Early Universe
R. Branden- berger
Cosmology What was before the Big Bang? Framework Space-Time Cosmology of the Very Early Universe Std. Cosmology
Inflation
String gas Robert Brandenberger Conclusions McGill University
February 21, 2013
1 / 68 Outline
Early Universe
R. Branden- berger 1 What is Cosmology? Cosmology Framework 2 Space-Time Framework Std. Cosmology Space-Time Inflation Standard Big Bang Cosmology String gas
Conclusions 3 Inflationary Cosmology
4 String Cosmology
5 Conclusions
2 / 68 Plan
Early Universe
R. Branden- berger 1 What is Cosmology? Cosmology Framework 2 Space-Time Framework Std. Cosmology Space-Time Inflation Standard Big Bang Cosmology String gas
Conclusions 3 Inflationary Cosmology
4 String Cosmology
5 Conclusions
3 / 68 Goals of Early Universe Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework 1. Understand origin and early evolution of the universe. Space-Time Std. Cosmology What is the “Big Bang"? Inflation Was there a “Big Bang"? String gas
Conclusions What was before the “Big Bang"?
2. Explain observed large-scale structure.
4 / 68 Goals of Early Universe Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework 1. Understand origin and early evolution of the universe. Space-Time Std. Cosmology What is the “Big Bang"? Inflation Was there a “Big Bang"? String gas
Conclusions What was before the “Big Bang"?
2. Explain observed large-scale structure.
4 / 68 Goals of Early Universe Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework 1. Understand origin and early evolution of the universe. Space-Time Std. Cosmology What is the “Big Bang"? Inflation Was there a “Big Bang"? String gas
Conclusions What was before the “Big Bang"?
2. Explain observed large-scale structure.
4 / 68 Goals of Early Universe Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework 1. Understand origin and early evolution of the universe. Space-Time Std. Cosmology What is the “Big Bang"? Inflation Was there a “Big Bang"? String gas
Conclusions What was before the “Big Bang"?
2. Explain observed large-scale structure.
4 / 68 Goals of Early Universe Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework 1. Understand origin and early evolution of the universe. Space-Time Std. Cosmology What is the “Big Bang"? Inflation Was there a “Big Bang"? String gas
Conclusions What was before the “Big Bang"?
2. Explain observed large-scale structure.
4 / 68 Optical Telescopes: Gemini Telescope
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
5 / 68 Galaxies: Building Blocks of the Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
6 / 68 Large-Scale Structure
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
From: talk by O. Lahav
7 / 68 Microwave Telescopes on the Earth: ACT Telescope
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
8 / 68 Microwave Telescopes on the Earth: SPT Telescope
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
9 / 68 Microwave Telescopes in Space: WMAP Telescope
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
10 / 68 Isotropic CMB Background
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
11 / 68 Anisotropies in the Cosmic Microwave Background (CMB)
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Credit: NASA/WMAP Science Team 12 / 68 Quantification of the CMB data
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Credit: NASA/WMAP Science Team
13 / 68 Goals of Early Universe Cosmology
Early Universe
R. Branden- berger 1. Understand origin and early evolution of the universe.
Cosmology What is the “Big Bang"? Framework Space-Time Was there a “Big Bang"? Std. Cosmology What was before the “Big Bang"? Inflation
String gas Conclusions 2. Explain observed large-scale structure. Patterns in the distribution of galaxies on large scales. Anisotropies in CMB maps.
3. Make predictions for future observations.
14 / 68 Goals of Early Universe Cosmology
Early Universe
R. Branden- berger 1. Understand origin and early evolution of the universe.
Cosmology What is the “Big Bang"? Framework Space-Time Was there a “Big Bang"? Std. Cosmology What was before the “Big Bang"? Inflation
String gas Conclusions 2. Explain observed large-scale structure. Patterns in the distribution of galaxies on large scales. Anisotropies in CMB maps.
3. Make predictions for future observations.
14 / 68 Plan
Early Universe
R. Branden- berger 1 What is Cosmology? Cosmology Framework 2 Space-Time Framework Std. Cosmology Space-Time Inflation Standard Big Bang Cosmology String gas
Conclusions 3 Inflationary Cosmology
4 String Cosmology
5 Conclusions
15 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory?
16 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory?
16 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory?
16 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory?
16 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory?
16 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory?
16 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory ?
16 / 68 Framework
Early Universe R. Branden- The Universe is: berger Space-time Cosmology Framework Matter which lives in space-time. Space-Time Std. Cosmology To describe the Universe: Inflation String gas Space-time described by Einstein’s theory of General Conclusions Relativity. Matter as described by Physics. More specifically: matter described on large scale by classical physics, on small scales by quantum mechanics and on even smaller scales by superstring theory ?
