courses:ast403:redshift-surveys
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| courses:ast403:redshift-surveys [2026/04/06 10:08] – [2dF Galaxy Redshift Survey] shuvo | courses:ast403:redshift-surveys [2026/04/06 22:27] (current) – [DESI BAO Survey] shuvo | ||
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| For graduate students studying large-scale structure, understanding the progression of SDSS is crucial, as its distinct phases introduced new observational techniques and targeted different cosmic epochs. | For graduate students studying large-scale structure, understanding the progression of SDSS is crucial, as its distinct phases introduced new observational techniques and targeted different cosmic epochs. | ||
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| + | About SDSS: https:// | ||
| **The First Detection: SDSS-I and II (2000–2008): | **The First Detection: SDSS-I and II (2000–2008): | ||
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| The 2005 detection localized the BAO peak at a comoving separation of approximately $100\ h^{-1}$ Mpc (equivalent to $r_s \approx 147$ Mpc) using a sample of about 46,000 LRGs out to $z \approx 0.47$. | The 2005 detection localized the BAO peak at a comoving separation of approximately $100\ h^{-1}$ Mpc (equivalent to $r_s \approx 147$ Mpc) using a sample of about 46,000 LRGs out to $z \approx 0.47$. | ||
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| **The Baryon Oscillation Spectroscopic Survey (SDSS-III, 2009–2014): | **The Baryon Oscillation Spectroscopic Survey (SDSS-III, 2009–2014): | ||
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| **BAO Reconstruction: | **BAO Reconstruction: | ||
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| These automated micromotors can reconfigure the arrangement of the 5,000 fibers in a matter of minutes, aligning them with new target galaxies to an accuracy of a few microns. The light from these fibers is fed into ten spectrographs, | These automated micromotors can reconfigure the arrangement of the 5,000 fibers in a matter of minutes, aligning them with new target galaxies to an accuracy of a few microns. The light from these fibers is fed into ten spectrographs, | ||
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| + | DESI focal plane: https:// | ||
| **The Tracers: A Multi-Target Strategy: | **The Tracers: A Multi-Target Strategy: | ||
| To map the universe continuously from the local volume out to the era of matter domination, DESI utilizes a multi-target strategy, targeting different classes of objects at different redshifts: | To map the universe continuously from the local volume out to the era of matter domination, DESI utilizes a multi-target strategy, targeting different classes of objects at different redshifts: | ||
| - | //1. Bright Galaxy Sample (BGS):// Probes the low-redshift universe ($z < 0.4$). | + | //1. Bright Galaxy Sample (BGS):// Probes the low-redshift universe ($z < 0.4$).\\ |
| - | //2. Luminous Red Galaxies (LRGs):// Extends from $0.4 < z < 0.8$. | + | //2. Luminous Red Galaxies (LRGs):// Extends from $0.4 < z < 0.8$.\\ |
| - | //3. Emission Line Galaxies (ELGs)// Star-forming galaxies mapped from $0.8 < z < 1.6$, representing the bulk of DESI's target catalog. | + | //3. Emission Line Galaxies (ELGs)// Star-forming galaxies mapped from $0.8 < z < 1.6$, representing the bulk of DESI's target catalog.\\ |
| //4. Quasars (QSOs):// Used both as discrete density tracers ($1.6 < z < 2.1$) and as backlights for the **Lyman-$\alpha$ forest** ($z > 2.1$). | //4. Quasars (QSOs):// Used both as discrete density tracers ($1.6 < z < 2.1$) and as backlights for the **Lyman-$\alpha$ forest** ($z > 2.1$). | ||
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| When combined with Cosmic Microwave Background (CMB) data from the Planck satellite, the derived Hubble constant is measured at: | When combined with Cosmic Microwave Background (CMB) data from the Planck satellite, the derived Hubble constant is measured at: | ||
| $$H_0 = 67.97 \pm 0.38 \text{ km s}^{-1} \text{ Mpc}^{-1}$$ | $$H_0 = 67.97 \pm 0.38 \text{ km s}^{-1} \text{ Mpc}^{-1}$$ | ||
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| **The Evolving Equation of State: A Hint of New Physics? | **The Evolving Equation of State: A Hint of New Physics? | ||
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| $$w(a) = w_0 + w_a (1 - a)$$ | $$w(a) = w_0 + w_a (1 - a)$$ | ||
| - | Here: | + | Here:\\ |
| - | * $w_0$ is the current value of the dark energy equation of state at $z = 0$. | + | * $w_0$ is the current value of the dark energy equation of state at $z = 0$.\\ |
| - | * $w_a$ dictates how quickly $w$ evolves with time. | + | * $w_a$ dictates how quickly $w$ evolves with time.\\ |
| - | * *(Note: $\Lambda$CDM strictly requires $w_0 = -1$ and $w_a = 0$)*. | + | * (Note: $\Lambda$CDM strictly requires $w_0 = -1$ and $w_a = 0$).\\ |
| When the DESI collaboration combined their Y1 BAO measurements with CMB data and Type Ia Supernova data, the statistical fit preferred a parameter space where **$w_0 > -1$ and $w_a < 0$**. | When the DESI collaboration combined their Y1 BAO measurements with CMB data and Type Ia Supernova data, the statistical fit preferred a parameter space where **$w_0 > -1$ and $w_a < 0$**. | ||
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| While this does not meet the $5\sigma$ threshold required to officially claim a " | While this does not meet the $5\sigma$ threshold required to officially claim a " | ||
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courses/ast403/redshift-surveys.1775491736.txt.gz · Last modified: by shuvo
