1 Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 12 Nov. 18, 2015
2 Today Big Bang Nucleosynthesis and Neutrinos Particle Physics & the Early Universe Standard Model of Particle Physics Relic Dark Matter particles Baryogenesis
3 Assignments This week: read Hawley and Holcomb, Chapter 12. This Friday: Essay 4 due on HH, Chapter 12. Final project: choose a topic in cosmology from popular books or an article in the reputable press: Scientific American, NY Times, Astronomy Magazine, Discover, Science News, write a 3-page essay in the style of a newspaper or magazine article on that theme, in your own words.
4 Some Possible Project Topics Recent Measurements of the Cosmic Expansion Rate 100 th Anniversary of General Relativity Einstein s Views on the Cosmological Constant Evidence for Black Holes in the Universe Experiments searching for Dark Matter Cosmic Surveys constraining the nature of Dark Energy (DES, eboss, DESI, LSST, WFIRST, Euclid, ) Theories of Dark Energy Theories of Modified Gravity to explain Cosmic Acceleration Experiments Measuring the Cosmic Microwave Background (Planck, SPT, ACT, BICEP, ) (Testing) Theories of Primordial Inflation Computer Simulations of the formation and evolution of large-scale structure and galaxies
5 Cosmic History Going back in time from the present toward the Big Bang, first significant epoch we reached was Hydrogen recombination/ photon decoupling at t ~ 380,000 years (T ~ 3000 deg). Continuing back, the next major epoch is that of Big Bang Nucleosynthesis (BBN), at t ~ 3 minutes (T ~ 10 9 deg).
6 BBN abundances h = H 0 /(100 km/sec/mpc) Fraction of baryonic mass in He 4 Deuterium to Hydrogen ratio Lithium to Hydrogen ratio Boxes: observed abundances Wide vertical band: BBN (mainly D) Narrow band: CMB Lithium in old stars is discordant
7 BBN as a Probe of Particle Physics Observed light element abundances (except for Lithium) agree with predictions of Hot Big Bang Cosmology, nuclear physics (which determines fusion reaction rates), and the Standard Model of Particle Physics and are concordant with measurements of the CMB anisotropy. We can therefore use BBN as a laboratory to constrain physical phenomena not described by (i.e., that are beyond) the Standard Model of Particle Physics. Example: neutrinos and other relativistic particle species
8 The Structure of Baryonic Matter 1 1/10,000 1/100,000 1/100,000,000
9 Particles of the Standard Model
10 Particles of the Standard Model Half-integer spin Integer spin Electromagnetic force (interacts with electric charge) Strong force (interacts with color charge, only carried by quarks) Weak force (interacts with flavor) Weak force
11 BBN as a Probe of Particle Physics Observed light element abundances (except for Lithium) agree with predictions of Hot Big Bang Cosmology, nuclear physics (which determines fusion reaction rates), and the Standard Model of Particle Physics and are concordant with measurements of the CMB anisotropy. We can therefore use BBN as a laboratory to constrain physical phenomena not described by (i.e., that are beyond) the Standard Model of Particle Physics. Example: neutrinos and other relativistic particle species
12 Particles of the Standard Model Photon Gluon Protons and neutrons each composed of 3 up (u) and down (d) quarks, `held together by gluons
13 Cosmic Neutrinos Massless (or extremely light), electrically neutral particles that only interact via the Weak Force (with W, Z bosons) Standard Model includes 3 massless neutrinos: ν e ν μ ν τ In the early Universe, they are produced in weak interactions between quarks and leptons and should be about as abundant as the photons of the CMB. They form a Cosmic Neutrino Background (CNB) analogous to the Cosmic Microwave (Photon) Background. Just as CMB photons decouple around t rec =380,000 years or T rec ~3000 deg K, cosmic neutrinos decouple (stop interacting) at t F ~1 second or T F ~10 10 K. Thus, if we could observe this CNB, it would give us a snapshot of the Universe when it was 1 second old. So far, haven t come up with a way to detect CNB neutrinos directly (they have very low energy and interact very weakly).
14 Cosmic Neutrinos Massless (or extremely light), electrically neutral particles that only interact via the Weak Force (with W, Z bosons) Standard Model includes 3 massless neutrinos: ν e ν μ ν τ In the early Universe, they are produced in weak interactions between quarks and leptons and should be about as abundant as slightly the colder photons than the of CMB the CMB. They form a Cosmic Neutrino Background (CNB) analogous to the Cosmic Microwave (Photon) Background. Just as CMB photons decouple around t rec =380,000 years or T rec ~3000 deg K, cosmic neutrinos decouple (stop interacting) at t F ~1 second or T F ~10 10 K. Thus, if we could observe this CNB, it would give us a snapshot of the Universe when it was 1 sec old. So far, haven t come up with a way to detect CNB neutrinos directly.
