... 2 - (6 + 5 + 3 ) sin - (4 5 + 2 3 ) cos + 6 cos = S1 , m (2) v cos cos 2 - v sin cos 2 - 2 v cos sin 2 + +6 v cos sin 2 - 4 v sin cos 1 + 2 v sin sin 1 + 2 2 2 + (6 + 4 + 2 ) cos + (4 5 + 2 3 ) sin + 6 sin = S2 , m (3) v sin cos 1 + v cos cos 1 - 1 v sin ...
... Alam M.S. Dept of Geology and Mining University of Rajshahi Rajshahi 6205 Bangladesh ... Durham University M.J.Alexander@durham.ac.uk South Road Durham City DH1 3LE Great ...
... jet, where t jet is the epoch when the bulk Lorentz factor of the ejecta becomes ... gcn3 Mangano, V., Capalbi, M., Pagani, C., Goad, M., Kennea, J., & Burrows, D. Foley ...
... M.I.Rjabov, A.L.Suharev, R.A.Sych, H.D.Aller, M.F.Aller WAVELET ANALYSIS ACTIVITY "CORE-JET" OF QUASARS AND BLAZARS IN ... c . 1. () , . , , . : M= N ? mM , m ? N ? . - M - m oo M= 2 4 m G hc 2 mMm 2. , . (t) tвз = mm ? ...
... 99). 51 With m (M. yr1) feeback 103 . 104 m . ... 104 m . evap 10 100 m* (M.) 1,000 Figure 2 | Feedback-limited accretion. ... Change in mass (m) versus _ protostellar mass (m*) for a number of key processes. ...
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