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Feb 2, 2015 at 10:18 comment added kutschkem Are you sure the wave-function has this much entropy?
Dec 29, 2012 at 14:38 comment added Anixx This is not a precise answer. It is true only if you are speaking about a storage that can operate with variables of no less than 1 bit size. In that case you need $10^{80}$ such variables. But the majority of that space is wasted, because in reality each variable does not need a FULL bit. That is by compressing several such variables into one bit you'll need much less storage. Unfortunately the classical devices cannot independently manipulate quantities of information less than 1 bit.
Aug 3, 2012 at 15:26 vote accept z5h
Aug 1, 2012 at 7:02 comment added Ron Maimon @Raskolnikov: Quantum monte-carlo only works well for bosonic systems, it is very hard to do with fermions, and this is the "sign problem". It is extraordinarily depressing that something as simple and dumb as a large atom is so hard to simulate.
Apr 21, 2011 at 22:05 comment added z5h I think the key is that in order for us to care, the events must be measurable. If they are not all measurable, we don't need all of them in our simulation. see here: en.wikipedia.org/wiki/Infrared_divergence
Apr 21, 2011 at 21:57 comment added Lagerbaer Couldn't you have an arbitrary number of virtual particles albeit on a small timescale?
Apr 21, 2011 at 21:53 comment added z5h "in a black body, for example, you can have an infinite number of photons". If we assume finite energy and finite space in the universe, and we can encode a 1 bit of data per photon, this disagrees with the Bekenstein bound. The other option is that although we have infinite photons, we cannot decode the information stored. So we can discard them from our simulation. no?
Apr 20, 2011 at 8:29 comment added Raskolnikov Hah, I answered my own question. I iz a winnah!
Apr 20, 2011 at 8:27 comment added Raskolnikov This makes me wonder, isn't there a stochastic (Monte Carlo) way of simulating quantum mechanical systems akin to what is done when solving SDE and Markov processes and such?
Apr 20, 2011 at 3:33 comment added Lagerbaer This is the nasty thing about quantum mechanics. You have to store the value of the wavefunction for each of the possible combinations of your $\vec{x}_i$. You have $n$ for the first, $n$ for the second, $n$ for the third... so in total $n^m$.
Apr 20, 2011 at 3:17 comment added yayu @lagerbaer basic question: if you wish to encode an m parameter function over n points, why would it be $n^m$?
Apr 20, 2011 at 0:31 history answered Lagerbaer CC BY-SA 3.0