View Full Version : two questions for Uncle Al
Charlie Stromeyer Jr.
Jun1-04, 04:43 AM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>\nUncle Al, you wrote earlier that parity effects are explicitly absent\nin metric gravitation (and Newton), but are explicitly present in\naffine gravitation. Does this mean that you are thinking of some type\nof affine gravity which is different from metric-affine gravity, i.e.\nthe gauge theory of the 4d affine group in the presence of a metric as\ne.g. in paper [gr-qc/9402012] ?\n\n(Btw, there may be some serious theoretical problems with coframe or\nteleparallel theories of gravity and I will soon post some references\nto papers which examine these problems. However, I myself am not going\nto think about these problems because they are potentially very\ndifficult, because there are already other topics I am currently\nthinking about, and because it would be more efficient to first wait\nand see if either the Gravity Probe B or your own chiral Eotvos\nexperiment reveal anything that seems to be both new and non-trivial.)\n\nMy second question: On your website you wrote that zero point\nfluctuations affect Rabi oscillations. Can you explain further what\nRabi oscillations are and how they are related to ZPF or do you know\nof some good introductory literature?\n\nI know that I could look up this info for myself, but perhaps you\nalready know some about this topic which would save me some time, and\nI am interested in knowing more about this question because I found\nthis abstract of this paper which discusses a noncausal effect in a\nparticular type of crystal:\n\nhttp://www.opticsinfobase.org/abstract.cfm?id=69273\n\nTIA.\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>Uncle Al, you wrote earlier that parity effects are explicitly absent
in metric gravitation (and Newton), but are explicitly present in
affine gravitation. Does this mean that you are thinking of some type
of affine gravity which is different from metric-affine gravity, i.e.
the gauge theory of the 4d affine group in the presence of a metric as
e.g. in paper [http://www.arxiv.org/abs/gr-qc/9402012] ?
(Btw, there may be some serious theoretical problems with coframe or
teleparallel theories of gravity and I will soon post some references
to papers which examine these problems. However, I myself am not going
to think about these problems because they are potentially very
difficult, because there are already other topics I am currently
thinking about, and because it would be more efficient to first wait
and see if either the Gravity Probe B or your own chiral Eotvos
experiment reveal anything that seems to be both new and non-trivial.)
My second question: On your website you wrote that zero point
fluctuations affect Rabi oscillations. Can you explain further what
Rabi oscillations are and how they are related to ZPF or do you know
of some good introductory literature?
I know that I could look up this info for myself, but perhaps you
already know some about this topic which would save me some time, and
I am interested in knowing more about this question because I found
this abstract of this paper which discusses a noncausal effect in a
particular type of crystal:
http://www.opticsinfobase.org/abstract.cfm?id=69273
TIA.
Uncle Al
Jun1-04, 01:11 PM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>"Charlie Stromeyer Jr." wrote:\n>\n> Uncle Al, you wrote earlier that parity effects are explicitly absent\n> in metric gravitation (and Newton), but are explicitly present in\n> affine gravitation. Does this mean that you are thinking of some type\n> of affine gravity which is different from metric-affine gravity, i.e.\n> the gauge theory of the 4d affine group in the presence of a metric as\n> e.g. in paper [gr-qc/9402012] ?\n\nAffine theory that allows a gravitational stress-energy pseudotensor\nis supportive of net output from a parity Eotvos experiment.\nPseudotensors are anti-symmetric to parity transformation. All metric\ntheory as such predicts an exact null result. Neither test mass\nchemical composition nor structure appear in metric theory, that all\nbegins by postulating the Equivalence Principle (EP). All metric\ntheory via its tensors is symmetric to parity transformation.\n\nTeleparallel metric+affine theory is common; GR can have pseudotensor\nterms added. We know that chemical composition is inert in EP\nobservation (Nordtvedt effect) and testing (e.g, Eotvos balances) to\nfractional parts-per-trillion difference/average. The primary\nquestion still remains unanswered: Do calculated extremal parity test\nmasses (e.g., space group P3(1)21 vs P3(2)21 alpha-quartz) fall\ndifferently? Theory predicts both possible results to high confidence\nlevels - but only one can obtain in the real world.\n\nTheory tells experiment where to look, experiment tells theory what to\nthink. We\'ve MBA-embraced the former to the exclusion of the latter\n(unquantified risk!). The result has been oodles of mumbling\nphilosophy, not hard science that begets technology.\n\n> (Btw, there may be some serious theoretical problems with coframe or\n> teleparallel theories of gravity and I will soon post some references\n> to papers which examine these problems.\n\n"8^>) An acceptable outcome is to have rigorous theoretical basis for\nboth 100% expectation and 100% negated expection. The parity Eotvos\nexperiment can then proceed without bias... and we can discard a whole\nlot of theory afterward for being wrong (or add perturbation terms -\nlike watering a swamp).\n\nI\'m interested in seeing your references.\n\n> However, I myself am not going\n> to think about these problems because they are potentially very\n> difficult, because there are already other topics I am currently\n> thinking about, and because it would be more efficient to first wait\n> and see if either the Gravity Probe B or your own chiral Eotvos\n> experiment reveal anything that seems to be both new and non-trivial.)\n\nThe easiest and best route is to do the parity Eotvos experiment. If\nit nulls we have achieved the historical standard of excellence. If\nit gives net output, about 500 pounds of Phys. Rev. D becomes\nlandfill. Low cost and easy to do in existing equipment by the book;\nsmall risk vs. large gain.\n\nDiscovery is easier as experiment. You\'ve got to do it anyway (except\nuntestable M-theory). Start by looking in the back of the book for\nthe answer. I expect Gravity Probe B will perform exactly to spec -\nFrame dragging will accumulate as GR predicts; no anomalies due to\nfalling spinning bodies or spinning superconductors will be detected.\n\n> My second question: On your website you wrote that zero point\n> fluctuations affect Rabi oscillations. Can you explain further what\n> Rabi oscillations are and how they are related to ZPF or do you know\n> of some good introductory literature?\n\nhttp://www.mazepath.com/uncleal/eotvos.htm\nis a vast and somewhat sloppy accumulation of everything pertaining\nto and peripheral to the topic. Early on, when Bernhard Haisch\'s\nstochastic electrodynamics looked like a valid sourcing of inertia, I\nwondered if micro-structured solids could differentially interact with\nhis mechanism. Haisch\'s work has not born fruit, and his more recent\nmechnism of Unruh radiation was disavowed by Unruh.\n\nhttp://www.mazepath.com/uncleal/\nis the terse technical readout.\n\nI have removed references to ZPF. Fabrication of Casimatter -\nmicrostructured matter that is wholly stacked Casmir etalons optically\ncanceling to 115-120 nm wavelength - is cute, but a dead end. If it\nworked to spec and there were a reasonable effect to scale, it would\nbe at least 1000X too small to detect with current technologies. If\nsomebody has an idle vacuum coater,\n\nhttp://www.mazepath.com/uncleal/casimir3.htm\n\nA real world fabrication problem (one of many!) is the number of\nlayers needed to build thickness. A hair-thin Casimatter plate is\nabout 550 paired layers of aluminum and dielectric. What are the\nchances of keeping the layers optically smooth through that many\ndepositions? Then glue them together, which incorporates more inert\nmatter. A monolithic grown centimeter thickness seems unreachable by\na large margin. Stresses accumulating during hot deposition then\ncooling are serious concerns.\n\n> I know that I could look up this info for myself, but perhaps you\n> already know some about this topic which would save me some time, and\n> I am interested in knowing more about this question because I found\n> this abstract of this paper which discusses a noncausal effect in a\n> particular type of crystal:\n\nThat is intersting but out of my area of speculation. Narrow\ncontainement in passive and active lattices will embrace a wealth of\nelegant phenomena - some of them useful. My interest is circumscribed\nby a calculated extremal geometric parity test of the Equivalence\nPrinciple. I wish to pursue the sharp end of an icepick rather than\nthe face of a hammer.\n\n\n--\nUncle Al\nhttp://www.mazepath.com/uncleal/qz.pdf\nhttp://www.mazepath.com/uncleal/eotvos.htm\n(The parity Eotvos experiment is queued)\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>"Charlie Stromeyer Jr." wrote:
>
> Uncle Al, you wrote earlier that parity effects are explicitly absent
> in metric gravitation (and Newton), but are explicitly present in
> affine gravitation. Does this mean that you are thinking of some type
> of affine gravity which is different from metric-affine gravity, i.e.
> the gauge theory of the 4d affine group in the presence of a metric as
> e.g. in paper [http://www.arxiv.org/abs/gr-qc/9402012] ?
Affine theory that allows a gravitational stress-energy pseudotensor
is supportive of net output from a parity Eotvos experiment.
Pseudotensors are anti-symmetric to parity transformation. All metric
theory as such predicts an exact null result. Neither test mass
chemical composition nor structure appear in metric theory, that all
begins by postulating the Equivalence Principle (EP). All metric
theory via its tensors is symmetric to parity transformation.
Teleparallel metric+affine theory is common; GR can have pseudotensor
terms added. We know that chemical composition is inert in EP
observation (Nordtvedt effect) and testing (e.g, Eotvos balances) to
fractional parts-per-trillion difference/average. The primary
question still remains unanswered: Do calculated extremal parity test
masses (e.g., space group P3(1)21 vs P3(2)21 \alpha-quartz) fall
differently? Theory predicts both possible results to high confidence
levels - but only one can obtain in the real world.
