scholarly journals Upper Bound of 0.28 eV on Neutrino Masses from the Largest Photometric Redshift Survey

2010 ◽  
Vol 105 (3) ◽  
Author(s):  
Shaun A. Thomas ◽  
Filipe B. Abdalla ◽  
Ofer Lahav
2011 ◽  
Vol 106 (24) ◽  
Author(s):  
Shaun A. Thomas ◽  
Filipe B. Abdalla ◽  
Ofer Lahav

2015 ◽  
Vol 2015 (06) ◽  
pp. 042-042 ◽  
Author(s):  
Tobias Basse ◽  
Jan Hamann ◽  
Steen Hannestad ◽  
Yvonne Y.Y. Wong

2019 ◽  
Vol 123 (8) ◽  
Author(s):  
Arthur Loureiro ◽  
Andrei Cuceu ◽  
Filipe B. Abdalla ◽  
Bruno Moraes ◽  
Lorne Whiteway ◽  
...  

2014 ◽  
Vol 11 (S308) ◽  
pp. 555-560 ◽  
Author(s):  
Yan-Chuan Cai ◽  
Nelson Padilla ◽  
Baojiu Li

AbstractWe investigate void properties inf(R)models using N-body simulations, focusing on their differences from General Relativity (GR) and their detectability. In the Hu-Sawickif(R)modified gravity (MG) models, the halo number density profiles of voids are not distinguishable from GR. In contrast, the samef(R)voids are more empty of dark matter, and their profiles are steeper. This can in principle be observed by weak gravitational lensing of voids, for which the combination of a spectroscopic redshift and a lensing photometric redshift survey over the same sky is required. Neglecting the lensing shape noise, thef(R)model parameter amplitudesfR0=10-5and 10-4may be distinguished from GR using the lensing tangential shear signal around voids by 4 and 8 σ for a volume of 1 (Gpc/h)3. The line-of-sight projection of large-scale structure is the main systematics that limits the significance of this signal for the near future wide angle and deep lensing surveys. For this reason, it is challenging to distinguishfR0=10-6from GR. We expect that this can be overcome with larger volume. The halo void abundance being smaller and the steepening of dark matter void profiles inf(R)models are unique features that can be combined to break the degeneracy betweenfR0and σ8.


2019 ◽  
Vol 488 (4) ◽  
pp. 4565-4584 ◽  
Author(s):  
Rongpu Zhou ◽  
Michael C Cooper ◽  
Jeffrey A Newman ◽  
Matthew L N Ashby ◽  
James Aird ◽  
...  

ABSTRACT We present catalogues of calibrated photometry and spectroscopic redshifts in the Extended Groth Strip, intended for studies of photometric redshifts (photo-z’s). The data includes ugriz photometry from Canada–France–Hawaii Telescope Legacy Survey (CFHTLS) and Y-band photometry from the Subaru Suprime camera, as well as spectroscopic redshifts from the DEEP2, DEEP3, and 3D-HST surveys. These catalogues incorporate corrections to produce effectively matched-aperture photometry across all bands, based upon object size information available in the catalogue and Moffat profile point spread function fits. We test this catalogue with a simple machine learning-based photometric redshift algorithm based upon Random Forest regression, and find that the corrected aperture photometry leads to significant improvement in photo-z accuracy compared to the original SExtractor catalogues from CFHTLS and Subaru. The deep ugrizY photometry and spectroscopic redshifts are well suited for empirical tests of photometric redshift algorithms for LSST. The resulting catalogues are publicly available at http://d-scholarship.pitt.edu/36064/. We include a basic summary of the strategy of the DEEP3 Galaxy Redshift Survey to accompany the recent public release of DEEP3 data.


2003 ◽  
Vol 586 (2) ◽  
pp. 745-764 ◽  
Author(s):  
Hsiao‐Wen Chen ◽  
Ronald O. Marzke ◽  
Patrick J. McCarthy ◽  
P. Martini ◽  
R. G. Carlberg ◽  
...  

1990 ◽  
Vol 246 (1-2) ◽  
pp. 141-143 ◽  
Author(s):  
Ann E. Nelson ◽  
S.M. Barr
Keyword(s):  

2011 ◽  
Vol 415 (2) ◽  
pp. 1479-1508 ◽  
Author(s):  
J. L. Wardlow ◽  
Ian Smail ◽  
K. E. K. Coppin ◽  
D. M. Alexander ◽  
W. N. Brandt ◽  
...  

1995 ◽  
Vol 10 (20) ◽  
pp. 1471-1477 ◽  
Author(s):  
TAKEO INAMI ◽  
TADASHI KAWAKAMI ◽  
C.S. LIM

We show that precision measurements of the oblique correction parameters S and T can be used to derive an upper bound on the number of extra generations of heavy fermions Neg. The bound depends on the type of heavy neutrino masses. We have obtained Neg≤2 in the case of Dirac neutrinos and Neg≤5 in the case of neutrinos with Majorana masses, under some assumptions on the flavor and color contents of extra generations.


2001 ◽  
Vol 16 (supp01b) ◽  
pp. 709-711 ◽  
Author(s):  
J. M. NICZYPORUK

We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upper bound is [Formula: see text], where v ≃246 GeV is the weak scale and mν is the Majorana-neutrino mass. For neutrino masses implied by neutrino oscillation experiments, all but one of these bounds are less than the Planck scale, and they are all within a few orders of magnitude of the grand-unification scale.


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