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6 Nov 2018: a1/2da. (9.24). Performing the simple integration and now changing to redshift, we have:.

6 Nov 2018: IRJνIRJν. = 2y (10.23). and. y =. kT. mec2σT ne dl (10.24). ... Note that the so-called. Compton y parameter in eq. 10.24 increases with T, since the temperaturedetermines the average energy transfer per scattering event.

6 Nov 2018: Savelainen. 30,52, G. Savini. 96. , D. Scott. 24. , M.

13 Nov 2018: 20. 8πGmH(12.16). (Y is the baryonic mass fraction in He: Yp = 0.24) and. ... bT (. 2kT. mH. )1/2= 12.8 T. 1/24 km s. 1 (12.22).

22 Nov 2018: 16.22 is: 〈. v2〉. = 3 (880 km s1. )2(16.24). The half-mass radius is trickier. ... Experimentsusing solar, atmospheric, and reactor neutrinos have measured mass dif-. 24.

30 Jul 2018: 24). to eject particles, as for some planets, particles migrate pasttoo fast for them to be ejected. ... 24), and the solid line shows where the timescale for accretion is equal to that for PR-drag, according to the empiricalfit presented here,

31 Jul 2018: radius, and albedo Cont. 3 8.16 9.24 8.67 83 Existence of atmosphere Cont. ... The Messenger 143:16–24. Errmann R, Minardi S, Labadie L, Muthusubramanian B, Dreisow F, NolteS, Pertsch T (2015) Interferometric nulling of four channels with

2 Apr 2018: 95418 β UMa 4 A1 IV 2.341 2.38 4.2 24.5 316 Y/N 5,6. ... 173667 110 Her 0.126 0.096 0.101 0.115 24 0.561 0.157 cons.

30 Jul 2018: F7 V 4.126 2.83 2.4 13.7 137 N/– [22, 24, 28]. ... J., Stapelfeldt,K. R., and Wyatt, M. C., “Target Selection for the LBTI Exozodi Key Science Program,” ApJS 216, 24(Feb.

9 Nov 2018: θ λ Depth. 3542116 1268.2 11.0 1.05 0.24 0.23 0.001033542116 991.9 8.3 1.08 0.28 0.25 0.00074. ... For KIC 8027456, assuming M? = 2M, R? = 1.5R?,and θ = 0.24 days yields an upper limit of rt < 1.4au, and acircular period of 1.1 years.