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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=D⊗id,D2=id⊗D:A⊗RA→A⊗RA.

Notice that D1D2=D⊗D=D2D1. Now consider m:A⊗RA→A,m(u⊗v)=uv and ∂i=m∘Di.

Then we have the following equations:

∂1(u⊗v)=u′v,∂2(u⊗v)=uv′

And

D∘m=m∘(D1+D2)=∂1+∂2

Proposition.

Let T:X→Y be a morphism and S∈End(X),U∈End(Y). If ST=TU, then SnT=TUn.

Proof.

We use mathematical induction here.

Assume that Sn−1T=TUn−1, then

SnT=Sn−1(ST)=(Sn−1T)U=TUn◻

Corollary. Leibniz Law for Higher derivative.

Dn∘m(u⊗v)=m∘(D1+D2)n(u⊗v)=m(∑k=0n(nk)D1kD2n−k(u⊗v))

i.e.

Dn(uv)=(∑k=0n(nk)ukvn−k)◻

Integration by Parts and Polynomial Identities

image-20250503123511714

That is,

(∂2n+1+(−1)n+1∂1n+1)(u⊗v)=D∘m(∑k=0n(−1)k∂2k∂1n−k)(u⊗v)

But

D∘m=m∘(D1+D2)=∂1+∂2

Hence we have

(∂2n+1+(−1)n∂1n+1)(u⊗v)=(∂2+∂1)(∑k=0n(−1)k∂2k∂1n−k)(u⊗v)

That is a way to see the identity

xn+1+(−1)nyn+1=(x+y)∑k=0nxk(−y)n−k

 

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