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Dwarf galaxies in multistate scalar field dark matter halos
Dwarf galaxies in multistate scalar field dark matter halos

The effect of the environment on the HI scaling relations
The effect of the environment on the HI scaling relations

Ground-based variability surveys towards Centaurus A: worthwhile
Ground-based variability surveys towards Centaurus A: worthwhile

... Context. Difference imaging has proven to be a powerful technique for detecting and monitoring the variability of unresolved stellar sources in M 31. Using this technique in surveys of galaxies outside the Local Group could have many interesting applications. Aims. The goal of this paper is to test d ...
Dark bursts - indico in2p3
Dark bursts - indico in2p3

Morphology and Environment
Morphology and Environment

Dark baryonic matter
Dark baryonic matter

... cannot be distinguished : addition of images = amplification • But : amplification effect varies with time as lens passes in front of source - period T • Efficient for observation of e.g. faint stars ...
The paper on the Hubble constant published in 2010
The paper on the Hubble constant published in 2010

Chalmers Un
Chalmers Un

VLT adaptive optics search for luminous substructures in the lens
VLT adaptive optics search for luminous substructures in the lens

Carbon monoxide in clouds at low metallicity in the dwarf irregular
Carbon monoxide in clouds at low metallicity in the dwarf irregular

The Void Probability Function and Related Statistics
The Void Probability Function and Related Statistics

... Constraining the HOD parameters Berlind and Weinberg 2002, Tinker, Weinberg & Warren 2006 Void statistics expected to be sensitive to HOD at low halo masses BW02: M =(M/M1)a with a lower cutoff Mmin Strong correlation between the minimum mass scale Mmin / size of voids TWW06: M = M +
The Universe - the Scientia Review
The Universe - the Scientia Review

High molecular gas fractions in normal massive star
High molecular gas fractions in normal massive star

The life-cycle of star formation in distant clusters
The life-cycle of star formation in distant clusters

The Physical Nature of Cosmic Accretion of Baryons and Dark Matter
The Physical Nature of Cosmic Accretion of Baryons and Dark Matter

... our assumed mass profile inside the halo. For example, using an isothermal profile instead of NFW gives results that are consistent at the ∼ 10% level. Figure 2 shows the predicted values of the enclosed overdensity. Throughout this paper, we define overdensities relative to the mean matter density, ...
17.1 Introduction
17.1 Introduction

Coevolution of SMBHs and host galaxies at high z
Coevolution of SMBHs and host galaxies at high z

... • If the AGN fraction is larger in the protocluster simply due to the presence of more massive SMBHs, then an average protocluster AGN would be more luminous than an average field AGN by the same factor • For this to be the case, the SMBHs would have to be ≈3−10 times more massive in the protocluste ...


Comparing molecular gas across cosmic time
Comparing molecular gas across cosmic time

An additional term of the Galactic tide due to dark matter
An additional term of the Galactic tide due to dark matter

OLIMPO
OLIMPO

... • We have selected 40 nearby rich clusters to be measured in a single long duration flight. • For all these clusters high quality data are available from XMM/Chandra ...
The Components of a Spiral Galaxy
The Components of a Spiral Galaxy

Galaxies at High Redshift Encyclopedia of Astronomy & Astrophysics eaa.iop.org Mauro Giavalisco
Galaxies at High Redshift Encyclopedia of Astronomy & Astrophysics eaa.iop.org Mauro Giavalisco

A limit on the number density of bright z ≈ 7 galaxies
A limit on the number density of bright z ≈ 7 galaxies

Slides
Slides

... The gravitational potential determines where the galaxies form and where the ISW fluctuations are created! Thus the galaxies and the CMB should be correlated, though its not a direct template. Most of the cross correlation arises on large or intermediate angular scales (>1degree). The CMB is well de ...
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Weak gravitational lensing



While the presence of any mass bends the path of light passing near it, this effect rarely produces the giant arcs and multiple images associated with strong gravitational lensing. Most lines of sight in the universe are thoroughly in the weak lensing regime, in which the deflection is impossible to detect in a single background source. However, even in these cases, the presence of the foreground mass can be detected, by way of a systematic alignment of background sources around the lensing mass. Weak gravitational lensing is thus an intrinsically statistical measurement, but it provides a way to measure the masses of astronomical objects without requiring assumptions about their composition or dynamical state.
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