Pair Annihilation and Production
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Transcript Pair Annihilation and Production
Physical and Applicative
Overview
Joey Goodknight
Physics 129
October 21, 2010
Getting and Getting Rid of Them
Basic
Physical Mechanisms
Antimatter is Everywhere
Too Many Electrons!
How and Why the Positron?
1
•
•
•
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gram of anti-p+
2 X 1014 Joules
4 “Little Boy”s (Hiroshima)
2 “Fat Man”s (Nagasaki)
$25,000,000,000.00 (2009 Nasa Study)
~GDP of Yemen
Admittedly only 1/20 of US defense Spending
~Yearly Nuclear Weapons Spending (1998 )
Containment
Unrealistic past 1012 atoms
From Space: Classic “Doomsday Theory”
• Tungaska Event
Sorry, Back to e+/e-…
EM
Phenomenon
3 main methods:
• γ e+ + e• γ + γ e+ + e• Decay
Other
Possibilities?
E
Conservation
• E=hυ=~mec2
• λ~1 femtometer
• υ ~1023 Hz
• Well past gamma rays
P
Conservation
• Restricts Diagrams
Least
Expected
• Femtosecond 800nm focus
matter+anti-matter
• “Nothing”
Much
simpler than Prod.
P Conservation
Positronium
• Bound state
• L=0, annihilation!
Dirac
• 1929
Carl
Anderson
• 1932 under Millikan
Cloud Chamber Tracks
γ 208Tl
• 1936 Nobel
They’re All Around Us!
+q’
-q’
+q
Goop,
full of dipoles
E=?
E=?
-q
+q
Vacuum
Photons
• Create Virtual Pairs
• Shield Charge
• VacuumDielectric
QED Triumph
• spin
1997
Confirmation
Seein’ inside you
Weak Force Decay
11C, 40K, 13N, 18F etc.
γ
e+
e-
γ
•Photons Come out at 180 degrees to each other
•Complex Processing
•Density Map of Tracer
Always a Friend of Solid State Physicists
γ
γ
Positron Source
Na, usually
e+
•Scan Material
•Correlate emission with annihilation
•Generate map of open volume defects
•Gets trapped
•Live longer
•Defects are what make many
semiconductors cool
γ