Yet another talk to OSU Society of Physics Students about LHC & Higgs

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The Higgs is coming…
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OUTLINE
• Second
level
The Standard Model
• Third
level Physics
of Particle
Higgs & SUSY & friends
•
Fourth
level
The Large Hadron Collider
Higgs
Forecast
• Fifth
level
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What are the forces laws of physics?
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Second level
Third level
Fourth level
Fifth level
things are really small!
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proton=uud
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The Standard Model of Particle Physics
toModel
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The Click
Standard
particle physics
unites
Weak + EM + Strong Forces
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It• isClick
the most
successful
physics
model, ever!
• Second
level
Explains
all of
particle physics data for last ~50 yrs
½ particles:
•spin
Third
level quarks, leptons
spin 1 particles: photon, Z & W bosons
•mesons,
Fourth
level
bound
states of quark anti-quark pairs
baryons, bound states of 3 quarks (proton…)
• Fifth level
Lots of predictions that came true…
charm particles, Z and W boson, top quark…
32 Nobel Prizes since 1960 including 2008’s
BUT…….
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Problems with the Standard Model
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The SM needs many experimental inputs
12 quark and lepton masses
•12Click
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other to
numbers
(couplingtext
constants…..)
The
SM fundamental
particles have zero mass!
• Second
level
but we have mass!
• Third
level
The
origin
of mass is tied into the Higgs Field
Higgs field
•The
Fourth
levelgives particles their mass
Peter Higgs (1964) uses ideas
• Fifth level
from solid state physics & devises a
Prof. Peter Higgs,
U. of Edinburgh
5/29/2012
theoretical field to make
Energy can be stored
massless particles massive!
in a field, e.g. electric
Note: 2 other groups come with
Einstein: E=mc2
similar idea at same time!
mass  energy
Higgs particle could have been known
as the “Guralnik” or “Hagen” or”Kibble”
or “Brout” or “Englert”
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Problems with the Standard Model
to predict
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The Click
SM cannot
the mass of
the Higgs
The SM cannot tell us how many different Higgs
• Click exist.
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particles
The
minimum level
is one, but there can be more!
• Second
Some
scattering
processes
involving
a
Higgs
particle
• Third level
are infinite!
• Fourth level f
►
• Fifthhlevel
h
f
A higgs can turn into a
virtual fermion anti-fermion
pair. The probability for
this to happen in the SM
is infinite!!!!
►
Infinite cross sections violate unitarity!
Unitarity: a foundation of quantum mechanics
unitarity->sum of probabilities=1
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Even Worser SM Problems
Why are all elementary particles either quarks or leptons ?
Are there lepto-quarks ?
1MeV=106eV
Why do particles have such a wide range of masses?
1GeV=109eV
neutrino  very light but not massless (<< 1eV)
12eV
1TeV=10
top quark 175,000 MeV/c2 = 175 mp
Why is the electric charge of the proton identical to the electron?
• Second
electron is alevel
lepton but a proton is made up of 3 quarks
Do quarks and/or leptons have structure like atoms or protons ?
level
Why• isThird
the proton
stable?
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• Fourth level
• Fifth level
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The Standard Model Must be Replaced
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• Second
level
The
Standard
Model of particle physics has
basically
taken the problems that appeared
• Third level
in HEP in the 1960’s and moved them from one
• Fourth
area
to thelevel
next without ever solving the
real
problem(s)…
• Fifth
level
How do we get out of this mess?
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Supersymmetry-I
SUSY is a grand unified theory with symmetry between
fermions & bosons. Eliminates “infinities.”
Grand Unified=includes gravity
SUSY
compatible
stringtext
theory
& SM
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styles
For every SM particle there is a SUSY particle with a spin
•that
Second
differs level
by ½.
• Third
level
SUSY
predicts
lots of new particles:
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bosons
squarks
sleptons
Higgs
gluon
W, Z
photon
fermions
quarks
leptons
Higgsinos
gluinos
Winos+Zinos
photino
• Fourth level
• Fifth level