Theory tells experiment where to look, experiment tells theory what to
think. We've MBA-embraced the former to the exclusion of the latter
(unquantified risk!). The result has been oodles of mumbling
philosophy, not hard science that begets technology.
> (Btw, there may be some serious theoretical problems with coframe or
> teleparallel theories of gravity and I will soon post some references
> to papers which examine these problems.
"8^>) An acceptable outcome is to have rigorous theoretical basis for
both 100% expectation and 100% negated expection. The parity Eotvos
experiment can then proceed without bias... and we can discard a whole
lot of theory afterward for being wrong (or add perturbation terms -
like watering a swamp).
I'm interested in seeing your references.
> However, I myself am not going
> to think about these problems because they are potentially very
> difficult, because there are already other topics I am currently
> thinking about, and because it would be more efficient to first wait
> and see if either the Gravity Probe B or your own chiral Eotvos
> experiment reveal anything that seems to be both new and non-trivial.)
The easiest and best route is to do the parity Eotvos experiment. If
it nulls we have achieved the historical standard of excellence. If
it gives net output, about 500 pounds of Phys. Rev. D becomes
landfill. Low cost and easy to do in existing equipment by the book;
small risk vs. large gain.
Discovery is easier as experiment. You've got to do it anyway (except
untestable M-theory). Start by looking in the back of the book for
the answer. I expect Gravity Probe B will perform exactly to spec -
Frame dragging will accumulate as GR predicts; no anomalies due to
falling spinning bodies or spinning superconductors will be detected.
> My second question: On your website you wrote that zero point
> fluctuations affect Rabi oscillations. Can you explain further what
> Rabi oscillations are and how they are related to ZPF or do you know
> of some good introductory literature?
http://www.mazepath.com/uncleal/eotvos.htm
is a vast and somewhat sloppy accumulation of everything pertaining
to and peripheral to the topic. Early on, when Bernhard Haisch's
stochastic electrodynamics looked like a valid sourcing of inertia, I
wondered if micro-structured solids could differentially interact with
his mechanism. Haisch's work has not born fruit, and his more recent
mechnism of Unruh radiation was disavowed by Unruh.
http://www.mazepath.com/uncleal/
is the terse technical readout.
I have removed references to ZPF. Fabrication of Casimatter -
microstructured matter that is wholly stacked Casmir etalons optically
canceling to 115-120 nm wavelength - is cute, but a dead end. If it
worked to spec and there were a reasonable effect to scale, it would
be at least 1000X too small to detect with current technologies. If
somebody has an idle vacuum coater,
http://www.mazepath.com/uncleal/casimir3.htm
A real world fabrication problem (one of many!) is the number of
layers needed to build thickness. A hair-thin Casimatter plate is
about 550 paired layers of aluminum and dielectric. What are the
chances of keeping the layers optically smooth through that many
depositions? Then glue them together, which incorporates more inert
matter. A monolithic grown centimeter thickness seems unreachable by
a large margin. Stresses accumulating during hot deposition then
cooling are serious concerns.
> I know that I could look up this info for myself, but perhaps you
> already know some about this topic which would save me some time, and
> I am interested in knowing more about this question because I found
> this abstract of this paper which discusses a noncausal effect in a
> particular type of crystal:
That is intersting but out of my area of speculation. Narrow
containement in passive and active lattices will embrace a wealth of
elegant phenomena - some of them useful. My interest is circumscribed
by a calculated extremal geometric parity test of the Equivalence
Principle. I wish to pursue the sharp end of an icepick rather than
the face of a hammer.
--
Uncle Al
http://www.mazepath.com/uncleal/qz.pdf
http://www.mazepath.com/uncleal/eotvos.htm
(The parity Eotvos experiment is queued)
Charlie Stromeyer Jr.
Jun2-04, 03:56 AM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>\ncstromey@hotmail.com (Charlie Stromeyer Jr.) wrote in message news:\n\n> (Btw, there may be some serious theoretical problems with coframe or\n> teleparallel theories of gravity and I will soon post some references\n> to papers which examine these problems. [...]\n\nActually, the problems I were aware of are from papers written during\nthe 1980s which discuss the Cauchy problem and the problem of\npotentially non-physical states for teleparallel theories of gravity.\n\nHowever, there are newer papers which may change this view. Paper [1]\ndiscusses possible reasons not to favor theories of gravity with\ntorsion, whereas papers [2] imply that teleparallel gravity can be\nformulated such that there is no non-trivial difference with GTR.\n\n\n[1] http://arxiv.org/abs/gr-qc/0103029\n\n[2] http://arxiv.org/abs/gr-qc/0403101\n\nhttp://arxiv.org/abs/gr-qc/0403074\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>cstromey@hotmail.com (Charlie Stromeyer Jr.) wrote in message news:
> (Btw, there may be some serious theoretical problems with coframe or
> teleparallel theories of gravity and I will soon post some references
> to papers which examine these problems. [...]
Actually, the problems I were aware of are from papers written during
the 1980s which discuss the Cauchy problem and the problem of
potentially non-physical states for teleparallel theories of gravity.
However, there are newer papers which may change this view. Paper [1]
discusses possible reasons not to favor theories of gravity with
torsion, whereas papers [2] imply that teleparallel gravity can be
formulated such that there is no non-trivial difference with GTR.
[1] http://arxiv.org/abs/http://www.arxiv.org/abs/gr-qc/0103029
[2] http://arxiv.org/abs/http://www.arxiv.org/abs/gr-qc/0403101
http://arxiv.org/abs/http://www.arxiv.org/abs/gr-qc/0403074
Urs Schreiber
Jun2-04, 05:56 AM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>\n"Uncle Al" <UncleAl0@hate.spam.net> schrieb im Newsbeitrag\nnews:40BCA941.C25EFFF9@hate.spam.net. ..\n\n> The primary\n> question still remains unanswered: Do calculated extremal parity test\n> masses (e.g., space group P3(1)21 vs P3(2)21 alpha-quartz) fall\n> differently?\n\nOne would not expect any dependence on the shape of a molecule or crystal.\nThat would be very strange whether we come from a "metric theory" of\ngravity or not.\n\nWhat one might reasonably look for is dependence on\nelementary spin, because for instance torsion terms would couple to spin. Is\nthat what you are trying to do?\n\nAs you probably know, the "EotWash" experiment\n\nhttp://www.npl.washington.edu/eotwash/index.html\n\nis doing, among other things, just that:\n\nhttp://www.npl.washington.edu/eotwash/spin1.html ,\n\nnamely dropping electron-spin polarized bodies onto attractors with no\nmagnetic field.\n\n\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>"Uncle Al" <UncleAl0@hate.spam.net> schrieb im Newsbeitrag
news:40BCA941.C25EFFF9@hate.spam.net...
> The primary
> question still remains unanswered: Do calculated extremal parity test
> masses (e.g., space group P3(1)21 vs P3(2)21 \alpha-quartz) fall
> differently?
One would not expect any dependence on the shape of a molecule or crystal.
That would be very strange whether we come from a "metric theory" of
gravity or not.
What one might reasonably look for is dependence on
elementary spin, because for instance torsion terms would couple to spin. Is
that what you are trying to do?
As you probably know, the "EotWash" experiment
http://www.npl.washington.edu/eotwash/index.html
is doing, among other things, just that:
http://www.npl.washington.edu/eotwash/spin1.html ,
namely dropping electron-spin polarized bodies onto attractors with no
magnetic field.
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>\n\n\n\n"Urs Schreiber" <Urs.Schreiber@uni-essen.de> wrote in message news:<40bdb255\\$1@news.sentex.net>...\n> "Uncle Al" <UncleAl0@hate.spam.net> schrieb im Newsbeitrag\n> news:40BCA941.C25EFFF9@hate.spam.net...\n>\n> > The primary\n> > question still remains unanswered: Do calculated extremal parity test\n> > masses (e.g., space group P3(1)21 vs P3(2)21 alpha-quartz) fall\n> > differently?\n>\n> One would not expect any dependence on the shape of a molecule or crystal.\n> That would be very strange whether we come from a "metric theory" of\n> gravity or not.\n>\n> What one might reasonably look for is dependence on\n> elementary spin, because for instance torsion terms would couple to spin. Is\n> that what you are trying to do?\n\nI think Al is asserting that spiral staircases fall differently than\ngood ole\' straight staircases.\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>"Urs Schreiber" <Urs.Schreiber@uni-essen.de> wrote in message news:<40bdb255$1@news.sentex.net>...
> "Uncle Al" <UncleAl0@hate.spam.net> schrieb im Newsbeitrag
> news:40BCA941.C25EFFF9@hate.spam.net...
>
> > The primary
> > question still remains unanswered: Do calculated extremal parity test
> > masses (e.g., space group P3(1)21 vs P3(2)21 \alpha-quartz) fall
> > differently?
>
> One would not expect any dependence on the shape of a molecule or crystal.
> That would be very strange whether we come from a "metric theory" of
> gravity or not.
>
> What one might reasonably look for is dependence on
> elementary spin, because for instance torsion terms would couple to spin. Is
> that what you are trying to do?
I think Al is asserting that spiral staircases fall differently than
good ole' straight staircases.
