Cosmos 6: The Cosmic Background Radiation, the Cosmic Temperature, and Recombination

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    1. Keywords: blackbody radiation, blackbody spectrum (AKA Planck's law), Compton scattering, cosmic microwave background (CMB, T = 2.72548(57) K (Fixsen 2009)), dex → factor of 10, diffuse extragalactic background radiation (DEBRA), extragalactic background light (EBL), inverse centimeter (cm**(-1)), inverse Compton scattering, jansky (Jy) = 10**(-26) W/(m**2*Hz), microwave band (fiducial range 0.1--100 cm, 0.01--10 cm**(-1)), Sachs-Wolfe effect (Non-integrated Sachs-Wolfe effect, integrated Sachs-Wolfe effect), Sunyaev-Zel'dovich effect, Thomson scattering, Wien's law (see wien_law.html), etc.

    2. Blackbody file: blackbody_spectra.html

    3. Blackbody file: wien_law.html: Wien's law temperature allows you to determine of blackbody radiation field just by measuring the wavelength or frequency of the spectrum maximum.

    4. Cosmology file: cmb.html: See CMB features: T_0=2.7260(13) K (Fixsen 2009). The CMB is a nearly perfect blackbody spectrum: maybe almost the most perfect in nature that is NOT hidden in optically thick systems with temperature varying on a scale longer than photon mean free paths: i.e., the interior of opaque solids, liquids, and gases (e.g., the interior stellar structure of stars). For reference, see Wikipedia: Cosmic microwave background (CMB).

    5. Optical depth τ_rec since reionization: Most modern value 0.0561(71) which means I_modern=I_recombination*exp(-τ) ≅ I_recombination*(1-τ) ≅ 0.94*I_recombination. So most CMB has NOT been scattered by free electrons by Thomson scattering which randomize its direction. Randomization would erase our ability to know about know of the primordial density fluctuations at the recombination era t = 377,770(3200) Jyr = 1.192*10**13 s (z = 1089.80(21)). About the same amount of scattering has occurred to diffuse extragalactic background radiation (DEBRA).
      Note, if the τ_rec >> 1, there would still probably be fluctuations in the CMB and DEBRA, but they would NOT be primordial, but would be due to fluctuations free electron density in the intergalactic medium (IGM) due to a hypothetical higher density of the intergalactic medium (IGM) and/or some hypothetical feature of structure formation (AKA large-scale structure formation).
      Actually, in the late 1980s and early 1990s, people were worrying if the primordial density fluctuations were too small to be seen even if τ_rec << 1 as it is.

      The CMB temperature standard deviation (i.e., σ) is ∼ 100 microkelvins around the cosmic present CMB mean temperature T = 2.72548(57) K (Fixsen 2009). Put another way, the relative temperature variations are only 1 in 25000 (Wikipedia: Cosmic microwave background radiation: Features).

    6. Cosmology file: diffuse_extragalactic_background_radiation.html: Diffuse extragalactic background radiation (DEBRA): See Schematic DEBRA (2007), Barry Madore DEBRA (c.2000), Southampton DEBRA (c.2018?).

    7. Cosmology file: cmb_dipole_anisotropy.html.

    8. Cosmology file: cmb_wmap.html: In an all-sky sky map in Mollweide projection (see Wikipedia: Cosmic microwave background: Microwave background observations). The fluctuations are about 1/25000 or 100 μK (see Wikipedia: Cosmic microwave background: Features). This distorations result from primordial density fluctuations at the recombination era t = 377,770(3200) Jyr = 1.192*10**13 s (z = 1089.80(21)).

      Note, Stephen Hawking's (1942--) initials in dark blue embedded in the CMB all-sky sky map.

    9. Cosmology file: cosmic_temperature.html: Cosmic temperature evolution from 1e-10 s to 1e+16 s = 0.3 Gyr.
      For a better version, see Hergt & Scott, 2024, p. 5 and their table of important cosmic time points.
      in the Λ-CDM model.
      See also Cahill 2017, The eras of radiation, matter, and dark energy: new information from the Planck Collaboration for the time evolution of the cosmic scale factor according to the Λ-CDM model.

    10. inflation_horizon_problem.html: For CMB coming from all directions from the near the particle horizon and the horizon problem.

    11. cmb_power_spectrum.html.