On Sunday, November 3, 2019 at 4:03:46 AM UTC-7, Bruno Marchal wrote:
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>
> On 1 Nov 2019, at 22:10, Alan Grayson <[email protected] <javascript:>> 
> wrote:
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>
>
> On Friday, November 1, 2019 at 3:57:39 AM UTC-6, Bruno Marchal wrote:
>>
>>
>> On 31 Oct 2019, at 23:49, Alan Grayson <[email protected]> wrote:
>>
>>
>>
>> On Thursday, October 31, 2019 at 6:04:58 AM UTC-6, Bruno Marchal wrote:
>>>
>>>
>>> On 30 Oct 2019, at 21:50, Alan Grayson <[email protected]> wrote:
>>>
>>>
>>>
>>> On Tuesday, October 29, 2019 at 5:53:10 PM UTC-6, Alan Grayson wrote:
>>>>
>>>>
>>>> On Tuesday, October 29, 2019 at 5:18:45 PM UTC-6, Brent wrote:
>>>>>
>>>>>
>>>>> On 10/29/2019 3:48 PM, Alan Grayson wrote:
>>>>>
>>>>>
>>>>> On Tuesday, October 29, 2019 at 1:55:17 PM UTC-6, Brent wrote: 
>>>>>>
>>>>>>
>>>>>>
>>>>>> On 10/29/2019 12:46 PM, Alan Grayson wrote:
>>>>>>
>>>>>>
>>>>>>
>>>>>> On Tuesday, October 29, 2019 at 1:25:43 PM UTC-6, Brent wrote: 
>>>>>>>
>>>>>>>
>>>>>>>
>>>>>>> On 10/29/2019 11:43 AM, Alan Grayson wrote:
>>>>>>>
>>>>>>> What does that mean?  No one even detects them.  They need not even 
>>>>>>>> be absorbed, but could simply fly off to infinity.
>>>>>>>>
>>>>>>>> Brent
>>>>>>>>
>>>>>>>
>>>>>>> What exactly is the situation? Interference is destroyed, more and 
>>>>>>> more, as they get hotter, but without any observations? AG 
>>>>>>>
>>>>>>>
>>>>>>> Right.
>>>>>>>
>>>>>>> Brent
>>>>>>>
>>>>>>
>>>>>> It sounds like some sort of hidden variable (don't take this too 
>>>>>> literally), where the particles send out information of whether 
>>>>>> interference will occur or not, and it doesn't matter if it's observed. 
>>>>>> This could fit into my model of superposition with some modification; 
>>>>>> namely, it you do a which-way experiment, OR if information about 
>>>>>> which-way 
>>>>>> is available, interference is destroyed. And what goes through the slits 
>>>>>> in 
>>>>>> the absence of these conditions is a wave going through both slits. AG
>>>>>>
>>>>>>
>>>>>> OK.  Except "send out" doesn't make sense.   It implies signaling, 
>>>>>> which would be at less than light speed (c.f. delay choice quantum 
>>>>>> eraser 
>>>>>> experiment).
>>>>>>
>>>>>> Brent
>>>>>>
>>>>>
>>>>> What descriptive term do you prefer? Those IR photons travel at the 
>>>>> SoL. The point is that if there's information available for which-way, 
>>>>> even 
>>>>> if not observed, the interference is destroyed. AG
>>>>>
>>>>>
>>>>> What does "available" mean?  The information that left at the speed of 
>>>>> light is not "available" in any conventional sense at the screen or 
>>>>> detector in the experiment.
>>>>>
>>>>> Brent
>>>>>
>>>>
>>>> That's the mystery we have to figure out. What we know, is that the 
>>>> particles release IR photons which could be observed, and when that 
>>>> emission occurs, interference disappears. It doesn't even depend on any 
>>>> observations being made. AG 
>>>>
>>>
>>> I would revise my interpretation this way; the electron, or whatever, 
>>> behaves as a wave when no information exists to distinguish which-way, and 
>>> that wave goes through both slits producing interference. When such 
>>> information exists, even if it isn't used or measured, the interference 
>>> ceases to exist. Obviously, there's a huge mystery how the existence of 
>>> such information is sufficient to destroy interference, but that's what the 
>>> experimental results demonstrate. AG
>>>
>>>
>>> That huge mystery disappears when you apply QM to the particles *and* to 
>>> the observers and all things they interact with. The interferences are 
>>> never destroyed, 
>>>
>>
>>
>> I don't see how this simplifies anything. Sometimes the local observer 
>> sees interference; sometimes not depending on whether which-way information 
>> exists. How does your model explain this? AG 
>>
>>
>> Take the cat C, assuming it well isolated in its box. The cat is in the 
>> state 1/sqrt(2) (a + d). Now imagine that the box was not so well isolated, 
>> and some particle P interact with it. Let us describe the state of the 
>> particle, in case the cat would ba alive by P_a, and P_d if the cat was 
>> dead. As the cat is in the state a + d, the new state is:
>> 1/sqrt(2) (P_a a + P_d d). OK?
>>
>> If I was ware of that particles, I could in principle obtain interference 
>> pattern from that (pure) superposition. In particular, I could erase the 
>> “memory” of the interaction of the particle, so that I can factor again P 
>> from the state above, and get back the interference available from a + d.
>>
>> But if I cannot track that particle, I am unable to do that, and the 
>> interaction with the particle has destroyed my mean to get back to the a + 
>> d state, and I am confronted with what I will take as a mixed state. It 
>> looks like a collapse, but it is only because the superposition of the cat 
>> has leaked to the environment in a way making impossible for me to get back 
>> to the a + d state. 
>>
>> So, there is no collapse, but the fact that the superposition has leaked 
>> in the environment, without me knowing any details on this, makes the state 
>> of the cat equivalent to a mixture of a and d state. FAPP, the cat is 
>> either dead or alive after that unknown and untrackable information.
>>
>> We see that a measurement is only an entanglement, and we don’t need a 
>> collapse postulate to explain why even an “unknown measurement made by some 
>> cosmic particle” prevents me to keep the superposition of the cat available 
>> to me.
>>
>> Bruno
>>
>
> Forget about collapse or no collapse; forget about cats. 
>
>
> I cannot really do this when confronted with a superposition. To get the 
> observed mixed state from the SWE only, I need to consider the 
> superposition of myself, even if I observe only an electron.
>
>
>
>
> The fact is that with electrons or whatever, sometimes we see interference 
> patterns, and sometime not. In the latter case it occurs when which-way 
> information exists, and it doesn't matter if we use or observe that data by 
> instruments or by human observers. 
>
>
> Exactly, that is the main reason to choose “MW” instead of a collapse.
>
>
> I don't see how your previous message remotely offers an explanation. AG
>
>
> Well, in once case we can factor me on the a + d, or up + down state, but 
> once a particle that I am unaware of has interact with the object (micro or 
> macro) described by a + d, or up + down, I can no more factorise the wave, 
> and I can see only a mixed state. Reread my last post with this in mind, it 
> is very basic quantum mechanics (without collapse).
>
> Bruno
>

I have no idea what you're talking about. If anyone else does, please speak 
up. AG 

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>
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>
>>
>>
>>
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>>     but assuming that the observers are machines and that they obey to QM 
>> explains entirely why they feel like memorising that the interference have 
>> disappeared, and why they are locally right about this.
>>
>> Either the observer obeys QM, and inherits the superposition of what they 
>> are observing through measurement/entanglement, or QM is false for the 
>> observer, and we have to wait for some theory of what is an observer, 
>> together with some criteria for when and where we can use QM.
>>
>> Bruno
>>
>>
>>
>>
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