16 / 68 Space-Time as Described by General Relativity
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology Space-time dynamical (no longer absolute like in Inflation Newtonian theory) String gas Conclusions Matter curves space-time.
17 / 68 Space-Time as Described by General Relativity
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology Space-time dynamical (no longer absolute like in Inflation Newtonian theory) String gas Conclusions Matter curves space-time.
17 / 68 Mass curves Space-Time
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
18 / 68 Space-Time as Described by General Relativity
Early Universe
R. Branden- berger
Cosmology Space-time dynamical (no longer absolute like in
Framework Newtonian theory) Space-Time Std. Cosmology Matter curves space-time: Space-time is dynamical. Inflation Note: Newton’s gravitational force is a consequence of String gas the curvature of space. Conclusions Einstein Equivalence Principle determines the motion of matter in curved space-time. Space with a homogeneous distribution of matter cannot be static - it must expand (or contract).
19 / 68 Space-Time as Described by General Relativity
Early Universe
R. Branden- berger
Cosmology Space-time dynamical (no longer absolute like in
Framework Newtonian theory) Space-Time Std. Cosmology Matter curves space-time: Space-time is dynamical. Inflation Note: Newton’s gravitational force is a consequence of String gas the curvature of space. Conclusions Einstein Equivalence Principle determines the motion of matter in curved space-time. Space with a homogeneous distribution of matter cannot be static - it must expand (or contract).
19 / 68 Space-Time as Described by General Relativity
Early Universe
R. Branden- berger
Cosmology Space-time dynamical (no longer absolute like in
Framework Newtonian theory) Space-Time Std. Cosmology Matter curves space-time: Space-time is dynamical. Inflation Note: Newton’s gravitational force is a consequence of String gas the curvature of space. Conclusions Einstein Equivalence Principle determines the motion of matter in curved space-time. Space with a homogeneous distribution of matter cannot be static - it must expand (or contract).
19 / 68 Space-Time as Described by General Relativity
Early Universe
R. Branden- berger
Cosmology Space-time dynamical (no longer absolute like in
Framework Newtonian theory) Space-Time Std. Cosmology Matter curves space-time: Space-time is dynamical. Inflation Note: Newton’s gravitational force is a consequence of String gas the curvature of space. Conclusions Einstein Equivalence Principle determines the motion of matter in curved space-time. Space with a homogeneous distribution of matter cannot be static - it must expand (or contract).
19 / 68 The Expanding Universe
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
20 / 68 Evidence for the Expansion of Space
Early Universe The Hubble diagram for type Ia supernovae. R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Kirshner R P PNAS 2004;101:8-13
©2004 by National Academy of Sciences 21 / 68 Standard Big Bang Cosmology
Early Universe
R. Branden- berger Standard Big Bang Cosmology (SBB): the old paradigm of cosmology (ca. 1960). Cosmology
Framework Space-Time The SBB is based on: Std. Cosmology Inflation Cosmological principle: universe homogeneous and String gas isotropic on large scales. Conclusions General Relativity governing dynamics of space-time. Classical matter as source in the Einstein equations. Classical matter: cold (pressure-less) matter (describing the galaxies) + radiation(describing the CMB).
22 / 68 Standard Big Bang Cosmology
Early Universe
R. Branden- berger Standard Big Bang Cosmology (SBB): the old paradigm of cosmology (ca. 1960). Cosmology
Framework Space-Time The SBB is based on: Std. Cosmology Inflation Cosmological principle: universe homogeneous and String gas isotropic on large scales. Conclusions General Relativity governing dynamics of space-time. Classical matter as source in the Einstein equations. Classical matter: cold (pressure-less) matter (describing the galaxies) + radiation(describing the CMB).
22 / 68 Standard Big Bang Cosmology
Early Universe
R. Branden- berger Standard Big Bang Cosmology (SBB): the old paradigm of cosmology (ca. 1960). Cosmology
Framework Space-Time The SBB is based on: Std. Cosmology Inflation Cosmological principle: universe homogeneous and String gas isotropic on large scales. Conclusions General Relativity governing dynamics of space-time. Classical matter as source in the Einstein equations. Classical matter: cold (pressure-less) matter (describing the galaxies) + radiation(describing the CMB).
22 / 68 Standard Big Bang Cosmology
Early Universe
R. Branden- berger Standard Big Bang Cosmology (SBB): the old paradigm of cosmology (ca. 1960). Cosmology
Framework Space-Time The SBB is based on: Std. Cosmology Inflation Cosmological principle: universe homogeneous and String gas isotropic on large scales. Conclusions General Relativity governing dynamics of space-time. Classical matter as source in the Einstein equations. Classical matter: cold (pressure-less) matter (describing the galaxies) + radiation(describing the CMB).