Urs Schreiber
Jun2-04, 08:49 AM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>"ksh95" <ksh95@yahoo.com> schrieb im Newsbeitrag\nnews:38a3ceaf.0406020519.6aec9c7@post ing.google.com...\n\n> I think Al is asserting that spiral staircases fall differently than\n> good ole\' straight staircases.\n\nThis was discussed here years ago already, but since it comes up repeatedly\nit might be worth reemphasizing it:\n\nIf left-handed screws fell differently than right-handed screws this would\nbe a rather weird violation of locality on scales far, far away (even\nassuming that the screws are of melecular size) from any scales on which we\nmight speculate about non-local effects due to some theory of quantum\ngravity or something similar.\n\nThis has nothing to do with what flavor of gravitational theory one is\nusing. The Einstein-Hilbert action, the Palatini action, teleparallel\nformulations, theories of torsion gravity, etc are all local. Their\nequations of motion pertain to every point of spacetime seperately, e.g.\n\nG(x) = T(x) for all x in your manifold\n\nThere are indeed some non-local effects in theories of non-commuative fields\nand in effective field theories of strings, for instance, but\n\n1) This non-locality is expected to be at roughly the Planck scale.\n\n2) Even if it were of the scale of Angstroms (which it is not!), it is\npretty inconceivable how it could scan space in such a way so as to\ndetermine the handedness of macroscopic objects and pull them to the ground\naccording to that result.\n\n\nHence it is wrong to say that theory is undecided about the result\nof the "Parity-Eotvos" experiment (if, as you say, this concerns macroscopic\nhandedness instead of intrinsic fundamental spin). If such an experiment\nyielded a non-null result physics as we know it would be completely\noverthrown.\n\nOn the other hand, I would be interested in learning more about experiments\nthat might check for _torsion_ and hence an EP violation of stuff carrying\nelementary spin:\n\nhttp://golem.ph.utexas.edu/string/archives/000310.html .\n\nBTW, in the context of a current sci.physics.strings thread\n\nhttp://groups.google.de/groups?selm=c9agts%24qgm%2403%241-100000%40news.t-online.com\n\nI have taken the time to collect some links to experiments in the spirit of\nUncle Al\'s experiments that try to discover "new physics" without using\nhigh-energy particle accelerators. (There seems to be a problem with the\nnewsserver at Harvard and the post does not seem to have propagated to other\nnewsservers at the time I am writing this.):\n\nHere is a set of slides by Pisin Chen from SLAC discussing some implications\nof possible astrophysical observations for new physics:\n\nhttp://www-conf.slac.stanford.edu/orion/PAPERS/A09.PDF\n\nand\n\nhttp://www.aapps.org/archive/bulletin/vol13/13_1/13_1_p03p10.pdf\n\n\nPeople are looking in particular at the following effects:\n\n1) Ultra High Energy Cosmic Rays\n2) Lorentz violation on small scales\n3) Detection of dark matter\n4) Search for additional spatial dimensions and violations of the\nequivalence\nprinciple\n5) Spacetime granularity\n\n\nI\'ll give some links and comments for all these 5 points (but this is of\ncourse far from being a comprehensive review):\n\n1) Ultra High Energy Cosmic Rays should on theoretical grounds be cut off at\n5x10^19 eV, the so-called Greisen-Zatzepin-Kuzmin (GZK) limit, due to the\nabsorbtion of highly energetic rays by the cosmic microwave background:\n\nhttp://encyclopedia.thefreedictionary.com/GZK%20limit .\n\nBut at least one experiment has claimed to have seen particles boyond the\nGZK\nlimit.\n\nRecently Edward Witten commented on this experiment in the thread\n\nhttp://groups.google.de/groups?selm=33023f5e.0405111526.6a07f7d0-100000%40posting.google.com\n\nwhere he said:\n>>>\nalistair <alistair@goforit64.fsnet.co.uk> wrote in message\nnews:<861c1b21.0404291048.2658d8c4-100000@posting.google.com>...\n\n> What do the string theories have to say about something like the GZK\n> paradox where ultra high energy cosmic ray protons reach the Earth when\n> they should have been absorbed by the cosmic microwave background?\n\nIt is not clear at the moment that there is anything to explain.\nOne of the two main experimental groups (AGASA) reported\nas of over a year ago that their high energy data are in accord\nwith the expected GZK cutoff. The other group continues\nto report a discrepancy. We\'ll see what happens as data improve.\nEdward Witten\n<<<\n\n\n2) People are apparently looking for violation of Lorentz invariance at\nsmall\nscales/large energies.\n\nhttp://qom.physik.hu-berlin.de/prl_91_020401_2003.pdf\nhttp://cfa-www.harvard.edu/Walsworth/Activities/posters/lliposter.pdf\n\nFrom some theories of quantum gravity one might expect such effects,\nprobably\nnot from string theory.\n\n\n\n3) Nature of dark matter.\n\nSeveral people are trying to determine the presence and maybe the nature of\ndark matter.\n\nFor instance the DAMA collaboration\n\nhttp://www.lngs.infn.it/lngs/htexts/dama/dama39.html\n\nand the UK Dark Matter collaboration\n\nhttp://hepwww.rl.ac.uk//UKDMC/ukdmc.html\n\nas briefly summarized in this message:\n\nhttp://groups.google.de/groups?selm=b848qo%24epr%241%40glue.ucr.edu\n\nOf course the true nature of dark matter may be a very important clue for\nhow\nthe true theory of quantum gravity looks like, but current experiments are\nof\ncourse very far from saying anything about this.\n\n\n\n4) Search for additional spatial dimenions and violations of the equivalence\nprinciple\n\nThere are potentially very interesting high-precision measurements of the\nequivalence principle, most notably by the "EotWash" group\n\nhttp://www.npl.washington.edu/eotwash/ .\n\nVariation of the usual 1/r^2 force law of gravity on small scales could be\nrelated to extra dimensions and or torsion, for instance.\n\nBTW, what does string theory say about phenomenogically observable torsion?\nThe Kalb-Ramond field enters the background equations of motion at the same\norder (lowest order in \\alpha\') as the Einstein-Hilber term, and a\nnon-vanishing B-field corresponds to a torsion effect with torsion equal to\n\\pm dB. If we say that string theory "predicts gravity" shouldn\'t we also\nsay\nthat it predicts torsion?\n\nI have a brief note and some literature on this question at the String\nCoffee\nTable:\n\nhttp://golem.ph.utexas.edu/string/archives/000310.html\n\n\n\n\n5) Spacetime granularity\n\nFrom quantum gravity some people expect that on extremely small scales\nspacetime will show some sort of foamy structure, maybe being topologically\nnon-trivial. An old idea by Percival and collaborators is that atom\ninterferometry, e.g. the 2-slit experiment with heavy stuff such as\nBuckminster Fullerenes (Nature Vol. 401, No. 6754, p. 680 (1999).) as done\nby Zeilinger\'s group (http://www.edge.org/3rd_culture/bios/zeilinger.html), may\nbe sensitive to such a spacetime grabularity.\n\nI had mentioned that in the past from time to time\n\nhttp://groups.google.de/groups?selm=9a4m0g%24bvq1%40rs04.hrz.uni-essen.de\nhttp://groups.google.de/groups?selm=3E5A1BAC.F2755C1B%40uni-essen.de\n\ngiving some references.\n\nI am not sure what string theory really says about "quantum spacetime foam"\nat small scales.\n\nWhen we discussed Smolin\'s paper http://arxiv.org/abs/hep-th/0303185 it was\nargued that string theory (on Minkowski space, say) predicts smooth\nspacetime down to all scales. I argued in\n\nhttp://groups.google.de/groups?selm=3E64A7EC.D4DC1E00%40uni-essen.de\nhttp://groups.google.de/groups?selm=3E7B059B.87CC7802%40uni-essen.de\n\nbased on the discussion in\n\nFedele Lizzi anmd Richard Szabo,\nDuality Symmetries and Noncommutative Geometry of String Spacetimes,\nhep-th/9707202\n\nthat this is not quite correct, since as you try to probe the smooth\nbackground with highly energetic strings you will eventually see stringy\neffects and not be able to resolve the smoothness of the classical\nbackground\nat all, so that effectively it is not smooth on small scales.\n\nSo might stringy physics effect the phase of atoms/molecues used in matter\ninterferometry ever so slightly?\n\n\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>"ksh95" <ksh95@yahoo.com> schrieb im Newsbeitrag
news:38a3ceaf.0406020519.6aec9c7@posting.google.co m...
> I think Al is asserting that spiral staircases fall differently than
> good ole' straight staircases.
This was discussed here years ago already, but since it comes up repeatedly
it might be worth reemphasizing it:
If left-handed screws fell differently than right-handed screws this would
be a rather weird violation of locality on scales far, far away (even
assuming that the screws are of melecular size) from any scales on which we
might speculate about non-local effects due to some theory of quantum
gravity or something similar.
This has nothing to do with what flavor of gravitational theory one is
using. The Einstein-Hilbert action, the Palatini action, teleparallel
formulations, theories of torsion gravity, etc are all local. Their
equations of motion pertain to every point of spacetime seperately, e.g.
G(x) = T(x) for all x in your manifold
There are indeed some non-local effects in theories of non-commuative fields
and in effective field theories of strings, for instance, but
1) This non-locality is expected to be at roughly the Planck scale.