~
~
W   H   ~   charginos
~ ~
~
~  Z  h 0  H 0  ~ 0  neutralino s
SUSY may contain a new quantum number, R=(-1)3(B-L)+2S
with B=baryon #, L=lepton #, S=spin, R=1 for SM, -1 for SUSY particles
Because of R, SUSY particles must be produced in pairs.
Lightest SUSY particle stable and may be dark matter!
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Supersymmetry-II
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Besides its mathematical elegance the strongest evidence
for SUSY is the unification of coupling constants:
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Second level
Third level
Fourth level
Fifth level
reminder…
SUSY can also be tied to String Theory
May be able to unify gravity with strong + weak + EM
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• Second level
• Third level
• Fourth
level
SUSY
particles
have not yet been observed.
If SUSY were a perfect symmetry: mass of selectron = mass of electron.
• Fifth
Perhaps
SUSYlevel
particles are too massive to be produced in previous
experiments
Perhaps they don’t exist.
SUSY predicts at least 5 Higgs bosons!
Another annoying thing about SUSY:
About 100 free parameters in Minimal SUSY (MSSM)!!!
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How do we study quarks & leptons?
Small distance  high energy
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DeBroglie: wavelength = planck’s constant/momentum
Einstein: rest energy=m0c2
c =speed of light in vacuum=3x108m/s
Einstein: (momentum)c = (energy2 - rest energy2)½
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edit (momentum)c
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styles
So,• for
high to
energy:
energylevel
particle has small wavelength
• high
Second
What momentum do we need to “see” a nucleus ?
Size
of nucleus
≈ 10-15 m
• Third
level
p=h/λ=(4.14x10-24 GeV-s)/(10-15 m) = 4.14x10-9 GeV-s/m = 1.2 GeV/c
Could
do this with
an electron with » 1 GeV Energy ! (big battery)
• Fourth
level
Use particle accelerators to make high energy probes
• FifthCERN
level
Fermilab,
accelerate protons to > 1000X rest energy
Collide the probes into a target
probe could be another beam of protons or anti-protons
Use detectors to examine the results of the collisions
how many particles produced?
what types of particles were produced? (pions, kaons, protons, ……)
measure energy and/or momentum of particles
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How much energy do we need?
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Protons: 3 valence quarks+sea of gluons + qq pairs
Each quark can have momentum between 0 and Ebeam
p
p
Ebeam
Ebeam
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styles
• Second level
So, if you want to create a particle with mass ~ 1TeV the proton
beams
must have
energy >> 1TeV
• Third
level
• Higgs
Fourth level
Production
• Examples
Fifth level
Rather than build a new accelerator tunnel CERN is re-using a tunnel
from the 1980’s. The radius of the tunnel and the strength of the
bending magnets dictates the energy of the beam:
Ebeam = 7 TeV and Ecm=14 TeV
Upper limit: p=0.3BR, R~4km, B=7.5T gives p~9TeV
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Finding interesting events is like looking
for a needle in a Haystack
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Interesting cross section:
~10-15 barn
Typical cross section for pp collison
~10-3 barn
Need to search trillions of events!
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Second level
Raw event rate will be ~ 40MHz!
Third level
Interesting rate much much lower!
Fourth level
Event rate at LHC >100X Fermilab
Fifth level
# of events=(cross section)(Luminosity)
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The Large Hadron Collider
LHC is located at CERN
CERN is located near Geneva
Part of CERN is in France
The LHC collides protons
Center of Mass E=14 TeV ~7X Fermilab
Very high luminosity ~100X Fermilab
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Goal: discover Higgs+SUSY+???
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ATLAS
site
main lab
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The Large Hadron Collider
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ATLAS site
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~4.3km level
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main lab
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A Toroidal LHC ApparatuS
ATLAS is one of the 4 major experiments planned for the LHC
Goal is to find Higgs + physics beyond the standard model (SUSY??)
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The ATLAS detector stresses:
good charged particle tracking
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2 magnets
