To disabuse the map of the universe.doc

免费查阅精品论文To disabuse the map of the universeDeng XiaomingChief Engineering Office, Kaiming Engineering Consultancy1607-1612, Huatian Building,6, North Xiaomachang, Haidian District, Beijing, PRC 100038dxmchinayahoo.com.cnAbstractThe redshift distribution of galaxies (SDSS data) on the logarithmic map of the universe is explained by the linear expansion hyperspherical model. Our computed result show that the density distribution of galaxies take two peaks at redshift 0.108 and 0.362 and two minimum at redshift 0.229 and 0.510. It is shown that our model may fit the map well. It is proposed that celestial sphere should be defined by the comoving coordinates system.Key words: redshift distribution, cosmic sound wave, large scale structure of the universe, redshift periodicity, SDSS, redshift survey, hyperspherical universe.1. IntroductionJ. Richard Gott III and his partners have done a great job. A magical logarithmic map of the universe 1 shows us a panoramic view of the universe. The present paper will try to explain the section of the map run from redshift 0.01 to 4.196 by the linear expansion hyperspherical model.Readers also may skip the following part in this section and start on section 2. As a matter of convenience for readers to follow the thread of our argument, first we review the useful equations, deductions or conclusions from before:As we know, the R-W metric for the case of spherical space isd 2 = c 2 dt 2 - R 2 (t)d 2 + sin 2 (d 2 + sin 2d 2 )If R(t)=kt 23(k is a constant) and let d=0 and coordinates =0, then- 1 -t 0 cdttR(t)= 0 d ,t 0 cdttkt= 0 d andk =cln t 0 .tForR(t0 ) = t0= 1 + Z , we have the redshift formulaR(t )tk = ln(1 + Z)c(1)We know that the period of Bolometric flux in the linear expansion hyperspherical universe is 43. If we consider that Karlssons quasar redshift periodicity 56 (statistical formulaln(1 + Z) 0.206 ) may be caused by the quasars nearby poles =, 2, 3(see the polar effector the lens effect of cosmic entire space 234), Eq. (1) can be written as:ln(1 + Z nk) =nc= k(n + ) , n= 1, 2, 3, where is a infinitesimal. The period is:cWe have discussed about comoving coordinates system for the case of spherical space before 7,- 2 -n +1 - n = , thenln(1 + Z) = ln(1 + Zn +1) ln(1 + Z n1 + Z kn +1 .) = ln =1 + Z ncLet =k/c，then ln(1+Z)= and k=c/. Where 0.206 is “the half periodic parameter”2(as we had defined before). By the way, the significance of was first clearly understood in the paper titled the linear expansion hyperspherical universe 3. By substituting k=c/ to Eq. (1), we have/=ln(1+Z), or Z= e-1.(2)Thus we obtain the solvable functional relations between redshift Z and coordinate .Bolometric flux in the linear expansion hyperspherical universe isl =04R 2 (tL)(1 + Z ) 2 sin 2 L. Substituting Eq. (2) to the left equation, we have0Ll =, let =, we obtain04R 2 (t)e 2 / sin 2 04R 2 (t )l = 0e 2 / sin 2 .(3)Where 0 is a constant 3.The periodic attenuation of Bolometric flux at identical phase position isl(n + f )=1，n=0, 1, 2, 3(4)l ( f )e 2nWhere f is a fixed phase and 0<f <.The derived function of Eq.(3) isdl = d2 0e 2 / sin 2 ( + ctg )3 and letdl = 0 , thendtg = . Solving theequation, we obtain = n + tg 1 ( ) , n=1, 2, 3(5)nWhere n is the positions where to get the interzone, n, (n+1) n=0, 1, 2, minimum value of brightness lmin.In the present paper, we need the formula to show the number of galaxies distributed in thedifferential interval of . Since the derivation step is too long to be shown here, see paper 3, theformula isdn = 2 N sin 2 .(6)d Where dn is the number of the galaxies in d and N is a constant, its signification is the total number of the galaxies in the universe.2. Comoving coordinates and Celestial sphereand a figure is shown belowReference Fig 1 (a), vector R, Rsin and Rsinsin are on mutually perpendicular plane P, P andP respectively.X1=OA=Rsinsinsin; X2=OB=Rsinsincos; X3=OC=Rsincos; X4=OD=Rcos- 9 -22222222We also have: R2=X1 +X2 +X3 +X4 =(OA)+(OB)+(OC)+(OD)Reference Fig 1 (b), on plane P, P and P, if angle increment of vector R, Rsin and Rsinsinare d, d and d respectively, the corresponding arc length are Rd, Rsind and Rsinsind,then at the end of vector R, we haveAD2=ds2=(Rd)2+(Rsind)2+(Rsinsind)2=R2d2+sin2 (d2+sin2d2)The so-called comoving coordinates system should define celestial sphere in math. Before, weconsider that the celestial sphere is an imaginary sphere of gigantic radius with the earth (or the sun) located at its center. Of course, such a coordinates system without altitude