22 / 68 Standard Big Bang Cosmology
Early Universe
R. Branden- berger Standard Big Bang Cosmology (SBB): the old paradigm of cosmology (ca. 1960). Cosmology
Framework Space-Time The SBB is based on: Std. Cosmology Inflation Cosmological principle: universe homogeneous and String gas isotropic on large scales. Conclusions General Relativity governing dynamics of space-time. Classical matter as source in the Einstein equations. Classical matter: cold (pressure-less) matter (describing the galaxies) + radiation(describing the CMB).
22 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite.
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite.
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite.
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite .
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite .
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite .
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite .
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite .
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger The universe is expanding now. Cosmology In the past it was hotter and more dense. Framework Space-Time Thus, it was expanding faster in the past. Std. Cosmology
Inflation At a finite time in the past the temperature was infinite .
String gas A finite box of space had zero size at that time. Conclusions This is the Big Bang!
What is the Big Bang? What was before the Big Bang?
To be taken seriously a theory must have made successful observational predictions.
23 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Standard Big Bang Cosmology (ctd.)
Early Universe
R. Branden- berger Universe begins as a homogeneous and very hot
Cosmology fireball. Framework Initially radiation dominates: hot plasma. Space-Time Std. Cosmology Space expands and matter cools. Inflation
String gas After about 30,000 years cold matter starts to dominate. Conclusions After about 300,000 years atoms (hydrogen) forms and universe becomes transparent to light Now the age of the universe is about 13 billion years.
Prediction: Existence and black body nature of the Cosmic Microwave Background.
24 / 68 Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Credit: NASA/WMAP Science Team
25 / 68 Spectrometer
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
26 / 68 Successes of the SBB Model
Early Universe Key success: Existence and black body nature of the CMB. R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
27 / 68 Unanswered Questions
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology Inflation What is the Big Bang? String gas What was before the Big Bang? Conclusions
28 / 68 Conceptual Problems of the SBB Model
Early Universe No explanation for the homogeneity, spatial flatness and R. Branden- berger large size and entropy of the universe.
Cosmology Horizon problem of the SBB:
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
t
t 0
l (t) p
t rec
l f (t) 0 x
29 / 68 Conceptual Problems of the SBB Model II
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology No explanation of the observed inhomogeneities in the Inflation distribution of matter and anisotropies in the Cosmic String gas
Conclusions Microwave Background possible!
30 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 What to do?
Early Universe
R. Branden- berger With a little help from a friend , the particle physicist:
Cosmology At very high temperatures close to the Big Bang Framework classical physics breaks down - and quantum Space-Time Std. Cosmology mechanics and particle physics give the right Inflation description of matter. String gas → Standard Big Bang theory breaks down. Conclusions In the very early universe matter is a plasma of elementary particles. All described in terms of quantum fields. Quantum field (scalar fields) can lead to a different expansion rate of space namely inflationary expansion.
31 / 68 Plan
Early Universe
R. Branden- berger 1 What is Cosmology? Cosmology Framework 2 Space-Time Framework Std. Cosmology Space-Time Inflation Standard Big Bang Cosmology String gas
Conclusions 3 Inflationary Cosmology
4 String Cosmology
5 Conclusions
32 / 68 Time line of inflationary cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
ti : inflation begins
tR: inflation ends, reheating
33 / 68 Successes of Inflationary Cosmology
Early Universe
R. Branden- berger The Inflationary Universe Scenario is the current paradigm
Cosmology of early universe cosmology (1980). Framework Space-Time Std. Cosmology Successes: Inflation
String gas Solves horizon problem Conclusions Solves flatness problem Solves size/entropy problem Provides a causal mechanism of generating primordial cosmological perturbations (Chibisov & Mukhanov, 1981).
34 / 68 Successes of Inflationary Cosmology
Early Universe
R. Branden- berger The Inflationary Universe Scenario is the current paradigm
Cosmology of early universe cosmology (1980). Framework Space-Time Std. Cosmology Successes: Inflation
String gas Solves horizon problem Conclusions Solves flatness problem Solves size/entropy problem Provides a causal mechanism of generating primordial cosmological perturbations (Chibisov & Mukhanov, 1981).
34 / 68 Successes of Inflationary Cosmology
Early Universe
R. Branden- berger The Inflationary Universe Scenario is the current paradigm
Cosmology of early universe cosmology (1980). Framework Space-Time Std. Cosmology Successes: Inflation
String gas Solves horizon problem Conclusions Solves flatness problem Solves size/entropy problem Provides a causal mechanism of generating primordial cosmological perturbations (Chibisov & Mukhanov, 1981).
