GOD PARTICLE OR GOD-DAMN PARTICLE? WORK AT THE LARGE HADRON COLLIDER - DR VICTORIA MARTIN UNIVERSITY OF EDINBURGH IESIS WES MCMILLAN LECTURE
←
→
Page content transcription
If your browser does not render page correctly, please read the page content below
God particle or god-damn particle? Work at the Large Hadron Collider Dr Victoria Martin University of Edinburgh IESIS WES McMillan Lecture 1
Contents •The world of particle physics and the need for the Higgs boson •A recipe: how to find a Higgs boson. •The Large Hadron Collider: an engineering marvel. •And, the results are in •Higgsteria! 3
The World of Particle Physics • Particle physics aims to understand the universe on the smallest accessible length scales. ➡ We investigate the smallest components of matter − the fundamental particles − that make up you and me. ➡ We investigate the interactions between these particles. 4
Interactions • The interactions of the quarks and leptons are governed by four forces • The strong nuclear force Strongest to weakest • The electromagnetic force • The weak nuclear force • Gravity • The strong and weak forces are only felt over very, very short distances e.g. (0.00000000000000001m = 10 −17 m) • The electromagnetic and gravitational forces can be felt over large distances. 6
Interactions • The interactions of the quarks and leptons are governed by four forces Force carrying particle • The strong nuclear force Strongest to weakest gluons, g • The electromagnetic force photons, γ • The weak nuclear force “W and Z bosons”, W, Z • Gravity gravitons • The strong and weak forces are only felt over very, very short distances e.g. (0.00000000000000001m = 10 −17 m) • The electromagnetic and gravitational forces can be felt over large distances. 6
The “Standard Model” of Particle Physics • The Standard Model of Particle Physics describes the quarks, leptons and the strong, weak and electromagnetic interactions between using: • Einstein’s theory of special relativity (physics of the very fast) • Quantum physics (physics of the very small) • Symmetries (observed in many areas of physics) • Possibly the best tested and validated theory in physics! 7
The W-boson • The effects of the W-boson were know since Enrico Fermi in the 1930s • The W-boson was discovered by the UA1 and UA2 experiments at CERN, 30 years ago. 8
The Z-boson • The effects of the Z-boson were discovered in 1973 at the Gargamelle experiment at CERN. • The UA1 and UA2 experiments at CERN also discovered the Z-boson. 9
W-boson in the Sun • The W-boson can change the nature of particles: ➡ it can turns protons into neutrons, and vice-versa • proton → neutron + anti-electron + neutrino H + H → 2H + e+ + νe • W-bosons facilitate the first step of Hydrogen gas burning in the sun! 10
The Higgs Mechanism • Proposed The Higgs Mechanism was proposed in 1964 separately by Higgs; Brout & Englert; Guralnik, Hagen & Kibble. • The Higgs mechanism an proposes an extra potential: V (φ) = −µ2 φ2 + λφ4 V(ϕ) • The depth of the potential is proportional to the W boson mass. • Also related to the Z-boson mass. 11
The Higgs Mechanism • Proposed The Higgs Mechanism was proposed in 1964 separately by Higgs; Brout & Englert; Guralnik, Hagen & Kibble. • The Higgs mechanism an proposes an extra potential: V (φ) = −µ2 φ2 + λφ4 V(ϕ) • The depth of the potential is proportional to the W boson mass. • Also related to the Z-boson mass. 11
The Higgs Boson 12
The Higgs Boson In 1964 Peter Higgs was the only one of the six to observe this potential would also create a new boson: the Higgs boson! 12
The Higgs Mechanism 1. IESIS members before the James Watt Dinner; all free to move around the room. 13
The Higgs Mechanism 1. IESIS members before the James Watt Dinner; all free to move around the room. 13
The Higgs Mechanism 1. IESIS members before the James 2. In comes Muffy Calder; everyone Watt Dinner; all free to move around wants to speak to her. the room. Everyone crowds around her. Muffy is not free to move around; she has gained inertia by interacting with the crowd. 13
