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Title: What


1
Whats the Matter With Antimatter?Or, The
Leftover Universe
  • Dr. Natalie A. Roe
  • Lawrence Berkeley National Laboratory

2
Outline
  • What is Antimatter? (What is Matter? )
  • What is the Matter with Antimatter
  • New Result on CP Violation from the Asymmetric B
    Factory
  • Why Does it Matter?

3
What is Matter?
  • What are the fundamental constituents?
  • Greeks Earth, Air, Fire, Water
  • 1800s Periodic table of the elements
  • 1897 Thomson discovers the electron
  • 1919 Rutherford discovers the proton
  • 1932 Chadwick discovers the neutron
  • 1967 Kendall, Friedman and Taylor discover
    quarks in electron-nucleon scattering experiments
    at SLAC.
  • Quarks
  • are fractionally charged
  • always occur in pairs or triplets, never singly
  • come in 6 different kinds, arranged in 3
    generations

4
Why Three Generations?
  • Only the first generation of particles is needed
    to make our world
  • proton (uud) and neutron (udd)
  • protons and neutrons form nuclei, electrons to
    form neutral atoms
  • 3 fundamental particles to make all of the
    Universe!

Charge
2/3 -1/3 0 -1
  • Nature has 2 additional generations of heavier,
    unstable particles
  • Why?
  • What determines the quark and lepton masses?
  • Central questions for particle physicists

Increasing Mass --gt
5
The Prediction of Antimatter
  • Nature is full of symmetries mathematics is the
    language we use to describe symmetry
  • Diracs equation for motion of a relativistic
    electron (1928) had two solutions
  • one was the electron
  • the other was an electron with
    negative energy
  • Dirac originally attributed this
    solution to the proton (only known
    positively charged particle in
    1928!)

6
Matter and Energy
  • Einstein first realized the equivalence of matter
    and energy
  • When matter and antimatter meet, they annihilate
    into energy
  • Energy can also materialize as particle-antipartic
    le pairs

7
The Discovery of Antimatter
  • The positron was discovered in 1932 in cosmic
    rays by Carl Anderson at Caltech
  • The photograph shows how positrons were first
    identified in cosmic rays using a cloud chamber,
    magnetic field and lead plate

8
More About Antimatter
  • All charged leptons and quarks have
    anti-matter
    partners
  • n may be its own anti-particle
  • Anti-proton was discovered
    in 1955 at Berkeley
  • billions are now produced
    every year
    at accelerator labs
  • Quark-antiquark combinations
    called mesons also exist
  • p ud K0 ds
  • B0 bd B0 bd

9
Imaging With Antimatter
  • PET scans use positrons created in radioactive
    beta decay, by detecting the photons created in
    the subsequent e e- annihilation

10
How to create and store anti-particles
1. create p p pairs separate out the p
2. store p with magnetic fields accelerate with
RF cavities
11
Colliding protons and anti-protons
  • At Fermilab, located near Chicago, protons and
    antiprotons collide with the highest energy
    available in the world
  • The discovery of the top quark was made in 1995
    at the Tevatron Collider

12
Colliding electrons and positrons
Stanford Linear Accelerator Center, Stanford,
California
  • At Stanford, electron-positron collisions have
    been used to discover the charm quark, the tau
    lepton - and to study the matter-antimatter
    asymmetry.

13
What is the Matter with Antimatter?
  • In the Big Bang particle-antiparticle pairs
    were created from pure energy in a spontaneous
    explosion
  • Today we cannot detect significant amounts of
    antimatter in the universe - why not?
  • Matter and antimatter then annihilated into
    photons but a small amount of matter survived -
    but how?
  • In 1967, Sakharov stated
    three conditions necessary
    to
    create an excess of
    matter in the early

    Universe - one of which
    is CP Violation in
    particle
    interactions.

14
What is CP Violation?
  • C Charge conjugation particle
    ?antiparticle P Parity (mirror
    reflection) x ? -x
  • C and P together change matter to antimatter. If
    the world were CP symmetric, an antimatter world
    would be indistinguishable from our world. Any
    difference between matter and antimatter is
    evidence for CP Violation.Until 1964, most
    physicists assumed that CP symmetry was obeyed in
    all particle interactions.

CP Mirror
15
CP Violation Was Discovered In 1964
1980 NOBEL PRIZE
V. Fitch
J.Cronin
Cronin and Fitch discovered the violation of CP
in the decay of the long-lived, CP-odd neutral K
meson into a CP-even final state Br(KL -gt
pp- ) 0.2 There is a difference between
matter and antimatter! We are hopeful that at
some epoch, perhaps distant, this cryptic message
from nature will be deciphered. J. Cronin
16
The Motivation for Asymmetric B Factories
  • CP violation in K0 ( sd) meson decays has been
    exhaustively studied, but the effect is small and
    theoretical uncertainties are large.
  • In B0 ( bd) meson decays, the Standard Model
    predictions for CP violation are theoretically
    clean.
  • Large asymmetries between B and anti-B meson
    decay rates into special CP eigenstates are
    expected (10- 50), but the decay rates are small
    gt need a B meson factory
  • To observe the CP asymmetry between B and anti-B
    mesons, a special type of ee- collider is
    required with unequal beam energies - the
    Asymmetric B Factory, proposed by Pier Oddone of
    Berkeley Lab in 1987

