Russell Standish wrote:> > According to Wikipedia, Born's rule is that the
probability of an> observed result \lambda_i is given by <\psi|P_i|\psi>, where
P_i is the> projection onto the eigenspace corresponding to \lambda_i of the>
observable. > > This formula is only correct if \psi is normalised. More
correctly,> the above formula should be divided by <\psi|\psi>.> > This
probability can be interpreted as a conditional probability - the> probability
of observing outcome \lambda_i for some observation A,> _given_ a
pre-measurment state \psi.> > What is important here is that it says nothing
about what the state> vector is after the measurement occurs. There is a (von
Neumann)> projection postulate, which says that after measurement, the system>
will be found in the state P_i|\psi>, but as I said before, this is>
independent of the Born rule, and also it does not state what the> "amplitude"
(ie magnitude) of the state is. The v-N PP is also distinctly not> a feature of
the MWI (it is basically the Copenhagen collapse).The projection postulate
needs to work *effectively* in the MWI though, in order for it to make the same
predictions about actual experimental results as the Copenhagen interpretation.
If an observer makes one measurement and then makes a later measurement of the
same system, they can collapse the system's quantum state onto an eigenstate at
the moment of the first measurement and evolve that new state forward, and this
will give correct predictions about the probabilities of different outcomes
when the second measurement is made. I think part of the difficulty with
connecting the MWI to actual observed probabilities is explaining *why* this
rule should work in an effective sense.> > > I think the quote I was responding
to was the following:> > "In an ordinary quantum mechanical situation (without
deaths), and> assuming the Born Rule holds, the effective probability is
proportional> to the total squared amplitude of a branch."> > If you compare it
with the description of the Born rule above (which> computes a conditional
probability), there is no sense in which one> can say that "the effective
probability is proportional to the total> squared amplitude of a branch"
follows directly from the Born> rule. Jacques is assuming something else
entirely - perhaps> einselection?The notion that probability is proportional to
squared amplitude is equivalent to the wikipedia definition you posted above.
The projection operator P_i onto a given eigenstate |\lambda_i> is really just
|\lambda_i><\lambda_i| (see the text immediately above 'Postulate 5' near the
bottom of the page at http://xbeams.chem.yale.edu/~batista/vvv/node2.html ),
which means that when this operator acts on a given state vector |\psi>, it
gives (|\lambda_i><\lambda_i|)|\psi> = |\lambda_i>(<\lambda_i|\psi>), and
(<\lambda_i|\psi>) is just a scalar c_i, so this becomes c_i * |\lambda_i>.
This c_i is referred to as the "amplitude" that the original state |\psi>
assigns to the eigenstate |\lambda_i> (by something called the 'expansion
postulate' it's possible to write |psi> as a weighted sum of all the
eigenstates of a measurement operator, and the weights on each eigenstate are
just the amplitudes for each eigenstate). So, if the probability is
<\psi|P_i|\psi> (which I think assumes that |\psi> has been normalized), then
since P_i = |\lambda_i><\lambda_i|, this is the same as saying the probability
is <\psi|\lambda_i><\lambda_i|\psi>. If <\lambda_i|\psi> is the amplitude c_i,
then <\psi|\lambda_i> is just the complex conjugate (c_i)*, so the probability
is just the amplitude times its own complex conjugate, often referred to as the
"amplitude-squared".Jesse
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