Brezis–Gallouet–Wainger remainder constant on the 2D torus

Description of constant

$C_{16} = L$ is the smallest constant for which the sharp Brezis–Gallouet inequality \(\|u\|_{L^\infty(\mathbb T^2)}^2 \le \frac{1}{4\pi}\,\|\nabla u\|_{L^2(\mathbb T^2)}^2 \Bigl[\ln\delta(u) + \ln\bigl(1+\ln\delta(u)\bigr) + L\Bigr]\) holds for all zero-mean functions $u \in H^2(\mathbb T^2)$ with sufficiently large frequency ratio \(\delta(u) := \frac{\|\Delta u\|_{L^2(\mathbb T^2)}^2}{\|\nabla u\|_{L^2(\mathbb T^2)}^2}.\)

Equivalently, $L$ is defined via the constrained extremal problem \(L = \max_{\delta \geq 1} \left[ 4\pi\Theta(\delta) - \ln\delta - \ln(1+\ln\delta) \right]\) where $\Theta(\delta) := \sup\lbrace|u(0)|^2 : \lVert\nabla u\rVert_2^2 = 1,\, \lVert\Delta u\rVert_2^2 = \delta\rbrace$.

Known upper bounds

Bound Reference Comments
$\approx 2.15627$ [BDZ2013] Numerical evaluation; maximum achieved at $\delta^{\ast} \approx 3.92888$

Known lower bounds

Bound Reference Comments
$\frac{\beta + \pi}{\pi} \approx 1.82283$ [BDZ2013]  

Here $\beta = \pi(2\gamma + 2\log 2 + 3\log\pi - 4\log\Gamma(1/4))$, where $\gamma$ is the Euler–Mascheroni constant.

Additional comments

References

For related results in Hölder space settings, see:

Contribution notes

This entry was prepared with LLM assistance (Claude) for literature synthesis and formatting.