The Higgs Mechanism 1. IESIS members before the James 2. In comes Muffy Calder; everyone Watt Dinner; all free to move around wants to speak to her. the room. Everyone crowds around her. Muffy is not free to move around; she has gained inertia by interacting with the crowd. This is analogous to how the particles acquire mass: by interacting with the Higgs field. Science advisors of different popularity gain different masses. 13
The Higgs Boson 3. Later in the evening; IESIS members enjoying a digestive. A rumour enters the room: Muffy has convinced Alex Salmond to appoint a minster for Engineering & Science ! 14
The Higgs Boson 3. Later in the evening; IESIS members enjoying a digestive. A rumour enters the room: Muffy has convinced Alex Salmond to appoint a minster for Engineering & Science ! 14
The Higgs Boson 3. Later in the evening; IESIS members enjoying a digestive. A rumour enters the room: Muffy has convinced Alex Salmond to appoint a minster for Engineering & Science ! 4. Everyone gather together to spread the rumour. The group of engineers acquire inertia. 14
The Higgs Boson 3. Later in the evening; IESIS members enjoying a digestive. A rumour enters the room: Muffy has convinced Alex Salmond to appoint a minster for Engineering & Science ! 4. Everyone gather together to spread the rumour. The group of engineers acquire inertia. The clustering of the field of engineers is as if a new massive particle has formed. This is the Higgs boson. 14
Q: Why care about the Higgs boson? A: The Higgs boson makes the W-boson heavy. The heaviness of the W-boson makes the burning of Hydrogen in the sun relatively slow. The slow burning means the sun will support life on earth for the next one billion years! 15
How to find a Higgs 16
A note on units Particle physicists don’t use SI units. We typically use: • GeV or TeV for energy. • 1 GeV is 1.6 × 10−10 Joules. • 1 TeV is 1.6 × 10−7 Joules, or about the energy of a flying mosquito • GeV/c 2 for mass. 1 GeV/c2 is: • 3.1 × 10−23 grams • 0.93 atomic mass units • roughly the mass of a proton 17
A simple recipe 18
A simple recipe 1. Take two very high energy protons (fresh from CERN). 18
A simple recipe 1. Take two very high energy protons (fresh from CERN). 2. Smash together. 18
A simple recipe 1. Take two very high energy protons (fresh from CERN). 2. Smash together. 3. One in 100 billion collisions will form a Higgs boson. 18
A simple recipe 1. Take two very high energy protons (fresh from CERN). 2. Smash together. 3. One in 100 billion collisions will form a Higgs boson. 4. Once formed, the Higgs boson will decay after 10−22 seconds. 18
A simple recipe 1. Take two very high energy protons (fresh from CERN). 2. Smash together. 3. One in 100 billion collisions will form a Higgs boson. 4. Once formed, the Higgs boson will decay after 10−22 seconds. 5. Assemble a highly sophisticated, state-of- the-art detector around the collision point. 18
A simple recipe 1. Take two very high energy protons (fresh from CERN). 2. Smash together. 3. One in 100 billion collisions will form a Higgs boson. 4. Once formed, the Higgs boson will decay after 10−22 seconds. 5. Assemble a highly sophisticated, state-of- the-art detector around the collision point. 6. Observe the particles produced from the Higgs boson decay. 18
A simple recipe 1. Take two very high energy protons (fresh from CERN). 2. Smash together. 3. One in 100 billion collisions will form a Higgs boson. 4. Once formed, the Higgs boson will decay after 10−22 seconds. 5. Assemble a highly sophisticated, state-of- the-art detector around the collision point. 6. Observe the particles produced from the Higgs boson decay. 7. Repeat 25 million times a second for 1½ years. 18
