<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\ntorquemada@my-dejanews.com wrote in message http://groups.google.com/groups?&selm=746k7a%24a90%241%40nnrp1.dejanews.com\n\n"In P-violating systems: you get systems in which the direction of\nemission of a particle (a *vector*) depends directly on the spin (a\n*pseudovector*) of the parent particle - in practice it [means]\nslightly more particles fly off in the direction of the spin than in\nthe other direction."\n\nOther than extreme rarity, what\'s so unusual about a few parent\nparticles having the property of pointing to random directions and\nhaving the direction of emission of a daughter particle favoring the\ndirection it obviously inherits from its parent particle? What am I\nmissing?\n\nEugene Shubert\nhttp://www.everythingimportant.org\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>torquemada@my-dejanews.com wrote in message http://groups.google.com/groups?&selm=746k7a%24a90%241%40nnrp1.dejanews.com
"In P-violating systems: you get systems in which the direction of
emission of a particle (a *vector*) depends directly on the spin (a
*pseudovector*) of the parent particle - in practice it [means]
slightly more particles fly off in the direction of the spin than in
the other direction."
Other than extreme rarity, what's so unusual about a few parent
particles having the property of pointing to random directions and
having the direction of emission of a daughter particle favoring the
direction it obviously inherits from its parent particle? What am I
missing?
Eugene Shubert
http://www.everythingimportant.org
Uncle Al
Jul12-04, 04:44 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>\nPerfectly Innocent wrote:\n>\n> torquemada@my-dejanews.com wrote in message http://groups.google.com/groups?&selm=746k7a%24a90%241%40nnrp1.dejanews.com\n>\n>> "In P-violating systems: you get systems in which the direction of\n>> emission of a particle (a *vector*) depends directly on the spin (a\n>> *pseudovector*) of the parent particle - in practice it [means]\n>> slightly more particles fly off in the direction of the spin than in\n>> the other direction."\n>\n> Other than extreme rarity, what\'s so unusual about a few parent\n> particles having the property of pointing to random directions and\n> having the direction of emission of a daughter particle favoring the\n> direction it obviously inherits from its parent particle? What am I\n> missing?\n>\n> Eugene Shubert\n> http://www.everythingimportant.org\n\nReligion and science are orthogonal. Religion never worked out\nthe flush toilet, science has no interest in post-mortem escrow.\n\nParity violations are very big things indeed. They tell you that\nyour most general, backgroundless, fundamental tensor-based\ntheories are demonstrably wrong before you touch pencil to\npaper. Their maths are structurally wrong from the get-go.\n\nhttp://physics.nist.gov/GenInt/Parity/cover.html\nhttp://www.mazepath.com/uncleal/eotvos.htm#b21\n\nNewtonian physics and General Relativity (metric gravitation)\nsolve identically for (x,y,z) and (-x,-y,-z). Quantum mechanics\nlooked clean and neat, too, until that first link above. Things\nchanged drastically!\n\nhttp://pdg.lbl.gov/2004/tables/conlaw.pdf\nhttp://arXiv.org/abs/hep-ex/0207042\n\nAn empirical parity anomaly in gravitation would put much of\nM-theory in the wastebasket - to everybody\'s great gain.\nGravitation parity violation could violate the Equivalence\nPrinciple with parity pair test masses, empirically falsifying\nEinstein and validating Weitzenboek\n\nhttp://www.mazepath.com/uncleal/qz.pdf\nParity Eotvos experiment in quartz is queued in the Adelberger\ngroup,\nhttp://www.npl.washington.edu/eotwash/\n\nParity violation is the only apparent source, other than\nhappenstance, for biological homochirality,\n\nAngew. Chem. Int. Ed. 41(24) 4619 (2002)\nAngew. Chem. Int. Ed. 41(7) 1139 (2002)\nAngew. Chem. Int. Ed. 39(22) 4033 (2000)\nChem. Phys. Chem. 2(7) 409 (2001)\nPhys. Rev. Lett. 84(17) 3811 (2000)\n\nParity violation is a very big deal. It tells us how the\nuniverse *cannot* be built, starting with its math.\n\n--\nUncle Al\nhttp://www.mazepath.com/uncleal/\n(Toxic URL! Unsafe for children and most mammals)\nhttp://www.mazepath.com/uncleal/qz.pdf\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>Perfectly Innocent wrote:
>
> torquemada@my-dejanews.com wrote in message http://groups.google.com/groups?&selm=746k7a%24a90%241%40nnrp1.dejanews.com
>
>> "In P-violating systems: you get systems in which the direction of
>> emission of a particle (a *vector*) depends directly on the spin (a
>> *pseudovector*) of the parent particle - in practice it [means]
>> slightly more particles fly off in the direction of the spin than in
>> the other direction."