Second
level
good•calorimetry
(EM+Had)
electron ID
TRT+ECAL
• Third level
muon ID
ATLAS has limited (none?)
• Fourth level
p/K/p ID
• Fifth level
pixel+SCT+TRT
good momentum resolution
ATLAS superimposed on
the 5 story building 40 at CERN
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ATLAS Under Construction
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ATLAS Toroid Magnets
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•
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•
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style
After
15 years
of design
and title
construction
the LHC is ready to start!
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The Press takes notice
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Celebrities Come Out..
Jesse Dylan
(son of
Bob)
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Will I am
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Peter Higgs
Fifth level
Steven Hawkings
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YOUTUBE:
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http://www.youtube.com/TheATLASExperiment
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Hollywood comes to ATLAS/CERN
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Tom Hanks
Ayelet Zurer
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Angels and Demons follows Harvard
symbologist Robert Langdon (Hanks)
as he uncovers a plan to annihilate
the Vatican in an explosion of light,
using 0.25 grams of antimatter
stolen from CERN.
ClickRontoHoward
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Second level
Third level
Fourth level
Hanks admitted to scoring a D in
Fifth level
physics in school, but said that
the explanations of CERN antimatter
expert, Rolf Landua, who acted as
a scientific adviser on the film,
had made it seem much easier to
digest.
Tom
Hanks in the ATLAS control room
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September 9, 2008
OSU is there!
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Dear Professor Kass,
I just saw that you were in Geneva at the
start up of the LHC. I had the privilege of
visiting the LHC twice over the past five
years due to strong Vanderbilt physics
connections. I am so delighted that Ohio State
is equally involved.
Congratulations! Gordon
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Third level
Fourth level
Fifth level
Harris Kagan
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Waruna Fernando
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A Brief History of ATLAS Data Taking
September
Click9-10
to 2008
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First beams in the LHC
September 19 2008
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Major magnet-system failure
• Second
level 4 2010
March
30 2010-Nov
• First
Thirdcollisions
level at 7 TeV CM energy
LHC passes Fermilab as highest energy collider
•
Fourth
level
peak luminosity 3.6 x 10 cm s
March 13 2011-Dec. 2011
• Data
Fifthtaking
level at 7TeV again
LHC delivers record luminosity
2012:Taking data at 8 TeV, L=6x1033
2015: Full energy, 14 TeV
schedule goes to 2040!
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How Can ATLAS Discover the Higgs?
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to
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title
style
In
1
3years
of data
Standard Model
st
taking ATLAS is
expected to accumulate
20 fb-1 of data
#evts=Ls
makes predictions for
the Higgs production
cross section.
Many process contribute
depends on Higgs mass.
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L=luminosity=20x10 barns
• Second level
s= cross section~30x10 b@100GeV
#evts~6x10 Higgs produced
• Third level
• Fourth level
What the Higgs decays
• Fifth
into depends
on thelevel
value
If m ~120 GeV then
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-12
5
H
of it mass.
Best guess is mH~120GeV
the discovery modes
may be HZZ, H
HZ
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How Can ATLAS Discover the Higgs?
Use energy-momentum conservation to measure mass of Higgs
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Simulation of H
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Fourth level
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Simulation of HZZ
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How Can ATLAS Discover the Higgs?
What is so good about the decay modes HZZ, HZ and H
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If we measure the energy/momentum of the decay products then we can measure (reconstruct)
the mass of the Higgs.
For these decay modes it is possible to measure the energy and/or momentum of
all of its decay products:
H measure ’s in EM calorimeter