34 / 68 Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Credit: NASA/WMAP Science Team
35 / 68 Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Credit: NASA/WMAP Science Team
36 / 68 Review of Inflationary Cosmology
Early Universe
R. Branden- berger
Cosmology Context: Framework Space-Time General Relativity Std. Cosmology
Inflation Scalar Field Matter String gas Inflation: Conclusions phase with exponential expansion of space requires matter with negative pressure requires a slowly rolling scalar field ϕ
37 / 68 Review of Inflationary Cosmology
Early Universe
R. Branden- berger
Cosmology Context: Framework Space-Time General Relativity Std. Cosmology
Inflation Scalar Field Matter String gas Inflation: Conclusions phase with exponential expansion of space requires matter with negative pressure requires a slowly rolling scalar field ϕ
37 / 68 Review of Inflationary Cosmology
Early Universe
R. Branden- berger
Cosmology Context: Framework Space-Time General Relativity Std. Cosmology
Inflation Scalar Field Matter String gas Inflation: Conclusions phase with exponential expansion of space requires matter with negative pressure requires a slowly rolling scalar field ϕ
37 / 68 Review of Inflationary Cosmology
Early Universe
R. Branden- berger
Cosmology Context: Framework Space-Time General Relativity Std. Cosmology
Inflation Scalar Field Matter String gas Inflation: Conclusions phase with exponential expansion of space requires matter with negative pressure requires a slowly rolling scalar field ϕ
37 / 68 Review of Inflationary Cosmology II
Early Universe Space-time sketch of inflationary cosmology: R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Note: a˙ H = a curve labelled by k: wavelength of a fluctuation 38 / 68 Successes of Inflation
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time inflation renders the universe large, homogeneous and Std. Cosmology spatially flat Inflation String gas classical matter redshifts → matter vacuum remains Conclusions quantum vacuum fluctuations: seeds for the observed structure [Chibisov & Mukhanov, 1981]
39 / 68 Status of the Big Bang in Inflationary Cosmology
Early Universe
R. Branden- berger The inflationary phase had a beginning. Cosmology
Framework There was a Big Bang before the period of inflation. Space-Time Std. Cosmology Inflation Unanswered questions: String gas Conclusions What is the Big Bang? What was before the Big Bang?
Note: quantum field theory is not applicable very close to the singularity.
40 / 68 Status of the Big Bang in Inflationary Cosmology
Early Universe
R. Branden- berger The inflationary phase had a beginning. Cosmology
Framework There was a Big Bang before the period of inflation. Space-Time Std. Cosmology Inflation Unanswered questions: String gas Conclusions What is the Big Bang? What was before the Big Bang?
Note: quantum field theory is not applicable very close to the singularity.
40 / 68 Status of the Big Bang in Inflationary Cosmology
Early Universe
R. Branden- berger The inflationary phase had a beginning. Cosmology
Framework There was a Big Bang before the period of inflation. Space-Time Std. Cosmology Inflation Unanswered questions: String gas Conclusions What is the Big Bang? What was before the Big Bang?
Note: quantum field theory is not applicable very close to the singularity.
40 / 68 Challenges for the Current Paradigm
Early Universe
R. Branden- berger In spite of the phenomenological successes, the
Cosmology inflationary scenario suffers from several conceptual Framework problems. Space-Time Std. Cosmology In light of these problems we need to look for input from Inflation new fundamental physics to construct a new theory String gas which will overcome these problems. Conclusions Question: Can Superstring theory lead to a new and improved paradigm? Question: Can this new paradigm be tested in cosmological observations? Question: Was there a Big Bang ?
41 / 68 Challenges for the Current Paradigm
Early Universe
R. Branden- berger In spite of the phenomenological successes, the
Cosmology inflationary scenario suffers from several conceptual Framework problems. Space-Time Std. Cosmology In light of these problems we need to look for input from Inflation new fundamental physics to construct a new theory String gas which will overcome these problems. Conclusions Question: Can Superstring theory lead to a new and improved paradigm? Question: Can this new paradigm be tested in cosmological observations? Question: Was there a Big Bang ?
41 / 68 Challenges for the Current Paradigm
Early Universe
R. Branden- berger In spite of the phenomenological successes, the
Cosmology inflationary scenario suffers from several conceptual Framework problems. Space-Time Std. Cosmology In light of these problems we need to look for input from Inflation new fundamental physics to construct a new theory String gas which will overcome these problems. Conclusions Question: Can Superstring theory lead to a new and improved paradigm? Question: Can this new paradigm be tested in cosmological observations? Question: Was there a Big Bang ?
41 / 68 Challenges for the Current Paradigm
Early Universe
R. Branden- berger In spite of the phenomenological successes, the
Cosmology inflationary scenario suffers from several conceptual Framework problems. Space-Time Std. Cosmology In light of these problems we need to look for input from Inflation new fundamental physics to construct a new theory String gas which will overcome these problems. Conclusions Question: Can Superstring theory lead to a new and improved paradigm? Question: Can this new paradigm be tested in cosmological observations? Question: Was there a Big Bang ?
