courses:ast403:gunn-peterson-test
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| courses:ast403:gunn-peterson-test [2026/03/23 22:27] – [Gunn-Peterson Effect] shuvo | courses:ast403:gunn-peterson-test [2026/03/28 01:37] (current) – [Implications and Sensitivity] shuvo | ||
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| ====== Gunn-Peterson Effect ====== | ====== Gunn-Peterson Effect ====== | ||
| - | The Gunn-Peterson effect is a feature in the spectra of distant quasars caused by the presence of neutral hydrogen in the Intergalactic Medium (IGM). It serves as a powerful diagnostic tool for determining the ionization state of the universe | + | The Gunn-Peterson effect is a feature in the spectra of distant quasars caused by the presence of neutral hydrogen in the Intergalactic Medium (IGM). It serves as a powerful diagnostic tool for determining the ionization state of the Universe |
| - | The general explanation for this is the Gunn-Peterson effect | + | According to Gunn-Peterson effect beyond a certain redshift the Universe |
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| ===== Physical Concept ===== | ===== Physical Concept ===== | ||
| As light from a distant quasar travels toward Earth, it is continuously redshifted. If it encounters any neutral hydrogen ($HI$) along the way, photons that have been redshifted into the Lyman-alpha ($\text{Ly}\alpha$) resonance frequency ($121.6 \text{ nm}$) will be scattered. | As light from a distant quasar travels toward Earth, it is continuously redshifted. If it encounters any neutral hydrogen ($HI$) along the way, photons that have been redshifted into the Lyman-alpha ($\text{Ly}\alpha$) resonance frequency ($121.6 \text{ nm}$) will be scattered. | ||
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| ===== Mathematical Formulation ===== | ===== Mathematical Formulation ===== | ||
| The strength of the effect is measured by the Gunn-Peterson optical depth, denoted as $\tau_{GP}$. The optical depth for $\text{Ly}\alpha$ scattering at a redshift $z_{abs}$ is given by: | The strength of the effect is measured by the Gunn-Peterson optical depth, denoted as $\tau_{GP}$. The optical depth for $\text{Ly}\alpha$ scattering at a redshift $z_{abs}$ is given by: | ||
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| ===== Relation to Cosmological Parameters ===== | ===== Relation to Cosmological Parameters ===== | ||
| - | In a standard $\Lambda$CDM cosmology, for high redshifts where the universe | + | In a standard $\Lambda$CDM cosmology, for high redshifts where the Universe |
| $$\tau_{GP}(z) \approx 4.9 \times 10^5 \left( \frac{\Omega_m h^2}{0.13} \right)^{-1/ | $$\tau_{GP}(z) \approx 4.9 \times 10^5 \left( \frac{\Omega_m h^2}{0.13} \right)^{-1/ | ||
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| The most striking aspect of the formula is the coefficient ($~10^5$). This indicates that even a tiny amount of neutral hydrogen causes massive absorption: | The most striking aspect of the formula is the coefficient ($~10^5$). This indicates that even a tiny amount of neutral hydrogen causes massive absorption: | ||
| **High Sensitivity: | **High Sensitivity: | ||
| - | **The Reionization " | + | **The Reionization " |
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| ===== Comparison: LLS vs. Gunn-Peterson ===== | ===== Comparison: LLS vs. Gunn-Peterson ===== | ||
| While the Lyman-limit systems (LLSs) mentioned previously represent discrete, dense clouds (optically thick at $912 \text{ Å}$), the Gunn-Peterson effect represents the global, diffuse state of the IGM (optically thick at $1216 \text{ Å}$). | While the Lyman-limit systems (LLSs) mentioned previously represent discrete, dense clouds (optically thick at $912 \text{ Å}$), the Gunn-Peterson effect represents the global, diffuse state of the IGM (optically thick at $1216 \text{ Å}$). | ||
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| - | If the Gunn-Peterson trough is present, it suggests the observer is looking back into the Epoch of Reionization, | + | If the Gunn-Peterson trough is present, it suggests the observer is looking back into the Epoch of Reionization, |
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