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The strong power law behavior of the specific heat jump $\Delta C$ vs.
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In the strong pair-breaking limit ( Γ π > T c \Gamma_{\pi}>T_{c} ) where Δ F ∝ − N ( 0 ) Δ 4 Γ π 2 \Delta F\propto-N(0)\frac{\Delta^{4}}{\Gamma_{\pi}^{2}} is valid, the behavior of Δ ( T ) \Delta(T) should also change to Δ 2 ( T ) ∝ Γ π 2 ( 1 − T T c ) \Delta^{2}(T)\propto\Gamma_{\pi}^{2}(1-\frac{T}{T_{c}}) instead of the BCS behavior Δ 2 ( T ) ∝ T c 2 ( 1 − T T c ) \Delta^{2}(T)\propto T_{c}^{2}(1-\frac{T}{T_{c}}) . Then the SH jump in this limit becomes Δ C / T c ∼ N ( 0 ) Γ π 2 T c 2 \Delta C/T_{c}\sim N(0)\frac{\Gamma_{\pi}^{2}}{T_{c}^{2}} , quite opposite to the BNC scaling
Cited in the paper.
For the undoped parent compound BaFe 2 As 2 , our model assumes N ¯ h = N ¯ e = 0.5 \bar{N}_{h}=\bar{N}_{e}=0.5 . For electron doping in Ba(Fe 1-x
Cited in the paper.