the invisible world the elementary particles. study nature’s phenomena… look for the hidden laws...
TRANSCRIPT
• Length (meters) 10-15 m = size of atom’s nucleus 1 m = you 4.10+16 m = distance that separate us from the star Alpha Centauri (4 light-years)
• Time (seconds) 10-23 s = lifetime of particle Z0 1 s = you 10+17 s = sun’s lifetime
• Energies (Joules) 10-19 J = energy of a photon emitted by a lamp 10-7 J = landing of a mosquito 10+9 J = your meals during the day 10+16 J = atomic bomb of 1 Megaton 10+26 J = light energy from the sun…every second!
Scale factors
The electronic microscope
First electronic microscope : E. Ruska and M. Knoll , 1932 (Nobel prize 1986)
Optical microscope Electronic microscopeLight beam Electrons beamOptical lenses Electromagnetic lensesresolution 0.5 micrometer resolution 0.0002 micrometer
= h / p = longueur d’onde
h = constante de Planck
p = impulsion de la particule = mv
0.1 micron
Chloroplast within a plant cell
Detectors of the invisible
10-7 meter = 0.1 micron
The base of the hair and cells that make the eye of the fly
Lets enter the invisible world
A few examples of scalesThe small…
You need the same number of cells to make a human being as stars to make a galaxy (100 billions)
In 1990. the scanning tunneling microscope allowed researchers working at IBM to write the first letters in history written using nanotechnologies by placing 35 xenon atoms on a nickel surface.
First scanning tunneling microscope: G. Binnig et H. Rohrer in 1981 (IBM, Zürich), Nobel prize 1986
Scanning tunneling microscope (STM)
Voir aussi: http://www.cndp.fr/themadoc/micro3/rep_mcp.htm
Detectors of the invisible
10-10 meter = 1 Angström
A carbon atom. It is one of the element that makes a molecule found in DNA
Gold atoms deposited on a layer of carbon
Lets enter the invisible world
You need as many atoms to make an orange as oranges to fill the Earth
A few examples of scalesThe very small…
You need as many atom’s nucleus to fill an atom as oranges to cover France entirely…15 times!
A few examples of scalesThe very very small…
10-15 meter = 1 fermi
A proton in the nucleus (drawing)
A proton contains 3 quarks
Lets enter the invisible world
Unification of the interactions
1 GeV = 1.6 1010 Joules
102 105 1010 1015 GeV
Weak interaction + electromagnetic interaction = electroweak interaction
(1967-1973) Glashow, Salam, Weinberg
Need Higgs
Unification of the 3 interactions: electromagnetic, weak and strong
…and the anti-matter
1928 : P. Dirac predicts the existence of anti-matter
Collision between a electron and an anti-electron 1993: the LEP at CERN
Anti-electron trace in a C. Anderson bubble chamber
1932: C. Anderson discovers the anti-electron
…anti-matter (2)
A B
A B CPT(A) CPT(B)
C(A) C(B)
Three fundamental transformations:
P: parity inversion
C: matter anti-matter
T: time reversal
CP(A) CP(B)
http://ppd.fnal.gov/experiments/e871/public/phys_slides.html
…anti-matter (4)
≠
?
Right Left
Right
Left
Right
Left
• Symmetry violated: P parity
• Are there any other symmetries violated? Symmetry C matter ↔ anti-matter ?
…anti-matter (5)
Today in our universe
This ratio was though to be in the past
10105
photons
matière
photons
eantimatièrmatière
n
n
n
nnR
91036 R
• Diffuse cosmic background
• First nucleosynthesis models
• Number of stars
At the beginning, for 1 billion anti-matter particles,
there must have been 1 billion and 3 matter particles
Cosmic microwave background has been measured
One condition:
CP violation
…anti-matter (6)
The search for cosmic anti-matter
To observe anti-matter in space, we « only » need sending a magnet
matter Anti-matter
Cosmic ray
The experiment AMS (Alpha Magnetic Spectrometer) was conceived to observe anti-matter in space
we can count cosmic rays and classify them by types
…Anti-matter (7)
AMS 02
Space constraints
• Mass < 7 t
• 3 m x 3 m
• Power consumption < 2 kW
• Resistance :
• Temperature -50° / +50°
• Vacuum
• Vibrations
A simple magnet is not enough, we also need a particle physics detector
ATLAS for the LHC
• More than 7000 t
• 44 m x 20 m
• Power consumption > MW
• Immobilised 100m under ground
…anti-matter (8)
The detectors need to be very precise. We need to be able to reject:
1 proton in 104 positons1 Helium in 103 positons1 électron in 102 positons1 proton in 106 photons
Particle identification in AMS
Experiments that changed everything
E. Rutherford, H. Geiger et E. Marsdensent Helium particles (alpha particles) on gold leaf/sheet.
…
Surprise: the gold leaf/sheet looks like butter containing very small particles. Rutherford will interpret these as Gold atom’s nuclei
The mystery of beta disintegration
W. Pauli suggests a new particle: the neutrino
e
e
Experiments that changed everything
The first neutrino detector.
Built in 1956 by C. Cowan et F. Reines,near Savannah River’s nuclear reactor, USA
water+cadmium
1 neutrino out 1020 interacts with the detector !Reactor: 1020 neutrinos/sDetector at 12m3 neutrinos detected every hour
Experiments that changed everything
SLAC: discovery of quarksElectrons-protons collisions
SLAC and Brookhaven: discovery of quark « charme »electrons-positrons collisions
Fermilab: discovery of quark « bottom »protons-protons collisions
CERN: discovery of bosons W and Zprotons-antiprotons collisions
CERN: only three family of particleselectrons-positrons collisions
Fermilab: discovery of quark « top »proton-antiproton collisions
1968
1974
1977
1983
1993
1995
Experiments that changed everything
Giant detectors for tiny particles…
ALEPH detector studied high energy collisions
SuperKamiokande track the sun’s neutrinos
Today’s experiments
The theory that changed everything…quantum mechanics
E. Fermidescribed weak
interaction
W. Paulipredicted the
existence of the neutrino
P. Diracpredicted the existence
of anti-matter
L. De Brogliepredicted wave-particle
duality
Some of the players
Particle and wave wave function:
E = H
Orbitale 2s Orbitale 2p Orbitale 3d z
Distribution of the probability of finding an electron in an atom
Quantum mechanicsa new way to see the invisible
http://hypo.ge.ch/physic/simulations/orbitales/orbitales.html
« Old » way to look at electrons in an atom