courses:ast403:lyman-break-technique
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| courses:ast403:lyman-break-technique [2026/03/26 06:28] – [The "Dropout" Observation Method] 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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| They take images of the same patch of sky using multiple color filters—for example, Ultraviolet (U), Blue (B), Visible/ | They take images of the same patch of sky using multiple color filters—for example, Ultraviolet (U), Blue (B), Visible/ | ||
| - | **Finding a $z \approx 3$ Galaxy:** Because the Lyman break is shifted to about $3600 \text{ \AA}$, all light bluer than this is absorbed. When astronomers look at their images, the galaxy will be completely invisible in the U filter (which captures light around $3000 \mathring{A}$ - $4000 \mathring{A}$) but will suddenly appear brightly in the B, V, and R filters. Because the galaxy "drops out" of the U-band image, it is called a U-dropout.\\ | + | |
| - | **Finding a $z \approx 4$ Galaxy:** At this distance, the break shifts further into the visible spectrum (around $4500 \mathring{A}$). The galaxy will now be invisible in both the U and B filters, but visible in the V filter and beyond. This is a B-dropout. | + | [{{ : |
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| + | **Finding a $z \approx 3$ Galaxy:** Because the Lyman break is shifted to about $3600 \mathring{A}$, all light bluer than this is absorbed. When astronomers look at their images, the galaxy will be completely invisible in the U filter (which captures light around $3000 \mathring{A}$ - $4000 \mathring{A}$) but will suddenly appear brightly in the B, V, and R filters. Because the galaxy "drops out" of the U-band image, it is called a U-dropout.\\ | ||
| + | **Finding a $z \approx 4$ Galaxy:** At this distance, the break shifts further into the visible spectrum (around $4500 \mathring{A}$). The galaxy will now be invisible in both the U and B filters, but visible in the V filter and beyond. This is a B-dropout.\\ | ||
| **Finding a $z \approx 5$ Galaxy:** The break shifts further, making the galaxy a V-dropout. | **Finding a $z \approx 5$ Galaxy:** The break shifts further, making the galaxy a V-dropout. | ||
| Galaxies found using this method are collectively referred to as **Lyman-Break Galaxies (LBGs)**. | Galaxies found using this method are collectively referred to as **Lyman-Break Galaxies (LBGs)**. | ||
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| ===== Advantages and Limitations ===== | ===== Advantages and Limitations ===== | ||
| **Advantages: | **Advantages: | ||
| - | **Efficiency: | + | |
| + | **Efficiency: | ||
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| **Targeting: | **Targeting: | ||
| **Limitations: | **Limitations: | ||
| - | **Interlopers: | + | |
| + | **Interlopers: | ||
| **Selection Bias:** It primarily detects incredibly bright, actively star-forming galaxies (since they produce the UV light necessary for a strong break). Quiescent (dead) galaxies or highly dust-obscured galaxies at the same redshift might be missed entirely. | **Selection Bias:** It primarily detects incredibly bright, actively star-forming galaxies (since they produce the UV light necessary for a strong break). Quiescent (dead) galaxies or highly dust-obscured galaxies at the same redshift might be missed entirely. | ||
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courses/ast403/lyman-break-technique.1774528106.txt.gz · Last modified: by shuvo