CERN • CERN is the European Organization for Nuclear Research (Organisation européenne pour la recherche nucléaire). • Located at the Franco-Swiss border near Geneva, Switzerland. • A collaboration of 20 European countries, including the UK. • 3,900 employees • 10,000 visiting scientists and engineers from 608 Universities and Research facilities (including Edinburgh and Glasgow!) • CERN provides particle accelerators, used by 17 experiments. 19
CERN’s Large Hadron Collider • The Large Hadron Collider (LHC) is current CERN’s main activity. • Six experiments use the LHC. • A chain of accelerators, developed over decades, accelerates protons to 4 TeV, the highest ever energy for an accelerator. • From 2015, the LHC will run at 8 TeV. • Linear accelerator: up to 50 MeV • Proton Synchroton Booster: 50 MeV → 1.4 GeV • Proton Synchroton: 1.4 GeV → 26 GeV • Super Proton Synchroton: 26 GeV → 450 GeV • Large Hadron Collider: 450 GeV → 4 TeV 20
CERN’s Large Hadron Collider • The Large Hadron Collider (LHC) is current CERN’s main activity. • Six experiments use the LHC. • A chain of accelerators, developed over decades, accelerates protons to 4 TeV, the highest ever energy for an accelerator. • From 2015, the LHC will run at 8 TeV. • Linear accelerator: up to 50 MeV • Proton Synchroton Booster: 50 MeV → 1.4 GeV • Proton Synchroton: 1.4 GeV → 26 GeV • Super Proton Synchroton: 26 GeV → 450 GeV • Large Hadron Collider: 450 GeV → 4 TeV 20
LHC: Facts and Figures 21
LHC: Facts and Figures 21
LHC: Facts and Figures 21
LHC: Facts and Figures 21
LHC: Facts and Figures • 27km circumference • 50 to 175 m underground • 9300 magnets used to keep the beam in orbit • 1232 are dipole magnets: • 14.3 m long, • operate at 1.9 K, • provides 8.3 Tesla, • cost 500,000 CHF each 21
LHC: Facts and Figures 22
LHC: Facts and Figures •The ultimate atom smasher: •smashing 1011 protons into 1011 protons, •25 million times a second, •at 4 points around the circle. •The energy circulating around the LHC is equivalent to a aircraft carrier travelling at 10 knots 22
Finding the Higgs • One in every 10 10 collisions in the LHC will form a Higgs boson. • Once formed, the Higgs boson decays into other particles in 10−22 seconds. • We have a pretty good idea of what the Higgs bosons will decay into… ➡ pairs of Z-bosons: H→ZZ ➡ pairs of W-bosons: H→WW ➡ pairs of photons: H→γγ ➡ pairs of b-quarks: H→bb̅ ➡ pairs of τ-leptons: H→τ+τ− • A waiting game. We sift through all of the data from all the collisions and look for pairs of these particles. 23
Under the Genevois Soil 24
The ATLAS Experiment 25
The ATLAS Experiment 25
The ATLAS Experiment 25
ATLAS In Real Life • https://www.youtube.com/watch?v=QA3bUz9nodU 26
ATLAS In Real Life ATLAS is essentially the largest and most sophisticated digital camera ever built 45 meters long 25 meters high 7,000 tonnes • https://www.youtube.com/watch?v=QA3bUz9nodU 26
ATLAS Collaboration • 3,000 physicists at 175 institutions in 37 countries • 25 from the University of Edinburgh 27
ATLAS is not alone in this endeavour. Our friendly rivals CMS (Compact Muon Solenoid) built this: 28
ATLAS is not alone in this endeavour. Our friendly rivals CMS (Compact Muon Solenoid) built this: 28
Higgs Boson Decay to Two Photons 29
Higgs Boson Decay to Two Photons 29
H→ γγ Decay The Higgs boson can decay into two “photons”: H→ γγ Photons are particles of lights Right: two very high energy photons detected in ATLAS 30
Advanced Higgs Boson Physics 31
Advanced Higgs Boson Physics • The Higgs boson also can decay into Z-bosons: H→ZZ • Z-bosons themselves also decay very quickly. • Search for Z-bosons decay products: e.g. H→ZZ→e+e−e+e− 4 electrons 31
Advanced Higgs Boson Physics • The Higgs boson also can decay into Z-bosons: H→ZZ • Z-bosons themselves also decay very quickly. • Search for Z-bosons decay products: e.g. H→ZZ→e+e−e+e− 4 electrons 31
Advanced Higgs Boson Physics • The Higgs boson also can decay into Z-bosons: H→ZZ • Z-bosons themselves also decay very quickly. • Search for Z-bosons decay products: e.g. H→ZZ→e+e−e+e− 4 electrons • Right: Picture of four electrons in ATLAS from a collision. • The other 99,999,999 in 10,000,000,000 collisions (where no Higgs boson is produced) can produce a similar picture. • The challenge is to work out if each individual picture is from a Higgs boson, or from something else! 31
