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Basic problems |
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| Mar27-06, 11:05 AM | #18 |
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Basic problemsIt is interesting from your last link paper, (which also contains my quote from the earlier Turyshev et al. paper confirming an unexplained PA) that more data is available and only now being analysed, some narrowly missed being destroyed! What do they hope to achieve from this rescued data? In any case the observation should drive the theory, not the other way round! Why should there be this discrepency between PA & orbital theory? Perhaps as the PA is of the order of CH it is cosmological in origin and there is a discrepency between the applicability of the Schwarzschild and Cosmological solutions of GR? BTW wolram, marcus was complementing you. ![]() Garth |
| Mar27-06, 12:06 PM | #19 |
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The rest of your references refer to the "cuspy cores" problem, "small-scale structure" problem, and something that we understand too poorly to really be called a problem. The first two are genuine concerns with [itex]\Lambda CDM[/itex] and have been discussed at length in other threads. If the first isn't just an issue of numerical resolution (which is looking increasingly likely), then it's an issue of our lack of knowledge about the dark matter, which falls back into what I was saying about needing more measurements of dark matter properties. The second is, again, a possible issue with the simulations and may have nothing to do with fundamental theory. The third is another example of how we're data-starved. We don't have nearly enough high-z data to understand how the feedback process works. They are fair concerns, however. I wouldn't yet call them "weak points" with the model because it's still not clear to me that they're not problems with the simulations, but it's still worth keeping in mind. As for MOND, it comes as absolutely no surprise to me that a theory designed to fit rotation curves can do so with fewer parameters than the standard model. It also came as no surprise to me that relativistic MOND was completely inconsistent with the CMB. |
| Mar27-06, 12:13 PM | #20 |
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Garth |
| Mar27-06, 12:28 PM | #21 |
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By Garth,
BTW wolram, marcus was complementing you. Marcus, sorry if my post seemed gruff, it was not meant to be
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| Mar27-06, 12:35 PM | #22 |
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What you said: |
| Mar27-06, 12:57 PM | #23 |
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Perhaps if I had emphasised?: The curse of the fear of the false positive - ("Our meat is unsafe" - when it was safe) - you are left with the consequences of the false negative. ("Our meat is safe - when it was not) Garth |
| Mar27-06, 01:07 PM | #24 |
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| Mar28-06, 11:57 AM | #25 |
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By Marcus.
So, for instance, he is critical of his fellow cosmologists, at least of the run-of-the-mill university cosmologist, because they often simply ASSUME that k = 0 exactly. That is, they favor the EXACTLY FLAT case so much that they oftentimes just take it for granted, according to Ellis. Thanks for your help so far Marcus. At the moment i can not see an alternative to making some assumptions, if cosmologists have no data to work with, what else can they do. I would like a laymans review of the search for matter in QG theories, from what i have read string theories are all most out of the picture for now, i may have the wrong take on that, is there anything new ? Thankyou, Garth, Space Tiger, Can you shed any light on the (particle) supersymetry, higs, side of cosmology? |
| Mar28-06, 12:15 PM | #26 |
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| Mar28-06, 12:22 PM | #27 |
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However, I don't think a detection or non-detection of the Higgs boson will have much of an impact on cosmology. Inflation is more of a phenomonological model at this point and doesn't rely on the existence of a particular particle species. |
| Mar28-06, 12:28 PM | #28 |
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(Edit crossed with ST's post)
Big Bang studies has been a forced marriage between two incompatible partners: GR and QM, nevertheless the marriage has been, or has the potential of being, very fruitful. On the one hand GR cosmology has required Inflation, DM and DE, on the other fundamental particle physics has required higher and higher energy accelerators to test the Standard Theory, and you cannot get any higher energy than the BB itself! The Standard Theory has thrown up countless hypothetical particles that need experimental verification, if they cannot be found in a large accelerator, such as the LHC being built at present, then an alternative is to try to find them in the BB. Cosmological constraints have filtered out possible candidates, although there are many still to go. QM requires the Higgs Boson to impart inertial mass to particles and GR requires the energy of its scalar field, or of another hypothetical inflaton particle, to impart a massive exponential expansion in the first 10-35sec or so of the universe's history. It was predicted to be detectable in present particle accelerators but so far without success, perhaps the LHC will deliver. DM requires a particle with all the right properties to explain the large scale features of the universe including the rotation rates of spiral galaxies. One likely candidate at the moment is the LSP or lightest supersymmetric particle. We will only know what we are talking about when these particles have actually been discovered, their properties measured and been found concordant with the cosmological constraints. Until then GR and the Standard Model must remain, well, provisional. Garth |
| Mar28-06, 12:29 PM | #29 |
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ST, this may be a stupid question, but what evidence do we have that the
CMB is only observed as it is from our view, could observation from another galaxy give different results ? |
| Mar28-06, 12:38 PM | #30 |
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As such it would look more or less the same from any galaxy at this present epoch. Its temperature will depend on the epoch of observation. However the largest anisotropy of the CMB, 100X larger than the rest, is the dipole caused by our peculiar motion relative to that SLS. As each galaxy has its own peculiar motion, and planets their own trajectories within those galaxies it will be this dipole that will differ from planet to planet, star to star and galaxy to galaxy. Garth |
| Mar28-06, 12:39 PM | #31 |
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In situ measure of the cosmic microwave background temperature at a distance of 7.5 kiloparsecs It's not a very powerful technique, however, and can only give us very crude measurements of the temperature. Measuring the anisotropies remotely is probably a long way off, if possible at all. |
| Mar29-06, 07:01 AM | #32 |
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A question i have with held for lack of research, but, how can it be shown that the CMB is a relic of the BB, every one seems to assume it is, but i guess, there is not a unique signature for this radiation.
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| Mar29-06, 10:51 AM | #33 |
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There have been sugestions from the Steady State 'school' in the 1970s that the CMB might be either the sum total of background galaxies - Olber's paradox red-shifted into the micro-wave region.
Or, in Fred Hoyle's mass field theory fundamental particle masses decrease as you out in space until you reach the membrane where m = 0, which we interpret as the BB. The CMB was then claimed to be the smoothed out radiation from galaxies beyond that membrane, (presumeably with negaitve masses.) These suggestions were long shots, which did not explain the CMB isotropy and would not have survived the discovery of the anisotropies at the 10-5 level. Garth |
| Mar29-06, 01:02 PM | #34 |
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Thankyou , Garth, i admit i am learning a lot about the fundamental reasons
for the SM, but i am cursed with the ability to see other views, i think it is like a retail outlook, one sees an opening and tries to fill it, but this is wrong for cosmology, one should not try to fill in the gaps untill the market ressearch has been done. |
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