On Sunday, April 26, 2020 at 6:39:15 PM UTC-6, Brent wrote:
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> On 4/26/2020 3:22 PM, Alan Grayson wrote:
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> On Sunday, April 26, 2020 at 1:46:59 PM UTC-6, Brent wrote: 
>>
>>
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>> On 4/26/2020 9:24 AM, Alan Grayson wrote:
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>> On Sunday, April 26, 2020 at 9:48:45 AM UTC-6, John Clark wrote: 
>>>
>>> On Sat, Apr 25, 2020 at 12:49 PM Alan Grayson <[email protected]> 
>>> wrote:
>>>
>>> *> How does QM tell us that conservation of energy can be violated for 
>>>> brief durations? If you apply the time-energy form of the UP for your 
>>>> proof, please state the context of your proof, that is, exactly what do E 
>>>> and t stand for.*
>>>
>>>
>>> The shorter the time (t) a system is under observation the larger the 
>>> amount of energy (E) could pop into existence from nothing without direct 
>>> detection, enough energy to create virtual particles. And you can calculate 
>>> how large the indirect effects these virtual particles would have on the 
>>> system.
>>>
>>
>> As I understand the UP, it's a statistical statement about an ensemble of 
>> observations, say for position and momentum of identical particles. It says 
>> nothing about the result of events, say for the position and momentum of a 
>> single particle or event. Doing some arithmetic to get the time-energy form 
>> of the UP does not change this reality. As a result, your description of 
>> what happens to a single particle, virtual or not, is not intelligible. 
>> Please try again. AG 
>>
>>
>> The UP doesn't apply to virtual particles because it refers to the result 
>> of conjugate measurement (projection) operators.  You can't measure virtual 
>> particles.
>>
>> Brent
>>
>
> In its usual form, does the UP allow us to measure position and momentum 
> *simultaneously*, or must we measure each variable independently (for an 
> ensemble of identical particles, of course)? What is proper interpretation 
> of the time/energy form of the principle in statistical terms? TIA, AG 
>
>
> You can measure them simultaneously; but when you repeat the pair of 
> measurements on many identically prepared particles you find that there is 
> a scatter in the position  and a scatter in the momentum such that the HUP 
> is satisfied.
>
> Brent
>

Can you give an example of the ensembles used in applying the time-energy 
form of the UP? TIA, AG 

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