[net.physics] Why psi in net.physics

cooper@pbsvax.DEC (Topher Cooper HLO2-3/M08 DTN225-5819) (07/24/85)

Sorry to keep this going against such hostility, but I really do think that this
is relevant to physics.  Normally, I feel that posters who try to "explain" what
they said, are wasting their time, since they already said it. But, since I have
frequently admired the insight of Ethan Vishniac's postings (and agreed with
them more often then not) I must assume that I did not express myself clearly.
I will post separately, if at all (I really am not trying to annoy people), my
responses to points which did not seem to be simply my failure to communicate
clearly.

>							      The reason why 
>all this is not particularly interesting to physicists as an experimental 
>endeavor is that the problems here are unique to the field.

The point I was trying to make is that I can see no reason to assume that the
problems _are_ unique to the field (of parapsychology).  In particular
much of the modern (last 15 years) work in "PK" on "unselected" subjects, seems
as far as the mechanics of the experiments, very similar to many experiments
in modern physics.  An "operator" observes a device which measures some
quantity subject to a great deal of random fluctuation.  The operator has a
preference for some particular result (this factor is ignored in descriptions
of physics experiment, but is normally there).  The output from the measuring
device is analyzed statistically and any bias is noted (this applies also to
an underlying "noisy quantity" passing some threshold value, i.e., in a grain
of photographic film).

In parapsychology, when a bias is found, the experimenter says, in essence:
"we have found an example of an experimental anomaly, of the particular type
we call PK".  In physics, with essentially the same set up, when a bias is
found, the experimenter says, in essence: "my hypothesis is confirmed".

I should point out that in PK experiments, the operator (agent, subject)
doesn't seem to have to "do" anything, just to "want" a particular result.  As
a matter of fact, trying to do something seems to reduce the size of the
anomaly.  The strongest anomalies seem to happen quite consistently in the
time period immediately _after_ the subjects stops trying.  This is called the
"release of effort effect."

In what way is the Fabry-Perot optical interferometer used in a PK
experiment different from that used in a physics experiment?  In what way are
the parapsychologist's matched thermistors distinguishable from the
physicist's?  Is there any real difference between the apparent sub-atomic
events which trigger Schmidt's Geiger counter (already discussed here) and
those found in deep mines by scintillation detectors or those found by photon
counters in an X-ray telescope?

It doesn't really matter whether or not the cause of the anomalies is poor
controls, the incorrectness of elementary statistical theory, experimenter
fraud, operator fraud (e.g., a lab tech), or something mysterious that people
are able to do sometimes.  Why do we assume that physics experiments are more
immune to the source of the anomaly (whatever it is) than parapsychology
experiments?  How far can we trust the latest results about some new particle,
proton decay, fractional charges, magnetic monopoles or heavy neutrinos?

>Attempts to replicate experiments in ESP by independent, and skeptical observers
>seem to have a much higher chance of rejection than 1 in 9.  To date it would
>appear to be closer to 8 (or 9) in 9.

That's what I was trying to say.  Conventional statistics says that (with an
alpha of .05), one out of 20 carefully conducted experiments will produce false
positives, and that one out of 400 carefully conducted experiments will produce
false positive results in both the experiment and its replication (though pure
replication is very rarely attempted).  The results of parapsychology
experiments, which can be viewed as control runs in a test on general
experimental methods, indicate that when the effect size is small the actual
values are closer to one out of three and (therefore) one out of nine
respectively.

		Topher Cooper

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