2) Even if it were of the scale of Angstroms (which it is not!), it is
pretty inconceivable how it could scan space in such a way so as to
determine the handedness of macroscopic objects and pull them to the ground
according to that result.
Hence it is wrong to say that theory is undecided about the result
of the "Parity-Eotvos" experiment (if, as you say, this concerns macroscopic
handedness instead of intrinsic fundamental spin). If such an experiment
yielded a non-null result physics as we know it would be completely
overthrown.
On the other hand, I would be interested in learning more about experiments
that might check for _torsion_ and hence an EP violation of stuff carrying
elementary spin:
http://golem.ph.utexas.edu/string/archives/000310.html .
BTW, in the context of a current sci.physics.strings thread
http://groups.google.de/groups?selm=c9agts%24qgm%2403%241-100000%40news.t-online.com
I have taken the time to collect some links to experiments in the spirit of
Uncle Al's experiments that try to discover "new physics" without using
high-energy particle accelerators. (There seems to be a problem with the
newsserver at Harvard and the post does not seem to have propagated to other
newsservers at the time I am writing this.):
Here is a set of slides by Pisin Chen from SLAC discussing some implications
of possible astrophysical observations for new physics:
http://www-conf.slac.stanford.edu/orion/PAPERS/A09.PDF
and
http://www.aapps.org/archive/bulletin/vol13/13_1/13_1_p03p10.pdf
People are looking in particular at the following effects:
1) Ultra High Energy Cosmic Rays
2) Lorentz violation on small scales
3) Detection of dark matter
4) Search for additional spatial dimensions and violations of the
equivalence
principle
5) Spacetime granularity
I'll give some links and comments for all these 5 points (but this is of
course far from being a comprehensive review):
1) Ultra High Energy Cosmic Rays should on theoretical grounds be cut off at
5x10^19 eV, the so-called Greisen-Zatzepin-Kuzmin (GZK) limit, due to the
absorbtion of highly energetic rays by the cosmic microwave background:
http://encyclopedia.thefreedictionary.com/GZK%20limit .
But at least one experiment has claimed to have seen particles boyond the
GZK
limit.
Recently Edward Witten commented on this experiment in the thread
http://groups.google.de/groups?selm=33023f5e.0405111526.6a07f7d0-100000%40posting.google.com
where he said:
>>>
alistair <alistair@goforit64.fsnet.co.uk> wrote in message
news:<861c1b21.0404291048.2658d8c4-100000@posting.google.com>...
> What do the string theories have to say about something like the GZK
> paradox where ultra high energy cosmic ray protons reach the Earth when
> they should have been absorbed by the cosmic microwave background?
It is not clear at the moment that there is anything to explain.
One of the two main experimental groups (AGASA) reported
as of over a year ago that their high energy data are in accord
with the expected GZK cutoff. The other group continues
to report a discrepancy. We'll see what happens as data improve.
Edward Witten
<<<
2) People are apparently looking for violation of Lorentz invariance at
small
scales/large energies.
http://qom.physik.hu-berlin.de/prl_91_020401_2003.pdf
http://cfa-www.harvard.edu/Walsworth/Activities/posters/lliposter.pdf
From some theories of quantum gravity one might expect such effects,
probably
not from string theory.
3) Nature of dark matter.
Several people are trying to determine the presence and maybe the nature of
dark matter.
For instance the DAMA collaboration
http://www.lngs.infn.it/lngs/htexts/dama/dama39.html
and the UK Dark Matter collaboration
http://hepwww.rl.ac.uk//UKDMC/ukdmc.html
as briefly summarized in this message:
http://groups.google.de/groups?selm=b848qo%24epr%241%40glue.ucr.edu
Of course the true nature of dark matter may be a very important clue for
how
the true theory of quantum gravity looks like, but current experiments are
of
course very far from saying anything about this.
4) Search for additional spatial dimenions and violations of the equivalence
principle
There are potentially very interesting high-precision measurements of the
equivalence principle, most notably by the "EotWash" group
http://www.npl.washington.edu/eotwash/ .
Variation of the usual 1/r^2 force law of gravity on small scales could be
related to extra dimensions and or torsion, for instance.
BTW, what does string theory say about phenomenogically observable torsion?
The Kalb-Ramond field enters the background equations of motion at the same
order (lowest order in \alpha') as the Einstein-Hilber term, and a
non-vanishing B-field corresponds to a torsion effect with torsion equal to
\pm dB. If we say that string theory "predicts gravity" shouldn't we also
say
that it predicts torsion?
I have a brief note and some literature on this question at the String
Coffee
Table:
http://golem.ph.utexas.edu/string/archives/000310.html
5) Spacetime granularity
From quantum gravity some people expect that on extremely small scales
spacetime will show some sort of foamy structure, maybe being topologically
non-trivial. An old idea by Percival and collaborators is that atom
interferometry, e.g. the 2-slit experiment with heavy stuff such as
Buckminster Fullerenes (Nature Vol. 401, No. 6754, p. 680 (1999).) as done
by Zeilinger's group (http://www.edge.org/3rd_culture/bios/zeilinger.html), may
be sensitive to such a spacetime grabularity.
I had mentioned that in the past from time to time
http://groups.google.de/groups?selm=9a4m0g%24bvq1%40rs04.hrz.uni-essen.de
http://groups.google.de/groups?selm=3E5A1BAC.F2755C1B%40uni-essen.de
giving some references.
I am not sure what string theory really says about "quantum spacetime foam"
at small scales.
When we discussed Smolin's paper http://arxiv.org/abs/http://www.arxiv.org/abs/hep-th/0303185 it was
argued that string theory (on Minkowski space, say) predicts smooth
spacetime down to all scales. I argued in
http://groups.google.de/groups?selm=3E64A7EC.D4DC1E00%40uni-essen.de
http://groups.google.de/groups?selm=3E7B059B.87CC7802%40uni-essen.de
based on the discussion in
Fedele Lizzi anmd Richard Szabo,
Duality Symmetries and Noncommutative Geometry of String Spacetimes,
http://www.arxiv.org/abs/hep-th/9707202
that this is not quite correct, since as you try to probe the smooth
background with highly energetic strings you will eventually see stringy
effects and not be able to resolve the smoothness of the classical
background
at all, so that effectively it is not smooth on small scales.
So might stringy physics effect the phase of atoms/molecues used in matter
interferometry ever so slightly?
Michael Varney
Jun2-04, 01:28 PM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>\n\n"Urs Schreiber" <Urs.Schreiber@uni-essen.de> wrote in message\nnews:40bddad5\\$1@news.sentex.net...\n<SN IP>\n> 4) Search for additional spatial dimenions and violations of the\nequivalence\n> principle\n>\n> There are potentially very interesting high-precision measurements of the\n> equivalence principle, most notably by the "EotWash" group\n\nFeh.\nhttp://www.phys.lsu.edu/mog/mog22/node9.html\nhttp://www.nature.com/nature/links/030227/030227-6.html\nhttp://www.colorado.edu/physics/Web/index.html\nhttp://arxiv.org/abs/hep-ph/0210004\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>"Urs Schreiber" <Urs.Schreiber@uni-essen.de> wrote in message
news:40bddad5$1@news.sentex.net...
<SNIP>
> 4) Search for additional spatial dimenions and violations of the
equivalence
> principle
>
> There are potentially very interesting high-precision measurements of the
> equivalence principle, most notably by the "EotWash" group
Feh.
http://www.phys.lsu.edu/mog/mog22/node9.html
http://www.nature.com/nature/links/030227/030227-6.html
http://www.colorado.edu/physics/Web/index.html
http://arxiv.org/abs/http://www.arxiv.org/abs/hep-ph/0210004
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>\n"Urs Schreiber" <Urs.Schreiber@uni-essen.de> wrote in message news:<40bddad5\n> If such an experiment\n> yielded a non-null result physics as we know it would be completely\n> overthrown.\n\nThat\'s a pretty strong statement. I agree a, non-null result would\nimply something other than what Al thinks it would, but I\'m not sure\nphysics would be completely overthrown. A non-null result would\nsuggest some non-local gravitational effects (at such huge length\nscales that would indeed be troubling!!!), but QM is non-local,\nCondensed matter is non-local......who knows? There\'s a chance that a\nnon-null result would just highlight the need for a workable theory of\nquantum gravity.\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>"Urs Schreiber" <Urs.Schreiber@uni-essen.de> wrote in message news:<40bddad5
> If such an experiment
> yielded a non-null result physics as we know it would be completely
> overthrown.
That's a pretty strong statement. I agree a, non-null result would
imply something other than what Al thinks it would, but I'm not sure
physics would be completely overthrown. A non-null result would
suggest some non-local gravitational effects (at such huge length
scales that would indeed be troubling!!!), but QM is non-local,
Condensed matter is non-local......who knows? There's a chance that a
non-null result would just highlight the need for a workable theory of
quantum gravity.
