The Quantum Universe John Womersley Director of Particle Physics Rutherford Appleton Laboratory, UK

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Transcript The Quantum Universe John Womersley Director of Particle Physics Rutherford Appleton Laboratory, UK

The Quantum Universe
John Womersley
Director of Particle Physics
Rutherford Appleton Laboratory, UK
John Womersley
What is the universe made of?
•
A very old question, and one that has been approached in many ways
•
The only reliable way to answer this question is by observation and direct
enquiry of nature, through experiments
– The ‘scientific method’ is one of the greatest human inventions
John Womersley
The structure of matter
•
Centuries of experimentation and subsequent theoretical synthesis have
led to an understanding of
– Molecules, made of atoms – electrons orbiting nuclei
– Chemistry – the interactions of these electrons
– Nuclear physics – nuclei made of protons and neutrons
– Quarks – the components of protons and neutrons
•
Culminates in what we call the “Standard Model”
– A theory of matter and forces
– A quantum field theory
describing
point-like matter particles
quarks and leptons
which interact by
exchanging
force carrying particles
photons, W± and Z, gluons
Lightest particles stable
make up everyday matter
John Womersley
So we understand what matter is made of, then?
Yes – but there are two big problems.
First: a problem with what’s in the Standard Model
John Womersley
a revolução está vindo! *
John Womersley
* the revolution is coming
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The standard model makes precise and accurate predictions
It provides an understanding of what protons, neutrons, atoms, stars,
you and me are made of
But (like capitalism!) it contains the
seeds of its own destruction
•
Its spectacular success in describing phenomena
at energy scales below 1 TeV is based on
– At least one unobserved ingredient
• the Higgs Boson
– Whose mass is unstable in quantum mechanics
• requires additional new forces or particles to fix
– And in any case has an energy density 1060 times too great to exist in
the universe we live in
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The way forward is through experiments at particle accelerators
John Womersley
Why accelerators?
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Today’s universe is cold and empty: only the stable relics and leftovers of
the big bang remain. The unstable particles have decayed away with time,
and the symmetries that shaped the early universe have been broken as it
has cooled.
But every kind of particle that ever existed is still there, in the quantum
fluctuations of empty space. Empty space “still knows” about all the
equations, all the symmetries that governed the formation of the universe.
John Womersley
•
We use particle accelerators to pump sufficient energy into a point in
space to re-create the short-lived particles and uncover the forces and
symmetries that existed in the earliest universe.
•
Accelerators, which were invented to study the structure of matter, are
also tools to study the structure of space-time, the fabric of the universe
itself
•
With current accelerators we are exploring the forces that governed the
universe when it was about one trillionth of a second (one picosecond) old
John Womersley
Fermilab
Chicago
Inside the
Tevatron Tunnel
Tevatron
Booster
Batavia, Illinois
p source
Main Injector
& Recycler
John Womersley
• Fermilab’s Tevatron collider started operations in 1988
Run I – 1992-95
Run II – 2001-09 50 × more data, increased energy
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Detectors
CDF
•
D-Zero
Surround the collision points with arrays of instrumentation to intercept
the particles produced
– large (thousands of tons)
– complex (many subsystems, 106 – 107 channels of electronics)
– designed and built by collaborations of university and laboratory
physicists
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Tracker
Superconducting Magnet
protons
antiprotons
3 Layer
Muon
System
Electronics
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Muon
Electron
every
396 ns …
Jet
(experimental signature
of a quark or gluon)
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Missing transverse energy
(experimental signature
of a non-interacting particle)
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Proton-antiproton collisions
•
•
Proton beams can be accelerated to very high energies (good)
But the energy is shared among many constituents – quarks and gluons
(bad)
Transverse
momentum
•
To select high-energy collisions: look for outgoing particles produced with
high momentum perpendicular to the beamline (“transverse momentum”)
– Do this 2½ million times a second, as the collisions happen
– “triggering”
John Womersley
Computer programs reconstruct the
particle trajectories and energies in
each collision (each “event”)
John Womersley
Displaced vertex tagging
•
The ability to identify b-type quarks is very important
– signatures for the Higgs boson and many other interesting things
•
b quark forms a B-meson, travels ~ 1mm before decaying
B
to reconstruct this decay, need to measure
tracks with a precision at the 10m level
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Silicon sensor
Wire bonds
Silicon sensor
HDI (flex circuit
readout)
SVX2e readout chips
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Measuring ladder position
after insertion
Zeiss coordinate measuring machine
at Fermilab’s Silicon Detector Facility
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What do physicists actually do?