15 BBN and Neutrinos Energy density of neutrinos is comparable to the energy density of photons during BBN, and together they dominate over massive particles. The expansion rate (at fixed temperature) during BBN is determined by the total number of massless (or relativistic) species: more massless particles à higher density à higher expansion rate BBN involves competition between weak interaction rates and cosmic expansion rate: changing the expansion rate H(T) will change light element abundances, particularly 4 He. Agreement of BBN predictions with observed element abundances thus constrains the number of species of light particles (e.g., the number of light neutrinos), N eff.
17 CMB, BBN and Neutrinos Standard Model with N eff =3 light neutrinos fits: evidence for Cosmic Neutrino Background! Little room left for additional light particles 4 He measurements D measurements CMB Ω b h 2
18 Cosmology & Particle Physics The BBN constraint on neutrino properties was historically one of the first examples of the symbiotic interaction between cosmology & particle physics, a major theme over the last 35 years. Cosmology: to understand the early Universe, we need to understand physics at the highest energies Particle Physics: since accelerators cannot reach the highest energy scales, cosmology can constrain the physical laws at very high energies: probe physics beyond the Standard Model.
19 Logarithmic view of Cosmic History
20 Cosmology & Particle Physics: Offspring of the Marriage In addition to the light nuclei and the thermal Cosmic Microwave Background Radiation, there are a number of more speculative but well-motivated relics from the Hot Big Bang. Two prime examples: Cold Dark Matter particles Asymmetry between matter & anti-matter in the Universe (baryon asymmetry) Later, we will discuss what is perhaps the most remarkable child of this marriage: the Inflationary Scenario.
21 Non-baryonic Dark Matter Evidence on the amount of Dark Matter from Big Bang Nucleosynthesis and CMB indicates 25% of the Universe is in an exotic Dark Matter component, made of some as-yet undiscovered elementary particle. In order for it to be dark matter, this particle should be at most weakly interacting (i.e., interact with W, Z bosons, not photons) and have an abundance in the Universe of Ω dark matter = Models of Elementary Particle Physics provide a number of Dark Matter candidates, hypothetical particles with these requisite properties.
22 (Some) Dark Matter Candidates Neutrinos (mass ~ few electron Volts ~ 10-5 electron s mass) known to exist, should be as abundant as CMB photons. Weakly Interacting Massive Particles (WIMPS) (mass ~ x proton mass) Favorite candidate of particle physics theorists Axions (mass ~ 10-5 electron Volts ~ electron mass) Hypothetical particle that arises in theories that seek to explain certain features of the strong interactions Note: these candidates involve physics beyond the well-tested Standard Model of Particle Physics. Thus, determining the nature of the Dark Matter should tell us about fundamental physics.
23 Dark Matter Properties: Clustering Three `types of Dark Matter distinguished by the objects they can be found in: Cold DM: clusters on all scales; particles slowly moving,... Candidates: WIMPs, axions, Hot DM: these particles moved at near the speed of light early on, and can only cluster in objects as big as clusters (or larger): would not expect to find them in individual galaxy halos. Candidate: neutrinos Warm DM: clusters on scales of galaxies or larger. Candidate: heavy neutrinos (in certain cases)
24 Dark Matter & Large-scale Structure These 3 different types of DM (cold, hot, warm) lead to different scenarios for the formation of galaxies and large-scale structures in the Universe. Observations of the large-scale distribution of galaxies (from galaxy surveys) indicate that the bulk of the DM is cold (or at most slightly warm).
25 Computer Simulation of the formation of Galaxies and Clusters in Expanding Universe with Cold Dark Matter
26 Relic Cold Dark Matter WIMPs In the early Universe, consider a Weakly Interacting Massive Particle interacting with other particles via the Weak Interaction. At very high temperatures (very early times), when the typical thermal (kinetic) energy per WIMP is much larger than its rest mass, k B T >> m WIMP c 2, they move at essentially the speed of light and are as abundant as the background radiation photons. A critical interaction is the annihilation of a WIMP and anti-wimp into another weakly interacting particle (and anti-particle) and the inverse of this reaction: the creation of a WIMP/anti-WIMP pair.
27 Relic WIMPs When the temperature drops below the rest mass of the WIMP, k B T < m WIMP c 2, the rate of annihilation of WIMP/ anti-wimps becomes larger than their rate of production: the abundance of WIMPs falls compared to photons. At a certain point, the abundance of WIMPs and anti- WIMPs has dropped so low, that they can no longer find each other to annihilate. The WIMPs freeze out of thermal equilibrium (analogous to freeze-out of weak interactions just before BBN) and their abundance relative to photons thereafter remains fixed.
