The Hardy space $H^1$ consists of the integrable functions $f$ on unit circle whose Fourier coefficients $\widehat f(k)$ vanish for $k<0$. We are concerned with that have some additional (finitely many) holes in spectrum, so we fix a finite set $\mathcal K$ positive integers and consider "punctured" $$H^1_{\mathcal K}:=\{f\in H^1:\,\widehat f(k)=0\,\,\,\text{for all }\, k\in\mathcal K\}.$$ then...