41 / 68 Challenges for the Current Paradigm
Early Universe
R. Branden- berger In spite of the phenomenological successes, the
Cosmology inflationary scenario suffers from several conceptual Framework problems. Space-Time Std. Cosmology In light of these problems we need to look for input from Inflation new fundamental physics to construct a new theory String gas which will overcome these problems. Conclusions Question: Can Superstring theory lead to a new and improved paradigm? Question: Can this new paradigm be tested in cosmological observations? Question: Was there a Big Bang ?
41 / 68 Conceptual Problems of Inflationary Cosmology
Early Universe
R. Branden- berger
Cosmology Framework What is the scalar field? Space-Time Std. Cosmology Why does it have the special conditions to obtain Inflation inflation? String gas
Conclusions Trans-Planckian problem Singularity problem Applicability of General Relativity
42 / 68 Trans-Planckian Problem
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Success of inflation: At early times scales are inside the Hubble radius → causal generation mechanism is possible. Problem: If time period of inflation is slightly more than the minimal length it must have, then the wavelength is smaller than the Planck length at the beginning of inflation 43 / 68 → new physics MUST enter into the calculation of the fluctuations. Singularity Problem
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Standard cosmology: Penrose-Hawking theorems → Std. Cosmology
Inflation initial singularity → incompleteness of the theory. String gas Inflationary cosmology: In scalar field-driven Conclusions inflationary models the initial singularity persists [Borde and Vilenkin] → incompleteness of the theory.
44 / 68 Singularity Problem
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Standard cosmology: Penrose-Hawking theorems → Std. Cosmology
Inflation initial singularity → incompleteness of the theory. String gas Inflationary cosmology: In scalar field-driven Conclusions inflationary models the initial singularity persists [Borde and Vilenkin] → incompleteness of the theory.
44 / 68 Singularity Problem
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Standard cosmology: Penrose-Hawking theorems → Std. Cosmology
Inflation initial singularity → incompleteness of the theory. String gas Inflationary cosmology: In scalar field-driven Conclusions inflationary models the initial singularity persists [Borde and Vilenkin] → incompleteness of the theory.
44 / 68 Applicability of GR
Early Universe
R. Branden- berger
Cosmology Framework Einstein’s theory breaks down at extremely high Space-Time Std. Cosmology densities. Inflation In models of inflation, the energy scale of at which String gas inflation takes place is close to the limiting scale for the Conclusions validity of Einstein’s theory. We cannot trust the predictions made using GR.
45 / 68 Applicability of GR
Early Universe
R. Branden- berger
Cosmology Framework Einstein’s theory breaks down at extremely high Space-Time Std. Cosmology densities. Inflation In models of inflation, the energy scale of at which String gas inflation takes place is close to the limiting scale for the Conclusions validity of Einstein’s theory. We cannot trust the predictions made using GR.
45 / 68 Applicability of GR
Early Universe
R. Branden- berger
Cosmology Framework Einstein’s theory breaks down at extremely high Space-Time Std. Cosmology densities. Inflation In models of inflation, the energy scale of at which String gas inflation takes place is close to the limiting scale for the Conclusions validity of Einstein’s theory. We cannot trust the predictions made using GR.
45 / 68 Zones of Ignorance
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
46 / 68 Message I
Early Universe
R. Branden- berger The current cosmological paradigm has serious Cosmology conceptual problems. Framework Space-Time We need a new paradigm of very early universe Std. Cosmology
Inflation cosmology. String gas With a little help from a friend - the string theorist! Conclusions New cosmological model motivated by superstring theory: String Gas Cosmology (SGC) [R.B. and C. Vafa, 1989]. New structure formation scenario emerges from SGC [A. Nayeri, R.B. and C. Vafa, 2006].
47 / 68 Message I
Early Universe
R. Branden- berger The current cosmological paradigm has serious Cosmology conceptual problems. Framework Space-Time We need a new paradigm of very early universe Std. Cosmology
Inflation cosmology. String gas With a little help from a friend - the string theorist! Conclusions New cosmological model motivated by superstring theory: String Gas Cosmology (SGC) [R.B. and C. Vafa, 1989]. New structure formation scenario emerges from SGC [A. Nayeri, R.B. and C. Vafa, 2006].
47 / 68 Message I
Early Universe
R. Branden- berger The current cosmological paradigm has serious Cosmology conceptual problems. Framework Space-Time We need a new paradigm of very early universe Std. Cosmology
Inflation cosmology. String gas With a little help from a friend - the string theorist! Conclusions New cosmological model motivated by superstring theory: String Gas Cosmology (SGC) [R.B. and C. Vafa, 1989]. New structure formation scenario emerges from SGC [A. Nayeri, R.B. and C. Vafa, 2006].
