A Summing Up — Question 2

Section 44-14 · Physics pages 7554–7555

Question 2 A relic neutrino changes from radiation-like to matter-like behavior For a decoupled relic use Tν0 = 1.95 K, typical momentum pc = 3.15kBTν and Tν = Tν0(1 + z). Let mass energy be .050 eV and kB = 8.62 × 10−5 eV/K. t hot decoupling today Schematic; labels, not drawing lengths, specify the data. (a) Estimate the redshift where typical pc equals the rest energy. (b) For total particle plus antiparticle density 112 cm−3 for this mass eigenstate, estimate present rest-energy density and state its later scale-factor dependence.
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Question 2 - Solution A relic neutrino changes from radiation-like to matter-like behavior t hot decoupling today (a) Method and calculation 1 + znr = .050 3.15(8.62 × 10−5)(1.95). 1 + znr ≃94.43, znr ≃93.43 . (b) Interpretation and further calculation uν,0 ≃nνmc2 = 112(.050) = 5.60 eV/cm3 . uν ∝a−3 when nonrelativistic, uν ∝a−4 when relativistic . Physical check The transition is gradual across a momentum distribution. The specified density refers to one eigenstate including its antiparticle, avoiding an extra factor of two.

Question 2

A relic neutrino changes from radiation-like to matter-like behavior

For a decoupled relic use Tν0=1.95T_{\nu0}=1.95 K, typical momentum pc=3.15kBTνpc=3.15k_BT_\nu and Tν=Tν0(1+z)T_\nu=T_{\nu0}(1+z). Let mass energy be .050 eV and kB=8.62×10−5k_B=8.62\times10^{-5} eV/K.

Diagram shown in the original SVG worksheet.

  1. Estimate the redshift where typical pc equals the rest energy.

  2. For total particle plus antiparticle density 112 cm−3^{-3} for this mass eigenstate, estimate present rest-energy density and state its later scale-factor dependence.

Question 2 - Solution

A relic neutrino changes from radiation-like to matter-like behavior

Diagram shown in the original SVG worksheet.

(a) Method and calculation

1+znr=.0503.15(8.62×10−5)(1.95).1+z_{\mathrm{nr}}=\frac{.050}{3.15(8.62\times10^{-5})(1.95)}.1+znr≃94.43,znr≃93.43.\boxed{1+z_{\mathrm{nr}}\simeq94.43,\quad z_{\mathrm{nr}}\simeq93.43}.

(b) Interpretation and further calculation

uν,0≃nνmc2=112(.050)=5.60eV/cm3.\boxed{u_{\nu,0}\simeq n_\nu mc^2=112(.050)=5.60\ {\mathrm{eV/cm^3}}}.uν∝a−3when nonrelativistic,uν∝a−4when relativistic.\boxed{u_\nu\propto a^{-3}\ \text{when nonrelativistic},\quad u_\nu\propto a^{-4}\ \text{when relativistic}}.

Physical check

The transition is gradual across a momentum distribution. The specified density refers to one eigenstate including its antiparticle, avoiding an extra factor of two.