facenian
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If a system is in state |\psi> before a meassurement, then after we find a value a_n the system is in state
\frac{P_n|\psi>}{\sqrt{<\psi|P_n|\psi>}}
so for instance if |\psi>=c_1|a_1>+c_2|a_2>+c_3|a_3> after we find a_1 the system is in the state |\psi>'=e^{i\theta}|a_1> where \theta= is the argument of complex a_1.
I know that |\psi>' and |a_1> represent two different vectors of the Hilbert space of states but the same physical state.
My question is, is there any way that the phase factor e^{\theta} manifest itself in a physical experiment? or put in another way, does this factor have any physical significance?
I ask this because some systems when rotated 360 degrees transforms like |a> \rightarrow -|a> and this sign can be detected exparimentally
\frac{P_n|\psi>}{\sqrt{<\psi|P_n|\psi>}}
so for instance if |\psi>=c_1|a_1>+c_2|a_2>+c_3|a_3> after we find a_1 the system is in the state |\psi>'=e^{i\theta}|a_1> where \theta= is the argument of complex a_1.
I know that |\psi>' and |a_1> represent two different vectors of the Hilbert space of states but the same physical state.
My question is, is there any way that the phase factor e^{\theta} manifest itself in a physical experiment? or put in another way, does this factor have any physical significance?
I ask this because some systems when rotated 360 degrees transforms like |a> \rightarrow -|a> and this sign can be detected exparimentally