On Sunday, May 6, 2018 at 3:55:06 AM UTC, [email protected] wrote:
>
>
>
> On Friday, May 4, 2018 at 5:49:15 PM UTC, Lawrence Crowell wrote:
>>
>> On Friday, May 4, 2018 at 8:21:52 AM UTC-5, Bruce wrote:
>>>
>>>
>>> Unfortunately, it is not the case that you can implement absolutely any 
>>> unitary transformation in this way. For instance, you cannot implement the 
>>> unitary transformation that would reverse a totally decohered event. Your 
>>> quantum computer ceases to function if there is any decoherence! For 
>>> example, you cannot implement a unitary transformation that would resurrect 
>>> my dead grandfather, even though his life and death were entirely unitary.  
>>> So you cannot reverse a recorded measurement.
>>>
>>> Bruce
>>>
>>
>> Weak measurements are or come close to being reversible. There is an 
>> effort to know what the limits are on this, So far the boundary between a 
>> hard and weak measurement appears flexible. This means that if one had some 
>> vast master equation for all the reservior of interacting states that a 
>> hard measurement might be reversible. Of course from a practical 
>> perspective this becomes implausible.
>>
>> LC 
>>
>
> I have been exploring that model for the reversibility of quantum 
> measurements. But as I recently posted in reply, the existence of such a 
> reversible process would contradict Bell experiments. Wouldn't running 
> those reservoir states backward, imply the existence of huge set of local 
> hidden variables? AG
>

The question I am raising is this; if we could identify a single reservoir 
state that was entangled with the wf of the system being measured, and if 
it could be reversed by some identifiable, describable physical process, 
would this imply a local hidden variable for this particular entangled 
system disallowed by Bell experiments? AG 

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