can not satisfy with modern astroobservation.In fact, the celestial sphere system is not imaginary but really exists, they are uninterrupted cosmic historical section observed on earth. In cosmic three-dimensional curved space, there isnt any gigantic radius but the objective value of redshift (yes, we can give the radius r=Rsin, but nor significance here). It is the redshift that measure the spatial deepness between a celestial object and the earth. We have already set up the relation between redshift and comoving coordinates by Eq. (2).See Fig 2 (a), in the linear expansion hyperspherical universe, the celestial sphere at =/4(redshift 0.053); /2 (redshift 0.108); 3/4 (redshift 0.167) are different in size and not concentric. Not like three-dimensional flat space, the size of the celestial sphere is maximum at =/2 (redshift 0.108) and zero at =0 (redshift 0) and (redshift 0.229). Because of cosmic expansion, the celestial sphere at =/4 (redshift 0.053) is bigger than it at 3/4 (redshift 0.167) in size. Where just is schematic, the same case is in normal region n, (n+1) n=0, 1, 2.From the following discussion in next section, we will see that all galaxies with same redshifts are distributed on a certain celestial sphere.For farther understanding, we might as well consider the two-dimensional case. See also Fig 2 (b), place our Earth at =0 (the end of R0) on the sphere S0 (note that the different spheres Sn, n=0, 1,2 are the cosmic evanescence space). The loops at =/4 on the sphere S1, at =/2 on thesphere S2 and at =3/4 on the sphere S3 can be looked as, see also Fig 2 (a), the celestial spheresat =/4 (redshift 0.053), at =/2 (redshift 0.108) and at =3/4 (redshift 0.167) inthree-dimensional case.3. To unscramble the logarithmic map of the universe from redshift 0.01 to 4.196J. Richard Gott III and his partners 1 have produced a new conformal map of the universe illustrating recent discoveries. On this, we are only interested in the region run from redshift 0.01 to 4.196. The dots appearing beyond M81 in their map are the 126,594 SDSS galaxies and quasars (with z < 5) in the equatorial plane (-2o<<2o), but these exclude regions 3.7hr8.7hr, andapproximately 16.7hr20.7hr because they cover the zone of avoidance close to the Galactic plane.The selective space form is flat case, they project the slices directly onto a two-dimensional flat sheet.Before farther discussion, we might as well notice that space types would affect the interpretation of a sample. See also Fig 2, if the cosmic space is hypersphere, the 3D picture or video that we used to demonstrate redshift slice survey would poses an optical illusion. Especially, the density distribution of galaxies would be factitiously diluted with the increase of redshift distance on the fan-shaped cone diagram.It is a great work indeed! When we got the first glance at the visual aid logarithmic map of the universe, what did we see? The rhythmic pattern of the universe came into view! It is such a projection that reveals the rhythmic features of the cosmic large-scale structure on two-dimensional rectangle plan. With the map that apparently accord with our visual habits, we can go in-depth step.First, we put our mark symbol on the clippings of the map run from redshift 0.01 to the top, seeFig 3.We have fully discussed about the distribution of galaxies and quasars in the linear expansion hyperspherical universe 3, and obtain the versiform Bolometric flux marked with Eq. (3) in this paper:l = 0e 2 / sin 2 3.Where =0.206; 0 =L/4R2(t0) is a constant. L is the absolute luminosity of an emission sourceslocated at coordinates , and l is its brightness observed by us at =0 (or time t0). For the record,L also can be defined as Lgalaxy, Lstar or Lquasar according to different subjects investigated. The number of galaxies distributed in the differential interval of is Eq. (6):dn = 2 N sin 2 3.d Where dn is the number of the galaxies in d and N is a constant, its signification is the total number of the galaxies in the universe. Supposing that a survey covers a solid angle of and Ns is the total number of galaxies in the solid angle, then N=4Ns/, and substituting it into above equation, we obtain another graspable formdn = 8N s sin 2 .(7)d Where Ns/ is also constant.By substituting Eq. (2) and its differentiald =dZ(1 + Z )to Eq. (7), we obtain other formdn =8N ssin 2 ln(1 + Z ) .