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Alan Guth, Cosmology, 8.962 Lecture 26, May 16, 2018, p. 1. –1– –2– –3–

–3– –1–web.mit.edu/8.962/www/lecnotes/sl26-post-4up-s18.pdf · 2018. 5. 24. · 8.962 Lecture 26 May 16, 2018 COSMOLOGY Ripples in the Cosmic Microwave Background –1

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Page 1: –3– –1–web.mit.edu/8.962/www/lecnotes/sl26-post-4up-s18.pdf · 2018. 5. 24. · 8.962 Lecture 26 May 16, 2018 COSMOLOGY Ripples in the Cosmic Microwave Background –1

Alan Guth, Cosmology, 8.962 Lecture 26, May 16, 2018, p. 1.

8.962 Lecture 26

May 16, 2018

COSMOLOGY

Ripples in the Cosmic Microwave Background

–1–

Spectrum of CMB Ripples

–2–

Planck 2015 TE Power Spectrum

–3–

Page 2: –3– –1–web.mit.edu/8.962/www/lecnotes/sl26-post-4up-s18.pdf · 2018. 5. 24. · 8.962 Lecture 26 May 16, 2018 COSMOLOGY Ripples in the Cosmic Microwave Background –1

Alan Guth, Cosmology, 8.962 Lecture 26, May 16, 2018, p. 2.

Planck 2015 EE Power Spectrum

–4–

Gaussianity of the CMB

Nongaussianites are measured by fNL, where Planck 2015 set thebounds

f localNL = 0.8± 5.0 ,

f equilNL = −4± 43 ,

forthoNL = −26± 21 (68% CL statistical).

Local, equil, and ortho refer to three different “shapes” for the3-point function (bispectrum). fNL is defined by

Φ = Φg + fNLΦ2g ,

where Φ is the Bardeen potential. Note that the nongaussian termwill be comparable to the gaussian term when fNL ∼ 105, so thelimits imply that the CMB is VERY gaussian.

Alan Guth

Massachusetts Institute of Technology

8.962 Lecture 26, May 16, 2018 –5–