LHC and the neutrino paradigm

author: Goran Senjanović, ICTP - The Abdus Salam International Centre for Theoretical Physics
published: April 10, 2012,   recorded: April 2012,   views: 210
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Slides

Slides
0:00 Neutrino Paradigm and LHC
1:57 Is Nature Left-Right Symmetric?
2:31 Symmetries and Particles
3:02 Why does gravity matter?
3:31 Theme 1 (1)
3:51 Theme 1 (2)
3:55 ... elementary particles
4:25 Matter = atoms
4:39 Nucleus = protons and neutrons
5:27 Protons and neutrons (1)
5:29 Protons and neutrons (2)
6:20 Protons and neutrons (3)
7:03 Forces: messengers (1)
7:27 Forces: messengers (2)
7:42 Forces: messengers (3)
8:27 Messengers of forces
9:10 Bombshell: anti-particles (1)
11:23 Bombshell: anti-particles (2)
11:25 Bombshell: anti-particles (3)
11:26 Ettore Majorana (1)
11:40 Ettore Majorana (2)
11:51 Not neutrino ?
11:53 Ettore Majorana (3)
12:53 Who saw him?
13:01 Fermi
13:46 Theme 2
14:33 Neutrinos: why so special?
15:00 Discovering neutrinos (1)
16:01 Discovering neutrinos (2)
16:23 Discovering neutrinos (3)
16:26 Discovering neutrinos (4)
16:38 article
17:27 How to see it?
17:43 Discovering neutrinos (4)
17:46 How to see it?
18:13 Cosmic Gall by John Updike (1)
18:47 Cosmic Gall by John Updike (2)
19:16 Savannah River Reactor
20:21 Beta decay : messenger W boson
20:39 W boson: the shiny (hairy) guy (1)
20:47 W boson: the shiny (hairy) guy (2)
21:22 1956: bombshell of Lee and Yang
22:46 Discovery of P violation
23:30 Beta decay: messenger W boson
23:46 Discovering W bosons
24:23 LEP experiment (1)
24:57 LEP experiment (2)
25:00 LEP experiment (3)
25:05 Modern Times
25:17 Majorana Program
26:12 Double-beta decay (1)
26:17 Double-beta decay (2)
26:26 Double-beta decay (1)
27:16 Majorana Program
27:34 Double-beta decay (2)
27:34 Double-beta decay (1)
27:55 Neutrino-less double beta decay (1)
27:56 Neutrino-less double beta decay (2)
28:24 GERDA experiment
29:00 future is here
29:09 Standard Model (1)
31:07 Standard Model (2)
31:10 Why parity: L - R broken? (1)
31:31 Why parity: L - R broken? (2)
31:40 L-R symmetry
32:56 L-R symmetry breaking (1)
33:17 L-R symmetry breaking (2)
33:36 L-R symmetry breaking (3)
33:45 Neutrino: Majorana mass
33:57 L-R symmetry
34:09 L-R symmetry breaking (1)
34:10 L-R symmetry breaking (2)
34:12 L-R symmetry breaking (3)
34:14 Neutrino: Majorana mass
36:30 WR = big dog
36:37 Atmospheric neutrinos
37:26 New source for ...
38:00 WR@ TeV = 1000 GeV (1)
38:22 WR@ TeV = 1000 GeV (2)
38:37 Rotation in a plane (1)
38:50 Rotation in a plane (2)
38:52 Rotation in a plane (1)
38:58 Rotation in a plane (2)
38:59 Rotation in a plane (3)
39:01 Production @ colliders (1)
39:07 Production @ colliders (2)
39:10 Production @ colliders (1)
39:20 Production @ colliders (2)
40:39 Production @ colliders (3)
41:04 Production @ colliders (4)
41:26 Large Hadron Collider (1)
41:45 Proton - proton scattering
42:35 Modern times: 3600 people
42:46 ... both CMS and ATLAS
43:54 Large Hadron Collider (2)
45:05 Hvala
48:08 Production @ colliders (2)
59:27 Neutrino: Majorana mass

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Description

Neutrinos, the most aloof of all elementary particles, have played a major role in shaping our understanding of physical forces in nature. Postulated originally in order to maintain energy conservation in nuclear decays, they needed more than twenty five years in order to be discovered. As suggested by the young Italian genius Ettore Majorana who disappeared mysteriously some more than seventy years ago, neutrinos may be unique particles in being their own antiparticles. This leads to a spectacular phenomenon: the creation of electrons 'out of nothing'. I show how the Large Hadron Collider can play a key role in this exciting process through the of restoration of Left-Right symmetry in elementary particle interactions.

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