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 $\delta^{\ast} \approx 3.92888$ (lies above the certified upper bound)
$2.1562256466^*$ certificate Cauchy–Schwarz dual bound with weights $\lvert k\rvert^2(1+\mu\lvert k\rvert^2)$; certified lattice sums with tail bounds; interval branch-and-bound over $\delta$

Known lower bounds

Bound Reference Comments
$\frac{\beta + \pi}{\pi} \approx 1.82283$ [BDZ2013]  
$2.156224$ [Pat2026] Rigorous. Truncated conditional extremal of [BDZ2013] on $\mathbb{T}^2=[0,2\pi]^2$: $u(x)=\sum c_k e^{ik\cdot x}$ over $0<\lvert k\rvert^2\le 4000^2$ with $c_k = 1/(\lvert k\rvert^2(\lvert k\rvert^2+\mu))$, $\mu=41/5$. With $S_0=\sum c_k$, $S_1=\sum\lvert k\rvert^2c_k^2$, $S_2=\sum\lvert k\rvert^4c_k^2$: $\delta(u)=S_2/S_1\approx 3.93181$ and, using $\lVert u\rVert_\infty\ge u(0)=S_0$, $L\ge S_0^2/(\pi S_1)-\ln\delta-\ln(1+\ln\delta)=2.1562247\ldots$, evaluated in interval arithmetic. Increasing the cutoff approaches the numerical value $2.15627$.
$2.1562247706^*$ certificate Explicit trial function $u=\sum_{0<\lvert k\rvert\le 4000} e^{ik\cdot x}/(\lvert k\rvert^2(1+\mu\lvert k\rvert^2))$, $\mu=0.1221$; lattice sums enclosed with outward rounding; refines $2.156224$ from #226

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. The bound from [Pat2026] was found with search and proof assistance from Claude (Anthropic); its value is recomputed by the scripts linked in that reference.