Introduction to Cosmology Ryden · Problem 2.6

Fundamental Observations

Physics — Astrophysics · blackbody-low-energy-fraction

Problem

Show that for an energy threshold E0≪kTE_0 \ll kT, the fraction of blackbody photons that have energy hf<E0hf < E_0 is n(hf<E0)nγ≈0.21(E0kT)2.(2.44)\frac{n(hf < E_0)}{n_{\gamma}} \approx 0.21 \left(\frac{E_0}{kT}\right)^2. \tag{2.44} Microwave (and far infrared) photons with a wavelength λ<3 cm\lambda < 3\,\mathrm{cm} are strongly absorbed by H2O\mathrm{H_2O} and O2\mathrm{O_2} molecules. What fraction of the photons in today's cosmic microwave background have λ>3 cm\lambda > 3\,\mathrm{cm}, and thus are capable of passing through the Earth's atmosphere and being detected on the ground?

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