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The best fit to the measured curves gives an effective temperature of 0.8S K. This is slightly higher than the actual temperature of the STM (0.6 K), which was measured by fitting dI/dV curves of a superconducting sample. This higher effective temperature is due mainly to residual high-frequency (RF) voltage noise.
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The standard deviation uncertainties quoted here are derived from the uncertainty in the fits at each field (error bars in Fig. 28). These uncertainties come from instrumental noise, and from background spectral features due to the tip and surface that happen to lie near the Zeeman energy. For simplicity we have chosen not to subtract these background spectral features before fitting the data.
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We gratefully acknowledge help with the construction of the 5TM from B. Melior and helpful discussions with J. Kroha, B. A. Jones, A. H. Castro-Neto, A. V. Balatsky, and D. Loss. This work was supported in part by the Defense Advanced Research Projects Agency.
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