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Sep 23, 2019 at 9:14 answer added Rob timeline score: 2
Jul 17, 2015 at 8:04 comment added Selene Routley @ArnoldNeumaier Thanks Arnold. I think Ron is right - I need to think on it a bit.
Jul 17, 2015 at 7:55 comment added Arnold Neumaier There is an answer at physicsoverflow.org/10366
Jan 24, 2015 at 18:10 history edited glS
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Oct 3, 2014 at 18:51 history tweeted twitter.com/#!/StackPhysics/status/518111121249939456
Aug 21, 2014 at 6:42 answer added Incnis Mrsi timeline score: 3
Aug 21, 2014 at 6:18 comment added Incnis Mrsi @Norbert Schuch: A system composed of N qubits is described by $2^N$-dimensional space, in other words, it has $2^N$ distinct/independent quantum states. Exactly the same thing as N classical bits that have $2^N$ states. I suppose a confusion between number of states and amount of information (that grows logarithmically).
Nov 2, 2013 at 19:54 comment added Norbert Schuch ... you might also want to check arxiv.org/abs/1306.4352.
Nov 2, 2013 at 12:55 comment added Norbert Schuch Yes, no, and no. Initializing one qubit dissipates $kT$ of energy, and thus, initializing N qubits dissipates an energy of $NkT$. (Note that if the energy would not scale linearly with the number of qubits, this would likely give rise to all kind of contradictions!) This is closely related to the question whether $N$ qubits "contain" $N$ bits or $2^N$ bits of information (and typically $N$ is the more appropriate answer) -- e.g., arxiv.org/abs/quant-ph/0507242 contains some arguments about that.
Nov 2, 2013 at 11:57 comment added Selene Routley @Trimok Ca marche bien pour moi! How very interesting indeed, thanks heaps.
Nov 2, 2013 at 10:04 comment added Trimok Interestingly, I found a paper ("unfortunately" in French), here, which states , that in the case of a hybrid optomechanic system (See fig $2$ page $7$, fig $5$ page $10$), the work necessary to initialize a qbit is proportionnal to the Rabi frequency, which plays the role of a temperature (formula $23$ page $12$)
Nov 2, 2013 at 3:24 history asked Selene Routley CC BY-SA 3.0