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We prove the claim. Put r=3−1/4r=3^{-1/4} and p(z)=z4+4r3zp(z)=z^4+4r^3z. The three critical points are

cj=rexp⁡((2j+1)πi/3),j=0,1,2.c_j=r\exp((2j+1)\pi i/3),\qquad j=0,1,2.

They satisfy cj3=−r3c_j^3=-r^3, so p(cj)=3r3cjp(c_j)=3r^3c_j and ∣p(cj)∣=3r4=1|p(c_j)|=3r^4=1. For 0≤s<10\le s<1,

p(scj)=4s−s43p(cj),0≤4s−s43<1.p(sc_j)=\frac{4s-s^4}{3}p(c_j),\qquad 0\le\frac{4s-s^4}{3}<1.

The segment from zero to each cjc_j, excluding its endpoint, therefore lies in the same component Ω\Omega of {∣p∣<1}\{|p|<1\}. All three cjc_j belong to ∂Ω\partial\Omega.

There are no critical points inside Ω\Omega. The restriction of pp to that component is a proper unramified map to the unit disc, hence a conformal bijection: an unramified connected cover of the simply connected disc has one sheet. Its inverse ϕ\phi extends continuously to the closed disc. Indeed an inverse branch of a polynomial has a convergent Puiseux expansion at each boundary critical value, and is analytic at the remaining boundary values. These expansions also make the boundary curve rectifiable. The radial identities above give ϕ(p(cj))=cj\phi(p(c_j))=c_j. Traversing the unit circle visits the three values p(cj)p(c_j) once each; applying the triangle inequality to the three arcs of the closed curve ϕ(T)\phi(\mathbf T) gives

length⁡(∂Ω)≥∣c0−c1∣+∣c1−c2∣+∣c2−c0∣=33r=35/4.\operatorname{length}(\partial\Omega) \ge |c_0-c_1|+|c_1-c_2|+|c_2-c_0| =3\sqrt3r=3^{5/4}.

For completeness, the boundary parameterization counts each regular boundary arc once. Two distinct arguments cannot have the same boundary image, since p∘ϕp\circ\phi is the identity on the closed disc. Thus its curve length is the boundary length used above.

Write ℓ0=ℓ(z4−1)\ell_0=\ell(z^4-1). Solving for the four inverse roots on the unit circle gives the density ∣1+eiθ∣−3/4|1+e^{i\theta}|^{-3/4}, and therefore

ℓ04=2−3/4∫0π/2(sin⁡u)−3/4 du≤2−3/4∫0π/2(2u/π)−3/4 du=21/4π<35/4.\frac{\ell_0}{4} =2^{-3/4}\int_0^{\pi/2}(\sin u)^{-3/4}\,du \le2^{-3/4}\int_0^{\pi/2}(2u/\pi)^{-3/4}\,du =2^{1/4}\pi<3^{5/4}.

The last strict inequality follows, for example, from π<22/7\pi<22/7. Combining the two estimates proves the claim. The other petals can be shorter; this argument concerns a proposed bound for each petal individually and does not refute a bound on their total length.