Uncle Al
Jun4-04, 02:48 PM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>Urs Schreiber wrote:\n>\n> "Uncle Al" <UncleAl0@hate.spam.net> schrieb im Newsbeitrag\n> news:40BCA941.C25EFFF9@hate.spam.net...\n>\n> > The primary\n> > question still remains unanswered: Do calculated extremal parity test\n> > masses (e.g., space group P3(1)21 vs P3(2)21 alpha-quartz) fall\n> > differently?\n>\n> One would not expect any dependence on the shape of a molecule or crystal.\n> That would be very strange whether we come from a "metric theory" of\n> gravity or not.\n>\n> What one might reasonably look for is dependence on\n> elementary spin, because for instance torsion terms would couple to spin. Is\n> that what you are trying to do?\n>\n> As you probably know, the "EotWash" experiment\n>\n> http://www.npl.washington.edu/eotwash/index.html\n>\n> is doing, among other things, just that:\n>\n> http://www.npl.washington.edu/eotwash/spin1.html ,\n>\n> namely dropping electron-spin polarized bodies onto attractors with no\n> magnetic field.\n\nA non-null parity Eotvos experiment anomaly as currently modeled is\nexquisitely sensitive to the shape of the test mass. An Eotvos\nbalance minimzes tidal forces (enforces locality) by using test masses\nwith equal inertial moments (and the rotor overall to three orders of\nmoments). That is also the requirment for maximum parity anomaly. It\nis easy to repeat the run using ellipsoidal or other deformed test\nmasses of the same mass, composition, and space group. Contrary to\nthe expectations of GR, the net output should then decrease. It is\ntrivally testable.\n\nEotWash *is* our collaborator for the parity Eotvos experiment. If\ngravitation is metric then it is symmetric to parity transformation\n(tensors only) and test mass geometry is inert. If gravitation is\naffine with a gravitation stress-energy pseudotensor, then\nenantiomorphic space group P3(1)21 vs. P3(2)21 alpha-quartz single\ncrystal balls will NOT fall identically because gravitation is\nanti-symmetric to parity transformation.\n\nOne of the parity test masses will fit into spacetime differently from\nthan the other and all achiral matter - a left foot in a right shoe.\nSince the balls are compositionally and macroscopically utterly\nidentical, there is no wiggle room to otherwise rationalize an Eotvos\nbalance non-null output. Composition Equivalence Principle tests are\nconstrained to less than 0.5 part-per-trillion difference/average\nanomaly by direct observation, plus the Nordtvedt effect and lunar\nlaser ranging vs. Earth/moon diffential compositions and gravitation\nbinding energies.\n\nAllowed EP anomaly for a parity Eotvos experiment is 3\nparts-per-trillion free on board. There are *zero* constraints of any\nkind in any venue, particle physics to cosmology, empirical or\ntheoretical, at 3 ppt. Around 10 ppt thermodynamics demands facile\ndetectablity in chemical calorimetry - if somebody ever looked. The\nEotWash II rotor has 1-sigma detection at 0.5 ppt, the EotWash III\nrotor at 0.1 ppt. Those levels require a 3-month continuous run. 3\nppt anomaly would be 1-sigma above noise in 24 hours. A positive\nresult would be unambiguous and reproducible at will.\n\nA non-null output would be followed by two hemi-parity Eotvos\nexperiments, single crystal P3(1)21 or P3(2)21 alpha-quartz balls\nagainst amorphous fused silica balls. Then other P3(1) vs. P3(2);\nP3(1)12 vs. P3(2)12; and P3(1)21 vs. P3(2)21 single crystal test\nmasses chosen by Petitjean\'s maximal CHI (quantitative parity\ndivergence) evaluation. Then less good test masses (e.g., organics in\nthose space groups), then merely chiral (which should be inert) single\ncrystal test masses, etc.\n\nCHI is a continuous function of nuclear coordinates only - independent\nof translation, scale, and size. However, CHI of a crystal lattice\nasymptotes to maximal CHI=1 with radius and inversely with lattice\nvolume/atom. Good and poor examples exist. CHI grows with\naggregation - single macroscopic forms like screws are NOT parity test\nmasses. You want 10^21 unit cells all pulling together.\n\nCHI depends on the moments of inertia of the body (maximizes when all\nare identical) and the binary products of the sums of the paired\ninertial products for massed points within the body (maximizes when\nall summed binary products are zero)\n\nSum_i (I_Xi*I_Yi) = 0\nSum_i (I_Xi*I_Zi) = 0\nSum_i (I_Yi*I_Zi) = 0\n\nThe smallest chiral aggregation is four points (a point group T\ndistorted tetrahedron), five in chemistry (central atom to bind the\nfour peripheral). The smallest CHI=1 aggregation we have found is 20\npoints, 21 if you want a non-planar graph by Kuratowski\'s theorem\n([5.5]chiralane). We have constructed molecules (sets of points) with\nall three inertial moments equal and CHI=0 (pentars).\n\nIf the first parity Eotvos experiment gives non-null output, there is\na tremendous volume of physics to be explored. Theory can play\ncatch-up as empirical results roll in.\n\n--\nUncle Al\nhttp://www.mazepath.com/uncleal/qz.pdf\nhttp://www.mazepath.com/uncleal/eotvos.htm\n(The parity Eotvos experiment is queued)\n\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>Urs Schreiber wrote:
>
> "Uncle Al" <UncleAl0@hate.spam.net> schrieb im Newsbeitrag
> news:40BCA941.C25EFFF9@hate.spam.net...
>
> > The primary
> > question still remains unanswered: Do calculated extremal parity test
> > masses (e.g., space group P3(1)21 vs P3(2)21 \alpha-quartz) fall
> > differently?
>
> One would not expect any dependence on the shape of a molecule or crystal.
> That would be very strange whether we come from a "metric theory" of
> gravity or not.
>
> What one might reasonably look for is dependence on
> elementary spin, because for instance torsion terms would couple to spin. Is
> that what you are trying to do?
>
> As you probably know, the "EotWash" experiment
>
> http://www.npl.washington.edu/eotwash/index.html
>
> is doing, among other things, just that:
>
> http://www.npl.washington.edu/eotwash/spin1.html ,
>
> namely dropping electron-spin polarized bodies onto attractors with no
> magnetic field.
A non-null parity Eotvos experiment anomaly as currently modeled is
exquisitely sensitive to the shape of the test mass. An Eotvos
balance minimzes tidal forces (enforces locality) by using test masses
with equal inertial moments (and the rotor overall to three orders of
moments). That is also the requirment for maximum parity anomaly. It
is easy to repeat the run using ellipsoidal or other deformed test
masses of the same mass, composition, and space group. Contrary to
the expectations of GR, the net output should then decrease. It is
trivally testable.
EotWash *is* our collaborator for the parity Eotvos experiment. If
gravitation is metric then it is symmetric to parity transformation
(tensors only) and test mass geometry is inert. If gravitation is
affine with a gravitation stress-energy pseudotensor, then
enantiomorphic space group P3(1)21 vs. P3(2)21 \alpha-quartz single
crystal balls will NOT fall identically because gravitation is
anti-symmetric to parity transformation.
One of the parity test masses will fit into spacetime differently from
than the other and all achiral matter - a left foot in a right shoe.
Since the balls are compositionally and macroscopically utterly
identical, there is no wiggle room to otherwise rationalize an Eotvos
balance non-null output. Composition Equivalence Principle tests are
constrained to less than .5 part-per-trillion difference/average
anomaly by direct observation, plus the Nordtvedt effect and lunar
laser ranging vs. Earth/moon diffential compositions and gravitation
binding energies.
Allowed EP anomaly for a parity Eotvos experiment is 3
parts-per-trillion free on board. There are *zero* constraints of any
kind in any venue, particle physics to cosmology, empirical or
theoretical, at 3 ppt. Around 10 ppt thermodynamics demands facile
detectablity in chemical calorimetry - if somebody ever looked. The
EotWash II rotor has 1-\sigma detection at .5 ppt, the EotWash III
rotor at .1 ppt. Those levels require a 3-month continuous run. 3
ppt anomaly would be 1-\sigma above noise in 24 hours. A positive
result would be unambiguous and reproducible at will.
A non-null output would be followed by two hemi-parity Eotvos
experiments, single crystal P3(1)21 or P3(2)21 \alpha-quartz balls
against amorphous fused silica balls. Then other P3(1) vs. P3(2);
P3(1)12 vs. P3(2)12; and P3(1)21 vs. P3(2)21 single crystal test
masses chosen by Petitjean's maximal \CHI (quantitative parity
divergence) evaluation. Then less good test masses (e.g., organics in
those space groups), then merely chiral (which should be inert) single
crystal test masses, etc.
\CHI[/itex] is a continuous function of nuclear coordinates only - independent
of translation, scale, and size. However, \CHI of a crystal lattice
asymptotes to maximal \CHI=1 with radius and inversely with lattice
volume/atom. Good and poor examples exist. \CHI grows with
aggregation - single macroscopic forms like screws are NOT parity test
masses. You want 10^21 unit cells all pulling together.
\CHI depends on the moments of inertia of the body (maximizes when all
are identical) and the binary products of the sums of the paired
inertial products for massed points within the body (maximizes when
all summed binary products are zero)
[itex]Sum_i (I_{Xi}*I_{Yi}) =Sum_i (I_{Xi}*I_{Zi}) =Sum_i (I_{Yi}*I_{Zi}) =
The smallest chiral aggregation is four points (a point group T
distorted tetrahedron), five in chemistry (central atom to bind the
four peripheral). The smallest \CHI=1 aggregation we have found is 20
points, 21 if you want a non-planar graph by Kuratowski's theorem
([5.5]chiralane). We have constructed molecules (sets of points) with
all three inertial moments equal and \CHI=0 (pentars).