>
> Other than extreme rarity, what's so unusual about a few parent
> particles having the property of pointing to random directions and
> having the direction of emission of a daughter particle favoring the
> direction it obviously inherits from its parent particle? What am I
> missing?
>
> Eugene Shubert
> http://www.everythingimportant.org
Religion and science are orthogonal. Religion never worked out
the flush toilet, science has no interest in post-mortem escrow.
Parity violations are very big things indeed. They tell you that
your most general, backgroundless, fundamental tensor-based
theories are demonstrably wrong before you touch pencil to
paper. Their maths are structurally wrong from the get-go.
Newtonian physics and General Relativity (metric gravitation)
solve identically for (x,y,z) and (-x,-y,-z). Quantum mechanics
looked clean and neat, too, until that first link above. Things
changed drastically!
An empirical parity anomaly in gravitation would put much of
M-theory in the wastebasket - to everybody's great gain.
Gravitation parity violation could violate the Equivalence
Principle with parity pair test masses, empirically falsifying
Einstein and validating Weitzenboek
http://www.mazepath.com/uncleal/qz.pdf
Parity Eotvos experiment in quartz is queued in the Adelberger
group,
http://www.npl.washington.edu/eotwash/
Parity violation is the only apparent source, other than
happenstance, for biological homochirality,
Parity violation is a very big deal. It tells us how the
universe *cannot* be built, starting with its math.
--
Uncle Al
http://www.mazepath.com/uncleal/
(Toxic URL! Unsafe for children and most mammals)
http://www.mazepath.com/uncleal/qz.pdf
tsnyder35@insightbb.com
Jul12-04, 10:41 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>\nperfectlyInnocent@as-if.com (Perfectly Innocent) wrote in message >\n> Other than extreme rarity, what\'s so unusual about a few parent\n> particles having the property of pointing to random directions and\n> having the direction of emission of a daughter particle favoring the\n> direction it obviously inherits from its parent particle? What am I\n> missing?\n>\n\nHow can a particle \'point\' in some direction? Keep in mind that\n\'spin\' does not really point in a definite direction except by\nconvention (right hand rule). Spin is a pseudo-vector that merely\ndetermines a plane in space without any preference for one side of the\nplane over the other (so everyone always thought, anyway). The same\ngoes for magnetic moment \'vectors\' and magnetic field \'vectors\'.\n\nTom S.\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>perfectlyInnocent@as-if.com (Perfectly Innocent) wrote in message >
> Other than extreme rarity, what's so unusual about a few parent
> particles having the property of pointing to random directions and
> having the direction of emission of a daughter particle favoring the
> direction it obviously inherits from its parent particle? What am I
> missing?
>
How can a particle 'point' in some direction? Keep in mind that
'spin' does not really point in a definite direction except by
convention (right hand rule). Spin is a pseudo-vector that merely
determines a plane in space without any preference for one side of the
plane over the other (so everyone always thought, anyway). The same
goes for magnetic moment 'vectors' and magnetic field 'vectors'.
Tom S.