47 / 68 Message I
Early Universe
R. Branden- berger The current cosmological paradigm has serious Cosmology conceptual problems. Framework Space-Time We need a new paradigm of very early universe Std. Cosmology
Inflation cosmology. String gas With a little help from a friend - the string theorist! Conclusions New cosmological model motivated by superstring theory: String Gas Cosmology (SGC) [R.B. and C. Vafa, 1989]. New structure formation scenario emerges from SGC [A. Nayeri, R.B. and C. Vafa, 2006].
47 / 68 Message I
Early Universe
R. Branden- berger The current cosmological paradigm has serious Cosmology conceptual problems. Framework Space-Time We need a new paradigm of very early universe Std. Cosmology
Inflation cosmology. String gas With a little help from a friend - the string theorist! Conclusions New cosmological model motivated by superstring theory: String Gas Cosmology (SGC) [R.B. and C. Vafa, 1989]. New structure formation scenario emerges from SGC [A. Nayeri, R.B. and C. Vafa, 2006].
47 / 68 Message II
Early Universe
R. Branden- berger String Gas Cosmology makes testable predictions for Cosmology cosmological observations Framework Space-Time Std. Cosmology Blue tilt in the spectrum of gravitational waves [R.B., A. Inflation Nayeri, S. Patil and C. Vafa, 2006] String gas Line discontinuities in CMB anisotropy maps [N. Kaiser Conclusions and A. Stebbins, 1984] Line discontinuities can be detected using the CANNY edge detection algorithm [S. Amsel, J. Berger and R.B., 2007, R. Danos and R.B., 2008, 2009]
48 / 68 Message II
Early Universe
R. Branden- berger String Gas Cosmology makes testable predictions for Cosmology cosmological observations Framework Space-Time Std. Cosmology Blue tilt in the spectrum of gravitational waves [R.B., A. Inflation Nayeri, S. Patil and C. Vafa, 2006] String gas Line discontinuities in CMB anisotropy maps [N. Kaiser Conclusions and A. Stebbins, 1984] Line discontinuities can be detected using the CANNY edge detection algorithm [S. Amsel, J. Berger and R.B., 2007, R. Danos and R.B., 2008, 2009]
48 / 68 Message II
Early Universe
R. Branden- berger String Gas Cosmology makes testable predictions for Cosmology cosmological observations Framework Space-Time Std. Cosmology Blue tilt in the spectrum of gravitational waves [R.B., A. Inflation Nayeri, S. Patil and C. Vafa, 2006] String gas Line discontinuities in CMB anisotropy maps [N. Kaiser Conclusions and A. Stebbins, 1984] Line discontinuities can be detected using the CANNY edge detection algorithm [S. Amsel, J. Berger and R.B., 2007, R. Danos and R.B., 2008, 2009]
48 / 68 Plan
Early Universe
R. Branden- berger 1 What is Cosmology? Cosmology Framework 2 Space-Time Framework Std. Cosmology Space-Time Inflation Standard Big Bang Cosmology String gas
Conclusions 3 Inflationary Cosmology
4 String Cosmology
5 Conclusions
49 / 68 What is String Theory?
Early Universe
R. Branden- berger String theory is a quantum theory of all forces of nature Cosmology including gravity. Framework Space-Time String theory unifies all forces of nature. Std. Cosmology
Inflation Basic objects: elementary strings. Compared to String gas elementary point particles. Conclusions String theory is mathematically consistent only in 10 space-time dimensions. Thus, string theory predicts extra spatial dimensions.
Note: string theory is “in development".
50 / 68 What is String Theory?
Early Universe
R. Branden- berger String theory is a quantum theory of all forces of nature Cosmology including gravity. Framework Space-Time String theory unifies all forces of nature. Std. Cosmology
Inflation Basic objects: elementary strings. Compared to String gas elementary point particles. Conclusions String theory is mathematically consistent only in 10 space-time dimensions. Thus, string theory predicts extra spatial dimensions.
Note: string theory is “in development".
50 / 68 What is String Theory?
Early Universe
R. Branden- berger String theory is a quantum theory of all forces of nature Cosmology including gravity. Framework Space-Time String theory unifies all forces of nature. Std. Cosmology
Inflation Basic objects: elementary strings. Compared to String gas elementary point particles. Conclusions String theory is mathematically consistent only in 10 space-time dimensions. Thus, string theory predicts extra spatial dimensions.
Note: string theory is “in development".
50 / 68 What is String Theory?
Early Universe
R. Branden- berger String theory is a quantum theory of all forces of nature Cosmology including gravity. Framework Space-Time String theory unifies all forces of nature. Std. Cosmology
Inflation Basic objects: elementary strings. Compared to String gas elementary point particles. Conclusions String theory is mathematically consistent only in 10 space-time dimensions. Thus, string theory predicts extra spatial dimensions.
