The Fourier transform is a bijection in by Ciro Santilli 35 Updated +Created
As mentioned at Section "Plancherel theorem", some people call this part of Plancherel theorem, while others say it is just a corollary.
This is an important fact in quantum mechanics, since it is because of this that it makes sense to talk about position and momentum space as two dual representations of the wave function that contain the exact same amount of information.
Radiation pressure by Ciro Santilli 35 Updated +Created
Personality type by Ciro Santilli 35 Updated +Created
Alpha Centauri by Ciro Santilli 35 Updated +Created
Khronos Group by Ciro Santilli 35 Updated +Created
The fact that they kept the standard open source makes them huge heroes, see also: closed standard.
Shame that many (most?) of their proposals just die out.
Signal protocol by Ciro Santilli 35 Updated +Created
Adenine by Ciro Santilli 35 Updated +Created
NP-intermediate by Ciro Santilli 35 Updated +Created
This is the most interesting class of problems for BQP as we haven't proven that they are neither:
New Testament part by Ciro Santilli 35 Updated +Created
Monstrous moonshine by Ciro Santilli 35 Updated +Created
Mitochondrial endosymbiosis by Ciro Santilli 35 Updated +Created
Likely happened between an archaea and a bacteria.
Mitochondrial DNA by Ciro Santilli 35 Updated +Created
Micro Bit simulator by Ciro Santilli 35 Updated +Created
nRF51 series by Ciro Santilli 35 Updated +Created
Picometer by Ciro Santilli 35 Updated +Created
k-transitive group by Ciro Santilli 35 Updated +Created
TODO why do we care about this?
Note that if a group is k-transitive, then it is also k-1-transitive.
Path integral formulation by Ciro Santilli 35 Updated +Created
This one might actually be understandable! It is what Richard Feynman starts to explain at: Richard Feynman Quantum Electrodynamics Lecture at University of Auckland (1979).
The difficulty is then proving that the total probability remains at 1, and maybe causality is hard too.
The path integral formulation can be seen as a generalization of the double-slit experiment to infinitely many slits.
Feynman first stared working it out for non-relativistic quantum mechanics, with the relativistic goal in mind, and only later on he attained the relativistic goal.
TODO why intuitively did he take that approach? Likely is makes it easier to add special relativity.
This approach more directly suggests the idea that quantum particles take all possible paths.

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