Perfectly Innocent
Jul13-04, 03:37 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\n\ntsnyder35@insightbb.com wrote in message news:<7a6e7454.0407120637.65341a0@posting.google.com>...\n> perfectlyInnocent@as-if.com (Perfectly Innocent) wrote in message news:<c45b45b3.0407100714.1d0a0c4f@posting.google.com>...\n> > Other than extreme rarity, what\'s so unusual about a few parent\n> > particles having the property of pointing to random directions and\n> > having the direction of emission of a daughter particle favoring the\n> > direction it obviously inherits from its parent particle? What am I\n> > missing?\n> >\n> How can a particle \'point\' in some direction? Keep in mind that\n> \'spin\' does not really point in a definite direction except by\n> convention (right hand rule). Spin is a pseudo-vector that merely\n> determines a plane in space without any preference for one side of the\n> plane over the other.\n>\n> How can a particle \'point\' in some direction?\n\nWe agree that every particle with spin determines a plane in space.\nWell, every plane uniquely determines two opposing directions. If a\nrare type of particle manifests P symmetry violations by having the\ndirection of emission of a daughter particle favoring the two opposing\ndirections symmetrically, then that\'s not terribly inconceivable, is\nit? It wouldn\'t be a violation of anything. If the favoritism is\nasymmetrical, then it\'s as if the original parent particles have a\nbuilt-in favorite orientation that\'s one level more specific than the\norientation of a plane.\n\nEugene Shubert\nhttp://www.everythingimportant.org\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>tsnyder35@insightbb.com wrote in message news:<7a6e7454.0407120637.65341a0@posting.google.com>...
> perfectlyInnocent@as-if.com (Perfectly Innocent) wrote in message news:<c45b45b3.0407100714.1d0a0c4f@posting.google.com>...
> > Other than extreme rarity, what's so unusual about a few parent
> > particles having the property of pointing to random directions and
> > having the direction of emission of a daughter particle favoring the
> > direction it obviously inherits from its parent particle? What am I
> > missing?
> >
> How can a particle 'point' in some direction? Keep in mind that
> 'spin' does not really point in a definite direction except by
> convention (right hand rule). Spin is a pseudo-vector that merely
> determines a plane in space without any preference for one side of the
> plane over the other.
>
> How can a particle 'point' in some direction?
We agree that every particle with spin determines a plane in space.
Well, every plane uniquely determines two opposing directions. If a
rare type of particle manifests P symmetry violations by having the
direction of emission of a daughter particle favoring the two opposing
directions symmetrically, then that's not terribly inconceivable, is
it? It wouldn't be a violation of anything. If the favoritism is
asymmetrical, then it's as if the original parent particles have a
built-in favorite orientation that's one level more specific than the
orientation of a plane.
Eugene Shubert
http://www.everythingimportant.org
John Baez
Aug18-04, 12:28 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>\nIn article <c45b45b3.0407121257.56e68edf@posting.google.com>,\nPerfectly Innocent <perfectlyInnocent@as-if.com> wrote:\n\n>We agree that every particle with spin determines a plane in space.\n>Well, every plane uniquely determines two opposing directions. If a\n>rare type of particle manifests P symmetry violations by having the\n>direction of emission of a daughter particle favoring the two opposing\n>directions symmetrically, then that\'s not terribly inconceivable, is\n>it?\n\nHeh, no, it\'s not inconceivable. Not anymore. In fact this sort\nof thing was first seen in 1956, and people won Nobel prizes for it -\nalthough the actual discover of the effect, Madame Chien-Shiung Wu,\ndid not:\n\nhttp://ccreweb.org/documents/parity/parity.html\n\n> It wouldn\'t be a violation of anything.\n\nYes, it would be a violation of P symmetry, the symmetry between\nleft and right - as you mention yourself! Once people thought\nthe world had this symmetry. It came as a huge shock to discover\nit didn\'t. Now we know it doesn\'t. Now it\'s not so surprising anymore.\n\nLee and Yang proposed the first experiment to detect parity\nviolation, and Wu did it. It was one of the most dramatic episodes\nin the history of physics. To quote the above site:\n\nEven before Lee and Yang\'s paper had been submitted to The Physical\nReview, Lee had discussed the experiment with Wu. At the time, Wu and\nher husband had planned a trip to Europe and the Far East. But she\nchose instead to remain and perform the experiment rather than lose the\nopportunity to other physicists who might recognize its importance.