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m  ( E level
E )  ( p  p )  2 p p (1  cosq )
• Second
Measure energy (= momentun) of ’s and the angle between them (q)
• Third
+e- or Zm+m- measure e’s and m’s tracking+calorimeter(+muon)
HZZ
with Zelevel
• Fourth level
Other Higgs decay modes involve “jets” and or decays with neutrinos:
HW
W or t level
t : Always a neutrino in the decay products as a W or t decay includes n’s
• Fifth
and n’s do not interact in ATLAS (not enough material)
2
H
+
-
1
2
2
1
2
2
1
2
+ -
Hbb or cc or gg: We can not measure the quarks (b, c) or gluons (g) directly.
The quarks and gluons turn into many other particles collectively
called a “jet”. The jet may contain neutrinos and/or some particles from
the jet may not be measured (efficiency and acceptance)
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Can ATLAS Discover the Higgs->γγ?
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title style
2011 Data
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Second level
Third level
hint?
Fourth level
Fifth level
Not convincing evidence…… (less than 3 sigma)
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Can ATLAS Discover the Higgs->4l?
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Second level
Third level
Fourth level
Fifth level
2011 Data
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I found the Higgs in Columbus!
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Summary
High Energy Physics tries to answer the most fundamental
questions about the laws of physics.
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The• SM
is attoitsedit
breaking
point!
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text
styles
The LHC has enough energy & lum. to:
Second
level
a) •find
the Higgs
particle(s).
window
•small
Third
levelnear 125 GeV
b) find evidence for SUSY
•find
Fourth
levelfor dark matter
a candidate
c) search
evidence of extra dimensions (black holes…)
• Fifthfor
level
d) something evener better-er
This year is do or die for Higgs & SUSY!
NOTE: Figuring out WHICH SUSY model is correct & how
many Higgs particles will take many more (>5) years and
maybe a new accelerator.
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How Can ATLAS Discover the Higgs?
mode
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edit
pixel to
SCT
TRT Master
ECAL HCALtitle
muonstyle
reconstruct m
H
veto
veto
veto
yes
no
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yes
yes
yes/eID yes
no
• Second
level
yes
yes
yes
no
no
Hbb
+ yes
yes
yes
yes
• Thirdyes
level
vertex
eID?
if e’s
• Fourth level
HW W
Wen
yes
yes
yes/eID yes
no
• Fifth level
HZZ
Ze+emm
+
no
yes
no
yes
yes
yes
yes
if m’s
maybe
no
yes
no
no
no
no
-
Wmn
Wquark n
tt
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yes
yes
yes
yes
yes
yes
no
no
no
yes
yes +
vertex
yes
yes
eID?
yes
if e’s
yes
yes
if
if m’s
hadrons
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no
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H
extra slides
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What are the requirements
to to
find
the Master
Higgs or SUSY?
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edit
title style
Must have enough energy to produce the particles
A detailed analyisis of the SM says that there must
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to edit
text
be• new
physics
with Master
mass scale
lessstyles
than ~ 1TeV
• Second
level
What
we already
know says that the masses must be
greater than ~ 100 GeV
• Third level
Must collect enough data so we have large samples
•
Fourth
level
of the new particles or convince ourselves that they
Fifth
level
do• not
exist.
Use measurements + physics models to estimate the
necessary collision rates.
Accelerator must have a collision rate much higher than
previous accelerators. Only way to do this is to use beams
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of protons
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How Can ATLAS Discover the Higgs?
What is so good about the decay modes HZZ, HZ and H
Click to edit Master title style
If we measure the energy/momentum of the decay products then we can measure (reconstruct)
the mass of the Higgs.
For these decay modes it is possible to measure the energy and/or momentum of
all of its decay products:
• Click to edit Master text styles
H measure ’s in EM calorimeter