•
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•
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Design and build hardware
– Detectors, electronics
Write software
Operate the detector
Interpret data
Present, refine, discuss our
results among ourselves
Publish papers
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The work
of many
people…
Example: The DØ detector
was built and is operated by
an international collaboration
of ~ 670 physicists
from 80 universities and
laboratories in 19 nations
> 50% non-USA
~ 120 graduate students
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Second big problem:
what’s not in the Standard Model
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Meanwhile, back in the universe …
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What shapes the cosmos?
– Old answer: the mass it
contains, through gravity
But we now know
– There is much more mass than
we’d expect from the stars we
see, or from the amount of
helium formed in the early
universe
• Dark matter
– The velocity of distant galaxies
shows there is some kind of
energy driving the expansion of
the universe, as well as mass
slowing it down
• Dark Energy
We do not know what 96% of the
universe is made of!
Quarks
and
leptons
4%
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Don’t let the
bright lights fool
you
The stars are only
a few percent of
what’s out there
The galaxies and
the entire
universe itself
have been shaped
by
invisible dark
matter…
… and dark matter
is not any of the
standard model
particles we are
familiar with
John Womersley
Particle
Physics
Experiments
Accelerators
Underground
Astronomy
Experiments
Telescopes
Satellites
Quantum
Field
Theory
(Standard
Model)
Standard
Cosmology
Model
10–18 m
1026 m
A Quantum Universe
John Womersley
Particle
Physics
Experiments
Accelerators
Underground
Astronomy
Experiments
Telescopes
Satellites
Quantum
Field
Theory
(Standard
Model)
Standard
Cosmology
Model
Consistent understanding?
10–18 m
1026 m
A Quantum Universe
John Womersley
Particle
Physics
Experiments
Accelerators
Underground
WIMPs
Astronomy
Experiments
Telescopes
Satellites
Quantum
Field
Theory
(Standard
Model)
Standard
Cosmology
Model
Dark Matter
Consistent understanding?
?
Goals for particle physics
- can we detect cosmic dark matter on earth?
- is it consistent with cosmological observations?
John Womersley
•
Dark Matter  low rate, small energy
deposits
– Very sensitive detectors
– Well shielded
– Underground to avoid cosmic
rays
1100 m
The Boulby Underground facility is
opened, 2003
John Womersley
Boulby Underground facility
ZEPLIN II liquid xenon detector in
shield and associated gas system
Interactions in the xenon
UK Dark Matter program
– Designed and constructed a series
of experiments
– Currently commissioning the
ZEPLIN II detector over half a mile
underground
• Uses Liquid Xenon to measure
scintillation light and
ionisation from dark matter
John Womersley
Intriguingly, dark matter points to the same place
where the standard model starts to break down …
Standard
Model
Higgs Boson
etc.
Dark matter
particles
mass and
interactions
John Womersley
Particle
Physics
Experiments
Accelerators
Underground
Quantum
Field
Theory
(Standard
Model)
WIMPs
Astronomy
Experiments
Telescopes
Satellites
Standard
Cosmology
Model
Supersymmetry
Dark Matter
Consistent understanding?
?
Goals for particle physics
- can we discover supersymmetry at colliders? Something else?
- is it consistent with cosmic dark matter?
John Womersley
What is this “Supersymmetry?”
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A proposed enlargement of the standard model
– We know all the particles have corresponding antiparticles
– If supersymmetry is correct, they would also have new, but much
more massive relatives called superpartners
Theoretically this is very nice
– eliminates mathematical problems in standard model
– allows unification of forces at much higher energies
– provides a path to the incorporation of gravity and string theory
These nice properties come at a cost: lots of new particles!
– multiple Higgs bosons
– squarks and gluinos, sleptons, charginos and neutralinos
– their masses depend on unknown parameters
– None of these particles has yet been seen – but they are expected to
be within reach of current accelerators
Lightest supersymmetric particle has all the
right properties for cosmic dark matter
John Womersley
How would we make a discovery?
