23 research outputs found

    Confrontation of a Double Inflationary Cosmological Model with Observations

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    CDM models with non-scale-free step-like spectra of adiabatic perturbations produced in a realistic double inflationary model are compared with recent observational data. The model contains two additional free parameters relatively to the standard CDM model with the flat (n=1n=1) initial spectrum. Results of the COBE experiment are used for the determination of a free overall spectrum normalization. Then predictions for the galaxy biasing parameter, the variance for "counts in cells", the galaxy angular correlation function, bulk flow peculiar velocities and the Mach number test are obtained. Also considered are conditions for galaxy and quasar formation. Observational data strongly restricts allowed values for the two remaining model parameters. However, a non-empty region for them satisfying all considered tests is found.Comment: 17 pages and 4 figures obtainable by request, LaTex, AIP 93-1

    HST Observations of the QSO pair Q1026-0045A,B

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    The spatial distribution of the Lyα\alpha forest is studied using new HST data for the quasar pair Q~1026--0045 A and B at zemz_{em} = 1.438 and 1.520 respectively. The angular separation is 36 arcsec and corresponds to transverse linear separations between lines of sight of ∼300h50−1\sim300h^{-1}_{50} kpc (qoq_{o} = 0.5) over the redshift range 0.833 < z < 1.438. From the observed numbers of coincident and anti-coincident Lyα\alpha absorption lines, we conclude that, at this redshift, the Lyα\alpha structures have typical dimensions of ∼500h50−1\sim500h^{-1}_{50} kpc, larger than the mean separation of the two lines of sight. The velocity difference, ΔV\Delta V, between coincident lines is surprisingly small (4 and 8 pairs with ΔV<50and200km/srespectively).Metallinesystemsarepresentat\Delta V < 50 and 200 km/s respectively). Metal line systems are present at z_{abs}=1.2651and1.2969inA, = 1.2651 and 1.2969 in A, z_{abs}=0.6320,0.7090,1.2651and1.4844inB.InadditionwetentativelyidentifyaweakMgIIsystemat = 0.6320, 0.7090, 1.2651 and 1.4844 in B. In addition we tentatively identify a weak Mg II system at z_{abs}=0.11inB.Itisremarkablethatthe = 0.11 in B. It is remarkable that the z_{abs}=1.2651systemiscommontobothlinesofsight.Thesystemat = 1.2651 system is common to both lines of sight. The system at z_{abs}=1.4844Thereisametal−poorassociatedsystemat = 1.4844 %is probably associated and has strong O~VI absorption. There is a metal-poor associated system at z_{abs}=1.4420alongthelineofsighttoAwithcomplexvelocityprofile.WedetectastrongLy = 1.4420 along the line of sight to A with complex velocity profile. We detect a strong Ly\alphaabsorptionalongthelineofsighttoBredshiftedbyonly300km/srelativelytotheassociatedsystem.Itistemptingtointerpretthisasthepresenceofadiskofradiuslargerthan300 absorption along the line of sight to B redshifted by only 300 km/s relatively to the associated system. It is tempting to interpret this as the presence of a disk of radius larger than 300h^{-1}_{50}$ kpc surrounding quasar A.Comment: 4 pages, 2 figures, A&A Letter acccepte

    Large-scale structure formation for power spectra with broken scale invariance

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    We have simulated the formation of large-scale structure arising from COBE-normalized spectra computed by convolving a primordial double-inflation perturbation spectrum with the CDM transfer function. Due to the broken scale invariance ('BSI') characterizing the primordial perturbation spectrum, this model has less small-scale power than the (COBE-normalized) standard CDM model. The particle-mesh code (with 5123512^3 cells and 2563256^3 particles) includes a model for thermodynamic evolution of baryons in addition to the usual gravitational dynamics of dark matter. It provides an estimate of the local gas temperature. In particular, our galaxy-finding procedure seeks peaks in the distribution of gas that has cooled. It exploits the fact that ``cold" particles trace visible matter better than average and thus provides a natural biasing mechanism. The basic picture of large-scale structure formation in the BSI model is the familiar hierarchical clustering scenario. We obtain particle in cell statistics, the galaxy correlation function, the cluster abundance and the cluster-cluster correlation function and statistics for large and small scale velocity fields. We also report here on a semi-quantitative study of the distribution of gas in different temperature ranges. Based on confrontation with observations and comparison with standard CDM, we conclude that the BSI scenario could represent a promising modification of the CDM picture capable of describing many details of large-scale structure formation.Comment: 15 pages, Latex using mn.sty, uuencoded compressed ps-file with 15 figures by anonymous ftp to ftp://ftp.aip.de/incoming/mueller/bsi.u
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