+ − + H→ZZ→µ µ µ µ − 32
ATLAS Higgs Search Result • Mass of photon pairs from LHC collisions, detected by ATLAS. • Small excess of events at mass mγγ ~ 125 GeV/c2 • We believe this is due to Higgs bosons with a mass of mH ~ 125 GeV 33
34
H→ZZ results Compatible with a peak at m4ℓ ~ 125 GeV/c2 in addition to background processes. 35
Higgsteria! 36
4 th of July 2012 at CERN 37
4 th of July 2012 at CERN 37
38
Me on the telly! 39
Some letters… 40
Some emails... Dear Sirs, We are a craft beer micro company (Ca l'Arenys- GUINEU BEER), and we would like to make a Brewing Special Edition (10hl) as an Homage to Mr. Higgs First of all we would like to know if there is any concern about it. The idea is absolutely NON lucrative -We would like to know, if possible, if Mr. Higgs likes beer and what styles does he prefer in order to adapt our receipt. Best Regards Xavier Serra info@calarenys.com Ca l'Arenys brewing Manager Valls de Torruella ( Barcelona ) Spain 41
Some emails... Dear Sirs,
Some emails... Dear Sirs,
September 2012: Published! Observation of a New Particle in the Search for the Standard Model Higgs Boson with the ATLAS Detector at the LHC Phys. Lett. B 716 (2012) 1-29 15 pages plus 14 page author list! “Clear evidence for the production of a neutral boson with a measured mass of 126.0 ± 0.4(stat) ± 0.4(sys) GeV is presented.” Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC Phys. Lett. B 716 (2012) 30–61 15 pages plus 16 page author list! “An excess of events is observed […] signalling the production of a new particle. [… with] a mass of 125.3 ± 0.4 (stat.) ± 0.5 (syst.) GeV.” 42
Peter Higgs visits ATLAS 43
Outlook: the LHC • This year and next year the LHC is being upgraded: • All connections (welds) between the magnets are being upgraded • ATLAS and CMS experiments also being upgraded: new detecting equipment added. • The LHC will start again early 2015 at twice the energy: 13 or 14 TeV. • We’ll run until 2019. • If funding is forthcoming future plan is to further upgrade the LHC and the detectors and run into the late 2020’s! • For the 2020s, plans are currently being developed to keep 44 running with higher intensity beams.
Outlook: the Higgs boson • ATLAS and CMS physicists still analysing the data taken in the last few months of 2012. • So far, all indications say new particle with mass is exactly as expected: it’s “a Higgs boson”. • The new LHC run will allow us to make further, more precise, measurements of our Higgs boson. • Only then we can find if our boson behaves precisely as the Standard Model of particle physics predicts… • or hopefully we’ll discover our Higgs boson is subtly different. 45
Outlook: the Higgs boson • ATLAS and CMS physicists still analysing the data taken in the last few months of 2012. • So far, all indications say new particle with mass is exactly as expected: it’s “a Higgs boson”. • The new LHC run will allow us to make further, more precise, measurements of our Higgs boson. • Only then we can find if our boson behaves precisely as the Standard Model of particle physics predicts… • or hopefully we’ll discover our Higgs boson is subtly different. 45
Outlook: the Higgs boson • ATLAS and CMS physicists still analysing the data taken in the last few months of 2012. • So far, all indications say new particle with mass is exactly as expected: it’s “a Higgs boson”. • The new LHC run will allow us to make further, more precise, measurements of our Higgs boson. • Only then we can find if our boson behaves precisely as the Standard Model of particle physics predicts… • or hopefully we’ll discover our Higgs boson is subtly different. • Of course, other new particles could yet be discovered by the LHC. 45
Thanks to: the ATLAS Edinburgh Team 46
47
You can also read