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Standard model predicts how
Highest missing ET event
many events expected as a
function of missing ET
Supersymmetry models modify
this prediction: more events expected
We found one very high missing-ET event in the first year of data
Will we find more?
John Womersley
Indirect searches for new particles
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Measure the rate of the rare decay
of Bs and Bd  
In the Standard Model,
cancellations lead to a very small
decay probability
– 3  10-9 and 10-10
New particles (e.g. SUSY)
contribute additional ways for this
to happen, increase probability
– up to 10-6
Mass of muon pairs
Carry out a “blind analysis”
•
Current best limits
– Observe no events
– Probability (Bs  ) < 2  10
– Probability (Bd  ) < 5  10-8
– Will keep getting better
John Womersley
Time to revisit the Higgs Boson
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Photons of light and W and Z particles interact with the same strength
– “Electroweak unification”
Yet while the universe (and this room) is filled with photons, the W and Z
are massive and mediate a weak force inside atomic nuclei
Where does their mass come from?
Massive W, Z
Massless fields
mix
Higgs field
Massless 
Higgs boson
The “Higgs Mechanism”
•
This Higgs field has never been seen. Is this picture correct?
– A question to be answered experimentally
– One clear prediction: there is a neutral particle which is a quantum
excitation of the Higgs field
• The “Higgs boson”
John Womersley
Particle
Physics
Experiments
Accelerators
Underground
Astronomy
Experiments
Telescopes
Satellites
Quantum
Field
Theory
(Standard
Model)
Standard
Cosmology
Model
Higgs Field
Dark Energy
Consistent understanding?
NO! > 1060
Goals for particle physics
- what can we learn about the Higgs field?
- is it as simple as we think?
John Womersley
Does there have to be a Higgs?
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No one has seen this particle – so why do we think it exists?
– The W and Z have mass
– Precision measurements of Top quark and W properties
– Ultimate test: “WW scattering”
q
W
X
W
q
•
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probability becomes > 1 as energy
increases – unless there is a Higgs
This is a real experiment – can’t have a
nonsense answer
The Higgs doesn’t have to be a single elementary particle.
But something has to play its role
John Womersley
John Womersley
John Womersley
Higgs searches
•
Current searches at the
Tevatron are 20-100 times less
sensitive than will be needed
to find a Higgs
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We will get a factor 20 more
data, but by itself that won’t
be enough
•
Experiments are improving
their techniques
– should be able to say
something interesting,
provided the mass of the
Higgs is low enough
John Womersley
The Top Quark
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The top quark offers an indirect window on to the Higgs
Because it is the most massive particle known, it interacts most strongly
with the Higgs
– Precise measurements of the top mass can tell us about the Higgs
mass
– Measurements of the way the top quark is produced and how it decays
may hint at new phenomena associated with the Higgs
• The top is in principle “just a very heavy quark” so we can
calculate its behavior in detail
• Look for any surprises, anomalies
John Womersley
How to catch a Top quark
Neutrino
Muon
W b
t
Wt
b
John Womersley
Top production
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If the top is “just” a very heavy quark, we can precisely calculate its
expected production rate (“cross section”) in proton-antiproton collisions
PLB 626, 35 (2005)
L=230 pb-1
1 secondary vertex tag
Expected
Top Signal
Looks very much as
expected
John Womersley
Top mass
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Because its mass is so large, the top quark should decay very rapidly
(yoctoseconds) into a W boson and a b quark; the W decays even more
rapidly into either two quarks or a lepton + neutrino
•
The top mass can be reconstructed from the energy of the b and of the W
decay products
It can be measured quite precisely – at the 2-3% level
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In the Standard Model, the top mass
W mass and Higgs are all related
– Hence we can check if it is all
consistent – yes, so far
– And get an indirect measurement
of the Higgs mass
• Points to a rather light Higgs
John Womersley
How does top decay?
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Does it really decay always to a W
plus a b-quark?
– Can test by using the silicon
detector to identify b quarks
– Distinguish b fromb by
charge of particles seen
All consistent with SM
i.e. 100% top  Wb
•
Does it decay to a W through the
normal weak interaction?