Note: string theory is “in development".
50 / 68 What is String Theory?
Early Universe
R. Branden- berger String theory is a quantum theory of all forces of nature Cosmology including gravity. Framework Space-Time String theory unifies all forces of nature. Std. Cosmology
Inflation Basic objects: elementary strings. Compared to String gas elementary point particles. Conclusions String theory is mathematically consistent only in 10 space-time dimensions. Thus, string theory predicts extra spatial dimensions.
Note: string theory is “in development".
50 / 68 What is String Theory?
Early Universe
R. Branden- berger String theory is a quantum theory of all forces of nature Cosmology including gravity. Framework Space-Time String theory unifies all forces of nature. Std. Cosmology
Inflation Basic objects: elementary strings. Compared to String gas elementary point particles. Conclusions String theory is mathematically consistent only in 10 space-time dimensions. Thus, string theory predicts extra spatial dimensions.
Note: string theory is “in development".
50 / 68 What is String Theory?
Early Universe
R. Branden- berger String theory is a quantum theory of all forces of nature Cosmology including gravity. Framework Space-Time String theory unifies all forces of nature. Std. Cosmology
Inflation Basic objects: elementary strings. Compared to String gas elementary point particles. Conclusions String theory is mathematically consistent only in 10 space-time dimensions. Thus, string theory predicts extra spatial dimensions.
Note: string theory is “in development".
50 / 68 Principles R.B. and C. Vafa, Nucl. Phys. B316:391 (1989)
Early Universe R. Branden- Idea: make use of the new symmetries and new degrees of berger freedom which string theory provides to construct a new Cosmology theory of the very early universe. Framework Assumption: Matter is a gas of fundamental strings Space-Time Std. Cosmology Assumption: Space is compact, e.g. a torus. Inflation Key points: String gas Conclusions New degrees of freedom: string oscillatory modes. Leads to a maximal temperature for a gas of strings, the Hagedorn temperature. New degrees of freedom: string winding modes. Leads to a new symmetry: physics at large R is equivalent to physics at small R.
51 / 68 Principles R.B. and C. Vafa, Nucl. Phys. B316:391 (1989)
Early Universe R. Branden- Idea: make use of the new symmetries and new degrees of berger freedom which string theory provides to construct a new Cosmology theory of the very early universe. Framework Assumption: Matter is a gas of fundamental strings Space-Time Std. Cosmology Assumption: Space is compact, e.g. a torus. Inflation Key points: String gas Conclusions New degrees of freedom: string oscillatory modes. Leads to a maximal temperature for a gas of strings, the Hagedorn temperature. New degrees of freedom: string winding modes. Leads to a new symmetry: physics at large R is equivalent to physics at small R.
51 / 68 Principles R.B. and C. Vafa, Nucl. Phys. B316:391 (1989)
Early Universe R. Branden- Idea: make use of the new symmetries and new degrees of berger freedom which string theory provides to construct a new Cosmology theory of the very early universe. Framework Assumption: Matter is a gas of fundamental strings Space-Time Std. Cosmology Assumption: Space is compact, e.g. a torus. Inflation Key points: String gas Conclusions New degrees of freedom: string oscillatory modes. Leads to a maximal temperature for a gas of strings, the Hagedorn temperature. New degrees of freedom: string winding modes. Leads to a new symmetry: physics at large R is equivalent to physics at small R.
51 / 68 “Large" is Equivalent to “Small" in String Theory
Early Universe
R. Branden- berger
Cosmology Framework T-Duality Space-Time Std. Cosmology Momentum modes: En = n/R Inflation String gas Winding modes: Em = mR Conclusions Duality: R → 1/R (n, m) → (m, n) Mass spectrum of string states unchanged
52 / 68 Temperature in String Cosmology R.B. and C. Vafa, Nucl. Phys. B316:391 (1989)
Early Universe
R. Branden- Temperature of a box of strings in thermal equilibrium. berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
53 / 68 Temperature in Standard and Inflationary Cosmology
Early Universe
R. Branden- berger
Cosmology Temperature of a box of particles in thermal equilibrium. Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
54 / 68 Dynamics
Early Universe
R. Branden- berger Assume some dynamical principle gives us R(t) Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
55 / 68 String Gas Cosmology R.B. and C. Vafa, Nucl. Phys. B316:391 (1989)
Early Universe
R. Branden- berger We will thus consider the following background dynamics for Cosmology the scale factor a(t): Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
56 / 68 Dimensionality of Space in SGC
Early Universe
R. Branden- berger Begin with all 9 spatial dimensions small, initial temperature close to T → winding modes about all Cosmology H spatial sections are excited. Framework Space-Time Std. Cosmology Expansion of any one spatial dimension requires the Inflation annihilation of the winding modes in that dimension. String gas
Conclusions
Decay only possible in three large spatial dimensions. → dynamical explanation of why there are exactly three large spatial dimensions.
