Fix 0<d<1/20<d<1/2. For τ>0\tau>0, z∈Rz\in\mathbb R, define qq as the unique root with q>∣z∣1/dq>|z|^{1/d} of

q−z2q1−2d=τ.q-z^2q^{1-2d}=\tau.

For r≥0r\ge0, set η=zq−d\eta=zq^{-d}, X=r2/(2q)X=r^2/(2q), and L=1−(1−2d)η2L=1-(1-2d)\eta^2. Then

τ=q(1−η2),∣η∣<1,L≥2d,q≍τ+∣z∣1/d.\tau=q(1-\eta^2),\quad |\eta|<1,\quad L\ge2d, \qquad q\asymp\tau+|z|^{1/d}.

The constants of depend only on dd.

Existence, uniqueness, and smoothness

The left side is zero at q=∣z∣1/dq=|z|^{1/d}, tends to infinity, and has derivative 1−(1−2d)z2q−2d≥2d1-(1-2d)z^2q^{-2d}\ge2d on that branch. For z=0z=0 the solution is q=τq=\tau. The gives smooth dependence wherever q>0q>0.

The lower bound follows from q≥max⁡(τ,∣z∣1/d)q\ge\max(\tau,|z|^{1/d}). If q≤2τq\le2\tau, the upper bound is immediate. Otherwise q/2≤z2q1−2dq/2\le z^2q^{1-2d}, so q≤21/(2d)∣z∣1/dq\le2^{1/(2d)}|z|^{1/d}. At τ=0,z≠0\tau=0,z\ne0, the scale extends smoothly locally with q=∣z∣1/dq=|z|^{1/d} and L=2dL=2d; the corner (τ,z)=(0,0)(\tau,z)=(0,0) is excluded.