courses:ast403:lyman-break-technique
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| courses:ast403:lyman-break-technique [2026/03/26 07:35] – [Advantages and Limitations] shuvo | courses:ast403:lyman-break-technique [2026/03/26 07:49] (current) – [Advantages and Limitations] shuvo | ||
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| If a galaxy is at a redshift of $z = 3$, the Lyman break is shifted from $912 \mathring{A}$ to roughly $3648 \mathring{A}$, | If a galaxy is at a redshift of $z = 3$, the Lyman break is shifted from $912 \mathring{A}$ to roughly $3648 \mathring{A}$, | ||
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| ===== The " | ===== The " | ||
| Astronomers do not usually have the time to take detailed spectra of every single point of light in the sky to see where this break occurs. Instead, they use a highly efficient shortcut called broadband photometry. | Astronomers do not usually have the time to take detailed spectra of every single point of light in the sky to see where this break occurs. Instead, they use a highly efficient shortcut called broadband photometry. | ||
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| **Efficiency: | **Efficiency: | ||
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| **Targeting: | **Targeting: | ||
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courses/ast403/lyman-break-technique.1774532100.txt.gz · Last modified: by shuvo
