On Thu, Aug 8, 2019, 5:51 AM Bruno Marchal <[email protected]> wrote:

>
> On 8 Aug 2019, at 11:56, Bruce Kellett <[email protected]> wrote:
>
> On Thu, Aug 8, 2019 at 7:21 PM Bruno Marchal <[email protected]> wrote:
>
>> On 8 Aug 2019, at 02:23, Bruce Kellett <[email protected]> wrote:
>>
>> On Wed, Aug 7, 2019 at 11:30 PM Bruno Marchal <[email protected]> wrote:
>>
>>> On 7 Aug 2019, at 14:41, Bruce Kellett <[email protected]> wrote:
>>>
>>>
>>> Superpositions are fine. It is just that they do not consist of
>>> "parallel worlds”.
>>>
>>>
>>> But then by QM linearity, it is easy to prepare a superposition with
>>> orthogonal histories, like me seing a cat dead and me seeing a cat alive,
>>> when I look at the Schoredinger cat. Yes, decoherence makes hard for me to
>>> detect the superposition I am in, but it does not make it going away
>>> (unless you invoke some wave packet reduction of course)
>>>
>>>
>>>
>>>> “Parallel worlds/histories” are just a popular name to describe a
>>>> superposition.
>>>>
>>>
>>> In your dreams, maybe. There is a clear and precise definition of
>>> separate worlds: they are orthogonal states that do not interact. The
>>> absence of possible interaction means that they are not superpositions.
>>>
>>>
>>> That is weird.
>>> The branches of a superposition never interact. The point is that they
>>> can interfere statistically, if not there is no superposition, nor
>>> interference, only a mixture.
>>>
>>
>> There some to be some fluidity is the concepts of superposition and basis
>> vectors inherent in this discussion. Any vector space can be spanned by a
>> set of orthogonal basis vectors. There are an infinite number of such
>> bases, plus the possibility of non-orthogonal bases given by any set of
>> vectors that span the space. If the basis vectors are orthogonal, these
>> basis vectors do not interact. But any general vector can be expressed as a
>> superposition of these orthogonal basis vectors. (Orthonormal basis for a
>> normed Hilbert space.)
>>
>> So the question whether the branches of a superposition can interact
>> (interfere) or not is simply a matter of whether the branches are
>> orthogonal or not. If we have a superposition of orthogonal basis vectors,
>> then the branches do not interact. However, if we have a superposition of
>> non-orthogonal vector, then the branches can interact.
>>
>> For example, the wave packet for a free electron is a superposition of
>> momentum eigenstates (and position eigenstates). These momentum eigenstates
>> are orthogonal and do not interact. The overlap function <p|p'> = 0 for all
>> p not equal to p'. This is the definition of orthogonal states. But this
>> does not mean that the wave packet of the electron is a mixture: It is a
>> pure state since there is a basis of the corresponding Hilbert space for
>> which the actual state is one of the basis vectors. (We can construct an
>> orthonormal set of basis vectors around this vector.)  On the other hand,
>> the two paths that can be taken by a particle traversing a two-slit
>> interference experiment are not orthogonal, so these paths can interact. So
>> when the quantum state is written as a superposition of such paths, there
>> is interference.
>>
>> Orthogonality is the key difference between things that can interfere and
>> those that cannot. So if separate worlds are orthogonal, there can be no
>> interference between them, and the absence of such interaction defines the
>> worlds as separate.
>>
>>
>> What I use is the fact that when we have orthogonal states, like I0> and
>> I1>, I can prepare a state like (like I0> + I1>), and then I am myself in
>> the superposition state Ime>( I0> + I1>), Now, in that state, I have the
>> choice between measuring in the base {I0>, I1>} or in the base {I0> + I1>,
>> I0> - I1>). In the first case, the “parallel” history becomes indetectoble,
>> but not in the second case, so we have to take the superposition into
>> account to get the prediction right in all situations.
>>
>
> I don't think this is actually correct. Take a concrete example that we
> all understand. If we prepare a silver atom with spin 'up' in the
> x-direction, then a measurement in the x direction does not produce a
> superposition -- the answer is 'up' with 100% certainty. But is we measure
> this state in the transverse, y-direction, the result is either 'up-y' or
> 'down-y' with equal probabilities. This is because the initial state 'up-x'
> is already a superposition of 'up-y' and 'down-y'. When we measure this in
> the x-direction, there is no parallel history. When we measure in the
> y-direction, we get either 'up-y' or 'down-y'. MWI says that for either
> result, the alternative occurs in some other world. And that alternative
> result is just as undetectable as the 'down-x' result for the x-measurement.
>
>
>
> The pure state up-x is the same state as the superposition of up-y and
> down-y.
> Me in front of up-x and Me in front of up-y + down-y are only different
> description of the same state. When measuring that state in the
> x-direction, I don’t made that y-superposition disappears.
>
>
>
>
> The point being that whatever measurement we perform, we get only one
> result, and the alternative results that may or may not have been possible
> are undetectable.
>
>
> Yes, that is why we can exploit the parallel worlds (aka superposition of
> states relative to me) only by isolating the computer from from me, so that
> I don’t get entangled with it.
>
>
>
>
> However, it is interesting how this discussion has morphed. We started
> with the observation that a quantum computer does not demonstrate the
> existence of parallel worlds because its operation can be understood
> completely in terms of unitary rotations of the state vector in the one
> world of Hilbert space.
>
>
> Unitary rotations conserves the superposition (and the relative
> probabilities).
>
>
>
>
> Now we seem to have ended up with a discussion  of the nature of
> superpositions, and the idea that unobserved outcomes from experiments have
> to be taken into account. How they are to be taken into account is never
> made clear.
>
>
>
> I don’t know why you say this. We need to take the superposition into
> account to get the probabilities right for arbitrary possible measurements.
>
>
>
> They are orthogonal, in fact, and cannot interact with the observed
> result. Parallel worlds, whether they "exist" or not, have no consequences
> for physics or experimental results. So Everett and MWI are otiose -- they
> have no conceivable effects, particularly in quantum computers, so they are
> irrelevant.
>
>
> If the superposition are not relevant, then I don’t have any minimal
> physical realist account of the two slit experience, or even the stability
> of the atoms.
>
> My goal is not in finding working theory, just to see if the current
> modern theory given by the physicists is consistent with digital mechanism,
> and indeed, its MWI aspect is the easiest prediction of mechanism. Then the
> math suggest we get also the negative interference and that QM confirms
> Digital Mechanism, unless we add the collapse postulate, which indeed is an
> option for the non-computationalist. But the collapse itself is not
> something that we can detect or observe in any way.
>

