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3.3 Global matching problem [0236]

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3.3 Global matching problem

We have solved the ODE with the prescribed initial condition, on the interval 0<t<10<t<1. For the application to the generalized Calabi ansatz, we need solutions over 0<t<∞0<t<\infty, and for this purpose the ODE (14) is inadequate. From the ODE (12), it is however a priori clear that t=1t=1 is not a singularity.

Lemma 3.6.

For any given w0>0w_{0}>0, the solution to the ODE (12) exists smoothly on 0<t<1+ϵ⁡(w0)0<t<1+\epsilon(w_{0}) for some ϵ⁡(w0)>0\epsilon(w_{0})>0.

Proof.

The ODE (12) can be smoothly extended as long as ww remains bounded positively below and (1−t)​w′+w(1-t)w^{\prime}+w remains bounded (which imply boundedness of w′′w^{\prime\prime}, and in particular the boundedness of w,w′w,w^{\prime}). Notice

dd​t​((1−t)​w′+w)=(1−t)​w′′>0,\frac{d}{dt}((1-t)w^{\prime}+w)=(1-t)w^{\prime\prime}>0,

so (1−t)​w′+w(1-t)w^{\prime}+w is monotone increasing, and in particular positive. By

dd​t​((1−t)​w′+w)n−1=1−tw3,\frac{d}{dt}((1-t)w^{\prime}+w)^{n-1}=\frac{1-t}{w^{3}},

we see (1−t)​w′+w(1-t)w^{\prime}+w will be bounded as long as ww is bounded positively below.

The convexity of ww is ensured whenever the solution is smooth. Thus for some small ϵ>0\epsilon>0,

w⁡(t)≥w⁡(ϵ)−w′​(ϵ)​(t−ϵ),t≥ϵ.w(t)\geq w(\epsilon)-w^{\prime}(\epsilon)(t-\epsilon),\quad t\geq\epsilon.

For small ϵ\epsilon, we have w0−w0​ϵ<w⁡(ϵ)<w0w_{0}-w_{0}\epsilon<w(\epsilon)<w_{0} and −w0<w′​(ϵ)<0-w_{0}<w^{\prime}(\epsilon)<0, so w⁡(ϵ)/w′​(ϵ)>1−ϵw(\epsilon)/w^{\prime}(\epsilon)>1-\epsilon, whence w⁡(t)w(t) has an a priori lower bound slightly beyond t=1t=1. ∎

Recall the ODE has a symmetry under t→t−1t\to t^{-1} (cf. Remark 3.3). Our strategy to achieve both the t=0t=0 and the t=∞t=\infty boundary conditions, is to look for symmetric solutions:

w⁡(t)=t​w~​(1/t),w⁡(t)=w~​(t).w(t)=t\tilde{w}(1/t),\quad w(t)=\tilde{w}(t).

This is a functional equation on w⁡(t)w(t), and it amounts to a matching condition at t=1t=1:

w⁡(1)=w~​(1),w′​(1)=w~′​(1).w(1)=\tilde{w}(1),\quad w^{\prime}(1)=\tilde{w}^{\prime}(1).

This is equivalent to

w′​(1)=12​w​(1).w^{\prime}(1)=\frac{1}{2}w(1). (20)

The problem is then to look for w0>0w_{0}>0 to solve (20). The key is to extract w′​(1)w^{\prime}(1) from the asymptote of 𝔴\mathfrak{w} as s→+∞s\to+\infty, namely t→1t\to 1. The starting point is the identity

w′​(t)=s​d​𝔴d​s−𝔴.w^{\prime}(t)=s\frac{d\mathfrak{w}}{ds}-\mathfrak{w}. (21)

which means the value of w′w^{\prime} is related to the Legendre transform of 𝔴\mathfrak{w}.

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