Particle Physics at the Energy Frontier Tevatron → LHC & The Very Early Universe Tony LissAir Force Institute of TechnologyApril 10, 2008.

Slides:



Advertisements
Similar presentations
Bruce Kennedy, RAL PPD Particle Physics 2 Bruce Kennedy RAL PPD.
Advertisements

The coldest and emptiest place in the solar system. The highest energies ever created. Cameras the size of cathedrals. A machine 27km long. LHC Overview.
The Expanding Universe!
ATLAS Experiment at CERN. Why Build ATLAS? Before the LHC there was LEP (large electron positron collider) the experiments at LEP had observed the W and.
THE SEARCH FOR THE HIGGS BOSON Aungshuman Zaman Department of Physics and Astronomy Stony Brook University October 11, 2010.
Cosmology The Origin and Future of the Universe Part 2 From the Big Bang to Today.
January 2011 David Toback, Texas A&M University Texas Junior Science and Humanities Symposium 1 David Toback Texas A&M University Texas Junior Science.
27 km ring Large Hadron Collider went online on Sept
Hunting for New Particles & Forces. Example: Two particles produced Animations: QPJava-22.html u u d u d u.
March 24, 2007Dark Puzzles of the Universe1 Prof. Bhaskar Dutta and Prof. Teruki Kamon Department of Physics Texas A&M University Saturday Morning Physics.
Physics with ATLAS and CMS Are there new symmetries or extra-dimensions? What is dark matter? Where does mass come from? The two big multi-purpose experiments.
March 2011 David Toback, Texas A&M University Davidson Scholars 1 David Toback Texas A&M University Davidson Scholars March 2011 The Big Bang, Dark Matter.
J. Nielsen1 The ATLAS experiment at the Large Hadron Collider Jason Nielsen UC Santa Cruz VERTEX 2004 July 28, 2010.
Particle Physics From Strings To Stars. Introduction  What is Particle Physics?  Large Hadron Collider (LHC)  Current Experiments – ALICE – ATLAS –
The Big Bang, the LHC and the Higgs Boson Dr Cormac O’ Raifeartaigh (WIT)
LHC’s Second Run Hyunseok Lee 1. 2 ■ Discovery of the Higgs particle.
January 2009 David Toback, Saturday Morning Physics 1 Prof. David Toback Texas A&M University January 2014 Dark Matter and the Big Bang Theory.
 Stable and unstable particles  How to observe them?  How to find their mass?  How to calculate their lifetime? 6/9/
The Big Bang. CMBR Discussion Why can’t the CMBR be from a population of unresolved stars at high redshift?
ROY, D. (2011). Why Large Hadron Collider?. Pramana: Journal Of Physics, 76(5), doi: /s
The Higgs Boson: without the maths and jargon David Hall Graduate Seminar Series St Catherine’s College MCR 11 th May 2011.
My Chapter 30 Lecture.
Joseph Haley Joseph Haley Overview Review of the Standard Model and the Higgs boson Creating Higgs bosons The discovery of a “Higgs-like” particle.
The Dark Side of the Universe What is dark matter? Who cares?
Point 1 activities and perspectives Marzio Nessi ATLAS plenary 2 nd October 2004 Large Hadron Collider (LHC)
Atomic Structure Basic and Beyond. What are the 3 major parts of an atom? Protons Electrons Neutrons.
School of Arts & Sciences Dean’s Coffee Presentation SUNY Institute of Technology, February 4, 2005 High Energy Physics: An Overview of Objectives, Challenges.
LHC and Search for Higgs Boson Farhang Amiri Physics Department Weber State University Farhang Amiri Physics Department Weber State University.
1 The Standard Model of Particle Physics Owen Long U. C. Riverside June 27, 2014.
Quarks, Leptons, Bosons, the LHC and all that. Tony Liss OLLI Lecture September 23, 2008.
Atomic theory explains what the world is and how it’s held together. The Atom.
Presented by Laura Johnson, Catherine Jones, Catherine Cutts and Victoria Green.
Recreating the Big Bang with the World’s Largest Machine Prof Peter Watkins Head of Particle Physics Group The University of Birmingham Admissions Talk.
The Professional Development Service for Teachers is funded by the Department of Education and Skills under the National Development Plan PARTICLE Physics.
Introduction to CERN David Barney, CERN Introduction to CERN Activities Intro to particle physics Accelerators – the LHC Detectors - CMS.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
What is the Higgs??? Prof Nick Evans University of Southampton.
INVASIONS IN PARTICLE PHYSICS Compton Lectures Autumn 2001 Lecture 8 Dec
A singularity formed by a previous collapsed Universe? Multiple Universes? We just don’t know… YET What Caused It?
ATLAS experiment at the CERN Large Hadron Collider Peter Watkins, Head of Particle Physics Group, University of Birmingham, UK
Alpha S. A measure of the strongest fundamental force of nature- The Strong Force.
SubAtomic Physics & Astrophysics Intimate Connexion between Very Large and Very Small.
Working Together Scientific Collaboration or Conspiracy?
Chapter 17 The Beginning of Time. Running the Expansion Backward Temperature of the Universe from the Big Bang to the present (10 10 years ~ 3 x
Re-creating the Big Bang Experiments at the Large Hadron Collider Dr Cormac O’ Raifeartaigh (WIT) Albert Einstein Ernest Walton.
Modern Physics. Reinventing Gravity  Einstein’s Theory of Special Relativity  Theorizes the space time fabric.  Describes why matter interacts.  The.
FSU Experimental HEP Faculty Todd Adams Susan Blessing Harvey Goldman S Sharon Hagopian Vasken Hagopian Kurtis Johnson Harrison Prosper Horst Wahl.
Introduction to CERN Activities
The Higgs Boson Observation (probably) Not just another fundamental particle… July 27, 2012Purdue QuarkNet Summer Workshop1 Matthew Jones Purdue University.
CERN, 8 February, 2001 Egil Lillestøl, CERN & Univ. of Bergen Lectures recorded at :
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
Introduction to Particle Physics I Sinéad Farrington 18 th February 2015.
Compelling Scientific Questions The International Linear Collider will answer key questions about matter, energy, space and time We now sample some of.
The Standard Model of the elementary particles and their interactions
Jonathan Nistor Purdue University 1.  A symmetry relating elementary particles together in pairs whose respective spins differ by half a unit  superpartners.
What about the Higgs Boson? What precisely is the Higgs? We describe dynamics of a system via a Lagrangian – One can completely replicate all of Newtonian.
1 Particle Physics, The Mysteries of the Universe, and The LHC Nhan Tran Johns Hopkins University.
1 The Standard Model of Particle Physics Owen Long U. C. Riverside March 1, 2014.
Particle Detectors January 18, 2011 Kevin Stenson.
Particle Physics Why do we build particle accelerators? The surface is flat Still flat Oh no its not Big balls cannot detect small bumps.
CERN Richard Jacobsson 1 Welcome to CERN!. CERN Richard Jacobsson 2 What is CERN? l European Organization for Nuclear Research, founded in 1954 l Currently.
880.P20 Winter 2006 Richard Kass 1 Detector Systems momentumenergy A typical detector beam looks something like: BaBar, CDF, STAR, ATLAS, GLAST…… particle.
Higgs in the Large Hadron Collider Joe Mitchell Advisor: Dr. Chung Kao.
Introduction to Particle Physics II Sinéad Farrington 19 th February 2015.
SPH4U Elementary Particles.
Particle Physics Theory
The Mysteries of Particle Physics and how we are trying to solve them
SUSY SEARCHES WITH ATLAS
Atomic Structure Basic and Beyond.
Atomic Structure Basic and Beyond.
Presentation transcript:

