Cosmic microwave background fits the blackbody radiation spectrum

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SUMMARY

The cosmic microwave background (CMB) exhibits a blackbody radiation spectrum with a temperature of 2.7 K and a peak wavelength of 1.9 nm. The relationship between radiant emittance and photon energy density is crucial for estimating the number of CMB photons per cm³ in outer space. High-energy cosmic rays, primarily protons, encounter a threshold energy limit known as the GZK cut-off due to interactions with CMB photons, specifically the reaction p + γ → Δ⁺, which subsequently decays into p + π⁰ or n + π⁰. The masses of protons and Δ baryons are approximately 938 MeV/c² and 1232 MeV/c², respectively.

PREREQUISITES
  • Understanding of blackbody radiation and its mathematical representation.
  • Familiarity with cosmic microwave background (CMB) properties.
  • Knowledge of high-energy particle interactions, particularly involving protons.
  • Basic concepts of particle physics, including baryon masses and decay processes.
NEXT STEPS
  • Calculate the number of CMB photons per cm³ using the formula for radiant emittance.
  • Research the GZK cut-off and its implications for cosmic ray physics.
  • Study the decay processes of Δ baryons and their conservation laws in particle physics.
  • Explore the relationship between temperature, wavelength, and energy in blackbody radiation.
USEFUL FOR

Astrophysicists, particle physicists, and students studying cosmic rays and blackbody radiation phenomena will benefit from this discussion.

rbwang1225
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Homework Statement


(a)The cosmic microwave background fits the blackbody radiation spectrum well with a temperature of 2.7 K and a corresponding peak wavelength at 1.9nm. Applying the relationship between the radiant emittance, i.e. the total power emitted per unit area, and the photon energy density for the blackbody radiation to estimate the number of CMB photons per \mathrm{cm}^3 in outer space.

(b) The high energy cosmic rays are believed to be mostly protons and the max energies observed on Earth seem to have a bound. This upper bound is explained by collisions between the high energy protons traveling from extra-galactic space and the CMB photons. If the proton energy is high enough and exceed a threshold value, the following process could occur p+\gamma\rightarrow\Delta^+, \Delta^+\rightarrow p\pi^0\text{ (or }n\pi^0\text{)}. Therefore, the proton energy observed on Earth is decreased and there exists a so called GZK cut-off. Please determine this energy threshold in eV. The masses of the proton and \Delta baryons are about 938Mev/c^2 and 1232 MeV/c^2.

The Attempt at a Solution


Is the answer of (a) be \sigma T^4/hc^2/\lambda?
I have no idea about (b).
Any help would be appreciated.
 
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rbwang1225 said:

Homework Statement


(a)The cosmic microwave background fits the blackbody radiation spectrum well with a temperature of 2.7 K and a corresponding peak wavelength at 1.9nm. Applying the relationship between the radiant emittance, i.e. the total power emitted per unit area, and the photon energy density for the blackbody radiation to estimate the number of CMB photons per \mathrm{cm}^3 in outer space.

(b) The high energy cosmic rays are believed to be mostly protons and the max energies observed on Earth seem to have a bound. This upper bound is explained by collisions between the high energy protons traveling from extra-galactic space and the CMB photons. If the proton energy is high enough and exceed a threshold value, the following process could occur p+\gamma\rightarrow\Delta^+, \Delta^+\rightarrow p\pi^0\text{ (or }n\pi^0\text{)}. Therefore, the proton energy observed on Earth is decreased and there exists a so called GZK cut-off. Please determine this energy threshold in eV. The masses of the proton and \Delta baryons are about 938Mev/c^2 and 1232 MeV/c^2.

The Attempt at a Solution


Is the answer of (a) be \sigma T^4/hc^2/\lambda?
I don't know if your expression is anywhere near correct, but I just wanted to ask if you meant
##\sigma T^4/(hc^2/\lambda)## or ##(\sigma T^4/hc^2)/\lambda##.

Explain how you came up with your answer.

I have no idea about (b).
Any help would be appreciated.
You're asked to find the energy threshold. Why would ##p+\gamma\rightarrow\Delta^+## happen at some energies and not others?

By the way, ##\Delta^+ \to n\pi^0## violates conservation of charge. It can't happen. Perhaps you meant ##\Delta^+ \to n\pi^+##.
 

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