(8)dZ(1 + Z )See also Fig 3, the distribution graph of dn/d or dn/dZ take two peak values at redshift 0.108 (=/2) and 0.362 (=3/2) , and take two minimum values at redshift 0.229 (=) and 0.510 (=2) in the region redshift Z<0.510 or < 2. Our model seems to fit the map well.We are only interested in the positions where the peak values and minimum values obtained, and do not care too much about the distribution form because there are several influence factors to distort the distribution curve. Such as the foreground celestial objects is hiding the background celestial objects from view; brightness variation of distant celestial objects; the distortion in size 4 etc. All of these factors result in missing galaxies in some part or making up the number in other part in sample space. Hereon we just discuss about the case of distortion in brightness.See also Fig 3, the bottom curve shows that the brightness of celestial objects nearby poles 3(=n, n=1, 2, 3or redshift 0.229, 0.510, 0.855) is brighter than they at other parts. The brightness of celestial objects marked as A, B, C.at =n , see Eq. (5), get the interzone minimum value, and the concrete value of Eq. (5) is n=n-1.50532. It is seen that n is nearbyn-/2, n=1, 2, 3.Comparing the brightness curve with the distribution graph of dn/d or dn/dZ in Fig 3, we see that the number of galaxies on the celestial sphere at =/2 and 3/2 or redshift distance 0.108 and0.362 get maximum value, see both Fig 2 and 3, but the brightness of the galaxies nearby the two points are the minimum value. It means that there are more missed galaxies around the two regions. In contrast, the number of galaxies on the celestial sphere nearby = and 2 or redshift distance 0.229 and 0.510 is close to zero, but the brightness of the galaxies nearby the two points is at maximum. This means that there is less or no missed galaxies around the two regions, and even some dark or dwarf galaxies appear to be there to make up the number.Fig 3 shows that our fundamental concern is the region run from the redshift 0.01 to 0.510 (<2) , where most of the celestial objects are SDSS galaxies. Especially, the dactylogram of our universe is vivid in the region run from the redshift 0.01 to 0.229 (<), and thereinto contains all famous patterns, such as the great wall etc. In the region = to 2 or the redshift 0.229 to 0.510, It looks a bit faint but the ridge along redshift 0.362 in vertical direction is obvious, and the valley along the redshift 0.510 in vertical direction is still visible.See Eq. (4), there is the periodic attenuation of Bolometric flux, and the degree of attenuation atidentical phase position isl (n + f )=1，n=0, 1, 2, 3 Where f is a fixed phase andl ( f )e 2n0<f <. Supposing that the interzone n, (n+1) n=0, 1, 2 lowest brightness in Fig 3 are lA, lB, lC .(see points A, B and C), if l(f)=lA, according to the formula, then lB=lA/e2 and lC=lA/e4, since =0.206, lB is 66.2% of lA and lC is 43.9% of lA through the rapid is decaying exponentially.Supposing that lg (brightness) express the minimal Bolometric flux of galaxies that can be discerned by receiver. If lA > lg in Fig 3, it means that all of the galaxies in the region from redshift0.01 to 0.229 or < could be seen, and if lA < lg, some of galaxies would be missed. By the way, the value of lg will become smaller and smaller with the development of the astronomical telescope.See also Fig 3, in the region from redshift 0.229 to 0.510 or = to 2, lB is 66.2% of lA, considering the bottom of brightness curve is relatively flat, it means that more galaxies were missing. Furthermore, in the region from redshift 0.510 to 0.855 or =2 to 3, lC is 43.9% of lA, which means that we could hardly see galaxies except those that are not too far from the poles (=n, n=1, 2, 3). Maybe this case corresponds to our guess. In fact, there should be more galaxies around the redshift 0.674 or =5/2, but they are too dark to be seen. It is seen that geometrical factor predominate if and how many galaxies can be seen in the region redshift Z<0.510 or <2, but beyond the region, the flux would be the leading factor.On the map, beyond the redshift 0.510 (or >2), most of the celestial objects are SDSS quasars. As we know, the condition of quasars is completely different from galaxies. See also Eq. (3) and 0 =L/4R2(t0), as a matter of distinction, the absolute luminosity L of celestial objects also can be defined as Lgalaxy of galaxy, Lstar of star and Lquasar of quasaraccording to different subjects investigated. The absolute luminosity of galaxy has been discussed before 3. Lgalaxy may be regarded as the average of absolute luminosities of all galaxies (except for so called dwarf galaxy), and the