If the first parity Eotvos experiment gives non-null output, there is
a tremendous volume of physics to be explored. Theory can play
catch-up as empirical results roll in.
--
Uncle Al
http://www.mazepath.com/uncleal/qz.pdf
http://www.mazepath.com/uncleal/eotvos.htm
(The parity Eotvos experiment is queued)
Uncle Al
Jun4-04, 02:49 PM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>"Charlie Stromeyer Jr." wrote:\n>\n> cstromey@hotmail.com (Charlie Stromeyer Jr.) wrote in message news:\n>\n> > (Btw, there may be some serious theoretical problems with coframe or\n> > teleparallel theories of gravity and I will soon post some references\n> > to papers which examine these problems. [...]\n>\n> Actually, the problems I were aware of are from papers written during\n> the 1980s which discuss the Cauchy problem and the problem of\n> potentially non-physical states for teleparallel theories of gravity.\n>\n> However, there are newer papers which may change this view. Paper [1]\n> discusses possible reasons not to favor theories of gravity with\n> torsion, whereas papers [2] imply that teleparallel gravity can be\n> formulated such that there is no non-trivial difference with GTR.\n>\n> [1] http://arxiv.org/abs/gr-qc/0103029\n\nAdding spacetime torsion to a theory postulating the Eqivalence\nPrinciple and spacetime curvature is contradictory to first order.\nThe EP cannot be both true and not true. His argument is not\nmeaningful for affine gravitation. His arguments in empirical support\nof metric gravitation are anomalies in theory but are not detectable\nin the real world by many orders of magnitude (e.g., EP violation by\nphysically spinning or spin-polarized test masses).\n\n"We will conclude from these arguments that torsion rather should not\nbe introduced into theory of\ngravity." Predictions of affine gravitation are indistinguishable\nfrom predictions of metric gravitation, except for the EP. The only\nEP test that could have detectable output in current technologies is\nthe parity Eotvos experiment for reasons of test mass property\namplitude (100% active mass vs 0.2% in the best composition case) and\nallowed anomaly (10x10^(-12) maximum for parity; 0.5x10^(-12) maximum\nfor composition).\nParity EP tests are remarkably good:\n\n(100/0.2)(10/0.5) =3D 10,000-fold larger signal\n\nJanusz Garecki presents an eloquent exposition *for* doing the parity\nEotvos experiment. It is 100% in the face of his analyses. One\ncannot attempt a more potent falsification than that.\n\n> [2] http://arxiv.org/abs/gr-qc/0403101\n\n"This can be understood in terms of the equivalence principle: the\ngravitational field cannot be detected at a point." Parity pair test\nmasses are the first test masses that do not default to point masses!\nParity is an emergent phenomenon. It has a non-vanishing threshhold\nvolume (0.11301 nm^3 for quartz, vs. a spherical Planck length\ndiameter ball volume of 2.21=B710^(-78) nm^3).\n\n> http://arxiv.org/abs/gr-qc/0403074\n\nA parity pair of test masses will have at least two contributors to\ntheir trajectories. There will be the Newtonian background. In\naffine/teleparallel gravitation with spacetime torsion, a\nparity-antisymmetric anomaly will be present. Affine gravitation is\nforce equations analogous to the Lorentz force equation of\nelectrodynamics. Vector products are not symmetric to coordinate\ninversion. Parity pair test masses fall differently if they pursue\nminimum energy trajectories (*not* metric geodesics).\n\nAs I have said, theory is both 100% supportive and 100% contradictory\nto parity Eotvos experiment net output. The answer, then, is to stop\nsmearing ink on paper and look at the real world answer. We\'ll know\nin less than two years, as the parity run comes to the front of the\nEotWash queue.\n\nThanks for the references!\n\n--\nUncle Al\nhttp://www.mazepath.com/uncleal/qz.pdf\nhttp://www.mazepath.com/uncleal/eotvos.htm\n(The parity Eotvos experiment is queued)\n\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>"Charlie Stromeyer Jr." wrote:
>
> cstromey@hotmail.com (Charlie Stromeyer Jr.) wrote in message news:
>
> > (Btw, there may be some serious theoretical problems with coframe or
> > teleparallel theories of gravity and I will soon post some references
> > to papers which examine these problems. [...]
>
> Actually, the problems I were aware of are from papers written during
> the 1980s which discuss the Cauchy problem and the problem of
> potentially non-physical states for teleparallel theories of gravity.
>
> However, there are newer papers which may change this view. Paper [1]
> discusses possible reasons not to favor theories of gravity with
> torsion, whereas papers [2] imply that teleparallel gravity can be
> formulated such that there is no non-trivial difference with GTR.
>
> [1] http://arxiv.org/abs/http://www.arxiv.org/abs/gr-qc/0103029
Adding spacetime torsion to a theory postulating the Eqivalence
Principle and spacetime curvature is contradictory to first order.
The EP cannot be both true and not true. His argument is not
meaningful for affine gravitation. His arguments in empirical support
of metric gravitation are anomalies in theory but are not detectable
in the real world by many orders of magnitude (e.g., EP violation by
physically spinning or spin-polarized test masses).
"We will conclude from these arguments that torsion rather should not
be introduced into theory of
gravity." Predictions of affine gravitation are indistinguishable
from predictions of metric gravitation, except for the EP. The only
EP test that could have detectable output in current technologies is
the parity Eotvos experiment for reasons of test mass property
amplitude (100% active mass vs .2% in the best composition case) and
allowed anomaly (10x10^(-12) maximum for parity; .5x10^(-12) maximum
for composition).
Parity EP tests are remarkably good:
(100/0.2)(10/0.5) =3D 10,000-fold larger signal
Janusz Garecki presents an eloquent exposition *for* doing the parity
Eotvos experiment. It is 100% in the face of his analyses. One
cannot attempt a more potent falsification than that.
> [2] http://arxiv.org/abs/http://www.arxiv.org/abs/gr-qc/0403101
"This can be understood in terms of the equivalence principle: the
gravitational field cannot be detected at a point." Parity pair test
masses are the first test masses that do not default to point masses!
Parity is an emergent phenomenon. It has a non-vanishing threshhold
volume (0.11301 nm^3 for quartz, vs. a spherical Planck length
diameter ball volume of 2.21=B710^(-78) nm^3).
> http://arxiv.org/abs/http://www.arxiv.org/abs/gr-qc/0403074
A parity pair of test masses will have at least two contributors to
their trajectories. There will be the Newtonian background. In
affine/teleparallel gravitation with spacetime torsion, a
parity-antisymmetric anomaly will be present. Affine gravitation is
force equations analogous to the Lorentz force equation of
electrodynamics. Vector products are not symmetric to coordinate
inversion. Parity pair test masses fall differently if they pursue
minimum energy trajectories (*not* metric geodesics).
As I have said, theory is both 100% supportive and 100% contradictory
to parity Eotvos experiment net output. The answer, then, is to stop
smearing ink on paper and look at the real world answer. We'll know
in less than two years, as the parity run comes to the front of the
EotWash queue.
Thanks for the references!
