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$θ$ dependence of $T_c$ in 4d SU(3) Yang-Mills theory with histogram method and the Lee-Yang zeros in the large $N$ limit

The phase diagram on the $θ$-$T$ plane in four dimensional SU(3) Yang-Mills theory is explored. We revisit the $θ$ dependence of the deconfinement transition temperature, $T_c(θ)$, on the lattice through the constraint effective potential for Polyakov loop. The $θ$ term is introduced by the reweighting method, and the critical $β$ is determined to $θ\sim 0.75$, where the interpolation in $β$ is carried out by the multipoint reweighting method. The $θ$ dependence of $T_c$ obtained here turns out to be consistent with the previous result by D'Elia and Negro \cite{DElia:2012pvq,DElia:2013uaf}. We also derive $T_c(θ)$ by classifying configurations into the high and low temperature phases and applying the Clausius-Clapeyron equation. It is found that the potential barrier in the double well potential at $T_c(θ)$ becomes higher with $θ$, which suggests that the first order transition continues robustly above $θ\sim 0.75$. Using information obtained here, we try to depict the expected $θ$ dependence of the free energy density at $T < T_c(0)$, which crosses the first order transition line at an intermediate value of $θ$. Finally, how the Lee-Yang zeros associated with the spontaneous CP violation appear is discussed formally in the large $N$ limit, and the locations of them are found to be $(θ_R,θ_I)=\left( (2m+1)π, \frac{2n+1}{2χV_4} \right)$ with $n$ and $m$ arbitrary integers.