On Tue, Aug 6, 2019 at 7:23 PM Bruno Marchal <[email protected]> wrote:

> On 6 Aug 2019, at 10:28, Bruce Kellett <[email protected]> wrote:
>
>
> No, you are just attempting to divert attention away from the fact that
> you have no answer to my original argument that a quantum computer can
> quite reasonably do the calculation by rotating the state vector in Hilbert
> space, and consequently, there is no need to imagine a large number of
> parallel worlds in which the calculations are performed by a series of
> clunky linear processing Turing machines. The hypothetical observer is
> entirely irrelevant.
>
>
>
>> In that state, O has still the choice to look at this in the {a, b} base,
>> or in the {a+b, a-b} base. In the first, the universal ray will describe
>> ((O seeing a) a + (O seeing b) b) (well normalised),
>>
>
> A change of base does not make the idea that there are parallel worlds any
> more convincing. Again, this is just a diversionary tactic.
>
>
> You are a bit too much fuzzy for me. I don’t see how a rotating ray in an
> Hilbert space fail to described superposition states, and without wave
> collapse the local (partial trace description) of the situation above makes
> the superposition of the observer states not eliminable.
>

I do not understand your objections here. They make no sense. All I am
claiming is some basic facts about vector spaces. If you have a vector
space, you can form an arbitrary number of sets of basis vectors that span
the space. Any vector in the space can be described in terms of its
projections onto these basis vectors. Correspondingly, any set of values
along the basis vectors can be summed to give a single vector (or ray) in
the space. Any change to either the basis vector components, or the vector
itself, is reflected in the other representation. In other words, change
the vector and you change the projections on to the basis. Or change these
basis components and you change the vector.

In the case of a quantum computer, description of the calculation in terms
of some set of basis vectors is completely captured in the corresponding
changes to the summation vector. Consequently, the description of the QC
action in terms of some set of basis vectors is entirely unnecessary -- the
same action of the QC is entirely captured by the unitary rotations of the
summation vector in the Hilbert space.

That is all that there is to it. The advantage of the vector description is
that such a description is independent of the chosen basis -- what happens
to the vector can be described in terms of any one of the infinite number
of possible alternative bases. This is the basis ambiguity, or problem of a
preferred basis. To pick out one set of base vectors and claim that these
vectors represent a set of parallel worlds in which the computations
actually occur, is simply unnecessary -- description in terms of the single
summation vector eliminates this stupidity.


Maybe you can tell me what happens in that situation. Note that even after
> measurement, we can get back the interference effect by erasing the
> memorised outcome of the result. Without collapse pure state remains pure,
> and decoherence is relative to each “copies” of the observer in the terms
> of the (universal)
>


These observations are entirely beside the point. You cannot erase the
memory of the result because memory is intrinsically irreversible. Quantum
erasure is a technical matter that occurs only in highly constrained
situations. I think you should catch up on some recent work on quantum
foundations, in which Everett does not necessarily require the continuing
purity of the quantum state. Measurement changes the pure state into a
mixture. Zureck has made considerable progress in this direction in recent
years. Quantum foundations has moved on since 1957.

Bruce

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