m  ( E level
E )  ( p  p )  2 p p (1  cosq )
• Second
HZZ with Ze e or Zm m measure e’s and m’s tracking+calorimeter(+muon)
• Third level
The HZZ is more complicated, we must reconstruct the 2 Z’s. Need Z decay modes that do
not involve neutrinos or jets. Use Z decays to electrons or muons:
• Fourth level 

m  ( p  p )  (E  E )  ( p  p )
m  ( p  p )  (E  E )  ( p  p )

m

(
p

p
)

(
E

E
)

(
p
p )
• Fifth level
2
H
1
2
2
+ -
2
Z1
2
l 1
2
H
2
2
l1
2
l 1
l1
2
Z2
2
Z2
l 1
2
Z1
1
+ -
2
l1
1
2
l 2
2
Z1
Z2
l 2
2
l 2
l 2
l 2
2
l 2
2
Z1
Z2
Other Higgs decay modes involve “jets” and or decays with neutrinos:
HW+W- or t+t-: Always a neutrino in the decay products as a W or t decay includes n’s
and n’s do not interact in ATLAS (not enough material)
Hbb or cc or gg: We can not measure the quarks (b, c) or gluons (g) directly.
The quarks and gluons turn into many other particles collectively
called a “jet”. The jet may contain neutrinos and/or some particles from
the jet may not be measured (efficiency and acceptance)
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How Can ATLAS Discover the Higgs?
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Master title style
Simulation of Hbb
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•
•
•
•
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Second level
a b-quark “jet”
Third level
Fourth level
Fifth level
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How Can ATLAS Discover the Higgs?
ATLAS detector simulations:
ClickFrom
to
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The statistical significance of Higgs observation
as function of Higgs mass and decay mode
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•
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MC simulation of H with
3 years of data collection
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Third level
Fourth level
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There can be > 1 Higgs….
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How well Can ATLAS Determine the Higgs
Properties?
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It is not enough to just show that the Higgs particle(s) exist!
Must measure their properties too.
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to edit Master textHiggs
styles
Branching Fraction
mH measurement
Second level
Third level
Fourth level
Fifth level
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How can ATLAS find Supersymmetry?
SUSYClick
particles
to decay into
toexpected
edit Master
title“ordinary
style
particles” + other SUSY particles
Some
SUSY
will not
• Click
toparticles
edit Master
textinteract
styles with matter
These particles are undetectable in ATLAS
• Second
So, unlike
the Higgslevel
we will NOT be able to measure the
energy and momentum of all the decay products of a SUSY particle
• Third level
We can detect the presence of
• Fourth
levelby noticing that
SUSY
particles
there
is “missing”
energy in an
• Fifth
level
me  e  ) max  m~ 0  m~ 0
2
1
event.
BUT must show that the missing energy
is NOT due to neutrinos and/or detector
resolution.
Can learn about mass of SUSY particles by
measuring
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SPS in its decay.
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Searching for SUSY with ATLAS data
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to
edit
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title
style
Although ATLAS has a small data sample the search for
SUSY is in full swing…
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•
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Two
Second
levelSUSY-like events…
Third level
Fourth level
Fifth level
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Searching for SUSY with ATLAS data
Examine the event sample for SUSY like events.
Compare the data with expected rates from known processes
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look at data as a function of number jets & number of leptons
Use• a Click
SUSY to
model
show where
“signal” would
edittoMaster
textthe
styles
be in the data plot (Monte Carlo method)
• Events
Second
with level
missing energy & jets
• Third level
• Fourth level
• Fifth level
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Events with
missing energy & jets & leptons
No hint of SUSY SPS
in the data!
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Searching for SUSY with ATLAS data
Even though we do not (yet) see evidence of SUSY we can
make model dependent statements about masses of SUSY
particles.
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everything
below red line
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the data
MANY other exclusions plots have been produced
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Detector Systems
A typical detector looks something like:
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BaBar, CDF, STAR, ATLAS, CMS……
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outside
detector
inside
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Let’s
look at the ATLAS DetectorSPS
as an example of a “real” system 43
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The Large Hadron Collider
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ATLAS site
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The Large Hadron Collider
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50-175m
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How Do We Get 7 TeV Protons?
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~7 TeV final beam energy
LINACPSBPSSPSLHC
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~10
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LHC: Just the Facts…….
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http://lhc-machine-outreach.web.cern.ch/lhc-machine-outreach/lhc-interesting-facts.htm
List of facts for the PPARC website. Compiled by Hazel Morris April 2004
Fact 3) The combined strands of the superconducting cable being produced for the LHC would go around the equator 6.8 times. If you added all the filaments of the strands together
they would stretch to the sun and back 5 times with enough left over for a few trips to the moon.
Fact 4) Part of the LHC will be the world's largest fridge. It could hold 150 000 fridge full of sausages at a temperature colder than deep outer space.
