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Saturday, May 3, 2025

Tensor–Operator Framework for Integration-by-Parts Identities and the Higher-Order Leibniz Rule

This blog rewrites my work from two years ago in a more precise way.

A good explanation for Leibniz's rule for higher derivatives is similar to the Binomial theorem(in general, multinomia theorem)

Integration by Parts and Polynomial Identities (sum and difference of the n-th powers of x and y)

Leibniz's rule for higher derivatives

Let A=C(R),D=ddx. Define D1=Did,D2=idD:ARAARA.

Notice that D1D2=DD=D2D1. Now consider m:ARAA,m(uv)=uv and i=mDi.

Then we have the following equations:

1(uv)=uv,2(uv)=uv

And

Dm=m(D1+D2)=1+2

Proposition.

Let T:XY be a morphism and SEnd(X),UEnd(Y). If ST=TU, then SnT=TUn.

Proof.

We use mathematical induction here.

Assume that Sn1T=TUn1, then

SnT=Sn1(ST)=(Sn1T)U=TUn

Corollary. Leibniz Law for Higher derivative.

Dnm(uv)=m(D1+D2)n(uv)=m(k=0n(nk)D1kD2nk(uv))

i.e.

Dn(uv)=(k=0n(nk)ukvnk)

Integration by Parts and Polynomial Identities

image-20250503123511714

That is,

(2n+1+(1)n+11n+1)(uv)=Dm(k=0n(1)k2k1nk)(uv)

But

Dm=m(D1+D2)=1+2

Hence we have

(2n+1+(1)n1n+1)(uv)=(2+1)(k=0n(1)k2k1nk)(uv)

That is a way to see the identity

xn+1+(1)nyn+1=(x+y)k=0nxk(y)nk

 

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