ScalingStacks

Proof. [02YN]

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Proof.

To prove this result it suffices to compute the two integrals appearing in Lemma 8.22. However

L⁡(y)=a0+∑ℓ=1r(aℓ−a0)​yℓ=a0​y0+⋯+ar​yr,L(y)=a_{0}+\sum_{\ell=1}^{r}(a_{\ell}-a_{0})y_{\ell}=a_{0}y_{0}+\dots+a_{r}y_{r},

with y0=1−y1−⋯−yry_{0}=1-y_{1}-\dots-y_{r}, and therefore

L​(y)n=∑|α|=nα∈ℕr+1(nα0,…,αr)​∏ℓ=0r(aℓ​yℓ)αℓL(y)^{n}=\sum_{\stackrel{{\scriptstyle\alpha\in\mathbb{N}^{r+1}}}{{\scriptscriptstyle|\alpha|=n}}}\binom{n}{\alpha_{0},\dots,\alpha_{r}}\prod_{\ell=0}^{r}(a_{\ell}y_{\ell})^{\alpha_{\ell}}

and similarly for L​(y)n+1L(y)^{n+1}. Now, Corollary 7.19 gives :

∫Δry0α0​y1α1​…​yrαr​d​y\displaystyle\int_{\Delta^{r}}y_{0}^{\alpha_{0}}y_{1}^{\alpha_{1}}\dots y_{r}^{\alpha_{r}}\,\text{\rm d}y =α0!​…​αr!(|α|+r)!,\displaystyle=\frac{\alpha_{0}!\dots\alpha_{r}!}{(|\alpha|+r)!},
∫Δry0α0​y1α1​…​yrαr​log⁡(yj)​d​y\displaystyle\int_{\Delta^{r}}y_{0}^{\alpha_{0}}y_{1}^{\alpha_{1}}\dots y_{r}^{\alpha_{r}}\log(y_{j})\,\text{\rm d}y =−α0!​…​αr!(|α|+r)!∑ℓ=αj+1|α|+r1ℓ,\displaystyle=-\frac{\alpha_{0}!\dots\alpha_{r}!}{(|\alpha|+r)!}\sum_{\ell=\alpha_{j}+1}^{|\alpha|+r}\frac{1}{\ell},

which, combined with the above expression for L​(y)nL(y)^{n} and L​(y)n+1L(y)^{n+1}, gives

∫ΔrL​(y)n​𝑑y\displaystyle\int_{\Delta^{r}}L(y)^{n}dy =∑|α|=nα∈ℕr+1n!(n+r)!​∏ℓ=0raℓαℓ=∑i0+⋯+ir=ni0,…,ir∈ℕ∏ℓ=0raℓiℓ\displaystyle=\sum_{\stackrel{{\scriptstyle\alpha\in\mathbb{N}^{r+1}}}{{\scriptscriptstyle|\alpha|=n}}}\frac{n!}{(n+r)!}\prod_{\ell=0}^{r}a_{\ell}^{\alpha_{\ell}}=\sum_{\stackrel{{\scriptstyle i_{0},\dots,i_{r}\in\mathbb{N}}}{{\scriptscriptstyle i_{0}+\dots+i_{r}=n}}}\prod_{\ell=0}^{r}a_{\ell}^{i_{\ell}}
∫ΔrL​(y)n+1​𝑑y\displaystyle\int_{\Delta^{r}}L(y)^{n+1}dy =∑|α|=n+1α∈ℕr+1(n+1)!(n+1+r)!​∏ℓ=0raℓαℓ=∑i0+⋯+ir=n+1i0,…,ir∈ℕ∏ℓ=0raℓiℓ\displaystyle=\sum_{\stackrel{{\scriptstyle\alpha\in\mathbb{N}^{r+1}}}{{\scriptscriptstyle|\alpha|=n+1}}}\frac{(n+1)!}{(n+1+r)!}\prod_{\ell=0}^{r}a_{\ell}^{\alpha_{\ell}}=\sum_{\stackrel{{\scriptstyle i_{0},\dots,i_{r}\in\mathbb{N}}}{{\scriptscriptstyle i_{0}+\dots+i_{r}=n+1}}}\prod_{\ell=0}^{r}a_{\ell}^{i_{\ell}}
∫ΔrL​(y)n​εr​(y)​𝑑y\displaystyle\int_{\Delta^{r}}L(y)^{n}\varepsilon_{r}(y)dy =−∑m=0r∑|α|=nα∈ℕr+1n!​(αm+1)(n+1+r)!(∏ℓ=0raℓαℓ)∑ℓ=αm+2n+1+r1ℓ\displaystyle=-\sum_{m=0}^{r}\sum_{\stackrel{{\scriptstyle\alpha\in\mathbb{N}^{r+1}}}{{\scriptscriptstyle|\alpha|=n}}}\frac{n!(\alpha_{m}+1)}{(n+1+r)!}\bigg(\prod_{\ell=0}^{r}a_{\ell}^{\alpha_{\ell}}\bigg)\sum_{\ell=\alpha_{m}+2}^{n+1+r}\frac{1}{\ell}
=−n!(n+1+r)!∑i0+⋯+ir=ni0,…,ir∈ℕ(∏ℓ=0raℓiℓ)∑m=0r(im+1)∑ℓ=im+2n+1+r1ℓ\displaystyle=-\frac{n!}{(n+1+r)!}\sum_{\stackrel{{\scriptstyle i_{0},\dots,i_{r}\in\mathbb{N}}}{{\scriptscriptstyle i_{0}+\dots+i_{r}=n}}}\bigg(\prod_{\ell=0}^{r}a_{\ell}^{i_{\ell}}\bigg)\sum_{m=0}^{r}(i_{m}+1)\sum_{\ell=i_{m}+2}^{n+1+r}\frac{1}{\ell}
=−2​n!(n+1+r)!∑i0+⋯+ir=ni0,…,ir∈ℕ(∏ℓ=0raℓiℓ)An,r(i0,…,ir).\displaystyle=-\frac{2\,n!}{(n+1+r)!}\sum_{\stackrel{{\scriptstyle i_{0},\dots,i_{r}\in\mathbb{N}}}{{\scriptscriptstyle i_{0}+\dots+i_{r}=n}}}\bigg(\prod_{\ell=0}^{r}a_{\ell}^{i_{\ell}}\bigg)A_{n,r}(i_{0},\dots,i_{r}).

The statement follows from these expressions together with Lemma 8.22. ∎

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