We have determined for the first time the "electronic" specific heat coefficient y(x,T) of YBa2Cu306+x for 0.160.9. However, the continuous development of the entropy S(x,T) with x and T across the entire series suggests a progressive modification of the low energy spin spectrum with hole doping rather than a simple band model. Fermi statistics and A>space pairing are indicated by the magnitude and T dependence of S Cx, T).PACS numbers: 65.40.Em, 74.20.Mn, 74.25.Bt Fundamental questions relating to the normal and superconducting states of cuprate superconductors include the statistics of the carriers, the nature of the condensate (/c-space pairing or condensation of real space bosons), the dominant low lying excitations, and the pairing mechanism. The specific heat (C) is a bulk thermodynamic quantity determined uniquely for any material by its spectrum of excitations, and the magnitude and temperature dependence of the electronic specific heat coefficient y = C el /T provides an important test for proposed theories. Unfortunately the electronic term is only (1-2)% of the phonon term over most of the relevant temperature range and investigations of y using conventional techniques are generally limited to the vicinity of the superconducting transition (for recent reviews see Refs.[l] and [2]). Using a high resolution differential technique [3] we determined [4] from 1.8 to 300 K the difference in electronic terms between Yl^CCui-^Zn^Ov-s (0
The findings suggest that severe childhood abuse is associated with abnormally increased activation in classical dorsomedial frontal error-processing regions; furthermore, the increased activation in the supplementary motor area was abuse specific. However, childhood abuse was not associated with inhibitory dysfunction. Increased sensitivity of error-detection networks in participants in the childhood abuse group may be due to the constant need to monitor their own actions in order to avoid painful mistakes, which are often associated with harsh punishment in abusive settings.
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