The Oxford Particle Physics Program · (thanks Prof. Daniela Bortoletto& PP colleagues) Higgs as a...
Transcript of The Oxford Particle Physics Program · (thanks Prof. Daniela Bortoletto& PP colleagues) Higgs as a...
1
Particle Physics Open Day
The Oxford Particle Physics
Program
Farrukh Azfar
Director of Graduate Studies for
Particle Physics(thanks Prof. Daniela Bortoletto& PP colleagues)
Higgs as a new tool for
discovery
Identify the new
physics of dark
matter
Oxford is addressing the science drivers of particle physics
2
The physics of
Neutrino mass
Understanding
cosmic
acceleration
Explore the
unknown: new
particles and
new interactions
3
The Standard Model
4
The Standard Model
5
1964 SM Theory
1984 LHC Design
1996 Start LHC construction
2009: first collisions
2012: Higgs Discovery
Why look beyond the Standard Model?
Experimental Evidence
Non-baryonic dark matter
(~23%)
Inferred from gravitational effects
Rotational speed of galaxies
Orbital velocities of galaxies in
clusters
Gravitational lensing
..
Dark Energy (~73%)
Accelerated Expansion of the
Universe
Neutrinos have mass and mix
Baryon asymmetry
.. 6
The Higgs boson The discovery of the Higgs Boson raises many questions
7
The Higgs boson The discovery of the Higgs Boson raises many questions
8
27km
Circumference
ATLAS
LHCb
The Large Hadron Collider A Discovery Machine
9
Operates above energy scale of SM:
13 TeV in 2015
Probes new physics
ATLAS
10
Barr, Bortoletto, CooperSarkar, Gwenlan, Hays,
Huffman, Issever, Nickerson, Shipsey,
Viehhauser, Weidberg
The Oxford ATLAS Group Our goals:
Shed light on new Higgs boson
Measure its properties
Improve our understanding of SM
Discover new physics beyond SM
Can we make & discover Dark Matter?
Are there heavier Higgs bosons?
Is nature supersymmetric?
Look for more Exotics signatures
Build key parts of next generation LHC
detector11
Supersymmetry
12
New symmetry of
space and time
(extends rotations
and boosts)
Links fermions and
bosons
Provides
superpartner to
each SM particle
Lightest partner
Dark Matter
Path to unification
& string theory Dark matter
Oxford Higgs Group 3 academics: Bortoletto, Hays, Shipsey
2 Postdocs: Schopf (Hbb) and Artoni
(HZZ, H )
8 students: Ambroz, Foti, Karava, Marchese,
Tosciri, Wolker, Zemaityte, Zgubic
Measured the Higgs coupling to b-quarks!
More data will allow us to:
Probe the Higgs coupling to the second
generation
Test for physics beyond the SM (using for
example Effective Theory Interpretation)
Search for new scalar particles
Use of advanced analysis techniques (neural
networks) and major contributions to common
physics objects
Strong collaborations with theorists13
Higgs in run 2 of the LHC Oxford recent highlight contributions
Hbb observed(expected) significance: 5.4(5.5)
14
Higgs in run 2 of the LHC
15
Until 6 years ago the
Yukawa coupling was
essentially a conjecture
no such term had ever
been seen in nature
16
Oxford SUSY group 2 Academics: Barr, Gwenlan
2 Postdocs: Backes (Electroweak
SUSY and triggers) and Nagai
(Strong SUSY)
5 DPhil Students: Liu, Nelson,
Gallardo, ONeill, Wuerzinger
Oxford students lead small teams &
have many world-first searches @LHC
Squarks, Gluinos, Scharm,
Higgsinos, Multijets,
Also contribute to ATLAS experiment
e.g. triggering on events with Dark
Matter
Possible to combine with theory studies
Supersymmetry example: Higgsinos Spin 1/2 partners of Higgs bosons
Excellent Dark Matter candidate
Should be at approx. same mass scale as Higgs
boson(s)
Search for leptons + invisible (weakly interacting)
17
As of this year we are just starting to get sensitivity
Lots of other
electroweak/Higgsy
SUSY processes just
getting ripe for analysis
No Higgsino
in red area
Still to be
explored
18
19
Instrumentation: Oxford Physics
Microstructure Detector Laboratory (OPMD)
A state-of-the art facility enhancing the development of new radiation sensors in Oxford and the UK
Development of novel detectors for particle physics, photon science, and astrophysics
Currently focusing on
Depleted Monolithic Pixel Detectors for ATLAS
Ultra Fast Silicon Detectors
CCD for LSST Sharma
ShipseyBortoletto
Arndt
Placket
Weatherill
Wood
Metodiev
What to expect as a Student in ATLAS Students work in small friendly teams
Have a big impact
Gain high visibility in ATLAS
Take responsibility for projects or
detectors
Long term stay at CERN
Shifts at the detector
21ATLAS CONTROL ROOM START OF RUN 2
LHCb
22
try
22
The LHCb experiment
23
Several trillion B hadrons have
so far been produced at LHCb.
to make precision measurements of CP violation
to search for New Physics in rare B decays
Critical for allowing this physics are particle identification and excellent vertex reconstruction.