\nHowever, the experiment could not be performed with only her expertise.\nReaching the low temperatures necessary to be able to orient the cobalt\nnuclei spins required equipment few laboratories possessed. Nevertheless,\none such laboratory existed in the United States --- the Cryogenics\nPhysics Laboratory at the National Bureau of Standards in Washington.\nEarly in June of 1956, Wu sought the help of Ernest Ambler at NBS.\nAmbler accepted enthusiastically. Indeed his doctoral thesis dealt\nwith the orientation of cobalt-60 nuclei. In addition, Ralph Hudson,\nwith expertise in cryogenics, and Raymond Hayward and Dale Hoppes,\nwith experience in radiation detection, joined the team. By early\nOctober they began to assemble and test their equipment. The same\nmonth saw the publication of Lee and Yang\'s paper.\n\nThe experimental problems were enormous. Temperatures as low as one\nhundredth of a Kelvin were necessary to attain a high degree of spin\norientations for the cobalt nuclei. While such temperatures could be\nreached through a process called adiabatic demagnetization, maintaining\nthe super coldness posed quite a problem for the group. Another problem\nwas leaks in the apparatus --- the experiment required the detectors and\ncobalt sample to be placed in a vacuum. Nevertheless, after reconstructing\ntheir equipment, several trials, and the use of cotton thread, the\nexperiment finally succeeded. The day was December 27, 1956.\n\nNews of the success reached Lee and Yang. At Columbia, in those\ndays, many of the physicists would gather on Fridays for "Chinese\nlunch" under the supervision of T. D. Lee. When Lee, during such\nan occasion, announced that positive results to parity violation\nwere being given by Wu\'s group, the physicist Leon Lederman was\namong those present. Lederman, who worked with Columbia\'s cyclotron,\nrealized that he could perform an independent test of parity with\nthe cyclotron. His experiment, which involved the decay of pi and\nmu mesons, had also been proposed by Lee and Yang in their paper.\nSoon, Lederman, along with his graduate students, Marcel Weinrich,\nand Richard Garwin began their experiments. At the same time, the\ngroup under Wu was running into problems. Wanting to verify their\nresults from December 27, they repeated the experiment. Their\noriginal finding of a large asymmetry in the beta ray distribution\nwas not consistently reproducible. However, after a week of solving\nproblems with the apparatus, consistent results were obtained. And\nthe results pointed to parity violation. Much consideration was\ngiven to the question of the origin of the beta ray asymmetry ---\nwas it really an indication of the failure of parity or some result\nintrinsic to the experiment? "The group worked around the clock,\nassembling the apparatus many times, and took their breaks for a\nfew hours sleep when the superfluid helium spoiled their vacuum by\nfinding its way around the stopper at the bottom of the cryostat.\nHoppes then slept beside the apparatus, telephoning to the others as\nsoon as its temperature was low enough to begin their experiments again.\nFinally, on Januray 9th, at 2 o\'clock in the morning, Hudson brought\nout a bottle of Chateau Lafite-Rothschild, 1949, and they drank to\nthe overthrow of the law of parity". As the closing door to the question\nof parity violation in weak interactions, results from Lederman\'s\ngroup at the cyclotron came quickly. They too had obtained distinct\nevidence for parity violation. Both groups submitted their papers\ntogether to The Physical Review on January 15, 1957. On that day,\nColumbia called for a press conference.\n\nAs newspaper headlines told of a physics principle demolished,\nstartled reactions emerged from the physicists. Feynman had lost his\nbet (and fifty dollars). From Zurich, Wolfgang Pauli wrote to Victor\nWeisskopf at MIT, "Now after the first shock is over, I begin to\ncollect myself. Yes, it was very dramatic." At Columbia\'s press\nconference, Isador Rabi said, "A rather complete theoretical\nstructure has been shattered at the base and we are not sure how\nthe pieces will be put together". Credulity of parity nonconservation\nhad taken hold among physicists.\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>In article <c45b45b3.0407121257.56e68edf@posting.google.com>,
Perfectly Innocent <perfectlyInnocent@as-if.com> wrote:
>We agree that every particle with spin determines a plane in space.
>Well, every plane uniquely determines two opposing directions. If a
>rare type of particle manifests P symmetry violations by having the
>direction of emission of a daughter particle favoring the two opposing
>directions symmetrically, then that's not terribly inconceivable, is
>it?
