The zero-field (ZF) spectrum
exhibited a Gaussian decay, which seemed to be the Gaussian
Kubo-Toyabe function in the slow fluctuation regime (see section
3.1). However, the LF dependence of the relaxation didn't
follow the predictions of the Gaussian Kubo-Toyabe theory. If the
Gaussian behavior in the zero-field were due to almost static Gaussian
field distribution, the relaxation should have been decoupled in a
LF200 G, while in fact, the relaxation was present up to
LF=2 kG. There are two unconventional behaviors presented in this result:
- (1)
- The weak LF dependence of the relaxation suggests persistent
dynamics in the spin system, even though the temperature (T=50 mK) is well below the
glass temperature ().
- (2)
- There has been no theories which allow the coexistence of the
zero-field Gaussian decay and fast field fluctuations. In the framework of
the conventional Kubo-Toyabe theory, fast fluctuation induces either an
exponential function (dense spin system) or a square-root exponential
function (dilute spin system), but never a Gaussian decay (see Chapter
3).
This result is further investigated in the next section.
Next: 6.2.4 Discussion
Up: 5.2 Haldane material YBaNiO
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