<?xml version="1.0" encoding="UTF-8"?><!-- generator="wordpress/2.3.1" -->
<rss version="2.0"
	xmlns:content="http://purl.org/rss/1.0/modules/content/"
	xmlns:dc="http://purl.org/dc/elements/1.1/"
	>
<channel>
	<title>Comments on: Constraints and Signatures in Particle Cosmology</title>
	<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/</link>
	<description>Random samplings from a universe of ideas.</description>
	<pubDate>Fri, 21 Nov 2008 18:28:22 +0000</pubDate>
	<generator>http://wordpress.org/?v=2.3.1</generator>
		<item>
		<title>By: Seed's Daily Zeitgeist: 6/27/2007 &#187; Chymistry</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29869</link>
		<dc:creator>Seed's Daily Zeitgeist: 6/27/2007 &#187; Chymistry</dc:creator>
		<pubDate>Mon, 16 Jul 2007 12:53:29 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29869</guid>
		<description>[...] Constraints and Signatures in Particle Cosmology Do you have a new idea about particle physics? Great! Use this checklist to be sure it jives with what we know from cosmology. [...]</description>
		<content:encoded><![CDATA[<p>[&#8230;] Constraints and Signatures in Particle Cosmology Do you have a new idea about particle physics? Great! Use this checklist to be sure it jives with what we know from cosmology. [&#8230;]</p>
]]></content:encoded>
	</item>
	<item>
		<title>By: Stefan</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29868</link>
		<dc:creator>Stefan</dc:creator>
		<pubDate>Sun, 01 Jul 2007 10:26:43 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29868</guid>
		<description>Thanks for this great overview!

Concerning the GZK cutoff: it seems to be there as predicted - seen in recent data both by HiRes (arXiv:astro-ph/0703099v1) and AUGER (arXiv:0706.2096, see Fig. 6). There will probably be more news next week from the International Cosmic Ray Conference ICRC’07 in Mexico. In the meantime, Bee at backreaction explains the GZK cutoff in detail.

It looks as if "boring" nuclear physics rules - data are consistent with interactions of cosmic ray protons with CMB photons as expected from boost invariance.</description>
		<content:encoded><![CDATA[<p>Thanks for this great overview!</p>
<p>Concerning the GZK cutoff: it seems to be there as predicted - seen in recent data both by HiRes (arXiv:astro-ph/0703099v1) and AUGER (arXiv:0706.2096, see Fig. 6). There will probably be more news next week from the International Cosmic Ray Conference ICRC’07 in Mexico. In the meantime, Bee at backreaction explains the GZK cutoff in detail.</p>
<p>It looks as if &#8220;boring&#8221; nuclear physics rules - data are consistent with interactions of cosmic ray protons with CMB photons as expected from boost invariance.</p>
]]></content:encoded>
	</item>
	<item>
		<title>By: Jim Graber</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29867</link>
		<dc:creator>Jim Graber</dc:creator>
		<pubDate>Sat, 30 Jun 2007 19:25:48 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29867</guid>
		<description>Mark, I wonder if you would like to comment on these two recent weak gravitational lensing observational results, one of which seems in line with standard dark matter expectations, and one of which seems to raise questions?

http://www.arxiv.org/PS_cache/arxiv/pdf/0705/0705.2171v1.pdf

http://www.arxiv.org/PS_cache/arxiv/pdf/0706/0706.3048v1.pdf</description>
		<content:encoded><![CDATA[<p>Mark, I wonder if you would like to comment on these two recent weak gravitational lensing observational results, one of which seems in line with standard dark matter expectations, and one of which seems to raise questions?</p>
<p><a href="http://www.arxiv.org/PS_cache/arxiv/pdf/0705/0705.2171v1.pdf" rel="nofollow">http://www.arxiv.org/PS_cache/arxiv/pdf/0705/0705.2171v1.pdf</a></p>
<p><a href="http://www.arxiv.org/PS_cache/arxiv/pdf/0706/0706.3048v1.pdf" rel="nofollow">http://www.arxiv.org/PS_cache/arxiv/pdf/0706/0706.3048v1.pdf</a></p>
]]></content:encoded>
	</item>
	<item>
		<title>By: spaceman</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29866</link>
		<dc:creator>spaceman</dc:creator>
		<pubDate>Sat, 30 Jun 2007 11:24:28 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29866</guid>
		<description>Lieu’s paper is a semi-professional version of the a dime a dozen anti-Big Bang tirades which, unfortunately, seem quite common. The paper stops short of the typical weak "what-if strategy" of these alternative cosmologies e.g. what if the dominant force in determining how matter is distributed universally is electrical rather than gravitational, what if redshift does not indicate distance, what if...what if pigs could fly and write sonnets. However, it does raise the following question: Why is there so much aversion and hostility toward Big Bang cosmology, as only a third of US citizens believe in the Big Bang and the internet is full to the brim with the Big Bang never happened blogs?</description>
		<content:encoded><![CDATA[<p>Lieu’s paper is a semi-professional version of the a dime a dozen anti-Big Bang tirades which, unfortunately, seem quite common. The paper stops short of the typical weak &#8220;what-if strategy&#8221; of these alternative cosmologies e.g. what if the dominant force in determining how matter is distributed universally is electrical rather than gravitational, what if redshift does not indicate distance, what if&#8230;what if pigs could fly and write sonnets. However, it does raise the following question: Why is there so much aversion and hostility toward Big Bang cosmology, as only a third of US citizens believe in the Big Bang and the internet is full to the brim with the Big Bang never happened blogs?</p>
]]></content:encoded>
	</item>
	<item>
		<title>By: Mark</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29865</link>
		<dc:creator>Mark</dc:creator>
		<pubDate>Fri, 29 Jun 2007 19:22:42 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29865</guid>
		<description>I’m rushing to get ready to leave on a trip so can only give a very brief answer to Paul (#33). One way in which extra dimensions are constrained by cosmology is that radiation from our brane into the extra dimensions provides another way for the 4d universe to cool (apart from the usual redshifting of photons due to the expansion). Since we have an extremely good handle on the rate of cooling as far back as nucleosynthesis, it better be that any modified cooling rate is only efficient above a few MeV or so. This puts bounds on the size and number of extra dimensions.

There are many other things, and I’ll try to post more when I get a little time.</description>
		<content:encoded><![CDATA[<p>I’m rushing to get ready to leave on a trip so can only give a very brief answer to Paul (#33). One way in which extra dimensions are constrained by cosmology is that radiation from our brane into the extra dimensions provides another way for the 4d universe to cool (apart from the usual redshifting of photons due to the expansion). Since we have an extremely good handle on the rate of cooling as far back as nucleosynthesis, it better be that any modified cooling rate is only efficient above a few MeV or so. This puts bounds on the size and number of extra dimensions.</p>
<p>There are many other things, and I’ll try to post more when I get a little time.</p>
]]></content:encoded>
	</item>
	<item>
		<title>By: Van</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29864</link>
		<dc:creator>Van</dc:creator>
		<pubDate>Fri, 29 Jun 2007 14:12:02 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29864</guid>
		<description>Nigel,
       It sounds to me like you are looking for a left-right symmetric model:

http://en.wikipedia.org/wiki/Left-right_symmetry

Regarding the rest of your post, it really doesn't make much sense to me.</description>
		<content:encoded><![CDATA[<p>Nigel,<br />
       It sounds to me like you are looking for a left-right symmetric model:</p>
<p><a href="http://en.wikipedia.org/wiki/Left-right_symmetry" rel="nofollow">http://en.wikipedia.org/wiki/Left-right_symmetry</a></p>
<p>Regarding the rest of your post, it really doesn&#8217;t make much sense to me.</p>
]]></content:encoded>
	</item>
	<item>
		<title>By: nigel</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29863</link>
		<dc:creator>nigel</dc:creator>
		<pubDate>Fri, 29 Jun 2007 09:04:54 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29863</guid>
		<description>Hi Van, glad you got my point. Thank you very much for referring to the Pati-Salam modem, SU(4) x SU(2)_L x SU(2)_R.  Yes I am interested in something that looks nearly identical, like SU(3) x SU(2)_L x SU(2)_R.  However, SU(4) x SU(2)_L x SU(2)_R is different in many ways. They chose that not due to experimental evidence or unique quantitative predictions it can make, but because it can undergo spontaneous symmetry breaking to produce &lt;i&gt;exactly&lt;/i&gt; the existing Standard Model, so that the Higgs field at low energy causes SU(4) x SU(2)_L x SU(2)_R to produce SU(3)xSU(2)xU(1).  At high energy where the symmetry is unbroken, it is a grand unification theory.

This approach has many problems both in methodology and in checking it. 1) It assumes the Standard Model is totally correct at low energies and it assumes that forces do unify at very high energy. 2) It doesn't make immediate predictions or post-dictions of the strength of gravity, cosmological effects, etc., that can validate the approach. 3) It doesn't actually seem to make any long-term checkable predictions that are useful. 4) It doesn't seem to make things simpler with regard to the Higgs field or the masses of different fundamental particles, which is the cause of most of the adjustable parameters in the existing Standard Model. 5) It doesn't seem to help resolve existing problems in physics or to point in the direction of simple mechanisms to improve understanding.  6) It doesn't get rid of U(1) at low energy, since U(1) emerges at low energy as a result of the symmetry breaking they are assuming.  7) It's a theory built on speculation instead of on empirial observations.

SU(2) does have several advantages in describing leptons as doublets: pair production produces lepton-antilepton pairs. A conversion of 100% of positrons into upquarks and 50% of electrons into downquarks in the big bang would explain the alleged lack of anti-matter in the universe: it's locked up by quark confinement in nucleons (the universe is mainly hydrogen, an electron, downqrark, and two upquarks). One simple mechanism based entirely on mainstream QFT is that the electric field of the core of a lepton is shielded by the polarization of pairs of virtual fermions around it. The virtual fermion pair production is, Schwinger showed, a result of the electric field of the electron core which extends out to about 1 fm radius where the electric field is above the threshold of 1.3*10^18 v/m required for pair-production. If at high energy in the big bang (very early times), N electrons were crowded together in a small space (against the Pauli exclusion principle), the polarization of the vacuum would be stronger, so the shielding factor due to the vacuum would be N times bigger. Thus, 3 electrons crowded together in a tiny space would still only give an overall electric charge of e; the contribution from each electron would be e/3 due to the extra shielding by the stronger polarized vacuum. This is just a simple heuristic mechanism for fractional charges. The energy conservation issue then comes to the fore: what happens to the 2/3rds of the electric charge energy (that is now being shielded by the stronger, shared vacuum polarization around the triplet)? Clearly, that energy is stopped at very short distances by the vacuum and used to produce loops of virtual particles which mediate short-range interactions. To avoid violating the Pauli exclusion principle (which would prevent a triplet of three identical quarks, since there are only two spin states available), colour charge must appear. This suggests that 'unification' of all forces doesn't occur at very high energy: the colour charge is powered by short-range vacuum loop effects and decreases towards zero when you are close enough to the particle core that there is no room for the vacuum to polarize (i.e. no space for virtual fermion pairs to move apart along the lines of the radial electric field).</description>
		<content:encoded><![CDATA[<p>Hi Van, glad you got my point. Thank you very much for referring to the Pati-Salam modem, SU(4) x SU(2)_L x SU(2)_R.  Yes I am interested in something that looks nearly identical, like SU(3) x SU(2)_L x SU(2)_R.  However, SU(4) x SU(2)_L x SU(2)_R is different in many ways. They chose that not due to experimental evidence or unique quantitative predictions it can make, but because it can undergo spontaneous symmetry breaking to produce <i>exactly</i> the existing Standard Model, so that the Higgs field at low energy causes SU(4) x SU(2)_L x SU(2)_R to produce SU(3)xSU(2)xU(1).  At high energy where the symmetry is unbroken, it is a grand unification theory.</p>
<p>This approach has many problems both in methodology and in checking it. 1) It assumes the Standard Model is totally correct at low energies and it assumes that forces do unify at very high energy. 2) It doesn&#8217;t make immediate predictions or post-dictions of the strength of gravity, cosmological effects, etc., that can validate the approach. 3) It doesn&#8217;t actually seem to make any long-term checkable predictions that are useful. 4) It doesn&#8217;t seem to make things simpler with regard to the Higgs field or the masses of different fundamental particles, which is the cause of most of the adjustable parameters in the existing Standard Model. 5) It doesn&#8217;t seem to help resolve existing problems in physics or to point in the direction of simple mechanisms to improve understanding.  6) It doesn&#8217;t get rid of U(1) at low energy, since U(1) emerges at low energy as a result of the symmetry breaking they are assuming.  7) It&#8217;s a theory built on speculation instead of on empirial observations.</p>
<p>SU(2) does have several advantages in describing leptons as doublets: pair production produces lepton-antilepton pairs. A conversion of 100% of positrons into upquarks and 50% of electrons into downquarks in the big bang would explain the alleged lack of anti-matter in the universe: it&#8217;s locked up by quark confinement in nucleons (the universe is mainly hydrogen, an electron, downqrark, and two upquarks). One simple mechanism based entirely on mainstream QFT is that the electric field of the core of a lepton is shielded by the polarization of pairs of virtual fermions around it. The virtual fermion pair production is, Schwinger showed, a result of the electric field of the electron core which extends out to about 1 fm radius where the electric field is above the threshold of 1.3*10^18 v/m required for pair-production. If at high energy in the big bang (very early times), N electrons were crowded together in a small space (against the Pauli exclusion principle), the polarization of the vacuum would be stronger, so the shielding factor due to the vacuum would be N times bigger. Thus, 3 electrons crowded together in a tiny space would still only give an overall electric charge of e; the contribution from each electron would be e/3 due to the extra shielding by the stronger polarized vacuum. This is just a simple heuristic mechanism for fractional charges. The energy conservation issue then comes to the fore: what happens to the 2/3rds of the electric charge energy (that is now being shielded by the stronger, shared vacuum polarization around the triplet)? Clearly, that energy is stopped at very short distances by the vacuum and used to produce loops of virtual particles which mediate short-range interactions. To avoid violating the Pauli exclusion principle (which would prevent a triplet of three identical quarks, since there are only two spin states available), colour charge must appear. This suggests that &#8216;unification&#8217; of all forces doesn&#8217;t occur at very high energy: the colour charge is powered by short-range vacuum loop effects and decreases towards zero when you are close enough to the particle core that there is no room for the vacuum to polarize (i.e. no space for virtual fermion pairs to move apart along the lines of the radial electric field).</p>
]]></content:encoded>
	</item>
	<item>
		<title>By: Van</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29862</link>
		<dc:creator>Van</dc:creator>
		<pubDate>Thu, 28 Jun 2007 23:14:49 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29862</guid>
		<description>Nigel,
       Regarding your ideas regarding replacing the U(1)_Y factor gauge group with an SU(2)_R group, perhaps you should have a look at Pati-Salam  and/or left-right symmetric models:  http://en.wikipedia.org/wiki/Pati-Salam_model</description>
		<content:encoded><![CDATA[<p>Nigel,<br />
       Regarding your ideas regarding replacing the U(1)_Y factor gauge group with an SU(2)_R group, perhaps you should have a look at Pati-Salam  and/or left-right symmetric models:  <a href="http://en.wikipedia.org/wiki/Pati-Salam_model" rel="nofollow">http://en.wikipedia.org/wiki/Pati-Salam_model</a></p>
]]></content:encoded>
	</item>
	<item>
		<title>By: Van</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29861</link>
		<dc:creator>Van</dc:creator>
		<pubDate>Thu, 28 Jun 2007 22:04:49 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29861</guid>
		<description>Neil,
     The helicity is the direction of the particle's spin as it moves.  You can determine the helicity by using the right hand rule:   point your thumb in the direction of motion and the direction (clockwise or counterclockwise) your fingers curl around is the helicity.  The chirality is right-handed or left-handed depending on which hand you need to use for this to work.  For a massless particle which travels at the speed of light, you can never move past it and reverse the direction of motion and thus the helicity.  However, for a massive particle you can do this so massive particles have both helicities.  Massless particles such as the photon or like the neutrino in the old days when it was thought to be massless will only have one helicity or the other.  The Standard Model neutrino (actually anti-neutrinos) are massless and purely left-handed.  The discovery that neutrinos have mass means that there exist a right-handed helicity for the neutrino as well.</description>
		<content:encoded><![CDATA[<p>Neil,<br />
     The helicity is the direction of the particle&#8217;s spin as it moves.  You can determine the helicity by using the right hand rule:   point your thumb in the direction of motion and the direction (clockwise or counterclockwise) your fingers curl around is the helicity.  The chirality is right-handed or left-handed depending on which hand you need to use for this to work.  For a massless particle which travels at the speed of light, you can never move past it and reverse the direction of motion and thus the helicity.  However, for a massive particle you can do this so massive particles have both helicities.  Massless particles such as the photon or like the neutrino in the old days when it was thought to be massless will only have one helicity or the other.  The Standard Model neutrino (actually anti-neutrinos) are massless and purely left-handed.  The discovery that neutrinos have mass means that there exist a right-handed helicity for the neutrino as well.</p>
]]></content:encoded>
	</item>
	<item>
		<title>By: Neil B.</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29860</link>
		<dc:creator>Neil B.</dc:creator>
		<pubDate>Thu, 28 Jun 2007 20:35:18 +0000</pubDate>
		<guid>http://blogs.discovermagazine.com/cosmicvariance/2007/06/26/constraints-and-signatures-in-particle-cosmology/#comment-29860</guid>
		<description>"well known anomalies in electromagnetism" - huh? I didn't think there were anomalies in "electromagnetism" as such. Do you mean odd properties of particles, that related to EM, or do you mean the problem issues like the field energy being more than particle mass below a certain radius (and therefore &lt;i&gt;not&lt;/i&gt; just a "quantum" issue!)

About chirality: it's the discussion from Diogenes (#24) in "MiniBooNE Neutrino Result - Guest Blog from Heather Ray" that I didn't get, but thanks for other background info:

&lt;i&gt;You are completely correct, and this effect is included in the theory of neutrino masses as appears in standard texts. The projection of the neutrino spin along its direction of motion is it's "helicity". There is another measure of the "handedness" of a relativistic spin one half-particle called "chirality" that is easily defined in terms of the matrices appearing in the Dirac equation, and this measure does NOT depend on the reference frame in which you observe the particle. For massless particles these measures of "handedness" agree, but for massive particles they can disagree for exactly the reason you describe, ie. by moving past the particle you can reverse it's direction of motion, hence it's apparent helicity.&lt;/i&gt;

I don't get the difference here, and which corresponds to plain "angular momentum"?</description>
		<content:encoded><![CDATA[<p>&#8220;well known anomalies in electromagnetism&#8221; - huh? I didn&#8217;t think there were anomalies in &#8220;electromagnetism&#8221; as such. Do you mean odd properties of particles, that related to EM, or do you mean the problem issues like the field energy being more than particle mass below a certain radius (and therefore <i>not</i> just a &#8220;quantum&#8221; issue!)</p>
<p>About chirality: it&#8217;s the discussion from Diogenes (#24) in &#8220;MiniBooNE Neutrino Result - Guest Blog from Heather Ray&#8221; that I didn&#8217;t get, but thanks for other background info:</p>
<p><i>You are completely correct, and this effect is included in the theory of neutrino masses as appears in standard texts. The projection of the neutrino spin along its direction of motion is it&#8217;s &#8220;helicity&#8221;. There is another measure of the &#8220;handedness&#8221; of a relativistic spin one half-particle called &#8220;chirality&#8221; that is easily defined in terms of the matrices appearing in the Dirac equation, and this measure does NOT depend on the reference frame in which you observe the particle. For massless particles these measures of &#8220;handedness&#8221; agree, but for massive particles they can disagree for exactly the reason you describe, ie. by moving past the particle you can reverse it&#8217;s direction of motion, hence it&#8217;s apparent helicity.</i></p>
<p>I don&#8217;t get the difference here, and which corresponds to plain &#8220;angular momentum&#8221;?</p>
]]></content:encoded>
	</item>
</channel>
</rss>