Heh, no, it's not inconceivable. Not anymore. In fact this sort
of thing was first seen in 1956, and people won Nobel prizes for it -
although the actual discover of the effect, Madame Chien-Shiung Wu,
did not:
http://ccreweb.org/documents/parity/parity.html
> It wouldn't be a violation of anything.
Yes, it would be a violation of P symmetry, the symmetry between
left and right - as you mention yourself! Once people thought
the world had this symmetry. It came as a huge shock to discover
it didn't. Now we know it doesn't. Now it's not so surprising anymore.
Lee and Yang proposed the first experiment to detect parity
violation, and Wu did it. It was one of the most dramatic episodes
in the history of physics. To quote the above site:
Even before Lee and Yang's paper had been submitted to The Physical
Review, Lee had discussed the experiment with Wu. At the time, Wu and
her husband had planned a trip to Europe and the Far East. But she
chose instead to remain and perform the experiment rather than lose the
opportunity to other physicists who might recognize its importance.
However, the experiment could not be performed with only her expertise.
Reaching the low temperatures necessary to be able to orient the cobalt
nuclei spins required equipment few laboratories possessed. Nevertheless,
one such laboratory existed in the United States --- the Cryogenics
Physics Laboratory at the National Bureau of Standards in Washington.
Early in June of 1956, Wu sought the help of Ernest Ambler at NBS.
Ambler accepted enthusiastically. Indeed his doctoral thesis dealt
with the orientation of cobalt-60 nuclei. In addition, Ralph Hudson,
with expertise in cryogenics, and Raymond Hayward and Dale Hoppes,
with experience in radiation detection, joined the team. By early
October they began to assemble and test their equipment. The same
month saw the publication of Lee and Yang's paper.
The experimental problems were enormous. Temperatures as low as one
hundredth of a Kelvin were necessary to attain a high degree of spin
orientations for the cobalt nuclei. While such temperatures could be
reached through a process called adiabatic demagnetization, maintaining
the super coldness posed quite a problem for the group. Another problem
was leaks in the apparatus --- the experiment required the detectors and
cobalt sample to be placed in a vacuum. Nevertheless, after reconstructing
their equipment, several trials, and the use of cotton thread, the
experiment finally succeeded. The day was December 27, 1956.
News of the success reached Lee and Yang. At Columbia, in those
days, many of the physicists would gather on Fridays for "Chinese
lunch" under the supervision of T. D. Lee. When Lee, during such
an occasion, announced that positive results to parity violation
were being given by Wu's group, the physicist Leon Lederman was
among those present. Lederman, who worked with Columbia's cyclotron,
realized that he could perform an independent test of parity with
the cyclotron. His experiment, which involved the decay of \pi and
\mu mesons, had also been proposed by Lee and Yang in their paper.
Soon, Lederman, along with his graduate students, Marcel Weinrich,
and Richard Garwin began their experiments. At the same time, the
group under Wu was running into problems. Wanting to verify their
results from December 27, they repeated the experiment. Their
original finding of a large asymmetry in the \beta ray distribution
was not consistently reproducible. However, after a week of solving
problems with the apparatus, consistent results were obtained. And
the results pointed to parity violation. Much consideration was
given to the question of the origin of the \beta ray asymmetry ---
was it really an indication of the failure of parity or some result
intrinsic to the experiment? "The group worked around the clock,
assembling the apparatus many times, and took their breaks for a
few hours sleep when the superfluid helium spoiled their vacuum by
finding its way around the stopper at the bottom of the cryostat.
Hoppes then slept beside the apparatus, telephoning to the others as
soon as its temperature was low enough to begin their experiments again.
Finally, on Januray 9th, at 2 o'clock in the morning, Hudson brought
out a bottle of Chateau Lafite-Rothschild, 1949, and they drank to
the overthrow of the law of parity". As the closing door to the question
of parity violation in weak interactions, results from Lederman's
group at the cyclotron came quickly. They too had obtained distinct
evidence for parity violation. Both groups submitted their papers
together to The Physical Review on January 15, 1957. On that day,
Columbia called for a press conference.
