Statement

Let g∈C1([0,L])g\in C^1([0,L]), L>0L>0, satisfy g(L/2)=0g(L/2)=0 and

−C/L≤g′(v)≤−c/L(0<c≤C).-C/L\le g'(v)\le-c/L\qquad(0<c\le C).

For the P(v)=exp⁡(∫L/2vg(s) ds)P(v)=\exp(\int_{L/2}^v g(s)\,ds),

exp⁡(−C(v−L/2)22L)≤P(v)≤exp⁡(−c(v−L/2)22L)≤1.\exp\left(-\frac{C(v-L/2)^2}{2L}\right) \le P(v)\le \exp\left(-\frac{c(v-L/2)^2}{2L}\right)\le1.
Proof and endpoint decay

The function h=log⁡Ph=\log P satisfies h(L/2)=h′(L/2)=0h(L/2)=h'(L/2)=0 and −C/L≤h′′≤−c/L-C/L\le h''\le-c/L. Integrating twice, or applying Taylor's theorem with integral remainder, gives the bounds on either side of the midpoint. In particular, P(0),P(L)≤e−cL/8P(0),P(L)\le e^{-cL/8}. A cutoff varying only in endpoint regions a fixed proportion away from the midpoint acts where P≤e−c′LP\le e^{-c' L}, for a fixed c′>0c'>0.