On Tuesday, May 13, 2025 at 4:54:55 AM UTC-6 Alan Grayson wrote:

On Monday, May 12, 2025 at 4:15:52 PM UTC-6 Brent Meeker wrote:



On 5/12/2025 1:58 PM, Alan Grayson wrote:



On Friday, May 9, 2025 at 10:40:42 PM UTC-6 Brent Meeker wrote:

On 5/9/2025 7:08 PM, Alan Grayson wrote:

*I can see that the measurement spreads due to instrument limitations are 
usually immensely larger than the much smaller spreads accounted for by the 
UP, but what causes these much smaller spreads? Is this a quantum effect? 
AG* 


Yes.  Quantum evolution is unitary, i.e. the state vector just rotates in a 
complex Hilbert space so that probability is preserved.  Consequently the 
infinitesimal time translation operator is U=1+e6/6t or in common notation 
1-i(e/h)H where H=ih6/6t and h is just conversion factor because we measure 
energy in different units than inverse time. It's not mathematics, but an 
empirical fact that h is a universal constant.

Brent 


*If one wants to prepare a system in some momentum state to be measured, 
doesn't this imply a pre-measurement measurement, *

Right, given that it's an ideal measurement.  Most measurements don't leave 
the system in the eigenstate that is the measurement result.  An ideal 
measurement is one that leaves the system in the state that the measurement 
yielded.


*and the observable to be measured remains in that state on subsequent 
measurements? *

Only if they're ideal measurements of that same variable or of other 
variables that commute with it.


*If so, how can the unitary operator, which just changes the state of the 
system's wf, create the quantum spread? *

You don't need a change in the wf to "create the quantum spread".  Having 
prepared in an eigenstate of A just measure some other variable B that 
doesn't commute with A.  In general A will be a superposition of other 
variables, say A=xC+yD; that's just a change of coordinates.  But the 
system is not in an eigenstate of C or D.

Brent


*Sorry, I really don't get it. Not at all! If we want to prepare a particle 
with some momentum p, why would we measure it with some non-commuting 
operator, and why would this, if done repeatedly, result in a spread of 
momentum? And what has this to do with a unitary operator which advances 
time? TY, AG *


*Is the spread in momentum caused by an imprecision in preparing a particle 
in some particular momentum? Generally speaking, how is that done? TY, AG *

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