As newspaper headlines told of a physics principle demolished,
startled reactions emerged from the physicists. Feynman had lost his
bet (and fifty dollars). From Zurich, Wolfgang Pauli wrote to Victor
Weisskopf at MIT, "Now after the first shock is over, I begin to
collect myself. Yes, it was very dramatic." At Columbia's press
conference, Isador Rabi said, "A rather complete theoretical
structure has been shattered at the base and we are not sure how
the pieces will be put together". Credulity of parity nonconservation
had taken hold among physicists.
Uncle Al
Aug18-04, 03:01 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\nJohn Baez wrote:\n>\n> In article <c45b45b3.0407121257.56e68edf@posting.google.com>,\n> Perfectly Innocent <perfectlyInnocent@as-if.com> wrote:\n>\n> >We agree that every particle with spin determines a plane in space.\n> >Well, every plane uniquely determines two opposing directions. If a\n> >rare type of particle manifests P symmetry violations by having the\n> >direction of emission of a daughter particle favoring the two opposing\n> >directions symmetrically, then that\'s not terribly inconceivable, is\n> >it?\n>\n> Heh, no, it\'s not inconceivable. Not anymore. In fact this sort\n> of thing was first seen in 1956, and people won Nobel prizes for it -\n> although the actual discover of the effect, Madame Chien-Shiung Wu,\n> did not:\n>\n> http://ccreweb.org/documents/parity/parity.html\n>\n> > It wouldn\'t be a violation of anything.\n>\n> Yes, it would be a violation of P symmetry, the symmetry between\n> left and right - as you mention yourself! Once people thought\n> the world had this symmetry. It came as a huge shock to discover\n> it didn\'t. Now we know it doesn\'t. Now it\'s not so surprising anymore.\n>\n> Lee and Yang proposed the first experiment to detect parity\n> violation, and Wu did it. It was one of the most dramatic episodes\n> in the history of physics. To quote the above site:\n[snip]\n\nhttp://www.ias.ac.in/resonance/Aug2001/pdf/Aug2001p32-43.pdf\nCo-60\n\nGiven parity transformation, polar vectors change sign and axial\nvectors (e.g., angular momentum J) do not.\nhttp://www.shef.ac.uk/physics/teaching/phy304/invariance.html\n\nIn general we see that strong fields are strongly conservative\nand weak fields admit to symmetry breakings. Physics is\nhistorically tremendously reluctant to consider any symmetry\nbreakings, then it dives into broken symmetries when they cause\nthings to reconcile (or empirical data says "pookie pookie").\nGravitation is by far the weakest field. Models of gravitation\nare tremendously parity-conserving (tensor theories). Affine\ngravitation and parts of M-theory admit to parity\nnonconservation. These are not popular parts.\n\nhttp://arxXiv.org/abs/hep-th/9811012.pdf\nhttp://www.ias.ac.in/pramana/v53/p1115/fulltext.pdf\nParity violation in affine gravitation\nhttp://www.iop.org/EJ/article/0264-9381/16/12/102/cq16012l1.html\n\nA uniqe difficulty in parity studies is the absence of a unit of\nparity or an obvious way to calculate it. How would one quantify\nwhose left hand is most left-handed? A d-dimensional set\ncontaining N=d+2 points can be continuously transformed into its\nmirror image without ever passing through an achiral\nintermediate.\n\nJ. Math. Chem. 17 185 (1995)\n\nWe thus need a function that passes from one extreme value to its\nopposite without the necessity of passing through zero\nin-between.\n\nA proposal to calculate the parity of single crystal test masses\nand perform a parity Eotvos experiment to look for gravitational\nparity violation\n\nhttp://www.mazepath.com/uncleal/qz.pdf\n\nis now queued for experiment in two physics groups, Eric\nAdleberger (solid single crystal alpha-quartz spheres) and Jun\nLuo (solid single crystal alpha-quartz cylinders).\n\nThe parity calculations for alpha-quartz are being redone at much\ndenser radius samplings,\n\nhttp://www.mazepath.com/uncleal/qzsparse.png\nPresented data, 711 points\nhttp://www.mazepath.com/uncleal/qzdense.png\nDense sampling; calculation still in progress, 15,700 points and\ngrowing\n\nIf anybody has a fast Linux box that isn\'t doing anything for a\nweek or so... organiker\'at sign\'lycos.com A fast Windows box\nwould be 40% slower for each point.\n\n--\nUncle Al\nhttp://www.mazepath.com/uncleal/\n(Toxic URL! Unsafe for children and most mammals)\nhttp://www.mazepath.com/uncleal/qz.pdf\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>John Baez wrote:
>
> In article <c45b45b3.0407121257.56e68edf@posting.google.com>,
> Perfectly Innocent <perfectlyInnocent@as-if.com> wrote:
>
> >We agree that every particle with spin determines a plane in space.