The RICH detectors were designed and build in Oxford
VELO is a major Oxford activity
LHCb is a general purpose experiment for
examining the forward region of the proton-proton
collisions
24
CP violation!
CP-violation in beauty hadrons
25
In beauty system, the SM predicts sizable CP-violation.
And this is what we see!
Rate of decay and CP-conjugated process are clearly different !
Often, the SM predictions are precise.
The goal then is to make Correspondingly precise measurements.
Any Inconsistencies would indicate New Physics at work !
B0K+-
B0barK-+Signal + residual
background
The apex of the CKM triangle is the world average measurement of their
value (from pre-LHC measurements of the triangles sides and angles). Large error on one of the key ingredients of a precise , determination!
Oxford driven analysis has measured =74+5 -6 deg using BD0K this
already equals the precision of previous measurements. Aiming to reduce
error to 3 deg
Precise CKM measurements
LHCb offers fantastic opportunities for graduate students
All graduate students are working on high-profile
analyses of LHC data.
Graduate students participate fully in the running
of the experiment at CERN.
BELOW: 3rd yr D.Phil. in the LHCb control
room
The Oxford LHCb Oxford enjoys an great position in the international
collaboration.
3 Academics + 1 RSF (Harnew, Wilkinson, John, Malde)
8 D.Phil (Bijorn, Gruberg Cazon, Murphy, Pili. Pullen,
Rollings Fischer, Scantlebury-Smead )
The physics of neutrinos T2K
HyperK
PROTODUNE
DUNE
SNO+
MICROBoNE
28
29
30
T2K Neutrino Oscillation experiment
Measure disappearance of muon neutrinos to determine 23 and m2
Measure electron neutrino appearance
Determine if neutrinos and antineutrinos behave the same. In fact, there is a
chance to find CP violation in THIS experiment.
The group is also studying future neutrino experiments for CP violation discovery.
T2K results so far
T2K results so far
CP conserving values outside of 2 region
for both hierarchies
Upgrade SK to Hyper-K Start ~2022Total water mass of 0.99 Mt
Future = Liquid Argon in USA and Water Cherenkov in Japan
DUNE: planned long baseline
experiment. Start ~2022
4x10kT
PROTODUNE
770 t LAr mass
Exposed to H2 (DP)
and H4 (SP)
testbeams at CERN
(, K, , , )
Prototyping
production and
installation
Validating the design
and long-term
operational stability
Understanding,
calibration, dE/dx,
PID etc.
PROTODUNE SP
2018 data taking
Daniela Bortoletto, LISHEP 2018,
Salvador34
35
36
37
38
The Dark Universe
LZ
LSST
7-tonne two-phase Xenon TPC (5.6t fiducial) to search for xenon
nuclei, recoiling in response to collisions by dark matter particles.
Oxford provides crucial TPC sensors/readout and simulations tools.
Full exploitation requires significant simulation and analysis effort.
Oxford group now focussing on analysis/simulation tasks.
Dark Matter Search with LZ (LUX-ZEPLIN)
Oxford team:Hans Kraus
Amy Cottle
Theresa Fruth
Andrew Stevens
Eilish Gibson
Matthew Tan
LZ at the Sanford Underground Research Facility48
50
ft b
elo
w
Installation and
Commissioning in
2019 / early 2020.
Plenty of D.Phil.
opportunities with
analysis of early
data!
41
Exploring the nature of dark energy
Oxford LSST Camera Test Stand
Particle Astro Synergy
PP: Azfar/Tseng/ShipseyAstro:Davies/Dunkley/Fender/Ferriera/Jarvis/Lintott/ Miller
Dark Energy LSST Meeting Oxford July, 2016
42
Mu3e Features
Charged lepton flavor violating
Via neutrino mixing
Suppressed by (m2/ mW
2)2
Expected BR(+e+e-e+) < 10-50
Importance
Observable BR only from New
Physics
43
Welcome to Oxford Particle Physics