Eva Miranda

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1,609 appearances 1 recordings 1 series first heard Jan 2025 last heard Jan 2025

Eva Miranda’s voice in public audio — every appearance, attributed to the second.

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Fantastic.

Right?

But there is a small problem.

Here we have these operators, okay, and these operators are functions.

Uh I mean are are uh these operators

R on L two R to N.

The Hilbert space that I'm considering are integrable functions, which is called square integrable functions.

Usually this is called.

But is of all R to N.

But what happens?

That the physics intuition tells me that this is wrong.

Because the physics intuition tells me that if I have a positions and momentum, I should have just the positions.

So I should have just L two in R N.

Okay, so we need to cut down the variable.

So this is at the same time.

A problem and an opportunity.

So we go back to Sun Tzu.

This is again chaos and an opportunity.

We have been seeing that finally Dirac formula commutator go to co Po Poisson bracket goes to commutator, as Dirac wanted, right?

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