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Where did we come from? ~ A quest for the physics that operates at - - PowerPoint PPT Presentation

MPI fr Astrophysik Where did we come from? ~ A quest for the physics that operates at the beginning of our Universe ~ Eiichiro Komatsu [Scientific Member since 2012 ] CPTS Sektionssitzung, February 23, 2017 Fluctuations existed Spectroscopy of


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Where did we come from?

~A quest for the physics that operates at the beginning of our Universe~

Eiichiro Komatsu [Scientific Member since 2012] CPTS Sektionssitzung, February 23, 2017

MPI für Astrophysik

Fluctuations existed at the beginning… …they grew gravitationally to form galaxies, stars, us Spectroscopy of the whole Universe!

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I am…

  • a “cosmologist”
  • or, someone between astronomy and physics
  • Theoretical and observational. I divide my research

time into

  • ~2/3 theory, ~1/3 data analysis
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Where did I come from?

500 km (only 2.5 hours by a bullet train “Shinkansen”!) Before I tell you where you came from…

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Where is our former president?

in office since Jan 1, 2017

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Where did I come from?

500 km (only 2.5 hours by a bullet train “Shinkansen”!) Before I tell you where you came from…

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Where did I come from?

Before I tell you where you came from…

KANSAI = Bayern in Japan

Bayern in Japan!!, because

  • We speak funny dialects,
  • Everyone else makes fun of us,
  • But we are very proud of ourselves,
  • Because we were once the center of the country

KANSAI Area

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“The Capital” 1.5 million Merchants and Comedians 2.7 million Beef and shoes 1.5 million

Takara-zuka

30 km 50 km (220k)

KANSAI Area

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Two things about Takarazuka that every single Japanese knows

Female-only Musical Performance

KAGEKI “Revue”

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Godfather of “Manga” and “Anime”

Osamu Tezuka

Two things about Takarazuka that every single Japanese knows

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Where did I come from?

Tohoku University in Sendai (1993–1999)

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Where did I come from?

In 1999: to Princeton Univ. (25 years old)

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Why did I leave Japan?

  • Because science I wanted to do for my PhD, i.e., to

learn about the beginning of the Universe using the light from the Big Bang, was not possible in Japan in 1999

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Sky in Optical (~0.5μm)

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Sky in Microwave (~1mm)

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Light from the fireball Universe filling our sky (2.7K) The Cosmic Microwave Background (CMB)

Sky in Microwave (~1mm)

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WMAP Science Team

July 19, 2002

  • WMAP was launched on June 30, 2001
  • The WMAP mission ended after 9 years of operation
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Outstanding Questions

  • Where does anisotropy in CMB temperature come

from?

  • This is the origin of galaxies, stars, planets, and

everything else we see around us, including

  • urselves
  • The leading idea: quantum fluctuations in

vacuum, stretched to cosmological length scales by a rapid exponential expansion of the universe called “cosmic inflation” in the very early universe

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Our Origin

  • WMAP taught us that

galaxies, stars, planets, and ourselves originated from tiny fluctuations in the early Universe

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Kosmische Miso Suppe

  • When matter and radiation were hotter than 3000 K,

matter was completely ionised. The Universe was filled with plasma, which behaves just like a soup

  • Think about a Miso soup (if you know what it is).

Imagine throwing Tofus into a Miso soup, while changing the density of Miso

  • And imagine watching how ripples are created and

propagate throughout the soup

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Outstanding Questions

  • Where does anisotropy in CMB temperature come

from?

  • This is the origin of galaxies, stars, planets, and

everything else we see around us, including

  • urselves
  • The leading idea: quantum fluctuations in

vacuum, stretched to cosmological length scales by a rapid exponential expansion of the universe called “cosmic inflation” in the very early universe

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Data Analysis

  • Decompose temperature

fluctuations in the sky into a set of waves with various wavelengths

  • Make a diagram showing the

strength of each wavelength

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Long Wavelength Short Wavelength 180 degrees/(angle in the sky)

Amplitude of Waves [μK2]

WMAP 9-year Data (2013)

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Long Wavelength Short Wavelength 180 degrees/(angle in the sky)

Amplitude of Waves [μK2]

WMAP 9-year Data (2013)

Sound waves in the Universe. Predicted by Rashid Sunyaev and others in 1970

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Long Wavelength Short Wavelength

Measuring Abundance of H&He

Amplitude of Waves [μK2]

180 degrees/(angle in the sky)

Density of H&He

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  • We determined the

abundance of various components in the Universe (2003–2013)

  • As a result, we came to

realise that we do not understand 95%

  • f our Universe…

H&He Dark Matter Dark Energy

Cosmic Pie Chart

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Origin of Fluctuations

  • Who dropped those Tofus into the cosmic Miso

soup?

