2015
DOI: 10.1093/mnras/stv1762
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Cold galaxies

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Cited by 10 publications
(10 citation statements)
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“…Table 2 shows a comparison of the sky seen at 60 and at 500 µm, as seen in the RIFSCz and HerMES-SWIRE catalogues (Rowan-Robinson et al 2014). The most striking contrasts of 500µm selection, compared to 60 µm selection, are (i) a much higher fraction of high redshift galaxies (as predicted by Franceschini et al 1991), (ii) a much higher fraction of lensed objects (as predicted by Blain et al 2002), (iii) a much higher fraction of galaxies with cool or cold dust (RR et al 2010, Rowan-Robinson and Clements 2015.…”
Section: Comparison With Other Studiesmentioning
confidence: 99%
“…Table 2 shows a comparison of the sky seen at 60 and at 500 µm, as seen in the RIFSCz and HerMES-SWIRE catalogues (Rowan-Robinson et al 2014). The most striking contrasts of 500µm selection, compared to 60 µm selection, are (i) a much higher fraction of high redshift galaxies (as predicted by Franceschini et al 1991), (ii) a much higher fraction of lensed objects (as predicted by Blain et al 2002), (iii) a much higher fraction of galaxies with cool or cold dust (RR et al 2010, Rowan-Robinson and Clements 2015.…”
Section: Comparison With Other Studiesmentioning
confidence: 99%
“…However, the idea of static universe was discarded by Einstein after Hubble's experiment in year 1929. The cosmological constant was not paid attention till the year 1967 [3][4][5] when the loitering in the universe's expansion was observed and to support this a positive cosmological constant was considered. The great discovery in year 1998 [6,7], which confirmed that the universe is accelerating, gave the birth of many theories such as quintessence, K-essence, phantom field based model, Chaplygin gas model, cosmological constant based theories etc.…”
Section: Introductionmentioning
confidence: 99%
“…This measurement shows that our motion is characterised by a velocity of v ≃ 384 km/s toward the (l, b) = (264 • , 48 • ) direction. Attempts to obtain this signal in the LSS appeared as early as the 1960s (De Vaucouleurs & Peters 1968), whose efforts increased given the rapidly growing improvements of infra-red and optical galaxy surveys, such as the IRAS PSCz and 2MASS, during the following decades (Yahil et al 1986;Lahav et al 1988;Lynden-Bell et al 1989;Strauss et al 1992;Basilakos & Plionis 1998;Rowan-Robinson et al 2000;Maller et al 2003;Erdoǧdu et al 2006;Basilakos & Plionis 2006;Bilicki et al 2011). The goal, in these cases, was the amplitude and direction of the so-called clustering dipole, which gives a preferred direction in the low-z LSS due to the galaxy clustering responsible for the acceleration of the Local Group, thus allowing one to deter-mine the consistency (and convergence) with the CMB kinematic dipole.…”
Section: Introductionmentioning
confidence: 99%