Feynman Parameters: Solving an Induction Problem

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Hey, this is a pretty simple induction problem, but I suck at induction and I think I'm missing something really obvious here, though trying to figure it out whilst having a pretty bad cold isn't much of a good idea.

The identity

\frac{1}{A_1\cdots A_n}=\int_0^1 dx_1\cdots dx_n \delta (\sum_i^nx_i-1) \frac{(n-1)!}{[A_1x_1+\cdots +A_nx_n]^n}

Can be proven inductively, given that we know it works for n=2, by the use of

\frac{1}{AB^n}=\int^1_0 dxdy \delta (x+y-1)\frac{ny^{n-1}}{[Ax+By]^{n+1}}

I get to a certain point then just can't see what to do. Gargh...
 
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Well, whatever it is, I can't really see the more relevant parts of your post... The identity and the hint.
Maybe you should edit and add it at the end until Tex decides to work again.
 
Put y = A_1A_2...A_{n-1}, it falls right out.

Carl
 
You can find the identity:
\frac{1}{A\*B^n}=...
useful
 
http://www.physics.thetangentbundle.net/wiki/Quantum_field_theory/Schwinger-Feynman_parameters
 
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Or better :

http://theoretical-physics.net/dev/src/math/feynman-parameters.html

Then they explain more precisely what happens to the limits of the integrals.
 
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Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA
If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!

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