> >Well, every plane uniquely determines two opposing directions. If a
> >rare type of particle manifests P symmetry violations by having the
> >direction of emission of a daughter particle favoring the two opposing
> >directions symmetrically, then that's not terribly inconceivable, is
> >it?
>
> Heh, no, it's not inconceivable. Not anymore. In fact this sort
> of thing was first seen in 1956, and people won Nobel prizes for it -
> although the actual discover of the effect, Madame Chien-Shiung Wu,
> did not:
>
> http://ccreweb.org/documents/parity/parity.html
>
> > It wouldn't be a violation of anything.
>
> Yes, it would be a violation of P symmetry, the symmetry between
> left and right - as you mention yourself! Once people thought
> the world had this symmetry. It came as a huge shock to discover
> it didn't. Now we know it doesn't. Now it's not so surprising anymore.
>
> Lee and Yang proposed the first experiment to detect parity
> violation, and Wu did it. It was one of the most dramatic episodes
> in the history of physics. To quote the above site:
[snip]
Given parity transformation, polar vectors change sign and axial
vectors (e.g., angular momentum J) do not.
http://www.shef.ac.uk/physics/teaching/phy304/invariance.html
In general we see that strong fields are strongly conservative
and weak fields admit to symmetry breakings. Physics is
historically tremendously reluctant to consider any symmetry
breakings, then it dives into broken symmetries when they cause
things to reconcile (or empirical data says "pookie pookie").
Gravitation is by far the weakest field. Models of gravitation
are tremendously parity-conserving (tensor theories). Affine
gravitation and parts of M-theory admit to parity
nonconservation. These are not popular parts.
http://arxXiv.org/abs/http://www.arxiv.org/abs/hep-th/9811012.pdf
http://www.ias.ac.in/pramana/v53/p1115/fulltext.pdf
Parity violation in affine gravitation
http://www.iop.org/EJ/article/0264-9381/16/12/102/cq16012l1.html
A uniqe difficulty in parity studies is the absence of a unit of
parity or an obvious way to calculate it. How would one quantify
whose left hand is most left-handed? A d-dimensional set
containing N=d+2 points can be continuously transformed into its
mirror image without ever passing through an achiral
intermediate.
J. Math. Chem. 17 185 (1995)
We thus need a function that passes from one extreme value to its
opposite without the necessity of passing through zero
in-between.
A proposal to calculate the parity of single crystal test masses
and perform a parity Eotvos experiment to look for gravitational
parity violation
http://www.mazepath.com/uncleal/qz.pdf
is now queued for experiment in two physics groups, Eric
Adleberger (solid single crystal \alpha-quartz spheres) and Jun
Luo (solid single crystal \alpha-quartz cylinders).
The parity calculations for \alpha-quartz are being redone at much
denser radius samplings,
http://www.mazepath.com/uncleal/qzsparse.png
Presented data, 711 points
http://www.mazepath.com/uncleal/qzdense.png
Dense sampling; calculation still in progress, 15,700 points and
growing
If anybody has a fast Linux box that isn't doing anything for a
week or so... organiker'at sign'lycos.com A fast Windows box
would be 40% slower for each point.
--
Uncle Al
http://www.mazepath.com/uncleal/
(Toxic URL! Unsafe for children and most mammals)
http://www.mazepath.com/uncleal/qz.pdf