In [1], authors note that by the seminal approach of M. Weinstein in [2] and [3], there is a non-trivial solution $Q\in H^s(\mathbb{R})$ which optimizes next Gagliardo-Nirenberg type inequality: $$\int_\mathbb{R}|u|^{\alpha+2}\,dx\leq C_{\alpha,s}\left(\int_\mathbb{R}|(-\Delta)^{s/2}u|^2\,dx\right)^{\alpha/4s}\left(\int_\mathbb{R}|u|^2\,dx\right)^{\alpha(2s-1)/4s+1},$$ for some admissible $\alpha$. I think the relativistic generalization of this inequality should hold as next form: $$\int_\mathbb{R}|u|^{\alpha+2}\,dx\leq C_{\alpha,s,m}\left(\int_\mathbb{R}|(-\Delta+m^2)^{s/2}u|^2\,dx\right)^{\alpha/4s}\left(\int_\mathbb{R}|u|^2\,dx\right)^{\alpha(2s-1)/4s+1},$$ with an optimizer in $H^s(\mathbb{R})$. But I am afraid that I cannot find a suitable reference. So I wonder if the existence of this optimizer proven already, or reasonable enough to deduce easily somehow, otherwise I can try the same approach of M. Weinstein.
Thank you in advance.
References
[1] Frank, Rupert L., and Enno Lenzmann. "Uniqueness of non-linear ground states for fractional Laplacians in R." Acta mathematica 210.2 (2013): 261-318.
[2] Weinstein, Michael I. "Modulational stability of ground states of nonlinear Schrödinger equations." SIAM journal on mathematical analysis 16.3 (1985): 472-491.
[3] Weinstein, Michael I. "Existence and dynamic stability of solitary wave solutions of equations arising in long wave propagation." Communication in partial Differential Equation 12.10 (1987): 1133-1173.