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Leading Idea

  • Quantum Mechanics at work in the early Universe
  • Heisenberg’s Uncertainty Principle:
  • [Energy you can borrow] x [Time you borrow] ~ h
  • Time was very short in the early Universe = You could

borrow a lot of energy

  • Those energies became the origin of fluctuations
  • How did quantum fluctuations on the microscopic scales

become macroscopic fluctuations over cosmological sizes?

Mukhanov & Chibisov (1981); Guth & Pi (1982); Hawking (1982); Starobinsky (1982); Bardeen, Turner & Steinhardt (1983)

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Cosmic Inflation

  • In a tiny fraction of a second, the size of an atomic

nucleus became the size of the Solar System

  • In 10–36 second, space was stretched by at least

a factor of 1026

Starobinsky (1980); Sato (1981); Guth (1981); Linde (1982); Albrecht & Steinhardt (1982)

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Stretching Micro to Macro

Inflation!

Quantum fluctuations on microscopic scales

  • Quantum fluctuations cease to be quantum
  • Become macroscopic, classical fluctuations
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Key Predictions of Inflation

  • Fluctuations we observe today in CMB and

the matter distribution originate from quantum fluctuations generated during inflation

  • There should also be ultra-long-wavelength

gravitational waves generated during inflation

ζ

scalar mode

hij

tensor mode

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We measure distortions in space

  • A distance between two points in space
  • ζ: “curvature perturbation” (scalar mode)
  • Perturbation to the determinant of the spatial metric
  • hij: “gravitational waves” (tensor mode)
  • Perturbation that does not change the determinant (area)

d`2 = a2(t)[1 + 2⇣(x, t)][ij + hij(x, t)]dxidxj

X

i

hii = 0

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Heisenberg’s Uncertainty Principle

  • [Energy you can borrow] x [Time you borrow] =

constant

  • Suppose that the distance between two points

increases in proportion to a(t) [which is called the scale factor] by the expansion of the universe

  • Define the “expansion rate of the universe” as

H ≡ ˙ a a [This has units of 1/time]

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Fluctuations are proportional to H

  • [Energy you can borrow] x [Time you borrow] =

constant

  • Then, both ζ and hij are proportional to H
  • Inflation occurs in 10–36 second - this is such a short

period of time that you can borrow a lot of energy! H during inflation in energy units is 1014 GeV H ≡ ˙ a a [This has units of 1/time]

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Long Wavelength Short Wavelength

180 degrees/(angle in the sky) Amplitude of Waves [μK2]

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180 degrees/(angle in the sky) Amplitude of Waves [μK2]

Long Wavelength Short Wavelength

Removing Ripples: Power Spectrum of Primordial Fluctuations

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180 degrees/(angle in the sky) Amplitude of Waves [μK2]

Long Wavelength Short Wavelength

Removing Ripples: Power Spectrum of Primordial Fluctuations

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180 degrees/(angle in the sky) Amplitude of Waves [μK2]

Long Wavelength Short Wavelength

Removing Ripples: Power Spectrum of Primordial Fluctuations

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180 degrees/(angle in the sky) Amplitude of Waves [μK2]

Long Wavelength Short Wavelength

Let’s parameterise like

Wave Amp. ∝ `ns−1

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180 degrees/(angle in the sky) Amplitude of Waves [μK2]

Long Wavelength Short Wavelength

Wave Amp. ∝ `ns−1

WMAP 9-Year Only [2013]: ns=0.972±0.013 (68%CL)

2001–2010

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South Pole Telescope [10-m in South Pole] Atacama Cosmology Telescope [6-m in Chile]

Amplitude of Waves [μK2]

1000 100

2001–2010

WMAP Collaboration [2013]

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1000 100

South Pole Telescope [10-m in South Pole] Atacama Cosmology Telescope [6-m in Chile]

Amplitude of Waves [μK2]

ns=0.965±0.010

2001–2010

WMAP Collaboration [2013]

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1000 100

South Pole Telescope [10-m in South Pole] Atacama Cosmology Telescope [6-m in Chile]

Amplitude of Waves [μK2]

2001–2010

ns=0.961±0.008

~5σ discovery of ns<1 from the CMB data combined with a galaxy survey data

WMAP Collaboration [2013]

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Residual

Planck 2013 Result!

