Recent content by vj3336

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    Quantum Mechanics, Simple harmonic oscillator, partition function

    I think the above expression evaluates to: \left.\left.\left.\left.\overset{\wedge }{1}|n\right\rangle +\frac{f^{(1)}(0)}{1!}\overset{\wedge }{n_k}{}^1|n\right\rangle +\frac{f^{(2)}(0)}{2!}\overset{\wedge }{n_k}{}^2|n\right\rangle +\text{...}+\frac{f^{(m)}(0)}{m!}\overset{\wedge...
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    Quantum Mechanics, Simple harmonic oscillator, partition function

    sorry , I still don't know how to do it, can you give me a more explicit hint ?
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    Quantum Mechanics, Simple harmonic oscillator, partition function

    The first excited state is when one of the oscillators is in the E1 state, the second excited state is when one of the oscillator is in the E2 state or one is in E1 state and some other is also in E1 state ... etc Isn't the answer to that question in how many ways I can distribute En energy...
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    Quantum Mechanics, Simple harmonic oscillator, partition function

    ok, I think that I can find energy eigenstates in this way: \left.\left.H|n\rangle =E_n\right|n\right\rangle \left.\left.\left.\left.\left(\sum _k (\hbar -\mu )a_k{}^+a_k-\frac{1}{2}\hbar \right)\right|n\right\rangle =E_n\right|n\right\rangle \left.\left...
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    Quantum Mechanics, Simple harmonic oscillator, partition function

    Homework Statement Compute the partition function Z = Tr(Exp(-βH)) and then the average number of particles in a quantum state <nα > for an assembly of identical simple harmonic oscillators. The Hamiltonian is: H = \sum _{k}[(nk+1/2)\hbar - \mu nk] with nk=ak+ak. Do the calculations once...
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    Quantum mechanics: density matrix purification

    thanks, if I take x to be a vector with components (x y) then, x†M(a)x = a(xx† + yy†) + (1/4)i(xy† + x†y) this then means a(xx† + yy†)≥(1/4)i(xy† + x†y) but term on the left hand side is real and term on the right hand side may be complex, so how can I conclude when is x†M(a)x≥0 ? also is my...
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    Quantum mechanics: density matrix purification

    Homework Statement Given a matrix M(a) = (a -(1/4)i ; (1/4)i a) (semicolon separates rows) a) Determine a so that M(a) is a density matrix. b) Show that the system is in a mixed state. c) Purify M(a) The Attempt at a Solution a) from conditions for a density matrices...
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    Statistics proof, identically distributed RVs and variance

    Thanks ! Your hints where very helpful pointing me in the right direction.
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    Statistics proof, identically distributed RVs and variance

    The general step is then : Var(1/n(X1+...+X2)) = 1/n*σ^2 + 2/n^2 *(1/2 * (n-1)n ) ρσ^2 = 1/n*σ^2 + (n-1)/n *ρσ^2 = ρσ^2 + 1/n*σ^2 + -1/n*ρσ^2 = ρσ^2 + 1/n*(1-ρ)σ^2
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    Statistics proof, identically distributed RVs and variance

    yes, I can do it , so: 1/2σ^2 + 1/2*ρ*σ^2 = 1/2*(2ρσ^2-ρσ^2) + 1/2*σ^2 = ρσ^2 - 1/2*ρσ^2 + 1/2*σ^2 = ρσ^2 + 1/2*(σ^2-ρσ^2) = ρσ^2 + 1/2*(1-ρ)σ ^2 So the next step is to try it with n instead of 2 ?, I'll try that now
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    Statistics proof, identically distributed RVs and variance

    but maybe I can rearrange this to your form ...I'll try it
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    Statistics proof, identically distributed RVs and variance

    The best thing I could do is : Var(1/2(X+Y))= Var(1/2*X + 1/2*Y)= 1/4σx^2 + 1/4σy^2 + 2*1/4*ρ Sqrt(σx^2)*Sqrt(σy^2) =1/4σ^2 + 1/4σ^2 +1/2*ρ*σ^2
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    Statistics proof, identically distributed RVs and variance

    right, so when X and Y are correlated Var(X+Y) = Var(X) + Var(Y) + 2ρ*Sqrt(Var(X))*Sqrt(Var(Y)) where ρ is corelattion coefficient between X and Y
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    Statistics proof, identically distributed RVs and variance

    I think I could, I would start with this : Var(X+Y) = Var(X) + Var(Y) = E[(X-μx)^2] - E[(Y-μy)^2] where μx is the mean of RV X, and μy the mean of RV Y
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    Statistics proof, identically distributed RVs and variance

    Homework Statement Show that for identically distributed, but not necessarily independent random variables with positive pairwise correlation ρ, the variance of their average is ρσ^2 + (1-ρ)σ^2/B. ρ - pairwise corellation σ^2 - variance of each variable B - number of samples...
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