How is the first peak of the CMB calculated?

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The discussion focuses on the calculation of the first acoustic peak in the Cosmic Microwave Background (CMB) and its relationship to the sound horizon as reported in the Planck study. The quoted sound horizon of 0.0104147 radians corresponds to a multipole moment of 302, but the first peak appears at a moment of approximately 220. Participants explore the discrepancies between these values, suggesting that different conventions in parameter usage may contribute to the confusion. The calculation of the sound horizon involves fitting model data to actual CMB data using Boltzmann equations, which may explain the differences observed. Ultimately, the conversation highlights the complexities in interpreting CMB data and the need for clarity in the parameters used.
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This is a follow up to an old thread: https://www.physicsforums.com/threads/the-first-acoustic-peak-in-cmb.475412/. In the final draft of the Plank study - http://arxiv.org/pdf/1303.5076v3.pdf - they quote the sound horizon at 1.04147 x 10-2. This equates to a multipole moment of 302. However, if you look at the diagram of the power curve, the first peak is at roughly 220.
Plank Power Spectrum.png


In the earlier post, someone suggested that there was a phase shift, but if you actually calculate the phase shift from the referenced document - using the r* from the Plank study - you get a factor of 0.5. So 302 x 0.5 = 150 which still doesn't equal a multipole moment of 220. So what is the relation between the quoted sound horizon of 0.0104147 and the first acoustic peak at a moment of 220?
 
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Chalnoth said:
Thanks for the post, but I've been through that NED document a couple of times. It doesn't help with the issue. I'd like to know how the sound horizon quoted in the Plank document, 0.014147 radians, relates to the first peak of the power spectrum at 220 in Figure 1 of the same document.
 

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George Jones said:
The location of the first of the peak depends on various parameters. I have attached page 271 from the second edition of "Fundamentals of Cosmology" by James Rich, and the approximate relationship (7.82) with n = 1 gives the shift between the first peak and the sound horizon. Reference [154] from this page is

http://arxiv.org/abs/astro-ph/9604166

For more detail, see the reference that I give in

https://www.physicsforums.com/threads/how-can-you-show-the-cmb-shift-parameter.804813/.
I'm sorry, but you seem to have misunderstood my question. I have a formula (see the reference in the original post). The one you reference appears to be the same form. I already took the numbers from Plank, plugged them into the formula and got a multipole movement of 152.2, so apparently I'm unable to pick the right numbers out of the Plank report. I'm looking for someone who can tell me what numbers from the final Plank report I can use to go from a quoted sound horizon of 0.014147 to a moment of roughly 220.
 
Dr. Strange said:
I'm sorry, but you seem to have misunderstood my question. I have a formula (see the reference in the original post). The one you reference appears to be the same form. I already took the numbers from Plank, plugged them into the formula and got a multipole movement of 152.2, so apparently I'm unable to pick the right numbers out of the Plank report. I'm looking for someone who can tell me what numbers from the final Plank report I can use to go from a quoted sound horizon of 0.014147 to a moment of roughly 220.
Btw, my bet is that this whole issue is a matter of different conventions being used for the parameters in the different sources. I'll see if I can't look into it in more detail when I get home later.
 
Dr. Strange said:
I'm looking for someone who can tell me what numbers from the final Plank report I can use to go from a quoted sound horizon of 0.014147 to a moment of roughly 220.

Since the first peak of 220 appears in the data, shouldn't this be turned around? Shouldn't the question be "How are the Planck data (all of the data, not just the peak at 220) used to to calculate the sound horizon at last scattering?"

A second, related question might be "Why is the calculated sound horizon different than the first peak?"

Computer code (see 2.1.5 in the Planck paper) that integrates Boltzmann equations for interactions is used to generate test CMB data for model universes that are parametrized by six or so parameters. These model data sets are statistically fitted to the the actual data to find a best-fit set of parameters, i.e., to find a best-fit universe. This best-fit universe is then used to calculate the sound horizon via equation (6) of the Planck paper.

The sound horizon is different from the first peak in the data because of reason given in the pdf that I attached above. See the paragraph that begins "the shift ##\Delta l##"
 
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