Exercises on analytic preparation

These two exercises and complete solutions use the proved analytic preparation and Puiseux treatment. The inverse-power example comes from Guillaume Valette’s On subanalytic geometry; its finite-refinement obstruction and the parameter/parity exercise are expanded here. The Valette component and these identified teaching additions are available under CC BY 4.0. Adapted by GPT-6.1 Sol (OpenAI), Ultra, October 2026; no endorsement is implied.

15. A bounded function that needs a negative preparation exponent

Level: advanced. On

C={(x,y):0<x<ϵ,x2<y<x},0<ϵ<1, C=\{(x,y):0<x<\epsilon,\ x^2<y<x\},\qquad 0<\epsilon<1,

consider f(x,y)=x3/yf(x,y)=x^3/y. It is positive and bounded. Show that a finite preparation of ff cannot have only nonnegative last-coordinate exponents, even if translations and analytic units are allowed. Use the convergent Puiseux theorem proved in the analytic preparation treatment.

Solution. We have 0<f<x<ϵ0<f<x<\epsilon. The formula f=x3y−1f=x^3y^{-1} is already a reduction with translation zero, unit one and exponent −1-1.

Suppose there is a finite cell preparation with all exponents nonnegative. Refine its one-dimensional base and shrink ϵ\epsilon so its base interval next to zero is (0,ϵ)(0,\epsilon). Over it, list the finitely many endpoints within the original band, including x2x^2 and xx:

x2=α0(x)<α1(x)<⋯<αN(x)=x. x^2=\alpha_0(x)<\alpha_1(x)<\cdots<\alpha_N(x)=x.

Duplicate endpoints are removed; every open interval between consecutive endpoints is a preparation cell. Each positive endpoint has a convergent Puiseux expansion with leading term cjxνjc_jx^{\nu_j}, where cj>0c_j>0. The bounds x2≤αj≤xx^2\le\alpha_j\le x force 1≤νj≤21\le\nu_j\le2. Since ν0=2\nu_0=2 and νN=1\nu_N=1, some consecutive pair α<β\alpha<\beta has strictly decreasing leading order. Thus α/β→0\alpha/\beta\to0.

On the corresponding band, write the supposed reduction as

f(x,y)=a(x)|y−θ(x)|rU(x,y),r≥0,0<m≤|U|≤M. f(x,y)=a(x)|y-\theta(x)|^rU(x,y),\qquad r\ge0, \qquad 0<m\le|U|\le M.

The coefficient cannot vanish, since f>0f>0. The center is outside the band, hence either θ≤α\theta\le\alpha or θ≥β\theta\ge\beta throughout this connected base interval. After shrinking it, take

yℓ=2α,yh=β/2,α<yℓ<yh<β. y_\ell=2\alpha,\qquad y_h=\beta/2, \qquad \alpha<y_\ell<y_h<\beta.

The actual ratio is

f(x,yh)f(x,yℓ)=4α(x)β(x)→0. \frac{f(x,y_h)}{f(x,y_\ell)} =\frac{4\alpha(x)}{\beta(x)}\longrightarrow0.

If θ≤α\theta\le\alpha, the distance ratio is at least one, so the prepared ratio is at least m/Mm/M. If θ≥β\theta\ge\beta, then

θ−yhθ−yℓ≥12, \frac{\theta-y_h}{\theta-y_\ell}\ge\frac12,

so the prepared ratio is at least 2−rm/M2^{-r}m/M. Both contradict its limit zero. Some negative exponent is therefore necessary. Boundedness of the whole function does not force nondegenerate preparation; its base coefficient can compensate for an inverse power on a narrowing band.

16. Even substitutions and parameter-dependent poles

Level: intermediate. Explain why the substitution t=τ2t=\tau^2 does not make t\sqrt t analytic on a two-sided neighborhood of zero, while t=τ4t=\tau^4 does. Then analyze the globally subanalytic function

f(x,t)=xt−1/2+t1/3,x∈ℝ,0<t<1. f(x,t)=xt^{-1/2}+t^{1/3}, \qquad x\in\mathbb R,\quad 0<t<1.

Give one common root-variable Laurent expansion and one even substitution that agrees with the actual function for both signs of the new variable. Determine the parameter pieces on which a continuous analytic extension at zero is possible.

Solution. The two compositions are |τ||\tau| and τ2\tau^2. A two-sided analytic substitution must make every cleared exponent even, not merely make the substitution exponent even.

With t=τ6t=\tau^6 on the positive τ\tau-axis the Laurent expansion is

f(x,τ6)=xτ−3+τ2,τ>0. f(x,\tau^6)=x\tau^{-3}+\tau^2,\qquad \tau>0.

For both signs, choose t=τ12t=\tau^{12}. Then

f(x,τ12)=xτ−6+τ4,τ≠0. f(x,\tau^{12})=x\tau^{-6}+\tau^4,\qquad \tau\ne0.

For x≠0x\ne0 the pole remains; no continuous extension is possible there. On the parameter cell {0}\{0\}, the function becomes τ4\tau^4, analytic across zero. The cells (−∞,0),{0},(0,∞)(-\infty,0),\{0\},(0,\infty) give one finite analytic parameter partition.

Even at (x,t)=(0,0)(x,t)=(0,0), continuity fails if one keeps all parameters together. Along x=t1/4x=t^{1/4}, the first summand equals t−1/4t^{-1/4} and diverges. The continuous-parameter theorem requires joint continuity on its stated neighborhood; continuity on the one slice x=0x=0 does not supply that hypothesis.