Particle Physics at the Energy Frontier Tevatron → LHC & The Very Early Universe Tony LissAir Force Institute of TechnologyApril 10, 2008

Two Views of the Universe High energy physicists study the smallest, most fundamental objects and the forces between them. Cosmologists study what there is on the largest possible scales and try to understand how it got that way. But these two very different approaches address many of the same questions: What is the Universe made of & how does it behave?

???? The High-Energy View The matter around us is made up of “quarks” and “leptons” And held together by four forces, each with a force carrier: A proton is made of U U D Add an electron to make a hydrogen atom Electromagnetic Strong Weak Gravity

Unification of the Forces Electric Magnetic Weak Strong Electromagnetic Electroweak “Low Energy” “High Energy” “Very (very)High Energy” Theory (“Standard Model”) works up to ~here … And you may notice that gravity isn’t in this picture… STRING THEORY ??? Part way to Einstein’s dream! Higgs Bosons born here

Cosmology, Particle Physics, the Universe and All That

Successes of Particle Physics + Big Bang Light elements (H to Li) were made in the early universe –And we can calculate how much! astron.berkeley.edu/~mwhite/darkmatter/bbn.html Predicted abundance depends on density of “baryons” – particles made of 3 quarks (like a proton or a neutron) About 1 He nucleus for every 10 protons (25% by mass) The grey band is where the measured & calculated abundances are.