– Can test by measuring the
angular distribution of the W
decay
All consistent with standard
weak decays
John Womersley
Particle
Physics
Experiments
Accelerators
Underground
Astronomy
Experiments
Telescopes
Satellites
Quantum
Field
Theory
(Standard
Model)
Standard
Cosmology
Model
Supersymmetry
Extra Dimensions
Quantum Gravity
Inflation
Consistent understanding?
Superstrings!
Goals for particle physics
– can we see evidence of extra dimensions?
John Womersley
What? Extra dimensions?
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String theories predict that there are actually 10 or 11 dimensions of
space-time
The “extra” dimensions may be too small to be detectable at energies less
than ~ 1019 GeV
– To a tightrope walker, the tightrope is one-dimensional: he can only
move forward or backward
– But to an ant, the rope has an extra dimension: the ant can travel
around the rope as well
John Womersley
Detecting extra dimensions
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If there are particles than can travel around the extra dimension(s), we’d
interpret this motion as being additional mass
– If the dimension is small, the motion would be quantized
– would look like a series of new, more massive relatives of a known
particle
• “Kaluza-Klein modes”
•
But what if none of the known particles can enter the extra dimension
except for gravity?
– We (the things we are made of) may be trapped on a (3+1)-dimensional
“brane” – the surface of a 10 or 11 dimensional universe
– This could explain why gravity seems so weak
– Extra dimensions could be large – even infinite
– The energies required to “see” them could be much lower
• within reach of current accelerators?
John Womersley
We are searching
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Look for a “Kaluza-Klein”
excitation of the graviton
– Assumed to decay to two
electrons or photons
Putative signal
data
High-mass electron pair event
mass = 475 GeV, cos * = 0.01
•
Look for enhancement to the
production of pairs of high
energy photons or electrons
•
See no deviation from 3+1
dimensions
– We can set limits on the
size and properties of extra
dimensions
John Womersley
Where do we go from here?
John Womersley
The Large Hadron Collider
14 TeV proton-proton collider at CERN
Magnets being installed
Over half the
dipole magnets
completed
First beam in 2007
John Womersley
The ATLAS and CMS detectors
CMS mid-2005
PbWO4 crystals
Final Barrel assembly at CERN
September 2005
ATLAS mid 2005
John Womersley
The International Linear Collider
•
•
Discoveries at the Tevatron or LHC
will leave us more questions than
answers:
– Have we really discovered the
Higgs
• Right quantum numbers?
• Does it couple to mass?
– Have we really discovered
supersymmetry?
• Superpartners have same
properties as their partners?
– Have we really discovered dark
matter?
• Does it have the right
properties?
An electron-positron linear collider is
the way to answer these questions
John Womersley
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The ILC is a high priority for the US Department of Energy, provided it is
affordable and scientifically justified
Seen as a fully international project
Northern Illinois (near Fermilab) is a candidate site
– Just to show the scale:
US study version 47 km long
•
Fermilab
site
John Womersley
International Linear Collider
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500 GeV, upgradeable to 1 TeV
Accelerator technology chosen
Global design group established
Professor Barry Barish
Caltech
Timeline
12/05
Baseline configuration
(done)
12/06
Reference design report
with cost estimate
2008
Technical design report
2010
Construction decision?
John Womersley
Conclusions
•
We have theory – the standard model – which makes precise and accurate
predictions but which we know is incomplete
– theoretically – points to the Higgs boson (or something else)
– experimentally – dark matter and dark energy
•
By connecting experiments at particle accelerators and in underground
labs with astronomical observations we can understand far more about
the universe than from either approach alone
– What is the cosmic dark matter?
Is it leftovers of Supersymmetry?
– Is the universe filled with energy?
How does this relate to the Higgs field?
– What is the structure of space and time?
Are there extra dimensions?
John Womersley
The quantum universe is a wonderful place
Perhaps the most wonderful aspect is that it is
possible for us to understand it
John Womersley
Questions, comments…
John Womersley
Particle
Physics
Experiments
Accelerators
Underground
Astronomy
Experiments
Telescopes
Satellites
Quantum
Field
Theory
(Standard
Model)
Standard
Cosmology
Model
Small CP violation
in quark decays
Matter dominates
Consistent understanding?
Not really
Goals for particle physics
- search for new sources of CP violation using quark mixing
- search for CP violation in the neutrino sector
John Womersley