Solution to Density Matrix Pure State Problem

LagrangeEuler
Messages
711
Reaction score
22

Homework Statement


Find condition for which ##\hat{\rho}## will be pure state density operator?
##\hat{\rho} = \begin{bmatrix}
1+a_1 & a_2 \\[0.3em]
a_2^* & 1-a_1
\end{bmatrix}##


Homework Equations


In case of pure state ##Tr(\hat{\rho}^2)=Tr(\hat{\rho})=1##.



The Attempt at a Solution


Using that condition I got
##\hat{\rho}^2 = \begin{bmatrix}
(1+a_1)^2+|a_2|^2 & (1+a_1)a_2+a_2(1-a_1) \\[0.3em]
(1+a_1)a_2^*+a_2^*(1-a_1) & (1-a_1)^2+|a_2|^2
\end{bmatrix}##
and from that
## 2|a|^2+2a_1^2=-1## which can not be true. Because ##a_1## must be real, condition to ##\hat{\rho}## is hermitian.
 
Physics news on Phys.org
I don't quite understand. That density operator you stated, it's not a pure state density operator, and that's why The trace of the square of rho will not be 1. It's correct. I afraid I did not understand your question.
 
Question is find condition put on ##a_1## and ##a_2## for which ##\hat{\rho}## is pure state density operator.
 
The problem occurs because you have not normalized the original density operator yet.
 
Tnx a lot Fightfish. I did not see that trace of given matrix is not ##1##. Density matrix must be
##\hat{\rho} =\frac{1}{2} \begin{bmatrix}
1+a_1 & a_2 \\[0.3em]
a_2^* & 1-a_1
\end{bmatrix}##
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top