But Wait! Most of the universe is not normal (“baryonic”) matter! Recent cosmological measurements put the density of the universe here.

Dark Matter (Not a New Idea) Speed of stuff out here Doesn’t match luminous matter in here! There’s DARK MATTER in Galaxies!!

Dark Matter In Between Galaxies Too! Motion of a galaxy out here Doesn’t agree with luminous matter in here The “Hydra” Galactic Cluster  matter ~ 0.3 from galactic clusters

Studying the Universe at Accelerators Accelerate particles to very high energies and smack them together. E=Mc 2 : Make new stuff and study how it behaves. This picture shows a proton and antiproton colliding to make a pair of top quarks. Top quarks were discovered 14 years ago at Fermilab Michael Goodman Fermi National Accelerator Laboratory

Hadron-Hadron Collisions Proton-antiproton (Tevatron) or proton-proton (LHC) collisions: Each collision (“event”) is between the hadron constituents. What can happen is…EVERYTHING

Cross Sections The total pp cross section is here at ~10 11 !

This happens only once in ~10 10 collisions

Data Taking (TeVatron) Protons & antiprotons collide at ~2.5 MHz 0.25Hz of W/Z production ~100 Hz of high E T jets ~100 Hz of b-quark production.0002 Hz of top quark production ?? Hz of new physics 1% “Acceptance” ~1% Analysis Mode ~10 -2 Hz for analysis 10% “Acceptance” ~40% Analysis Mode ~10 -5 Hz for analysis ?? “Acceptance” ?? Analysis Mode 20% “Acceptance” ~20% Analysis Mode ~10 -2 Hz for analysis Prescale/20 10% “Acceptance” 85% to analysis ~0.4 Hz for analysis

The CDF Detector at FNAL

 The Mass of the Top Quark  The Mass of the W Boson

Measuring the Top Mass There are many subtleties to improve S/B and resolution, but basically… Measure for each of the decay objects

Measuring the Top Mass

Measuring the W Boson Mass

A Window on the Higgs! Experimental bound (LEP) WW W H WW t b The result is marginally inconsistent with the SM… SUSY????

Making Higgs Bosons

Finding The Higgs The Higgs “couples to mass”, so it’s preferred decay channel depends on its (unknown) mass. As if life were not difficult enough…

Looking for Higgs (is hard)

No Higgs…yet

SUSY Every quark, lepton and force carrier has a SUSY partner (sparticles). –Sparticles would be made copiously in the early (HOT) universe. –They all decay away quickly, except for the lightest one (neutralino), which can’t. –The dark matter might be made up of neutralinos!! Make SUSY particles at an accelerator: E=Mc 2 happening here!

Another Reason to Believe in SUSY? Einstein’s dream of a “Unified Field Theory”, now needs SUSY: Energy Strength of force No SUSY Energy Strength of force SUSY EM weak strong

Searching for SUSY – an example SUSY models come in many different flavors, but one characteristic of many of them is signatures with large “Missing E T ” – Undetectable particles whose momentum is unmeasured. In these diagrams “charginos” and “neutralinos” are produced. In their subsequent decay, the lightest “neutralino” is produced but remains undetected.

Searching for Charginos & Neutralinos What the signal would look like (if it were there) The data Backgrounds

No SUSY So Far Many searches, no sightings… The hunt continues… At LHC there is 7x more “reach” (E=Mc 2 ) for making SUSY particles. But maybe SUSY isn’t the right model… We can find it anyway if M<E/c 2 !

On to the LHC!

ATLAS Detector at CERN

ATLAS is VERY BIG

ATLAS

A (simulated) Higgs event in ATLAS

A Black Hole in ATLAS

The Universe as We Know It Dark Matter Dark Energy This is NOT what we thought as recently as 10 years ago!! Our fabulously successful “Standard Model of particle physics” explains only 4% of the universe… So far… Atoms 73% 4% 23%

Perspective Our theories of cosmology and particle physics are extremely successful, but leave significant open questions. As new phenomena are discovered, we adapt the theories and test them with experiments & observations. The next ten years of accelerator experiments and cosmological measurements are guaranteed to bring new insights and new surprises!