From: Rock Brentwood on
On Oct 28, 7:04 am, Uncle Al <Uncle...(a)hate.spam.net> wrote:
> One gets the uncomfortable impression that physics needs a fundamental
> reformulation consistent with information and techniques acquired
> since the 1920s.  String theory ain't it, nor SUSY.

That's the Follow the Crowd approach. What everyone seems to forget is
that the Wisdom of the Masses phenomenon (in which the collective
intelligence of a group gets things right more than any of the group's
members) also has a flip side: the Stupidity of the Masses (i.e.,
because the group is right more often than its members, when the group
actually DOES get things wrong, it's magnified by the fact that
EVERYBODY is wrong!)

There is one objective way to judge matters. If a problem has
attracted the best and brightest for the better part of a century, and
nobody's come up with a clear-cut answer, then that probably means
everybody is going down the wrong path.

So, you can use the Lemming Test as an objective means to determine
what approaches are NOT the right answer. SUSY and string theory are
the wrong answer, solely because they fail the Lemming Test.

The very precept of there being such a thing as Quantum Gravity has
failed the Lemming Test. Gravity is not quantizable and for a very
elementary reason.

The metric and frame field are not part of a "natural bundle", but can
only be defined as part of a "gauge natural" bundle, if you accept a
local Lorentz symmetry as a gauge group. Gauge-natural bundles can be
effectively thought of as a partitioning of a natural bundle, each
subbundle giving you an INEQUIVALENT sector; no two inequivalent
sectors can be quantized within a single coherent state space.

A field cannot be quantized in any quantum theory that only has the
diffeomorphism group, unless the field is part of a natural bundle.

The connection is. The frame field and metric are not. This may be one
of the reasons Einstein looked early on at the idea of "purely affine"
geometries. It's why Kijowski and his people (who produced the LNP 107
volume) took on the idea of trying to formulate gravity as a purely
affine theory.

But if the metric appears as a fundamental field, then this breaks the
local GL(4) frame symmetry down to the orthogonal group SO(3,1). The
fields reside on a Lorentz bundle, but not on a natural bundle. The
reduction GL(4) -> SO(3, 1) is actually a form of symmetry breaking.
The 10 degrees of freedom lost in going over from the 16-d.o.f. GL(4)
symmetry to the 6-d.o.f SO(3,1) symmetry match (in number) the number
of frame components or metric components and they give you the
parametrization of a given subbundle.

Each subbundle has its own vacuum state. Two vacuum states from two
subbundles cannot be combined into a quantum superposition. The index
to the vector sectors (that is, the 10 degrees of freedom comprising
the metric/frame) are, in effect, a CLASSICAL and un-quantizable
field.

In other words: Penrose was right.
From: Uncle Al on
Rock Brentwood wrote:
>
> On Oct 28, 7:04 am, Uncle Al <Uncle...(a)hate.spam.net> wrote:
> > One gets the uncomfortable impression that physics needs a fundamental
> > reformulation consistent with information and techniques acquired
> > since the 1920s. String theory ain't it, nor SUSY.
>
> That's the Follow the Crowd approach. What everyone seems to forget is
> that the Wisdom of the Masses phenomenon (in which the collective
> intelligence of a group gets things right more than any of the group's
> members) also has a flip side: the Stupidity of the Masses (i.e.,
> because the group is right more often than its members, when the group
> actually DOES get things wrong, it's magnified by the fact that
> EVERYBODY is wrong!)
>
> There is one objective way to judge matters. If a problem has
> attracted the best and brightest for the better part of a century, and
> nobody's come up with a clear-cut answer, then that probably means
> everybody is going down the wrong path.

Either needs more genius or better observation to restrict or redefine
founding postulates. The minds are in place, the maths are rigorous
(as much as QM can be rigorous), consistent, and non-predictive. We
all know Uncle Al's position on this,

http://www.mazepath.com/uncleal/qz4.htm
Somebody should look.

Everything already exists to do the observation: Equipment, test
masses, experimental protocols, personnel, and teleparallel
gravitation theory. Somebody should look.

> So, you can use the Lemming Test as an objective means to determine
> what approaches are NOT the right answer. SUSY and string theory are
> the wrong answer, solely because they fail the Lemming Test.

http://www.mazepath.com/uncleal/reality.png
Science is empirical.
http://www.mazepath.com/uncleal/god.jpg
The universe ignores majority votes.

> The very precept of there being such a thing as Quantum Gravity has
> failed the Lemming Test. Gravity is not quantizable and for a very
> elementary reason.

Or quantizations are fundamentally in error at the starting line.
Quantized gravitations require an odd-parity Chern-Simons term in
addition to even-parity Einstein-Hilbert action. All quantized
gravitations demand the Equivalence Principle directly or obliquely
(BRST invariance in perturbational string theory). If chemically and
macroscopically identical, opposite parity atomic mass distributions
falsify the Equivalence Principle, there's your problem solved on both
sides.

> The metric and frame field are not part of a "natural bundle", but can
> only be defined as part of a "gauge natural" bundle, if you accept a
> local Lorentz symmetry as a gauge group. Gauge-natural bundles can be
> effectively thought of as a partitioning of a natural bundle, each
> subbundle giving you an INEQUIVALENT sector; no two inequivalent
> sectors can be quantized within a single coherent state space.

Lorentz symmetry would be (trace) violated by a trace chiral
pseudoscalar vacuum background restricted to the massed sector (inert
to EM). Detection woul require exquisite apparatus (Eotvos balance)
and test masses (opposed single crystal enantiomorphic space groups
P3(1) and P3(2) glycine gamma-polymorph, or P3(1)21 and P3(2)21
quartz). No prior observation, lab or astronomic, would be
contradicted. Somebody should look.

> A field cannot be quantized in any quantum theory that only has the
> diffeomorphism group, unless the field is part of a natural bundle.
>
> The connection is. The frame field and metric are not. This may be one
> of the reasons Einstein looked early on at the idea of "purely affine"
> geometries. It's why Kijowski and his people (who produced the LNP 107
> volume) took on the idea of trying to formulate gravity as a purely
> affine theory.
>
> But if the metric appears as a fundamental field, then this breaks the
> local GL(4) frame symmetry down to the orthogonal group SO(3,1). The
> fields reside on a Lorentz bundle, but not on a natural bundle. The
> reduction GL(4) -> SO(3, 1) is actually a form of symmetry breaking.
> The 10 degrees of freedom lost in going over from the 16-d.o.f. GL(4)
> symmetry to the 6-d.o.f SO(3,1) symmetry match (in number) the number
> of frame components or metric components and they give you the
> parametrization of a given subbundle.
>
> Each subbundle has its own vacuum state. Two vacuum states from two
> subbundles cannot be combined into a quantum superposition. The index
> to the vector sectors (that is, the 10 degrees of freedom comprising
> the metric/frame) are, in effect, a CLASSICAL and un-quantizable
> field.
>
> In other words: Penrose was right.

The jury remains in the court until all the physical evidence is
disclosed. Gravitation is a geometry not a stockroom. Somebody give

http://www.npl.washington.edu/eotwash/

a boot to the head. You'd think they'd grow tired of guaranteed
measuring zero from their stockroom,

<http://www.npl.washington.edu/eotwash/publications/pdf/lowfrontier2.pdf>

but you'd be wrong,

http://www.mazepath.com/uncleal/publon.htm
Ask Dr. Schund

Somebody should look.

--
Uncle Al
http://www.mazepath.com/uncleal/
(Toxic URL! Unsafe for children and most mammals)
http://www.mazepath.com/uncleal/qz4.htm