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Fact 5) The vacuum in the LHC is comparable to outer space, if it were a car tyre with a leak, there are so few gas molecules that it would take 10 000 years to go flat.
Fact 6) The ATLAS cavern could hold the nave of Notre Dam cathedral.
Fact 7) When the 27km long circular tunnel at CERN was excavated, between lake Geneva and the Jura mountain range, the two ends met up with just one centimetre of error.
Fact 8) LEP was sensitive to the departure of the TGV from Geneva train station, DC current feeds the tracks but the ground return is not good. The LEP electrical earthing network
is a better conductor and so some of the train current returned back through the LEP vacuum chamber.
Fact 10) The Large Hadron Collider at CERN could be the most ambitious scientific undertaking ever. The results of LHC experiments will probably change our fundamental
knowledge of the universe.
Fact 16) CERN is the world's largest laboratory dedicated to the pursuit of fundamental science.
Fact 17) Many of the parts for the ATLAS detector of the LHC were manufactured using the expertise of ex-arms scientists and factories, through collaboration with the International
Science and Technology Centre.
Fact 21) If the Higgs boson exists the LHC will be able to make this particle detectable. Confirming or contradicting the first evidence of the Higgs particle is an exciting prospect!
Fact 22) The Nobel prize in physics has twice been awarded to scientists whose experiments were conducted at CERN. The laboratory also boasts several additional Nobel
Laureates among its physicists.
Fact 24) On 1st October 2003 CERN and the California Institute of Technology set a new Internet Land Speed Record by transferring 1.1 terabytes of data in less than 30 minutes
across 7000km of network. The equivalent of transferring a full length DVD movie in 7 seconds.
Fact 25) In 1984 CERN translator, Francois Siohan, entered the French Guinness Book of Records for cycling up hill. Between 6:15am and 7:15pm on 1st July, he climbed 8848m,
the equivalent to Mount Everest, by cycling 13 times from Gex to La Faucille in the Jura mountain range.
Fact 26) In the 1960's CERN's main data network was the famous bicycle on line. Tapes of data were loaded into a basket on the bike and then rushed over to the computer centre.
Fact 29) The Grid is a service for sharing computer power and data storage capability over the Internet. Its ultimate aim is to turn the global network of computers into one vast
computational resource.
Fact 30) Verification of the theory that explains why the sun shines - the weak force - is one of CERN's biggest achievements.
Fact 31) The discovery of the neutral current was announced at CERN in 1973. The theory was finally confirmed in 1983 with the direct observation of W and Z particles.
Fact 34) Since 1962, 38 heads of state have visited CERN.
Fact 40) The CERN Fire and Rescue remit covers 40km of underground tunnels, radiation and chemical risks as well as the buildings above ground. CERN firemen train in abseiling
and rope rescue techniques in preparation for a tunnel emergency.
Fact 41) In 2003, 6.1% of traffic at Geneva International Airport was related to CERN, a total of 54 868 passengers.
Fact 42) X-ray and radiopharmaceutical techniques in medical imaging were developed by particle physicists, as was radiotherapy for cancer patients.
Fact 43) Particle accelerators are used to dry the paint on soft drinks cans.
For the replacements (23, 35, 36, 44 and 45) and 7 novel facts
There are firemen of 9 different nationalities, Bulgarian, British, Czech, Dutch, Finnish, French, German, Spanish and Italian tackling fires with the CERN fire brigade. When they are
called out they only speak in French over the radio.
The moon and snow/water load on the Jura mountains flexed the earth's crust a little bit which alters the circumference of the LEP ring, in this way the orbit of the moon was
detected by LEP.
Understanding all of the different forces of nature within one framework is one of the ultimate goals of physics. Decades of experiments at CERN are working towards this.
99.999999999999% of an atom's volume is empty space. If the proton were a pea, the electron would be in the back of the strands at Old Trafford.
When protons arrive in the LHC they are travelling at 0.999997828 times the speed of light. Each proton goes around the 27km ring over 11 000 times a second.
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How Can ATLAS Find Supersymmetry?
Several SUSY particles might be stable and not interact with matter
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Lightest SUSY particle might be responsible for dark matter…
Consider the following decay chain (one of many…)
assume
~g
~X
pp  g
m~ 0  97 GeV
2
~
~  bb
g
m~ 0  45 GeV
~
1
0
~
b  b 2
~0  
~ 0ee

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1
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We can
measure the
electrons (or muon) energy and momentum
Also look for the presence of two b-quark jets
Fourth
Key•is the
invariant level
mass of the lepton pair:
m
there is a sharp cutoff in m(e e ) that depends on the
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ee
+ -
) max  m~ 0  m~ 0
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p ~ 0  p ~ 0  pe   pe   p ~ 0  p ~ 0  pe   pe 
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me2 e   ( pe   pe  ) 2  ( p ~ 0  p ~ 0 ) 2
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Evaluate in the frame where 2 is at rest
me2 e   ( m~ 0  E ~ 0 ) 2  p 2~0  m 2~0  m 2~0  2m~ 0 E ~ 0
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0  m ~0 )
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 e  ) max  m ~0  m ~ 0  2 m

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The Large Hadron Collider
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Toroids, Calorimeters, Muon
Chambers
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How can ATLAS find Supersymmetry?
to with:
edit
LookClick
for events
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quark jets (q) from squarks & gluino decay
leptons
(l) from
Winos,
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slepton
decay
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missing transverse momentum
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simulated SUSY event in ATLAS
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