--
Uncle Al
http://www.mazepath.com/uncleal/qz.pdf
http://www.mazepath.com/uncleal/eotvos.htm
(The parity Eotvos experiment is queued)
Uncle Al
Jun4-04, 02:49 PM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>Urs Schreiber wrote:\n>\n> "ksh95" <ksh95@yahoo.com> schrieb im Newsbeitrag\n> news:38a3ceaf.0406020519.6aec9c7@posting.google.co m...\n>\n> > I think Al is asserting that spiral staircases fall differently than\n> > good ole\' straight staircases.\n>\n> This was discussed here years ago already, but since it comes up repeatedly\n> it might be worth reemphasizing it:\n>\n> If left-handed screws fell differently than right-handed screws this would\n> be a rather weird violation of locality on scales far, far away (even\n> assuming that the screws are of melecular size) from any scales on which we\n> might speculate about non-local effects due to some theory of quantum\n> gravity or something similar.\n>\n> This has nothing to do with what flavor of gravitational theory one is\n> using. The Einstein-Hilbert action, the Palatini action, teleparallel\n> formulations, theories of torsion gravity, etc are all local. Their\n> equations of motion pertain to every point of spacetime seperately, e.g.\n>\n> G(x) = T(x) for all x in your manifold\n>\n> There are indeed some non-local effects in theories of non-commuative fields\n> and in effective field theories of strings, for instance, but\n>\n> 1) This non-locality is expected to be at roughly the Planck scale.\n>\n> 2) Even if it were of the scale of Angstroms (which it is not!), it is\n> pretty inconceivable how it could scan space in such a way so as to\n> determine the handedness of macroscopic objects and pull them to the ground\n> according to that result.\n>\n> Hence it is wrong to say that theory is undecided about the result\n> of the "Parity-Eotvos" experiment (if, as you say, this concerns macroscopic\n> handedness instead of intrinsic fundamental spin). If such an experiment\n> yielded a non-null result physics as we know it would be completely\n> overthrown.\n[snip]\n\nNobody has ever observed calculated extremal opposite parity test\nmasses of identical chemical composition and macroscopic form\n(spherical balls) locally falling. There are no empirical constraints\nwhatsoever on them falling differently to a few parts-per-trillion\ndifference/average. Theory will follow experiment.\n\nFolks have been looking for composition Equivalence Principle\nviolations for more than 400 years, since Galileo. Plus physically\nspinning and spin-polarized test masses recently. All have been\nperfect nulls within experinental error. To say that after hundreds\nif not thousands of such examinations one should not look at *one*\nmaximal example of parity pair test masses because theory says they\ncannot possibly show an anomaly... is absurd. Theory said composition\ntest masses should diverge - or nobody would have looked. Theory is\nnot defining. Empirical observation is the only vote that counts.\n\nParity pair test masses are the *only* chance for breaking the EP.\nTheir divergent active mass concentration is 100% vs. a maximum of\n0.2% for the best net divergent composition property. Their allowed\nEP anomaly, difference/average, is thermodynamically constrained to\nabout 10 parts-per-trillion. Composition test masses cannot\nEP-diverge more than 0.5 ppt by empirical demonstration to date.\n\nhttp://www.mazepath.com/uncleal/eotvos.htm#b34\n(100/0.2)(10/0.5) = 10,000\n\nDon\'t gainsay a 10,000-fold improvement. Adelberger did a nautch\ndance to get a mere factor of five improvement in the EotWash III\nrotor.\n\n> On the other hand, I would be interested in learning more about experiments\n> that might check for _torsion_ and hence an EP violation of stuff carrying\n> elementary spin:\n\nThey are hopeless. Physically spinning objects of modest size cannot\nhave surface velocities of more than ~100 miles/sec (optically\nlevitated micron-diameter diamond balls in vacuum). That isn\'t\nanywhere near relativistic. Big lumps show null results,\n\nPhys. Rev. D 65 042005 (2002)\nPhys. Rev. D 66 022002 (2002)\n\nGravity Probe B will coincidentally be an exquisitely sensitive test\nof spinning body free fall - its 10,000 rpm fused silica gyroballs vs.\ntheir non-spinning fused silica housing. Patience.\n\nSpin-polarized test masses, zero external field ferrimagnets or\ncompensated ferromagnets, are hopeless. The largest possible active\nmass-% spin concentration achievable in any matter is 0.005% in\naligned undecatiplet manganese metal, if it were possible (only 50\nppm!). Real world numbers are small parts-per-million to -billion\nactive mass-%.\n\nhttp://www.mazepath.com/uncleal/eotvos.htm#b34\nLecture Notes in Physics 562 439 (2001)\nPhys. Rev. Lett. 70(6) 701 (1993)\nhttp://arXiv.org/abs/gr-qc/0102020\nhttp://www.npl.washington.edu/eotwash/publications/cpta.html\nhttp://www.npl.washington.edu/eotwash/publications/cpt01.pdf\nhttp://www.npl.washington.edu/eotwash/spin1.html\nPhys. Rev. D 42(4) 977 (1990)\nMod. Phy. Lett. A 16(12) 763 (2001)\nPhys. Uspekhi 39(6) 623 (1996)\n\nPolarized spin test masses are enormously too dilute to show a\ndetectable signal even if the EP were violated at full theoretical\nmaximum amplitude proposed.\n\nI am perpetually amazed at the physics community\'s insistance that all\nswans are white. If chemistry had failed at a synthesis for 400 years\nrunning and a new reaction mechanism were proposed, there would be a\npopping sound as air rushed into the voids were chemists were\nstanding. They\'d be running into the lab to try it out. As late as\nthe 1970s it was inarguable that Sn2-type of halide displacements,\nSnAr2, on an aromatic ring were fairy dust. It never happened except\nin extreme rigged circumstances.\n\nIn the 21st century palladium catalysis swallows aromatic halides (and\neven tosylates) without a burp. Proper choices of solvent and base\nallow general displacement of aromatic fluoride nice as you please.\nIt was always there, waiting for somebody to do something "stupid" and\ndiscover it. If your respected experts cannot do it, get an undergrad\nto think about it.\n\n[snip]\n\n> BTW, what does string theory say about phenomenogically observable torsion?\n> The Kalb-Ramond field enters the background equations of motion at the same\n> order (lowest order in \\alpha\') as the Einstein-Hilber term, and a\n> non-vanishing B-field corresponds to a torsion effect with torsion equal to\n> \\pm dB. If we say that string theory "predicts gravity" shouldn\'t we also\n> say\n> that it predicts torsion?\n\nModern theory predicts everything and its opposite - and with absolute\nmathematical certainty for both. We don\'t need more theory, we need\nmore empirically disproven theory.\n\n[snip]\n\n> So might stringy physics effect the phase of atoms/molecues used in matter\n> interferometry ever so slightly?\n\nNo. The best matter interferometers are good to no more than 0.1%\ndifference/average. It isn\'t nearly good enough. EP violations of\n*any* kind cannot be more than about 10 parts-per-trillion difference\naverage. If they were larger, plebeian calorimetry would scream the\nanomaly. Load up a pair of calorimeters, move one through the\nanomaly, compare simultaneous numbers,\n\n/_\\(m_eff) = /_\\E/c^2\n\n10 picograms is the mass-equivalent exotehrm of detonating 215 mg of\nTNT. Allowing for experimental slop, a 10x10^(-12) difference/average\nEP mass anomaly cannot be missed, even in heat of combustion\nexperiments that are notoriously difficult to obtain at high accuracy\nand precision. A 3x10^(-12) anomaly would nominally slip past the\nbest combustion calorimetry. A parity EP enthalpy of combustion\nexperiment is entirely doable:\n\n1) Grow small single crystals of space group P3(1)21 and P2(2)21\ntellurium. This is easily done to high quality in bulk by vapor phase\nchemical transport or solvent crystallization. Polarimetry under a\nmicroscope assigns space group. Both are cheap and easy at the\nmillimeter scale.\n\n2) Carve single crystal test masses with equal moments of inerita.\nSpheres would be best, and crystallographers have clever ways to do\nthis at 0.1 mm scales given reasonably isotropic materials. Hexagonal\nright cylinders with equal diameter and length are a better bet for\ntellurium. Still no big deal.\n\n3) Locate the experiment at 45 degrees laititude N or S. Load\npairs of combustion microcalorimeters with accurately weighed, single,\nopposite parity test masses. Align the parity pairs of calorimeters\ngeographic N-S or E-W (simultaneously at all four compass points to do\nit better. N-S and E-W results will be anti-phase). Burn runs at\ntrue 0000, 0600, 1200, and 1800 hrs local to get phase angles\' maxima\nand minimua effects between inertial planetary spin and gravitational\nplanetary orbit.\n\nTe + O2 --> TeO2 (racemic) + TeO3 (trace, and variable)\n\nplus /_\\H for the ignition wire, corrections for varying oxygen\npressure, and a host of other worries.\n\n4) Does /_\\H of combustion for single crystal Te vary with parity\nand inertial/gravitational acceleration phase angle? 20-50 full day\nruns at 3x10^(-12) relative anomaly will show signal, if any, to a\ncouple of sigma.\n\nhttp://www.mazepath.com/uncleal/eotvos.htm#b35\n(/_\\H_fusion is vastly preferable but won\'t work here. Te helical\nstructure in the crystal is largely retained in the melt over long\nperiods.)\n\nUnless there is a purely huge parity anomaly, a parity Etovos\nexperiment in quartz is the way to go. Melting quartz is no good - it\nfirst transitions to beta-quartz with variable twinning. Cooling\nbenzil is no good - second order cryogenic structural transition with\nvariable twinning.\n\n--\nUncle Al\nhttp://www.mazepath.com/uncleal/qz.pdf\nhttp://www.mazepath.com/uncleal/eotvos.htm\n(The parity Eotvos experiment is queued)\n\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>Urs Schreiber wrote:
>
> "ksh95" <ksh95@yahoo.com> schrieb im Newsbeitrag
> news:38a3ceaf.0406020519.6aec9c7@posting.google.co m...
>
> > I think Al is asserting that spiral staircases fall differently than
> > good ole' straight staircases.
>
> This was discussed here years ago already, but since it comes up repeatedly
> it might be worth reemphasizing it:
>
> If left-handed screws fell differently than right-handed screws this would
> be a rather weird violation of locality on scales far, far away (even
> assuming that the screws are of melecular size) from any scales on which we
> might speculate about non-local effects due to some theory of quantum
> gravity or something similar.
>
> This has nothing to do with what flavor of gravitational theory one is
> using. The Einstein-Hilbert action, the Palatini action, teleparallel
> formulations, theories of torsion gravity, etc are all local. Their
> equations of motion pertain to every point of spacetime seperately, e.g.
>
> G(x) = T(x) for all x in your manifold
>
> There are indeed some non-local effects in theories of non-commuative fields
> and in effective field theories of strings, for instance, but
>
> 1) This non-locality is expected to be at roughly the Planck scale.
>
> 2) Even if it were of the scale of Angstroms (which it is not!), it is
> pretty inconceivable how it could scan space in such a way so as to
> determine the handedness of macroscopic objects and pull them to the ground
> according to that result.
>
> Hence it is wrong to say that theory is undecided about the result
> of the "Parity-Eotvos" experiment (if, as you say, this concerns macroscopic
> handedness instead of intrinsic fundamental spin). If such an experiment
> yielded a non-null result physics as we know it would be completely
> overthrown.