57 / 68 Dimensionality of Space in SGC
Early Universe
R. Branden- berger Begin with all 9 spatial dimensions small, initial temperature close to T → winding modes about all Cosmology H spatial sections are excited. Framework Space-Time Std. Cosmology Expansion of any one spatial dimension requires the Inflation annihilation of the winding modes in that dimension. String gas
Conclusions
Decay only possible in three large spatial dimensions. → dynamical explanation of why there are exactly three large spatial dimensions.
57 / 68 Dimensionality of Space in SGC
Early Universe
R. Branden- berger Begin with all 9 spatial dimensions small, initial temperature close to T → winding modes about all Cosmology H spatial sections are excited. Framework Space-Time Std. Cosmology Expansion of any one spatial dimension requires the Inflation annihilation of the winding modes in that dimension. String gas
Conclusions
Decay only possible in three large spatial dimensions. → dynamical explanation of why there are exactly three large spatial dimensions.
57 / 68 Structure formation in inflationary cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
N.B. Perturbations originate as quantum vacuum fluctuations.
58 / 68 Background for string gas cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
59 / 68 Structure formation in string gas cosmology A. Nayeri, R.B. and C. Vafa, Phys. Rev. Lett. 97:021302 (2006)
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
N.B. Perturbations originate as thermal string gas fluctuations. 60 / 68 Power spectrum of cosmological fluctuations
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology Key features: Inflation scale-invariant like for inflation String gas Conclusions slight red tilt like for inflation
61 / 68 Anisotropies in the Cosmic Microwave Background (CMB)
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Credit: NASA/WMAP Science Team 62 / 68 Quantification of the CMB data
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology
Inflation
String gas
Conclusions
Credit: NASA/WMAP Science Team
63 / 68 Spectrum of Gravitational Waves
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time Std. Cosmology Key features: Inflation scale-invariant (like for inflation) String gas Conclusions slight blue tilt (unlike for inflation)
64 / 68 Status of the “Big Bang" in String Gas Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time The universe was very, very hot and dense 13 billion Std. Cosmology years ago. Inflation
String gas In this sense there was a hot “primordial" fireball. Conclusions But: there was no Big Bang Singularity. There was no beginning of time.
65 / 68 Status of the “Big Bang" in String Gas Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time The universe was very, very hot and dense 13 billion Std. Cosmology years ago. Inflation
String gas In this sense there was a hot “primordial" fireball. Conclusions But: there was no Big Bang Singularity. There was no beginning of time.
65 / 68 Status of the “Big Bang" in String Gas Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time The universe was very, very hot and dense 13 billion Std. Cosmology years ago. Inflation
String gas In this sense there was a hot “primordial" fireball. Conclusions But: there was no Big Bang Singularity. There was no beginning of time.
65 / 68 Status of the “Big Bang" in String Gas Cosmology
Early Universe
R. Branden- berger
Cosmology
Framework Space-Time The universe was very, very hot and dense 13 billion Std. Cosmology years ago. Inflation
String gas In this sense there was a hot “primordial" fireball. Conclusions But: there was no Big Bang Singularity. There was no beginning of time.
65 / 68 Plan
Early Universe
R. Branden- berger 1 What is Cosmology? Cosmology Framework 2 Space-Time Framework Std. Cosmology Space-Time Inflation Standard Big Bang Cosmology String gas
Conclusions 3 Inflationary Cosmology
4 String Cosmology
5 Conclusions
66 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Conclusions
Early Universe Cosmology is a vibrant field with lots of observational R. Branden- berger data. Paradigms of early universe cosmology have been Cosmology developed. Framework Space-Time Paradigm 1: Standard Big Bang Model. Std. Cosmology
Inflation Paradigm 2: Inflationary Universe scenario - current
String gas paradigm. Conclusions In both Paradigms 1 and 2 there was a Big Bang singularity. Paradigm 2 has conceptual problems → motivates the search for an improved paradigm. Superstring theory may provide a new paradigm. Superstring cosmology may resolve the Big Bang singularity. It is possible to observationally probe string cosmology.
67 / 68 Status of the “Big Bang"
Early Universe We know that going back in time 13 billion years there R. Branden- berger was a very hot early phase, a primordial fireball.
Cosmology If this is what you mean by “Big Bang": then there WAS
Framework a “Big Bang". Space-Time Std. Cosmology We do not know if there was a “Big Bang singularity", a Inflation beginning of time. String gas Our current paradigms of early universe cosmology Conclusions predict a beginning of time. But only if we extrapolate the models beyond where they can be used. Superstring theory may lead to a cosmology without a beginning of time. If this is true then there may not have been a “Big Bang" (singularity).
68 / 68