Ciro Santilli @cirosantilli  40

An "alternative" formulation of quantum mechanics that does not involve operators.

Implementations:

His combination of politically incorrect dirt talk with amazing quirky decks captures Ciro's imagination.

Anonymous no face-reveal.

The videos are heavily edited with all pauses cut out, which makes them very quick to watch and saves viewer time.

Modern focused, with some occasional newer formats mixed in.

When Wizards publishes several useless sets in a row without a single modern playable card, he's just forced into Standard.

$L^p$ for $p==2$.

$L^2$ is by far the most important of $L^p$ because it is quantum mechanics states live, because the total probability of being in any state has to be 1!

$L^2$ has some crucially important properties that other $L^p$ don't (TODO confirm and make those more precise):

TODO. I think this is the key point. Notably, $U(1)$ symmetry implies charge conservation.

More precisely, each generator of the corresponding Lie algebra leads to one separate conserved current, such that a single symmetry can lead to multiple conserved currents.

This is basically the local symmetry version of Noether's theorem.

Then to maintain charge conservation, we have to maintain local symmetry, which in turn means we have to add a gauge field as shown at Video "Deriving the qED Lagrangian by Dietterich Labs (2018)".

Forces can then be seen as kind of a side effect of this.

Bibliography: