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	<title>Comments on: Dark Matter: Just Fine, Thanks</title>
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	<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/</link>
	<description>Random samplings from a universe of ideas.</description>
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		<title>By: Uppsamling av fysiklänkar: mörk materia &#171; Stjärnstoft och kugghjul</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-160403</link>
		<dc:creator>Uppsamling av fysiklänkar: mörk materia &#171; Stjärnstoft och kugghjul</dc:creator>
		<pubDate>Tue, 26 Apr 2011 10:06:20 +0000</pubDate>
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		<description>[...] Dark matter just fine, thanks En artikel om vad det finns för problem med MOND (modified Newtonian dynamics) som alternativ till mörk materia. (Det här är något jag ofta får frågor om.) Framför allt: även med MOND behöver man mörk materia för en fullständig beskrivning av observationer som gjorts. [...]</description>
		<content:encoded><![CDATA[<p>[...] Dark matter just fine, thanks En artikel om vad det finns för problem med MOND (modified Newtonian dynamics) som alternativ till mörk materia. (Det här är något jag ofta får frågor om.) Framför allt: även med MOND behöver man mörk materia för en fullständig beskrivning av observationer som gjorts. [...]</p>
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		<title>By: Bob Sanders</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-157279</link>
		<dc:creator>Bob Sanders</dc:creator>
		<pubDate>Tue, 22 Mar 2011 21:46:39 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-157279</guid>
		<description>Let&#039;s forget about TeVeS or Bimond or generalized Einstein-Aether theories
or any of the complicated relativistic extensions of MOND.  Instead, consider
a minimalist definition:  MOND is an algorithm (and a very simple
algorithm) which allows one to calculate the distribution of force in an
astronomical object from the observed distribution of baryonic matter.
And, as evidenced by rotation curves, it works!  It works extremely well,
even explaining details in rotation curves which are clearly related to
corresponding details in the light or gas distribution.  This fact is remarkable,
and it constitutes a severe challenge to CDM or to any dark matter that
clusters on the scale of galaxies.   How can one image that dark matter
can reproduce this remarkable success of MOND?  To think that 
it could presupposes properties of dark matter that is totally at odds
with its perceived nature as a non-interacting (except for gravity),
non-dissipational fluid.  The dark matter fluid is very different from
the baryonic fluid;  the dm  is immune from 
influences that affect baryons:  the baryonic fluid can dissipate -- loose energy --,
it can be shocked, it can be removed by supernovae or stellar winds,
it can be swept out in collisions (e.g. the famous Bullet).  Why then should
these two fluids be so intimately connected and similarly distributed
as to subsume the existence of the MOND algorithm?  In fact, the success of
the MOND algorithm on the scale of galaxies is a falsification of CDM
or any dark matter that clusters on the scale of galaxies.  To blandly
state that dark matter exists and accounts for the observations of
galaxy kinematics is to turn a blind eye to a vast range of phenomena;
to imagine that dark matter will someday, when we have more understanding
of the complicated baryonic physics, reproduce the correspondence
of rotation curves to the distribution of baryonic matter is a
leap of faith that is more akin to religion than to science.   This goes as
well for the near perfect Tully-Fisher relation as pointed out by Stacy --
so perfect that the TF by itself implies a connection with physical
law rather than the messy details of galaxy formation.  And how
will dark matter explain the ubiquitous emergence of a0 --
as the acceleration below which the discrepancy appears in galaxies,
as the normalization of the Tully-Fisher and Faber-Jackson relations,
as the internal acceleration of near isothermal systems ranging
from globular clusters to clusters of galaxies, and, when expressed
as surface brightness, as the characteristic (Freeman) surface brightness
of galaxies.  If the putative dark matter particles are ever found
(and I doubt that they will be), then we have a lot of work ahead of us
to understand how these regularities, so neatly encapsulated by MOND,
emerge in the context of a non-interacting, dissipationless, dark matter fluid.</description>
		<content:encoded><![CDATA[<p>Let&#8217;s forget about TeVeS or Bimond or generalized Einstein-Aether theories<br />
or any of the complicated relativistic extensions of MOND.  Instead, consider<br />
a minimalist definition:  MOND is an algorithm (and a very simple<br />
algorithm) which allows one to calculate the distribution of force in an<br />
astronomical object from the observed distribution of baryonic matter.<br />
And, as evidenced by rotation curves, it works!  It works extremely well,<br />
even explaining details in rotation curves which are clearly related to<br />
corresponding details in the light or gas distribution.  This fact is remarkable,<br />
and it constitutes a severe challenge to CDM or to any dark matter that<br />
clusters on the scale of galaxies.   How can one image that dark matter<br />
can reproduce this remarkable success of MOND?  To think that<br />
it could presupposes properties of dark matter that is totally at odds<br />
with its perceived nature as a non-interacting (except for gravity),<br />
non-dissipational fluid.  The dark matter fluid is very different from<br />
the baryonic fluid;  the dm  is immune from<br />
influences that affect baryons:  the baryonic fluid can dissipate &#8212; loose energy &#8211;,<br />
it can be shocked, it can be removed by supernovae or stellar winds,<br />
it can be swept out in collisions (e.g. the famous Bullet).  Why then should<br />
these two fluids be so intimately connected and similarly distributed<br />
as to subsume the existence of the MOND algorithm?  In fact, the success of<br />
the MOND algorithm on the scale of galaxies is a falsification of CDM<br />
or any dark matter that clusters on the scale of galaxies.  To blandly<br />
state that dark matter exists and accounts for the observations of<br />
galaxy kinematics is to turn a blind eye to a vast range of phenomena;<br />
to imagine that dark matter will someday, when we have more understanding<br />
of the complicated baryonic physics, reproduce the correspondence<br />
of rotation curves to the distribution of baryonic matter is a<br />
leap of faith that is more akin to religion than to science.   This goes as<br />
well for the near perfect Tully-Fisher relation as pointed out by Stacy &#8211;<br />
so perfect that the TF by itself implies a connection with physical<br />
law rather than the messy details of galaxy formation.  And how<br />
will dark matter explain the ubiquitous emergence of a0 &#8211;<br />
as the acceleration below which the discrepancy appears in galaxies,<br />
as the normalization of the Tully-Fisher and Faber-Jackson relations,<br />
as the internal acceleration of near isothermal systems ranging<br />
from globular clusters to clusters of galaxies, and, when expressed<br />
as surface brightness, as the characteristic (Freeman) surface brightness<br />
of galaxies.  If the putative dark matter particles are ever found<br />
(and I doubt that they will be), then we have a lot of work ahead of us<br />
to understand how these regularities, so neatly encapsulated by MOND,<br />
emerge in the context of a non-interacting, dissipationless, dark matter fluid.</p>
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		<title>By: Phil_Osopher</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-157044</link>
		<dc:creator>Phil_Osopher</dc:creator>
		<pubDate>Mon, 21 Mar 2011 17:07:37 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-157044</guid>
		<description>An interesting post on MOND on another blog: http://www.scilogs.eu/en/blog/the-dark-matter-crisis/2011-03-21/question-c.ii-mond-works-far-too-well</description>
		<content:encoded><![CDATA[<p>An interesting post on MOND on another blog: <a href="http://www.scilogs.eu/en/blog/the-dark-matter-crisis/2011-03-21/question-c.ii-mond-works-far-too-well" rel="nofollow">http://www.scilogs.eu/en/blog/the-dark-matter-crisis/2011-03-21/question-c.ii-mond-works-far-too-well</a></p>
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		<title>By: Juan R. González-Álvarez</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156915</link>
		<dc:creator>Juan R. González-Álvarez</dc:creator>
		<pubDate>Sun, 20 Mar 2011 13:20:27 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156915</guid>
		<description>anand srivastava,

I agree with most of what you say. Effectively MOND &quot;&lt;i&gt;kills DM+GR at Galactic Scales&lt;/i&gt;&quot; and effectively this means that &quot;&lt;i&gt;GR needs modification&lt;/i&gt;&quot;.

I did not say that MOND works very well beyond Galactic scales. I said just the contrary and even explained why one must wait discrepancies: &quot;&lt;i&gt;MOND is being applied outside its range of empirical validity&lt;/i&gt;&quot;.

I also wrote in this blog how, thanks to a new theory, &lt;b&gt;we do not need DM (neither DE) to explain observations beyond the Galactic scale anymore&lt;/b&gt;.

FQXi Essays are limited in size by Contest rules, therefore I could not write about all the advantages beyond GR (my first draft Essay was over the size limit and I was forced to eliminate many interesting stuff! For instance, I gave some additional technical details, on how the new canonical theory goes beyond M-theory and the rest of quantum gravity approaches, in &lt;a href=&quot;http://fqxi.org/community/forum/topic/850&quot; rel=&quot;nofollow&quot;&gt;Dr. Tejinder Pal Singh Essay&lt;/a&gt;).

In despite of size limitations, details and further info are given in the cited literature and in the technical notes in my Essay. In the &lt;a href=&quot;http://fqxi.org/community/forum/topic/essay-download/853/__details/Gonzlezlvare_Digital_or_ana.pdf&quot; rel=&quot;nofollow&quot;&gt;technical note in page 9&lt;/a&gt;, I explain the &lt;b&gt;assumptions and approximations over the which GR is based&lt;/b&gt; and how we derive GR from a more fundamental theory. I explain how well-known problems of GR as &quot;&lt;i&gt;the lack of gravitational energy-momentum-stress tensor&lt;/i&gt;&quot;, &quot;&lt;i&gt;spacetime singularities&lt;/i&gt;&quot;, &quot;&lt;i&gt;the problem of the systems of reference&lt;/i&gt;&quot;, &quot;&lt;i&gt;violation of the usual conservation laws&lt;/i&gt;&quot;, and &quot;&lt;i&gt;the impossibility to obtain a consistent quantization of such [geo]metric theory&lt;/i&gt;&quot; are absent in the new theory.

Moreover, I have commented in &lt;a href=&quot;http://fqxi.org/community/forum/topic/875&quot; rel=&quot;nofollow&quot;&gt;Dr. Corda Essay&lt;/a&gt; how we can already go beyond MOND, PCG, TeVeS... explaining data that those theories cannot explain, and also commented I have not still studied Pioneer anomaly enough to say.</description>
		<content:encoded><![CDATA[<p>anand srivastava,</p>
<p>I agree with most of what you say. Effectively MOND &#8220;<i>kills DM+GR at Galactic Scales</i>&#8221; and effectively this means that &#8220;<i>GR needs modification</i>&#8220;.</p>
<p>I did not say that MOND works very well beyond Galactic scales. I said just the contrary and even explained why one must wait discrepancies: &#8220;<i>MOND is being applied outside its range of empirical validity</i>&#8220;.</p>
<p>I also wrote in this blog how, thanks to a new theory, <b>we do not need DM (neither DE) to explain observations beyond the Galactic scale anymore</b>.</p>
<p>FQXi Essays are limited in size by Contest rules, therefore I could not write about all the advantages beyond GR (my first draft Essay was over the size limit and I was forced to eliminate many interesting stuff! For instance, I gave some additional technical details, on how the new canonical theory goes beyond M-theory and the rest of quantum gravity approaches, in <a href="http://fqxi.org/community/forum/topic/850" rel="nofollow">Dr. Tejinder Pal Singh Essay</a>).</p>
<p>In despite of size limitations, details and further info are given in the cited literature and in the technical notes in my Essay. In the <a href="http://fqxi.org/community/forum/topic/essay-download/853/__details/Gonzlezlvare_Digital_or_ana.pdf" rel="nofollow">technical note in page 9</a>, I explain the <b>assumptions and approximations over the which GR is based</b> and how we derive GR from a more fundamental theory. I explain how well-known problems of GR as &#8220;<i>the lack of gravitational energy-momentum-stress tensor</i>&#8220;, &#8220;<i>spacetime singularities</i>&#8220;, &#8220;<i>the problem of the systems of reference</i>&#8220;, &#8220;<i>violation of the usual conservation laws</i>&#8220;, and &#8220;<i>the impossibility to obtain a consistent quantization of such [geo]metric theory</i>&#8221; are absent in the new theory.</p>
<p>Moreover, I have commented in <a href="http://fqxi.org/community/forum/topic/875" rel="nofollow">Dr. Corda Essay</a> how we can already go beyond MOND, PCG, TeVeS&#8230; explaining data that those theories cannot explain, and also commented I have not still studied Pioneer anomaly enough to say.</p>
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		<title>By: anand srivastava</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156912</link>
		<dc:creator>anand srivastava</dc:creator>
		<pubDate>Sun, 20 Mar 2011 11:01:46 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156912</guid>
		<description>@123
No MOND does not work very well beyond Galactic scales so we cannot conclude that at all. It is certainly possible, but we cannot determine that from the data alone. But that is not important MOND working at Galactic Scales kills DM+GR at Galactic Scales. This means GR needs modification. We don&#039;t know what the correct theory is going to be. I am not a physicist or a mathematics. I am just a software developer, with an interest in the MOND problem. I can only conclude if a model is good based on its applications and what it predicts. Unfortunately I did not see much effort at resolving different problems of GR in the quoted essay. Particularly MOND and Pioneer Anomaly.</description>
		<content:encoded><![CDATA[<p>@123<br />
No MOND does not work very well beyond Galactic scales so we cannot conclude that at all. It is certainly possible, but we cannot determine that from the data alone. But that is not important MOND working at Galactic Scales kills DM+GR at Galactic Scales. This means GR needs modification. We don&#8217;t know what the correct theory is going to be. I am not a physicist or a mathematics. I am just a software developer, with an interest in the MOND problem. I can only conclude if a model is good based on its applications and what it predicts. Unfortunately I did not see much effort at resolving different problems of GR in the quoted essay. Particularly MOND and Pioneer Anomaly.</p>
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		<title>By: Juan R. González-Álvarez</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156880</link>
		<dc:creator>Juan R. González-Álvarez</dc:creator>
		<pubDate>Sat, 19 Mar 2011 19:07:13 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156880</guid>
		<description>anand srivastava,

There is a third solution:

&lt;b&gt;1&#039;) DM does not exist at all.&lt;/b&gt;

&quot;The fact that MOND does not work as well at cluster or higher scales...&quot; This is only partially true

http://arxiv.org/abs/0704.0381

and, of course, discrepancies with MOND do not imply existence of DM, (ΛCDM has also difficulties http://adsabs.harvard.edu/abs/2010ApJ...718...60L), but that MOND is being applied outside its range of empirical validity and that a more general theory beyond MOND is needed.

As commented above (#101), MOND (and generalizations of it) can be derived from a truly general gravitational theory. You are right on that &quot;the encompassing physical theory&quot; was &quot;discovered from a totally unexpected direction&quot;!

Our goal was to correct other known deficiencies of GR (see the FQXi Essays cited above) and, as a bonus, we discovered that MOND and its acceleration scale were natural outcomes from the new theory.

If you look to my FQXi Essay, you will discover that the recent theory is much more general than Verlinde’s theory, which is based in a number of approximations and controversial assumptions.</description>
		<content:encoded><![CDATA[<p>anand srivastava,</p>
<p>There is a third solution:</p>
<p><b>1&#8242;) DM does not exist at all.</b></p>
<p>&#8220;The fact that MOND does not work as well at cluster or higher scales&#8230;&#8221; This is only partially true</p>
<p><a href="http://arxiv.org/abs/0704.0381" rel="nofollow">http://arxiv.org/abs/0704.0381</a></p>
<p>and, of course, discrepancies with MOND do not imply existence of DM, (ΛCDM has also difficulties <a href="http://adsabs.harvard.edu/abs/2010ApJ...718...60L" rel="nofollow">http://adsabs.harvard.edu/abs/2010ApJ&#8230;718&#8230;60L</a>), but that MOND is being applied outside its range of empirical validity and that a more general theory beyond MOND is needed.</p>
<p>As commented above (#101), MOND (and generalizations of it) can be derived from a truly general gravitational theory. You are right on that &#8220;the encompassing physical theory&#8221; was &#8220;discovered from a totally unexpected direction&#8221;!</p>
<p>Our goal was to correct other known deficiencies of GR (see the FQXi Essays cited above) and, as a bonus, we discovered that MOND and its acceleration scale were natural outcomes from the new theory.</p>
<p>If you look to my FQXi Essay, you will discover that the recent theory is much more general than Verlinde’s theory, which is based in a number of approximations and controversial assumptions.</p>
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		<title>By: anand srivastava</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156771</link>
		<dc:creator>anand srivastava</dc:creator>
		<pubDate>Fri, 18 Mar 2011 17:11:41 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156771</guid>
		<description>My problem with DM+GR is not that it does not fit the data.
My problem is that the MOND fits the data without needing DM.
Since this simple equation works very well at the galactic scale everywhere. The fits actually keep on improving with more data. There can only be two solutions.
1) DM does not exist at Galactic scale.
2) DM position in space is defined by BMs position in space. This is simply untenable if we believe DM to be separate particles. Also BM is not supposed to interact with DM except by gravitational force. This is totally non-sensible

So the real solution is that DM does not exist at the galactic scale.
I would have had no problem with DM, if MOND did not work so well at galactic scale.

The fact that MOND does not work as well at cluster or higher scales makes no difference. It is probably an indication that some form of DM exists on those scales. I don’t even think that MOND can be enhanced to form a theory. TeVeS is just a toy theory that shows how to build one, but I am pretty sure the encompassing physical theory will be discovered from a totally unexpected direction. The recent Verlinde’s theory of Entropic gravity looks interesting.

I liken MOND to an Empirical law. Any quantum theory of gravity needs to bring out MOND or it is not physical. Since GR in its present form does not predict MOND, it is not physical.

It is as simple as that. Empirical laws must be explained by all physical theories. If Newtons gravitational theory did not explain Kepler’s laws, it would be as useless (at the solar system scale) as GR is presently (at the galactic scale).</description>
		<content:encoded><![CDATA[<p>My problem with DM+GR is not that it does not fit the data.<br />
My problem is that the MOND fits the data without needing DM.<br />
Since this simple equation works very well at the galactic scale everywhere. The fits actually keep on improving with more data. There can only be two solutions.<br />
1) DM does not exist at Galactic scale.<br />
2) DM position in space is defined by BMs position in space. This is simply untenable if we believe DM to be separate particles. Also BM is not supposed to interact with DM except by gravitational force. This is totally non-sensible</p>
<p>So the real solution is that DM does not exist at the galactic scale.<br />
I would have had no problem with DM, if MOND did not work so well at galactic scale.</p>
<p>The fact that MOND does not work as well at cluster or higher scales makes no difference. It is probably an indication that some form of DM exists on those scales. I don’t even think that MOND can be enhanced to form a theory. TeVeS is just a toy theory that shows how to build one, but I am pretty sure the encompassing physical theory will be discovered from a totally unexpected direction. The recent Verlinde’s theory of Entropic gravity looks interesting.</p>
<p>I liken MOND to an Empirical law. Any quantum theory of gravity needs to bring out MOND or it is not physical. Since GR in its present form does not predict MOND, it is not physical.</p>
<p>It is as simple as that. Empirical laws must be explained by all physical theories. If Newtons gravitational theory did not explain Kepler’s laws, it would be as useless (at the solar system scale) as GR is presently (at the galactic scale).</p>
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		<title>By: Ben</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156284</link>
		<dc:creator>Ben</dc:creator>
		<pubDate>Tue, 15 Mar 2011 13:37:08 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156284</guid>
		<description>@question mark: No, I disagree. The M/L ratio is a &quot;free&quot; parameter but its best-fit obtained in mond from dynamics alone is ususally amazingly similar to what one expects from completely independent models based on stellar populations synthesis (that have nothing to do with dynamics): this has been, and still is, one of the strongest arguments for mond! In addition, this free parameter goes away when fitting gassy galaxies, and that was precisely the point of the whole press release of Stacy. Then, there is the distance, which again can sometimes be a little discrepant when set completely free, but which usually gives very good fits when constrained to lie within the range of distances obtained from various independent methods. So, yes there are free parameters (M/L and distance, and in the case of Stacy, only distance), but you wouldnt call a good fit a fit using a crazy value for these parameters, that are in the end not so free anymore... The point is that mond yields brilliant fits in most spiral galaxies with completely reasonable values of those parameters. This is neither overselling nor underselling what mond does. And again whatever the reason for it, its success should be, in my opinion, understood.</description>
		<content:encoded><![CDATA[<p>@question mark: No, I disagree. The M/L ratio is a &#8220;free&#8221; parameter but its best-fit obtained in mond from dynamics alone is ususally amazingly similar to what one expects from completely independent models based on stellar populations synthesis (that have nothing to do with dynamics): this has been, and still is, one of the strongest arguments for mond! In addition, this free parameter goes away when fitting gassy galaxies, and that was precisely the point of the whole press release of Stacy. Then, there is the distance, which again can sometimes be a little discrepant when set completely free, but which usually gives very good fits when constrained to lie within the range of distances obtained from various independent methods. So, yes there are free parameters (M/L and distance, and in the case of Stacy, only distance), but you wouldnt call a good fit a fit using a crazy value for these parameters, that are in the end not so free anymore&#8230; The point is that mond yields brilliant fits in most spiral galaxies with completely reasonable values of those parameters. This is neither overselling nor underselling what mond does. And again whatever the reason for it, its success should be, in my opinion, understood.</p>
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		<title>By: Juan R. González-Álvarez</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156280</link>
		<dc:creator>Juan R. González-Álvarez</dc:creator>
		<pubDate>Tue, 15 Mar 2011 12:29:46 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156280</guid>
		<description>Above I wrote that in dark matter model you have three times more freedom and still cannot match MOND predictions. A beautiful example of this is discussed in

&lt;i&gt;Extended rotation curves of spiral galaxies - Dark haloes and modified dynamics. Mon. Not. R. astr. Soc. 1991: 249, 523-537. Begeman, K. G.; Broeils, A. H.; Sanders, R. H.&lt;/i&gt;

Authors compare &lt;b&gt;three-parameter&lt;/b&gt; dark-matter fits (M/L for the visible disk, plus two parameters for the dark matter halo: the core radius and the asymptotic circular velocity of the halo) with &lt;b&gt;one-parameter&lt;/b&gt; MOND fits (M/L for the visible disk).

They find that &lt;b&gt;MOND works well and &quot;in some cases better than multi-parameter dark-halo fits.&quot;&lt;/b&gt;

I am sorry to say this to dark-matter enthusiasts, but MOND rocks...</description>
		<content:encoded><![CDATA[<p>Above I wrote that in dark matter model you have three times more freedom and still cannot match MOND predictions. A beautiful example of this is discussed in</p>
<p><i>Extended rotation curves of spiral galaxies &#8211; Dark haloes and modified dynamics. Mon. Not. R. astr. Soc. 1991: 249, 523-537. Begeman, K. G.; Broeils, A. H.; Sanders, R. H.</i></p>
<p>Authors compare <b>three-parameter</b> dark-matter fits (M/L for the visible disk, plus two parameters for the dark matter halo: the core radius and the asymptotic circular velocity of the halo) with <b>one-parameter</b> MOND fits (M/L for the visible disk).</p>
<p>They find that <b>MOND works well and &#8220;in some cases better than multi-parameter dark-halo fits.&#8221;</b></p>
<p>I am sorry to say this to dark-matter enthusiasts, but MOND rocks&#8230;</p>
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		<title>By: Juan R. González-Álvarez</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156275</link>
		<dc:creator>Juan R. González-Álvarez</dc:creator>
		<pubDate>Tue, 15 Mar 2011 10:46:07 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156275</guid>
		<description>Albert, Ben, and Question Mark,

MOND has &lt;b&gt;zero&lt;/b&gt; parameters. It is the dark matter model which uses &quot;free parameters that can be chosen to improve any fit&quot; (as Question Mark says).

I invite you to read again the section 5.2 of Gentile et al.

http://arxiv.org/abs/1004.3421

&lt;b&gt;Two parameters for Burkert dark matter model&lt;/b&gt; (central density and core radius).

&lt;b&gt;One/two parameters for the ΛCDM model&lt;/b&gt; of Navarro, Frenk &amp; White (concentration and virial mass). Gentile et al. use cosmological simulations to correlate both (see eq. 3), but due to bad fit to the data they repeated the fit leaving both parameters free (read section 6) and still obtained a bad fit and related difficulties.

&lt;b&gt;Zero parameters for MOND&lt;/b&gt; (see equation 6).

Regarding http://arxiv.org/abs/1005.5456, the authors use M/L as a free parameter to correlate velocity with light distribution, &lt;b&gt;not&lt;/b&gt; because M/L was a free parameter in MOND. MOND are equations 1 and 2 in that preprint and they have &lt;b&gt;zero&lt;/b&gt; parameters.

If you were to repeat their analysis using dark matter models you would use one or two parameters (of the dark halo) &lt;b&gt;plus&lt;/b&gt; the M/L ratio of the correlation to light.

I.e. using the Burkert dark matter model you have &lt;b&gt;three times more freedom&lt;/b&gt; (rho_0, r_{core}, and M/L) and still cannot match MOND predictions.

Precisely, the fact that MOND has &lt;b&gt;zero&lt;/b&gt; parameters is the reason which is so sensitive to uncertainties in distances, whereas the dark matter models can absorb distance uncertainties into the halo parameters.</description>
		<content:encoded><![CDATA[<p>Albert, Ben, and Question Mark,</p>
<p>MOND has <b>zero</b> parameters. It is the dark matter model which uses &#8220;free parameters that can be chosen to improve any fit&#8221; (as Question Mark says).</p>
<p>I invite you to read again the section 5.2 of Gentile et al.</p>
<p><a href="http://arxiv.org/abs/1004.3421" rel="nofollow">http://arxiv.org/abs/1004.3421</a></p>
<p><b>Two parameters for Burkert dark matter model</b> (central density and core radius).</p>
<p><b>One/two parameters for the ΛCDM model</b> of Navarro, Frenk &amp; White (concentration and virial mass). Gentile et al. use cosmological simulations to correlate both (see eq. 3), but due to bad fit to the data they repeated the fit leaving both parameters free (read section 6) and still obtained a bad fit and related difficulties.</p>
<p><b>Zero parameters for MOND</b> (see equation 6).</p>
<p>Regarding <a href="http://arxiv.org/abs/1005.5456" rel="nofollow">http://arxiv.org/abs/1005.5456</a>, the authors use M/L as a free parameter to correlate velocity with light distribution, <b>not</b> because M/L was a free parameter in MOND. MOND are equations 1 and 2 in that preprint and they have <b>zero</b> parameters.</p>
<p>If you were to repeat their analysis using dark matter models you would use one or two parameters (of the dark halo) <b>plus</b> the M/L ratio of the correlation to light.</p>
<p>I.e. using the Burkert dark matter model you have <b>three times more freedom</b> (rho_0, r_{core}, and M/L) and still cannot match MOND predictions.</p>
<p>Precisely, the fact that MOND has <b>zero</b> parameters is the reason which is so sensitive to uncertainties in distances, whereas the dark matter models can absorb distance uncertainties into the halo parameters.</p>
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	<item>
		<title>By: Juan R. González-Álvarez</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156273</link>
		<dc:creator>Juan R. González-Álvarez</dc:creator>
		<pubDate>Tue, 15 Mar 2011 10:17:57 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156273</guid>
		<description>Albert,

In this comment-page I have introduced six links from Stacy website. Only one part of one of the links discuss the wiggle. The other links discuss MOND predictions (all verified), samples of about a hundred of galaxies explained by MOND...

The same about the Gentile et al paper. They discuss the wiggle and more as ML ratios and overall fits.</description>
		<content:encoded><![CDATA[<p>Albert,</p>
<p>In this comment-page I have introduced six links from Stacy website. Only one part of one of the links discuss the wiggle. The other links discuss MOND predictions (all verified), samples of about a hundred of galaxies explained by MOND&#8230;</p>
<p>The same about the Gentile et al paper. They discuss the wiggle and more as ML ratios and overall fits.</p>
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		<title>By: Question Mark</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156264</link>
		<dc:creator>Question Mark</dc:creator>
		<pubDate>Tue, 15 Mar 2011 09:16:41 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156264</guid>
		<description>#116: So Ben, you are confirming that with MOND one does not get an improved representation over dark matter models since in MOND there are free parameters that can be chosen to improve any fit?</description>
		<content:encoded><![CDATA[<p>#116: So Ben, you are confirming that with MOND one does not get an improved representation over dark matter models since in MOND there are free parameters that can be chosen to improve any fit?</p>
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		<title>By: Ben</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156260</link>
		<dc:creator>Ben</dc:creator>
		<pubDate>Tue, 15 Mar 2011 08:38:00 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156260</guid>
		<description>Albert, you are probably right about overinterpretations of the wiggle of 1560, even though as I said it is much more *plausible*, I think, to explain it in mond or with HI-scaling than with a DM halo. But non-axisymmetric models in each of these paradigms are needed in order to prove this: hopefully it will come soon. Concerning showing the individual contributions of the gas and stars, it doesnt really make sense in mond as the theory is non-linear. Finally concerning the stellar M/L ratio being a free parameter, you are totally right (even though one of the strong arguments for mond is that the fitted ones follow well the trend expected from population synthesis models), but the whole point of Stacy&#039;s paper under discussion here was to take away that free parameter by considering gas-dominated galaxies. The fact that mond still works well for these is, I think, striking. But you are right that it is not true to state that mond has, in general, zero free parameters.</description>
		<content:encoded><![CDATA[<p>Albert, you are probably right about overinterpretations of the wiggle of 1560, even though as I said it is much more *plausible*, I think, to explain it in mond or with HI-scaling than with a DM halo. But non-axisymmetric models in each of these paradigms are needed in order to prove this: hopefully it will come soon. Concerning showing the individual contributions of the gas and stars, it doesnt really make sense in mond as the theory is non-linear. Finally concerning the stellar M/L ratio being a free parameter, you are totally right (even though one of the strong arguments for mond is that the fitted ones follow well the trend expected from population synthesis models), but the whole point of Stacy&#8217;s paper under discussion here was to take away that free parameter by considering gas-dominated galaxies. The fact that mond still works well for these is, I think, striking. But you are right that it is not true to state that mond has, in general, zero free parameters.</p>
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		<title>By: Albert</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156231</link>
		<dc:creator>Albert</dc:creator>
		<pubDate>Mon, 14 Mar 2011 22:30:00 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156231</guid>
		<description>Juan, having heard talks about MOND since its inception in the 1980s, I can assure you that the wiggle in NGC 1560 plays a prominent role in the presentations of MOND by its advocates since the early 1990s. I have seen that plot presented quite a number of times, and Stacy singles it out in his Web presentation as well. I don&#039;t think my sampling of MOND advocates is biased.</description>
		<content:encoded><![CDATA[<p>Juan, having heard talks about MOND since its inception in the 1980s, I can assure you that the wiggle in NGC 1560 plays a prominent role in the presentations of MOND by its advocates since the early 1990s. I have seen that plot presented quite a number of times, and Stacy singles it out in his Web presentation as well. I don&#8217;t think my sampling of MOND advocates is biased.</p>
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		<title>By: Juan R. González-Álvarez</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156208</link>
		<dc:creator>Juan R. González-Álvarez</dc:creator>
		<pubDate>Mon, 14 Mar 2011 19:57:19 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156208</guid>
		<description>Albert,

MOND ability to fit the wiggle in NGC 1560 is not the reason for which MOND advocates consider &quot;to take MOND seriously&quot;. The reasons are (i) a hundred of galaxies explained by MOND as well as (ii) the dozen of predictions done by MOND and verified up to the date.

Regarding the recent preprint by Gentile et al. they do not claim &quot;to take MOND seriously&quot; because of the wiggle, as you continue to believe, but because they got &quot;good fits using MOND&quot; and &quot;bad fits using the Navarro, Frenk &amp; White halo&quot; (an &#039;elegant&#039; ΛCDM model). Reproducing the wiggle is only one point of an overall score that has given MOND its good empirical status.

As explained in the section 5.2 of Gentile et al., the Burkert dark matter model uses TWO parameters (rho_0 and r_{core} in the eq. 1), whereas MOND uses ZERO parameters (see eqs. 6 and 7). For values of r_{core} = 5.6 kpc and rho_0 = 0.8x10^−24 g cm^−3, the best fit M/L ratio for the Burkert dark matter model is of 2.3. Using ZERO parameters, the best fit M/L ratio for MOND is 0.98. The reference value for the ratio obtained from stellar population analysis is 1.43.

If you take all the points together (chi-squared plus wiggle plus ML ratio plus total number of free parameters...) you will find that MOND works better and, indeed, Gentile et al. affirm that MOND does it better than Burkert model and much much better than ΛCDM (which is empirically falsified).

Regarding http://arxiv.org/abs/1005.5456, the authors claim that &quot;MOND is successful&quot; for roughly three quarters of the galaxies in a sample of 27 dwarf and low surface brightness galaxies and that &quot;This is remarkable, given that MOND is a one parameter fit with only M/L as a free parameter.&quot;

MOND does not adequately explain the observed rotation curves for the remaining one quarter. The authors also emphasize that for the discrepant galaxies poor predictions were expected due to strong uncertainties in inclinations and distances.

If you take a look to their sample, you will find that some of the galaxies (e.g. UGC 5750, UGC 6446) were already covered in the section &quot;Galaxies for which MOND fit is dubious&quot; of a link given in a previous post from mine (http://www.astro.umd.edu/~ssm/mond/fitroster.html). However, UGC 5750 was then listed in that section, whereas now is reported as being in good agreement with MOND predictions.

This sample adds 8 new galaxies to the section of &quot;Galaxies for which the MOND fit is dubious&quot; and 14 new to the section &quot;Galaxies well fit by MOND&quot; and moves UGC 5750. This gives an overall score of about 98-0-18, with the 18 being associated to strong uncertainties.</description>
		<content:encoded><![CDATA[<p>Albert,</p>
<p>MOND ability to fit the wiggle in NGC 1560 is not the reason for which MOND advocates consider &#8220;to take MOND seriously&#8221;. The reasons are (i) a hundred of galaxies explained by MOND as well as (ii) the dozen of predictions done by MOND and verified up to the date.</p>
<p>Regarding the recent preprint by Gentile et al. they do not claim &#8220;to take MOND seriously&#8221; because of the wiggle, as you continue to believe, but because they got &#8220;good fits using MOND&#8221; and &#8220;bad fits using the Navarro, Frenk &amp; White halo&#8221; (an &#8216;elegant&#8217; ΛCDM model). Reproducing the wiggle is only one point of an overall score that has given MOND its good empirical status.</p>
<p>As explained in the section 5.2 of Gentile et al., the Burkert dark matter model uses TWO parameters (rho_0 and r_{core} in the eq. 1), whereas MOND uses ZERO parameters (see eqs. 6 and 7). For values of r_{core} = 5.6 kpc and rho_0 = 0.8&#215;10^−24 g cm^−3, the best fit M/L ratio for the Burkert dark matter model is of 2.3. Using ZERO parameters, the best fit M/L ratio for MOND is 0.98. The reference value for the ratio obtained from stellar population analysis is 1.43.</p>
<p>If you take all the points together (chi-squared plus wiggle plus ML ratio plus total number of free parameters&#8230;) you will find that MOND works better and, indeed, Gentile et al. affirm that MOND does it better than Burkert model and much much better than ΛCDM (which is empirically falsified).</p>
<p>Regarding <a href="http://arxiv.org/abs/1005.5456" rel="nofollow">http://arxiv.org/abs/1005.5456</a>, the authors claim that &#8220;MOND is successful&#8221; for roughly three quarters of the galaxies in a sample of 27 dwarf and low surface brightness galaxies and that &#8220;This is remarkable, given that MOND is a one parameter fit with only M/L as a free parameter.&#8221;</p>
<p>MOND does not adequately explain the observed rotation curves for the remaining one quarter. The authors also emphasize that for the discrepant galaxies poor predictions were expected due to strong uncertainties in inclinations and distances.</p>
<p>If you take a look to their sample, you will find that some of the galaxies (e.g. UGC 5750, UGC 6446) were already covered in the section &#8220;Galaxies for which MOND fit is dubious&#8221; of a link given in a previous post from mine (<a href="http://www.astro.umd.edu/~ssm/mond/fitroster.html" rel="nofollow">http://www.astro.umd.edu/~ssm/mond/fitroster.html</a>). However, UGC 5750 was then listed in that section, whereas now is reported as being in good agreement with MOND predictions.</p>
<p>This sample adds 8 new galaxies to the section of &#8220;Galaxies for which the MOND fit is dubious&#8221; and 14 new to the section &#8220;Galaxies well fit by MOND&#8221; and moves UGC 5750. This gives an overall score of about 98-0-18, with the 18 being associated to strong uncertainties.</p>
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		<title>By: Albert</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156181</link>
		<dc:creator>Albert</dc:creator>
		<pubDate>Mon, 14 Mar 2011 15:24:57 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156181</guid>
		<description>Ben, as far as I understand it, the bump in the HI causes the wiggle in the expected rotation curve. Unfortunately, the MOND fits never show the contributions of the individual components in MOND (i.e. they show the individual contributions for the Newtonian case).

Juan, NGC 1560 has &#039;iconic status&#039; for MOND, i.e. the &#039;remarkable&#039; ability to fit the wiggle is widely quoted as a good reason to take MOND seriously. As for the hundred other galaxies &#039;perfectly well described&#039; by MOND, I advise you to read 
&lt;a href=&quot;http://arxiv.org/abs/1005.5456v1&quot; rel=&quot;nofollow&quot;&gt;http://arxiv.org/abs/1005.5456&lt;/a&gt; where more counterexamples are discussed. Good distances might indeed tighten the constraints on MOND, since now &lt;i&gt;de facto&lt;/i&gt; distance is used as a free parameter in MOND fits, in addition to the M/L ratio. Note that the M/L ratio is not predicted by MOND, contrary to your statement that MOND has ZERO free parameters. M/L ratios are rather uncertain, since the IMF is not very well constrained.</description>
		<content:encoded><![CDATA[<p>Ben, as far as I understand it, the bump in the HI causes the wiggle in the expected rotation curve. Unfortunately, the MOND fits never show the contributions of the individual components in MOND (i.e. they show the individual contributions for the Newtonian case).</p>
<p>Juan, NGC 1560 has &#8216;iconic status&#8217; for MOND, i.e. the &#8216;remarkable&#8217; ability to fit the wiggle is widely quoted as a good reason to take MOND seriously. As for the hundred other galaxies &#8216;perfectly well described&#8217; by MOND, I advise you to read<br />
<a href="http://arxiv.org/abs/1005.5456v1" rel="nofollow">http://arxiv.org/abs/1005.5456</a> where more counterexamples are discussed. Good distances might indeed tighten the constraints on MOND, since now <i>de facto</i> distance is used as a free parameter in MOND fits, in addition to the M/L ratio. Note that the M/L ratio is not predicted by MOND, contrary to your statement that MOND has ZERO free parameters. M/L ratios are rather uncertain, since the IMF is not very well constrained.</p>
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		<title>By: Juan R. González-Álvarez</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156173</link>
		<dc:creator>Juan R. González-Álvarez</dc:creator>
		<pubDate>Mon, 14 Mar 2011 13:41:18 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156173</guid>
		<description>Albert,

thanks for pointing to the figure in the reference page. In early posts, I did a series of corrections to unfounded attacks on MOND and added information about a hundred of galaxies being perfectly described by MOND as well as about a dozen of predictions done by MOND and that have been verified.

You have only focused in one wiggle around 300&#039;&#039; in one galaxy! Still, I commented about this wiggle and about how this would not hide the subsequent difficulties for the ΛCDM model, which, I repeat, has been experimentally falsified in galaxies (ΛCDM systematically fails to reproduce both the velocities and the shape of the observed rotation curves).

In fact, you cite now the &quot;core-cusp&quot; problem in ΛCDM and confirm the attitude of cosmologists as Sean Caroll to ignore empirical evidences and to make unfounded comments against MOND.

You affirm that &quot;by eye&quot; the Burkert model gives a better fit than MOND. I find that you again are missing the whole picture because you are ignoring (i) the fit to the wiggle (curiously the best-fit curve in the Burkert model goes through the region of the wiggle), (ii) the number of FREE parameters used in each fit (TWO in the Burkert model, ZERO in MOND), (iii) that MOND gives better M/L ratio that Burkert, and (iv) that ΛCDM gives a bad fit.

There is not inconsistency about distances but uncertainty. Adopting the 3.45+-0.36 Mpc in MOND reduces the fit quality (chi-square) about a 0.13 and there is lower distances than 2.94 Mpc reported by other methods. The comments in Stacy McGaugh&#039;s page are about the Broeils 1992 data not about Gentile et al. recent data. McGaugh emphasizes that &quot;The CDM fit is not unique&quot; and that &quot;Its prediction is more vague than that of MOND, and misses the mark by a wider margin.&quot; The same conclusions are found by  Gentile et al.: &quot;bad fits using the a Navarro, Frenk &amp; White halo&quot; (CDM), &quot;and good fits using MOND&quot;.

Now cosmologists as Sean Carroll would explain how is possible than the &#039;beautiful&#039; ΛCDM model once again fails to explain data, whereas &#039;ugly&#039; models as MOND explain the data (without free parameters).</description>
		<content:encoded><![CDATA[<p>Albert,</p>
<p>thanks for pointing to the figure in the reference page. In early posts, I did a series of corrections to unfounded attacks on MOND and added information about a hundred of galaxies being perfectly described by MOND as well as about a dozen of predictions done by MOND and that have been verified.</p>
<p>You have only focused in one wiggle around 300&#8221; in one galaxy! Still, I commented about this wiggle and about how this would not hide the subsequent difficulties for the ΛCDM model, which, I repeat, has been experimentally falsified in galaxies (ΛCDM systematically fails to reproduce both the velocities and the shape of the observed rotation curves).</p>
<p>In fact, you cite now the &#8220;core-cusp&#8221; problem in ΛCDM and confirm the attitude of cosmologists as Sean Caroll to ignore empirical evidences and to make unfounded comments against MOND.</p>
<p>You affirm that &#8220;by eye&#8221; the Burkert model gives a better fit than MOND. I find that you again are missing the whole picture because you are ignoring (i) the fit to the wiggle (curiously the best-fit curve in the Burkert model goes through the region of the wiggle), (ii) the number of FREE parameters used in each fit (TWO in the Burkert model, ZERO in MOND), (iii) that MOND gives better M/L ratio that Burkert, and (iv) that ΛCDM gives a bad fit.</p>
<p>There is not inconsistency about distances but uncertainty. Adopting the 3.45+-0.36 Mpc in MOND reduces the fit quality (chi-square) about a 0.13 and there is lower distances than 2.94 Mpc reported by other methods. The comments in Stacy McGaugh&#8217;s page are about the Broeils 1992 data not about Gentile et al. recent data. McGaugh emphasizes that &#8220;The CDM fit is not unique&#8221; and that &#8220;Its prediction is more vague than that of MOND, and misses the mark by a wider margin.&#8221; The same conclusions are found by  Gentile et al.: &#8220;bad fits using the a Navarro, Frenk &amp; White halo&#8221; (CDM), &#8220;and good fits using MOND&#8221;.</p>
<p>Now cosmologists as Sean Carroll would explain how is possible than the &#8216;beautiful&#8217; ΛCDM model once again fails to explain data, whereas &#8216;ugly&#8217; models as MOND explain the data (without free parameters).</p>
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		<title>By: Ben</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156156</link>
		<dc:creator>Ben</dc:creator>
		<pubDate>Mon, 14 Mar 2011 09:22:57 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156156</guid>
		<description>Just to clarify things, I am (a) not claiming that it is possible to simply replace *cosmological* DM with baryonic DM, we know that this is a priori impossible, (b) not even claiming that it is possible to *fully* replace galactic DM by baryonic DM, which is what I meant with the fact that HI-scaling would have troubles fitting the outermost datapoints of rotation curves (while in addition it also couldnt explain the near-sphericity of the potential obtained from fitting orbits of tidal streams, so you&#039;d still need an additional DM halo or modified gravity in the outermost parts), just that *a lot* of DM in galaxies could actually be in cold gas form, which could (i) help explaining the wiggles a-la-NGC 1560 and (ii) perhaps even ease the understanding of the baryonic Tully-Fisher relation from feedback mechanisms (and incidentally, it would drastically reduce the local non-baryonic DM density at the position of the Sun: no luck for direct detection experiments). I still think this last point about feedback is far from easy, and that &quot;plain MOND&quot; is still by far the easiest way to explain the baryonic TF relation. I am just not closed to the idea of a lot of baryonic DM being present in galaxies in the form of H2... easing the understanding of some observations but somehow also complicating the whole picture, both from the DM and from the modified gravity points of view... Who said it was all gonna be easy? </description>
		<content:encoded><![CDATA[<p>Just to clarify things, I am (a) not claiming that it is possible to simply replace *cosmological* DM with baryonic DM, we know that this is a priori impossible, (b) not even claiming that it is possible to *fully* replace galactic DM by baryonic DM, which is what I meant with the fact that HI-scaling would have troubles fitting the outermost datapoints of rotation curves (while in addition it also couldnt explain the near-sphericity of the potential obtained from fitting orbits of tidal streams, so you&#8217;d still need an additional DM halo or modified gravity in the outermost parts), just that *a lot* of DM in galaxies could actually be in cold gas form, which could (i) help explaining the wiggles a-la-NGC 1560 and (ii) perhaps even ease the understanding of the baryonic Tully-Fisher relation from feedback mechanisms (and incidentally, it would drastically reduce the local non-baryonic DM density at the position of the Sun: no luck for direct detection experiments). I still think this last point about feedback is far from easy, and that &#8220;plain MOND&#8221; is still by far the easiest way to explain the baryonic TF relation. I am just not closed to the idea of a lot of baryonic DM being present in galaxies in the form of H2&#8230; easing the understanding of some observations but somehow also complicating the whole picture, both from the DM and from the modified gravity points of view&#8230; Who said it was all gonna be easy?</p>
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		<title>By: Ben</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156093</link>
		<dc:creator>Ben</dc:creator>
		<pubDate>Sun, 13 Mar 2011 17:28:42 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156093</guid>
		<description>Albert, about NGC 1560, it is still intriguing that the wiggles in the rotation curve and in the HI surface density are at exactly the same position and on the same side of the galaxy. As stated in Gentile et al., it is unlikely that this is due to strong non-circular motions as in NGC 3031. It rather seems to be a true wiggle in the gas tangential velocity for orbits that are only slightly perturbed (but it is true that they are of course not circular stricto sensu). To settle this debate, mildly non-axisymmetric models of NGC 1560 reproducing the HI surface density on both sides and a mock &quot;rotation curve&quot; should be produced both in MOND and within a dark matter halo, and why not also by considering molecular gas in an &quot;HI-scaling&quot; fashion, which would probably produce an excellent fit too, apart from the very outer data points (see the impressive &quot;HI scaling&quot; rotation curve fits in http://arxiv.org/abs/astro-ph/0403154)... but I doubt the dark matter models (even the Burkert-based ones) will succeed... Related to HI scaling, an intriguing possibility to explain the baryonic Tully-Fisher relation and the MOND phenomenology in galaxies would be to investigate the consequences of internal physical factors in self-regulated gravitating disks where &quot;dark matter&quot; would mostly be in the form of molecular gas (i.e. multiplying the HI mass by a large factor, that could be of the order of 15 or even more depending on the galaxy), as advocated by, e.g., http://arxiv.org/abs/astro-ph/0409621 ... Of course, if this would be the true explanation of the success of the MOND phenomenology, it would be as unlikely as in the modified gravity hypothesis that XENON100 and other similar experiments will ever ever find a CDM particle...</description>
		<content:encoded><![CDATA[<p>Albert, about NGC 1560, it is still intriguing that the wiggles in the rotation curve and in the HI surface density are at exactly the same position and on the same side of the galaxy. As stated in Gentile et al., it is unlikely that this is due to strong non-circular motions as in NGC 3031. It rather seems to be a true wiggle in the gas tangential velocity for orbits that are only slightly perturbed (but it is true that they are of course not circular stricto sensu). To settle this debate, mildly non-axisymmetric models of NGC 1560 reproducing the HI surface density on both sides and a mock &#8220;rotation curve&#8221; should be produced both in MOND and within a dark matter halo, and why not also by considering molecular gas in an &#8220;HI-scaling&#8221; fashion, which would probably produce an excellent fit too, apart from the very outer data points (see the impressive &#8220;HI scaling&#8221; rotation curve fits in <a href="http://arxiv.org/abs/astro-ph/0403154" rel="nofollow">http://arxiv.org/abs/astro-ph/0403154</a>)&#8230; but I doubt the dark matter models (even the Burkert-based ones) will succeed&#8230; Related to HI scaling, an intriguing possibility to explain the baryonic Tully-Fisher relation and the MOND phenomenology in galaxies would be to investigate the consequences of internal physical factors in self-regulated gravitating disks where &#8220;dark matter&#8221; would mostly be in the form of molecular gas (i.e. multiplying the HI mass by a large factor, that could be of the order of 15 or even more depending on the galaxy), as advocated by, e.g., <a href="http://arxiv.org/abs/astro-ph/0409621" rel="nofollow">http://arxiv.org/abs/astro-ph/0409621</a> &#8230; Of course, if this would be the true explanation of the success of the MOND phenomenology, it would be as unlikely as in the modified gravity hypothesis that XENON100 and other similar experiments will ever ever find a CDM particle&#8230;</p>
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		<title>By: Albert</title>
		<link>http://blogs.discovermagazine.com/cosmicvariance/2011/02/26/dark-matter-just-fine-thanks/comment-page-2/#comment-156046</link>
		<dc:creator>Albert</dc:creator>
		<pubDate>Sat, 12 Mar 2011 22:25:18 +0000</pubDate>
		<guid isPermaLink="false">http://blogs.discovermagazine.com/cosmicvariance/?p=6267#comment-156046</guid>
		<description>#108. The basic point is that the rotation curve gives you the circular velocity of a test particle at a given radius, independent of azimuthal angle. In NGC 1560, at one side of the galaxy there is a local perturbation which causes a wiggle in the position-velocity curve at that side. This is mainly due to an uneven distribution of neutral gas. It is not clear to me that that wiggle can be interpreted as accurately reflecting the circular velocity there. Hence the &#039;true&#039; rotation curve of NGC 1560 is not necessarily the average of both sides, at least in my opinion. Whether or not MOND fits both sides separately (not even well) is immaterial : a galaxy in equilibrium has one rotation curve (and not two).

Gentile et al. don&#039;t give a chi-squared for the fits, but by eye the Burkert model gives a better fit than MOND. Furthermore, they assume a distance of 3.45 Mpc when fitting DM models, and for MOND they adopt a distance of 2.94 Mpc. The 3.45+-0.36 Mpc distance comes from the tip of the red giant branch method. So there is an inconsistency here - the best MOND fit is for a distance different from the best distance estimate -, as is also known for NGC 3198. Note that on Stacy&#039;s page the comments are the other way around : the Begeman et al. fit for D = 3.0 Mpc was not good enough, so they said the galaxy ought to be at 3.4 Mpc for a good fit! So not all is well here (OK, a 13% problem).

The dip in the wiggle in NGC 1560 coincides with a relative depletion of the HI in the northern part. Interestingly enough, there is an extension in the vertical direction in the HI there, see Figure 3 of the paper of Gentile et al. This is not further discussed in that paper, but it could be related to the uneven gas distribution in the main plane.

As for the Burkert model fitting better than a model using the NFW profile (Figures 10 and 11), this graphically illustrates the &#039;core-cusp&#039; problem in LCDM. It is indeed true that it took observers a lot of time to convince cosmologists that LCDM had that problem : their general attitude was (and partly is) still very close to the attitude displayed above by Sean (attitude of saying DM doing &quot;just fine&quot;, despite all the glaring problems; declaring MOND is ugly, as if 4% baryons + 23% unknown matter + 73% &#039;dark energy&#039; is not messy). In that sense, LCDM was, and continues to be, oversold. But that does not mean that MOND should be oversold as well: it also has subtle problems, such as the one I am pointing out about NGC 1560.</description>
		<content:encoded><![CDATA[<p>#108. The basic point is that the rotation curve gives you the circular velocity of a test particle at a given radius, independent of azimuthal angle. In NGC 1560, at one side of the galaxy there is a local perturbation which causes a wiggle in the position-velocity curve at that side. This is mainly due to an uneven distribution of neutral gas. It is not clear to me that that wiggle can be interpreted as accurately reflecting the circular velocity there. Hence the &#8216;true&#8217; rotation curve of NGC 1560 is not necessarily the average of both sides, at least in my opinion. Whether or not MOND fits both sides separately (not even well) is immaterial : a galaxy in equilibrium has one rotation curve (and not two).</p>
<p>Gentile et al. don&#8217;t give a chi-squared for the fits, but by eye the Burkert model gives a better fit than MOND. Furthermore, they assume a distance of 3.45 Mpc when fitting DM models, and for MOND they adopt a distance of 2.94 Mpc. The 3.45+-0.36 Mpc distance comes from the tip of the red giant branch method. So there is an inconsistency here &#8211; the best MOND fit is for a distance different from the best distance estimate -, as is also known for NGC 3198. Note that on Stacy&#8217;s page the comments are the other way around : the Begeman et al. fit for D = 3.0 Mpc was not good enough, so they said the galaxy ought to be at 3.4 Mpc for a good fit! So not all is well here (OK, a 13% problem).</p>
<p>The dip in the wiggle in NGC 1560 coincides with a relative depletion of the HI in the northern part. Interestingly enough, there is an extension in the vertical direction in the HI there, see Figure 3 of the paper of Gentile et al. This is not further discussed in that paper, but it could be related to the uneven gas distribution in the main plane.</p>
<p>As for the Burkert model fitting better than a model using the NFW profile (Figures 10 and 11), this graphically illustrates the &#8216;core-cusp&#8217; problem in LCDM. It is indeed true that it took observers a lot of time to convince cosmologists that LCDM had that problem : their general attitude was (and partly is) still very close to the attitude displayed above by Sean (attitude of saying DM doing &#8220;just fine&#8221;, despite all the glaring problems; declaring MOND is ugly, as if 4% baryons + 23% unknown matter + 73% &#8216;dark energy&#8217; is not messy). In that sense, LCDM was, and continues to be, oversold. But that does not mean that MOND should be oversold as well: it also has subtle problems, such as the one I am pointing out about NGC 1560.</p>
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