17
Measuring CP Violation with B0s
Not equal CP Violation!
CP violation occurs in the interference between
mixing and decay to a CP eigenstate,
eg B0 -gt p p -
18
PEP-II
Stanford Linear Accelerator Center, Stanford,
California
Approved as a Presidential Initiative in 1993
completed in 1999. Reached full
design luminosity in 2000. Japanese B Factory
has also been built with similar design.
19
The Asymmetric B Factory Concept
3 GeV e
9 GeV e-
20
The BaBar Detector
The BaBar Collaboration 500 physicists from
73 institutions and 9 countries
21
How the BaBar Detector Works
22
Silicon Vertex Tracker (SVT)
Uses five layers of silicon microstrip
detectors to measure B decay vertices to better
than 0.1 mm
23
Tracking Charged Particles in the SVT
24
Recipe for Measuring CP Violation in B Meson
Decays
  • Produce many B0 B0 pairs (several 10s of
    millions)
  • Reconstruct one B in a special decay called a CP
    eigenstate
  • Tag the other B0 to make the matter/antimatter
    distinction
  • Determine the time between the two B0 decays, Dt,
    using SVT
  • Compare Dt distributions for
    B0 and B0
    tagged events
    the difference measures

    CP violation, the difference

    between matter and
    antimatter

B tagged
B tagged
Dt (ps)
25
The PEP-II asymmetric ee? storage ring
E(e-) 9.0 GeV, E(e) 3.1 GeV
This result (56 fb-1)
v?? 0.56 c
Design Achieved
Run2b
Luminosity (cm-2 s-1) 3 x 1033 4.5 x
1033 Int. Lum / day (pb-1) 135
303 Int. Lum / month (fb-1) 3.3 6.3
2nd PRL (30 fb-1)
Run2a
1st PRL (20 fb-1)
Run1
26
First Observation of CP Violation in B Decays -
Announced July 6, 2001
NYT Tiny Discovery May Answer a Question About
the Big Bang
-6 -5 -4-3 -2-1 0 1 2 3 4 5 6 7
Dt in trillionths of a second
CP Asymmetry Measuurement sin2b0.590.14
27
Latest result Sin2???????????????
28
What does this result mean?
sin2b0.750.10
  • Maximum asymmetry gt sin2b 1
  • Zero asymmetry gt sin2b 0
  • Much larger CP asymmetry than in K0 decays
    (75 vs 0.2) and very small theoretical error
  • Error is 1/7 of the central value gt very
    unlikely to be a statistical fluctuation
  • The result is consistent with the prediction of
    the Standard Model, our best current particle
    theory
  • But Standard Model calculations of early
    Universe do not produce a large enough
    matter/antimatter asymmetry!

29
Why Does it Matter?
  • We believe there must be some new physics beyond
    the Standard Model - this is only one of several
    clues
  • As we collect more data, we will measure CP
    violation more precisely, and compare different
    types of asymmetries
  • These precision tests of the Standard Model may
    show us an inconsistency which will point the way
    to new physics
  • This approach is complementary to the searches
    for new particles at the energy frontier
    accelerators, such as the Fermilab Tevatron and
    the CERN Large Hadron Collider

30
Summary
  • Antimatter exists and can be created at
    accelerators but there is very little antimatter
    naturally occurring in our Universe
  • CP violation is required in any theory starting
    from the Big Bang to explain the dominance of
    matter over antimatter
  • CP symmetry between matter and antimatter is
    violated at the quark level
  • recent measurement of CP violation in B mesons by
    the BaBar experiment
  • We need more CP violation to produce our Universe
    - our theory is not complete!

31
Could Antiprotons Be Useful?
  • Antimatter engines on Starship Enterprise were
    powered by p p annihilation...
  • Creating, storing antiprotons requires a lot of
    energy, and trapping them is also very
    inefficient
  • All the antiprotons created in one year at
    Fermilab would only power a 100 watt bulb for 30
    minutes, even with 100 trapping and conversion
    efficiency!

Penning Trap
32
Creating Anti-hydrogen
Anti-protrons are created and stored, then passed
through cold xenon gas. An ee- pair is created
as the antiproton passes by the heavy xenon
nucleus. The antiproton and the positron will
occasionally form a stable bound state - an atom
of anti-hydrogen!
Detecting Anti-hydrogen
33
The Force Carriers
  • Quarks and leptons interact via four different
    types of forces, each with its own force
    carrier
  • electromagnetism - the photon, g
  • strong force - the gluon, g
  • weak force - the W and Z bosons
  • gravitational force - the graviton?
  • One more particle completes
    the minimal Standard
    Model-
    the Higgs particle
  • prime target at Fermilabs
    Tevatron Collider
  • CERNs Large Hadron Collider
    will continue search in
    2006

34
1957 Discovery of Parity Violation
ne
Co60
n -gt p e- n
B field
e-
Beta Decay of Co60
C.S. WU
The Universe knows its right hand from its left!
35
What really happens in beta decay?
proton W boson
neutron
d -gt u W-
proton electron anti-neutrino
W- -gt e- n
36
CP was still OK!!
Because P reverses the handedness of a particle,
a left-handed neutrino turns into a right-handed
neutrino in the P-mirror but right-handed
neutrinos do not exist in Nature!
n
n
P
Now if we reflect in the C-mirror and P-mirror
combined, a left-handed neutrino turns into a
right-handed anti-neutrino, which does exist.
n
n
C P
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