[snip]
Nobody has ever observed calculated extremal opposite parity test
masses of identical chemical composition and macroscopic form
(spherical balls) locally falling. There are no empirical constraints
whatsoever on them falling differently to a few parts-per-trillion
difference/average. Theory will follow experiment.
Folks have been looking for composition Equivalence Principle
violations for more than 400 years, since Galileo. Plus physically
spinning and spin-polarized test masses recently. All have been
perfect nulls within experinental error. To say that after hundreds
if not thousands of such examinations one should not look at *one*
maximal example of parity pair test masses because theory says they
cannot possibly show an anomaly... is absurd. Theory said composition
test masses should diverge - or nobody would have looked. Theory is
not defining. Empirical observation is the only vote that counts.
Parity pair test masses are the *only* chance for breaking the EP.
Their divergent active mass concentration is 100% vs. a maximum of
.2% for the best net divergent composition property. Their allowed
EP anomaly, difference/average, is thermodynamically constrained to
about 10 parts-per-trillion. Composition test masses cannot
EP-diverge more than .5 ppt by empirical demonstration to date.
http://www.mazepath.com/uncleal/eotvos.htm#b34
(100/0.2)(10/0.5) = 10,000
Don't gainsay a 10,000-fold improvement. Adelberger did a nautch
dance to get a mere factor of five improvement in the EotWash III
rotor.
> On the other hand, I would be interested in learning more about experiments
> that might check for _torsion_ and hence an EP violation of stuff carrying
> elementary spin:
They are hopeless. Physically spinning objects of modest size cannot
have surface velocities of more than ~100 miles/sec (optically
levitated micron-diameter diamond balls in vacuum). That isn't
anywhere near relativistic. Big lumps show null results,
Phys. Rev. D 65 042005 (2002)
Phys. Rev. D 66 022002 (2002)
Gravity Probe B will coincidentally be an exquisitely sensitive test
of spinning body free fall - its 10,000 rpm fused silica gyroballs vs.
their non-spinning fused silica housing. Patience.
Spin-polarized test masses, zero external field ferrimagnets or
compensated ferromagnets, are hopeless. The largest possible active
mass-% spin concentration achievable in any matter is .005% in
aligned undecatiplet manganese metal, if it were possible (only 50
ppm!). Real world numbers are small parts-per-million to -billion
active mass-%.
http://www.mazepath.com/uncleal/eotvos.htm#b34
Lecture Notes in Physics 562 439 (2001)
Phys. Rev. Lett. 70(6) 701 (1993)
http://arXiv.org/abs/http://www.arxiv.org/abs/gr-qc/0102020
http://www.npl.washington.edu/eotwash/publications/cpta.html
http://www.npl.washington.edu/eotwash/publications/cpt01.pdf
http://www.npl.washington.edu/eotwash/spin1.html
Phys. Rev. D 42(4) 977 (1990)
Mod. Phy. Lett. A 16(12) 763 (2001)
Phys. Uspekhi 39(6) 623 (1996)
Polarized spin test masses are enormously too dilute to show a
detectable signal even if the EP were violated at full theoretical
maximum amplitude proposed.
I am perpetually amazed at the physics community's insistance that all
swans are white. If chemistry had failed at a synthesis for 400 years
running and a new reaction mechanism were proposed, there would be a
popping sound as air rushed into the voids were chemists were
standing. They'd be running into the lab to try it out. As late as
the 1970s it was inarguable that Sn2-type of halide displacements,
SnAr2, on an aromatic ring were fairy dust. It never happened except
in extreme rigged circumstances.
In the 21st century palladium catalysis swallows aromatic halides (and
even tosylates) without a burp. Proper choices of solvent and base
allow general displacement of aromatic fluoride nice as you please.
It was always there, waiting for somebody to do something "stupid" and
discover it. If your respected experts cannot do it, get an undergrad
to think about it.
[snip]
> BTW, what does string theory say about phenomenogically observable torsion?
> The Kalb-Ramond field enters the background equations of motion at the same
> order (lowest order in \alpha') as the Einstein-Hilber term, and a
> non-vanishing B-field corresponds to a torsion effect with torsion equal to
> \pm dB. If we say that string theory "predicts gravity" shouldn't we also
> say
> that it predicts torsion?
Modern theory predicts everything and its opposite - and with absolute
mathematical certainty for both. We don't need more theory, we need
more empirically disproven theory.
[snip]
> So might stringy physics effect the phase of atoms/molecues used in matter
> interferometry ever so slightly?
No. The best matter interferometers are good to no more than .1%
difference/average. It isn't nearly good enough. EP violations of
*any* kind cannot be more than about 10 parts-per-trillion difference
average. If they were larger, plebeian calorimetry would scream the
anomaly. Load up a pair of calorimeters, move one through the
anomaly, compare simultaneous numbers,
/_\(m_{eff}) = /_\E/c^2
10 picograms is the mass-equivalent exotehrm of detonating 215 mg of
TNT. Allowing for experimental slop, a 10x10^(-12) difference/average
EP mass anomaly cannot be missed, even in heat of combustion
experiments that are notoriously difficult to obtain at high accuracy
and precision. A 3x10^(-12) anomaly would nominally slip past the
best combustion calorimetry. A parity EP enthalpy of combustion
experiment is entirely doable:
1) Grow small single crystals of space group P3(1)21 and P2(2)21
tellurium. This is easily done to high quality in bulk by vapor phase
chemical transport or solvent crystallization. Polarimetry under a
microscope assigns space group. Both are cheap and easy at the
millimeter scale.
2) Carve single crystal test masses with equal moments of inerita.
Spheres would be best, and crystallographers have clever ways to do
this at .1 mm scales given reasonably isotropic materials. Hexagonal
right cylinders with equal diameter and length are a better bet for
tellurium. Still no big deal.
3) Locate the experiment at 45 degrees laititude N or S. Load
pairs of combustion microcalorimeters with accurately weighed, single,
opposite parity test masses. Align the parity pairs of calorimeters
geographic N-S or E-W (simultaneously at all four compass points to do
it better. N-S and E-W results will be anti-phase). Burn runs at
true 0000, 0600, 1200, and 1800 hrs local to get phase angles' maxima
and minimua effects between inertial planetary spin and gravitational
planetary orbit.
Te + O2 --> TeO2 (racemic) + TeO3 (trace, and variable)
plus /_\H for the ignition wire, corrections for varying oxygen
pressure, and a host of other worries.
4) Does /_\H of combustion for single crystal Te vary with parity
and inertial/gravitational acceleration phase angle? 20-50 full day
runs at 3x10^(-12) relative anomaly will show signal, if any, to a
couple of \sigma.
http://www.mazepath.com/uncleal/eotvos.htm#b35
(/_\H_{fusion} is vastly preferable but won't work here. Te helical
structure in the crystal is largely retained in the melt over long
periods.)
Unless there is a purely huge parity anomaly, a parity Etovos
experiment in quartz is the way to go. Melting quartz is no good - it
first transitions to \beta-quartz with variable twinning. Cooling
benzil is no good - second order cryogenic structural transition with
variable twinning.
--
Uncle Al
http://www.mazepath.com/uncleal/qz.pdf
http://www.mazepath.com/uncleal/eotvos.htm
(The parity Eotvos experiment is queued)
Alfred Einstead
Jun16-04, 05:27 PM
<jabberwocky><div class="vbmenu_control"><a href="jabberwocky:;" onClick="newWindow=window.open('','usenetCode','toolbar=no, location=no,scrollbars=yes,resizable=yes,status=no ,width=650,height=400'); newWindow.document.write('<HTML><HEAD><TITLE>Usenet ASCII</TITLE></HEAD><BODY topmargin=0 leftmargin=0 BGCOLOR=#F1F1F1><table border=0 width=625><td bgcolor=midnightblue><font color=#F1F1F1>This Usenet message\'s original ASCII form: </font></td></tr><tr><td width=449><br><br><font face=courier><UL><PRE>cstromey@hotmail.com (Charlie Stromeyer Jr.) wrote:\n> whereas paper[s] [...] imply that teleparallel gravity can be\n> formulated such that there is no non-trivial difference with GTR.\n> http://arxiv.org/abs/gr-qc/0403074\n\nThe equivalence is only local. The only teleparallel manifolds\nare Lie groups and S_7. So, you only get equivalence modulo\ncurvature concentrated in conical singularities. The classical\nexample posed by Cartan for the sphere S_2 illustrates this quite\nwell (the singular points being the north and south poles).\n\n</UL></PRE></font></td></tr></table></BODY><HTML>');"> <IMG SRC=/images/buttons/ip.gif BORDER=0 ALIGN=CENTER ALT="View this Usenet post in original ASCII form"> View this Usenet post in original ASCII form </a></div><P></jabberwocky>cstromey@hotmail.com (Charlie Stromeyer Jr.) wrote:
> whereas paper[s] [...] imply that teleparallel gravity can be
> formulated such that there is no non-trivial difference with GTR.
> http://arxiv.org/abs/http://www.arxiv.org/abs/gr-qc/0403074
The equivalence is only local. The only teleparallel manifolds
are Lie groups and S_7. So, you only get equivalence modulo
curvature concentrated in conical singularities. The classical
example posed by Cartan for the sphere S_2 illustrates this quite
well (the singular points being the north and south poles).
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