right now I'm reading a paper by Blower (Displacement convexity for generalized orthogonal ensemble) and I'm stuck at a rather delicate point. He uses the following equality, which is supposed to be deducable from the mean value theorem:
Lemma: Let $v$ be twice differentiable, then for any $x,y \in \mathbb{R}$ and $s \in [0,1]$ there is a $\bar{s} \in (0,1)$ such that $(1-s)v(x) + sv(y) - v((1-s)x+sy) = \frac{1}{2} s(1-s)(x-y)^2 v''((1-\bar{s})x+\bar{s}y)$.
I've tried to use the mvt (or rather Taylors theorem) on the LHS as a function of $s$, with little success, and with $x$, from which I get the following equality: (call the LHS $H$)
$$ H(x) = H(x) - H(y) = (x-y) \left( (1-s)v'(\xi) - (1-s) v'((1-s)\xi + sy) \right)$$
where $\xi \in (x,y),$ i.e. $\xi = (1-t)x + ty, t \in (0,1)$. Upon a second use the mvt this becomes
$$ H(x) = (x-y)^2(1-s)s \left( v''(\bar{\xi}) (1-t)\right). $$
I do not get any further equalities, as I do not know whether I can take the midpoint $t = \frac{1}{2}$. I can bound this from below by $(1-t) \ge \frac{1}{2}$ (as I can interchange $x$ and $y$ (and hence $s$ and $(1-s)$) if $t > 1/2$), which is sufficient for the proof. However: is there any way to show equality in the Lemma?
Thanks in advance for your responses, Arthur