courses:ast403:baryon-acoustic-oscillation
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| courses:ast403:baryon-acoustic-oscillation [2026/04/04 00:51] – [Observational Signatures: The Standard Ruler] shuvo | courses:ast403:baryon-acoustic-oscillation [2026/04/06 09:58] (current) – [Observational Signatures: The Standard Ruler] shuvo | ||
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| - | Baryon Acoustic Oscillations (BAO) refer to the regular, periodic fluctuations in the density of the visible baryonic matter of the universe. Much like how sound waves travel through the air, these acoustic waves traveled through the primordial plasma of the early universe. Today, BAO provides a robust " | + | Baryon Acoustic Oscillations (BAO) refer to the regular, periodic fluctuations in the density of the visible baryonic matter of the Universe. Much like how sound waves travel through the air, these acoustic waves traveled through the primordial plasma of the early universe. Today, BAO provides a robust " |
| ===== The Physics of the Early Universe ===== | ===== The Physics of the Early Universe ===== | ||
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| **Photon-Baryon Fluid:** Electrons and photons were tightly coupled via Thomson scattering, and protons were coupled to electrons via Coulomb interactions. This created a single, relativistic photon-baryon fluid. | **Photon-Baryon Fluid:** Electrons and photons were tightly coupled via Thomson scattering, and protons were coupled to electrons via Coulomb interactions. This created a single, relativistic photon-baryon fluid. | ||
| - | When a dark matter overdensity collapsed under gravity, it pulled the photon-baryon fluid with it. However, the immense radiation pressure of the photons strongly resisted this compression, | + | When a dark matter overdensity collapsed under gravity, it pulled the photon-baryon fluid with it. However, the immense radiation pressure of the photons strongly resisted this compression, |
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| ===== Mathematical Formalism of the Acoustic Waves ===== | ===== Mathematical Formalism of the Acoustic Waves ===== | ||
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| $$c_s = \frac{c}{\sqrt{3(1+R)}}$$ | $$c_s = \frac{c}{\sqrt{3(1+R)}}$$ | ||
| - | In the very early universe, radiation dominates ($R \to 0$), and the sound speed approaches the relativistic limit $c/ | + | In the very early Universe, radiation dominates ($R \to 0$), and the sound speed approaches the relativistic limit $c/ |
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| **The Comoving Sound Horizon: | **The Comoving Sound Horizon: | ||
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| ===== Recombination and the Relic Signature ===== | ===== Recombination and the Relic Signature ===== | ||
| - | At recombination, | + | At recombination, |
| The **photons** streamed away freely, carrying the imprint of these temperature fluctuations to us as the Cosmic Microwave Background (CMB).\\ | The **photons** streamed away freely, carrying the imprint of these temperature fluctuations to us as the Cosmic Microwave Background (CMB).\\ | ||
| The **baryons**, | The **baryons**, | ||
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| Over billions of years, both the central dark matter peak and the spherical baryonic shell acted as gravitational seeds for structure formation. Therefore, for any given galaxy, there is a slightly enhanced probability of finding another galaxy exactly $147$ Mpc away. | Over billions of years, both the central dark matter peak and the spherical baryonic shell acted as gravitational seeds for structure formation. Therefore, for any given galaxy, there is a slightly enhanced probability of finding another galaxy exactly $147$ Mpc away. | ||
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| ===== Observational Signatures: The Standard Ruler ===== | ===== Observational Signatures: The Standard Ruler ===== | ||
| - | Because the scale of the sound horizon $r_s$ is firmly rooted in the well-understood physics of the early universe, it serves as a cosmological Standard Ruler. By observing the apparent size of the BAO scale in the clustering of galaxies at different redshifts, we can measure the geometry and expansion rate of the universe. | + | Because the scale of the sound horizon $r_s$ is firmly rooted in the well-understood physics of the early Universe, it serves as a cosmological Standard Ruler. By observing the apparent size of the BAO scale in the clustering of galaxies at different redshifts, we can measure the geometry and expansion rate of the Universe. |
| We measure the BAO signal in two directions relative to our line of sight: | We measure the BAO signal in two directions relative to our line of sight: | ||
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| + | An animation of the formation of BAO: [[https:// | ||
courses/ast403/baryon-acoustic-oscillation.1775285461.txt.gz · Last modified: by shuvo
