scholarly journals Study of the Virgo Cluster Using the B ‐Band Tully‐Fisher Relation

1997 ◽  
Vol 108 (2) ◽  
pp. 417-448 ◽  
Author(s):  
Naoki Yasuda ◽  
Masataka Fukugita ◽  
Sadanori Okamura
2003 ◽  
Vol 126 (6) ◽  
pp. 2622-2634 ◽  
Author(s):  
J. L. Hinz ◽  
G. H. Rieke ◽  
N. Caldwell

1997 ◽  
Vol 485 (1) ◽  
pp. 80-86 ◽  
Author(s):  
Anthony H. Gonzalez ◽  
S. M. Faber
Keyword(s):  

2008 ◽  
Vol 681 (1) ◽  
pp. 197-224 ◽  
Author(s):  
Eric W. Peng ◽  
Andrés Jordán ◽  
Patrick Côté ◽  
Marianne Takamiya ◽  
Michael J. West ◽  
...  

2004 ◽  
Vol 13 (07) ◽  
pp. 1297-1307
Author(s):  
HERMAN J. MOSQUERA CUESTA ◽  
KAREN FIUZA

During the core bounce of a supernova collapse resonant active-to-active (νa→νa), as well as active-to-sterile (νa→νs) neutrino (ν) oscillations can take place. Besides, over this phase weak magnetism increases antineutrino [Formula: see text] mean free paths, and thus its luminosity. Because the oscillation feeds mass-energy into the target ν species, the large mass-squared difference between species (νa→νs) implies a huge amount of power to be given off as gravitational waves (L GWs ~1049 erg s -1), due to anisotropic but coherent ν flow over the oscillation length. This anisotropy in the ν-flux is driven by both the universal spin-rotation and the spin-magnetic coupling. The new spacetime strain estimated this way is still several orders of magnitude larger than those from ν diffusion (convection and cooling) or quadrupole moments of the neutron star matter. This new feature turns these bursts the more promising supernova gravitational-wave signal that may be detected by observatories as LIGO, VIRGO, etc., for distances far out to the VIRGO cluster of galaxies.


2013 ◽  
Vol 764 (1) ◽  
pp. 60 ◽  
Author(s):  
E. Roediger ◽  
R. P. Kraft ◽  
W. R. Forman ◽  
P. E. J. Nulsen ◽  
E. Churazov

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