Bruno,

Forgive me if I have asked this before, but can you elaborate on the
how/why the math suggests negative interference?

I currently have no intuition for why this should be.

I recall reading something on continuous probability as being more natural
and leading to something much like the probability formulas in quantum
mechanics. Is that related?

Jason


> We cannot detect even one world. “World” are metaphysical notion. The old
> dream argument made this clear since long.
>
>
>
>
>
>
> When I talk about some pure state, I mean it as an object considered
>> before we male a measurement on it. And I *assume* QM (without collapse) to
>> be correct.
>>
>
> That is not necessarily a pure state. You can also prepare a mixed state
> before you make any measurement on it. A pure state is a state that can act
> as a basis vector in the relevant Hilbert space.
>
>
> I don’t contest this, albeit I doubt there is any real mixture in nature,
> just a pure universal state starting (say) at the Big Bang, but that’s not
> relevant here.
>
>
>
> QM without collapse might be correct, but you can never demonstrate this,
> because whether it is correct or not has no observable consequences. MWI is
> an interpretation of QM, not an alternative theory.
>
>
> QM is an alternative to QM + collapse. Those are different theories. Both
> have their interpretation problem. But only QM confirms Digital Mechanism,
> and if someone was able to detect the collapse, he would give a real
> evidence against the mechanist hypothesis.
>
> I don’t defend any theory. I only study their logical compatibility or
> inter-dependencies. Digital mechanism and QM are allies. Non-Mechanism and
> QM+collapse are allies.
>
> Now, this list is founded on the idea that everything is simpler to assume
> than any particular thing, and both Digital Mechanism and QM belongs to
> that type. QM+collapse and non-mechanism are of the type of assuming
> particular things.
>
> Bruno
>
>
>
>
>
>
>
> Bruce
>
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