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5e). The constant term is the zero-point difference between bolometric magnitudes and the rrii band-pass magnitudes at zero redshift. It is the "bolometric correction" in the standard Hterature. 40), N[z, qo) = ^ ^ [1 - ^ ( 1 +

1. The quoted magnitudes here are on the system of the observations themselves, not yet corrected "for the effects of redshift", incorrect as these K corrections later proved to be, now discussed. 1e). His K term was composed both of the technical effect to the measured magnitudes of shifting the energy distribution through the (fixed) filter band pass, (accounting for the shape of the SED), but contrary to modern practice he also included a term (or terms) for the "effects of redshift". 1) above, the two factors of (1 + z) for the "energy" and the "number" effect.

54) ^0 T h e solutions of the Friedmann equation for various values of Q are, of course, classical, leading to the famous "coasting" solutions of Lemaitre (1950 for a popular account of his 1927 model for example; or Bondi 1952) with their increased time scales. A, fc Gamow, G. 1948, Phys. Rev. C, 1953, Phys. A. C. 1948, Phys. Rev. A. C. 1950, Rev. Mod. Phys. 22, 153 Berry, M. A. 1988, Ann. Rev. Astron. Astrophys. 26, 509 Bondi, H. , & Hoyle, F. 1957, Rev. Mod. Phys. D. 1968, 1983 Principles of Stellar Evolution and Nucleosynthesis (Chicago: Univ.

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