180 degrees/(angle in the sky)

Amplitude of Waves [μK2]

2009–2013

ESA

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Residual

Planck 2013 Result!

180 degrees/(angle in the sky)

Amplitude of Waves [μK2]

2009–2013

ns=0.960±0.007

First >5σ discovery of ns<1 from the CMB data alone

ESA

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Predicted in 1981. We discovered it finally in 2013

  • Inflation must end
  • Inflation predicts ns~1, but not exactly

equal to 1. Usually ns<1 is expected

  • The discovery of ns<1 has been the

dream of cosmologists since 1992, when the CMB anisotropy was first discovered and ns~1 (to within 30%) was indicated

Slava Mukhanov (LMU) said in his 1981 paper that ns should be less than 1

He was awarded Max Planck Medal in 2015

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How do we know that primordial fluctuations were of quantum mechanical origin?

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[Values of Temperatures in the Sky Minus 2.725 K] / [Root Mean Square]

Fraction of the Number of Pixels Having Those Temperatures Quantum Fluctuations give a Gaussian distribution of temperatures. Do we see this in the WMAP data?

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[Values of Temperatures in the Sky Minus 2.725 K] / [Root Mean Square]

Fraction of the Number of Pixels Having Those Temperatures

YES!!

Histogram: WMAP Data Red Line: Gaussian

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Non-Gaussianity:

A Powerful Test of Quantum Fluctuations

  • The WMAP data show that the distribution of

temperature fluctuations of CMB is very precisely Gaussian

  • with an upper bound on a deviation of 0.2%
  • With improved data provided by the Planck

mission, the upper bound is now 0.03%

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CMB Research: Next Frontier

Primordial Gravitational Waves

Extraordinary claims require extraordinary evidence. The same quantum fluctuations could also generate gravitational waves, and we wish to find them

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Measuring GW

  • GW changes the distances between two points

d`2 = dx2 = X

ij

ijdxidxj d`2 = X

ij

(ij + hij)dxidxj

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Laser Interferometer

Mirror Mirror detector

No signal

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Laser Interferometer

Mirror Mirror

Signal!

detector

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Laser Interferometer

Mirror Mirror

Signal!

detector

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LIGO detected GW from binary blackholes, with the wavelength

  • f thousands of kilometres

But, the primordial GW affecting the CMB has a wavelength of billions of light-years!! How do we find it?

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Detecting GW by CMB

Isotropic electro-magnetic fields

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Detecting GW by CMB

GW propagating in isotropic electro-magnetic fields

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hot hot cold cold c

  • l

d c

  • l

d h

  • t

h

  • t

Detecting GW by CMB

Space is stretched => Wavelength of light is also stretched

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hot hot cold cold c

  • l

d c

  • l

d h

  • t

h

  • t

Detecting GW by CMB Polarisation

electron electron Space is stretched => Wavelength of light is also stretched

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hot hot cold cold c

  • l

d c

  • l

d h

  • t

h

  • t

Detecting GW by CMB Polarisation

Space is stretched => Wavelength of light is also stretched

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horizontally polarised

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March 17, 2014

BICEP2’s announcement

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January 30, 2015

Joint Analysis of BICEP2 data and Planck data

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  • Planck shows the evidence that the detected

signal is not cosmological, but is due to dust

  • No strong evidence that the detected signal

is cosmological

The search continues!!

Current Situation

1989–1993 2001–2010 2009–2013 202X–

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ESA

2025– [proposed]

JAXA

+ possibly NASA

LiteBIRD

2025– [proposed]

Target uncertainty: 100 times better than the current upper bound on the gravitational wave amplitude

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Summary

  • Left my country to study the beginning of the Universe

using physics and state-of-the-art data

  • With the WMAP team [2001–2013], we:
  • Determined the age and composition of the Universe
  • Found strong evidence for the quantum origin of

cosmic structures

  • Now hoping to find decisive evidence for inflation by

measuring primordial gravitational waves

  • The wavelength of billions of light years!
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If polarisation from GW is found…

  • Then what?
  • The next step is to nail the specific model of

inflation

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Tensor-to-scalar Ratio

  • We really want to find this quantity!

The current upper bound: r<0.07

r ⌘ hhijhiji hζ2i

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WMAP(temp+pol)+ACT+SPT+BAO+H0 WMAP(pol) + Planck + BAO

WMAP Collaboration

ruled

  • ut!