28 Relic WIMPs WIMP abundance relative to photons weaker stronger time Abundance at freeze-out determined by strength of the annihilation interactions: strongerà lower.
29 Relic WIMPs Recall for baryons, Ω b =0.05 from BBN and CMB. This corresponds to a baryon to photon ratio: n baryon /n photon = 6 x For WIMPs with characteristic Weak Interaction rates, their abundance relative to photons at freeze-out is of order or n WIMP /n photon ~ 3 x 10 9 (m proton /m WIMP ) Ω WIMP ~ 0.25 so WIMPs are `natural Dark Matter candidates! This is sometimes called the WIMP miracle.
30 What is the WIMP? It can t be one of the elementary particles of the Standard Model (quarks or leptons): they make up only 5% of the critical density, and we need 25%. It must come from (and would thus be evidence for) physics beyond the Standard Model.
31 Symmetries in Nature
32 Symmetries and Conservation Laws Certain systems in Nature exhibit symmetries in space and time: rotational invariance (e.g., of a sphere) spatial or time translation invariance reflection (left-right) symmetry Noether s theorem: for systems with symmetry, there are corresponding quantities that are conserved in time. Example: spatial translation invariance ß à conservation of momentum. Emmy Noether
33 External and Internal Symmetries External symmetries in space and time: rotational invariance (e.g., of a sphere) spatial or time translation invariance reflection (left-right) symmetry Internal symmetries (not involving spatial transformations): Elementary particles exhibit many such symmetries, and there are associated conservation laws. Example: gaugeinvariance of the electromagnetic field ß à conservation of electric charge
34 Symmetry & Unification well-tested speculative 1800 s: electricity & magnetism given a unified description in Maxwell s theory of Electromagnetism 1930 s: Initial Theory of Weak Interactions (Fermi) 1960 s: Electromagnetic & weak interactions unified in electroweak theory (Glashow, Weinberg, Salam) 1970 s: Theory of Strong Interactions (QCD) 1970 s: Standard Model of Particle Physics 1970 s: Electroweak & strong interactions unified in Grand Unified Theories (GUTs) 1980 s-20??: Unify electroweak, strong, and gravitational interactions in Superstring Theory
36 Symmetry and the Standard Model Weak & Electromagnetic interactions arise from a common Electroweak symmetry. This model now very precisely tested and confirmed in particle physics experiments at accelerators. But the manifestations of these two interactions appear to be very different: Electromagnetism: photon is massless--> EM force has infinite range Weak interaction: W,Z bosons are massive (~100 times proton mass) à weak force short range Why are they so different?
37 Spontaneous Symmetry Breaking Symmetries of the theory may not be manifest in Nature: they can be broken. Everyday Examples: Pencil balanced on its end is rotationally symmetric, looks the same from any angle. But when it falls, it must do so in a particular direction, thus breaking the rotational symmetry. People sitting at a round table must choose which glass to drink from, the one on their left or their right. Each is possible: initially, the system is left-right symmetric. However, once someone chooses, the symmetry is broken.
38 Higgs Boson & Symmetry Breaking Higgs Boson: spin-zero particle (scalar field) that breaks the electroweak symmetry and differentiates the electromagnetic from the weak interactions. The Higgs interacts with and gives mass to the W and Z Bosons and to all other elementary matter particles, but leaves the photon massless. Can think of it as a kind of `medium through which elementary particles move. It is a `field (like an electromagnetic or gravitational field) but with the same value throughout all of space. Like the photon of electromagnetism, the Higgs field has an associated particle, the Higgs boson, with a mass about 130 times the proton mass.
39 Large Hadron Collider now operating in Switzerland. This is where the Higgs Boson was discovered in 2012.
41 Supersymmetry (SUSY) Hypothetical symmetry between fermions and bosons. For every particle of the Standard Model, there would be a supersymmetric partner particle with different spin. Each particle and its SUSY partner would have the same mass. Such SUSY particles have not (yet) been seen at the LHC: they must be heavier than Standard Model particles: SUSY must be a broken symmetry in nature (or it may just not be a symmetry of nature at all).
42 Supersymmetry (SUSY) The lightest neutralino particle is expected to be stable (doesn t decay) and would be a natural WIMP candidate. Dark matter experiments searching for them.
43 Supersymmetry (SUSY) The lightest neutralino particle is expected to be stable (doesn t decay) and would be a natural WIMP candidate. Dark matter experiments searching for them.
44 Supersymmetry (SUSY)
45 The Theoretical Appeal of SUSY Explain hierarchy of energy scales in particle physics: W, Z bosons orders of magnitude lighter than GUT scale Coupling constant unification at GUT scale
46 Deep underground experiments are searching for Dark Matter WIMPs
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