Welcome to the Physics 880.02 home page!
URL: http://www.asc.ohio-state.edu/kilcup.1/courses/880.02/
Recent changes to this page:
Contents of this Page
If there is something you want to say, but for some reason
you don't want to reveal your identity, you can send a message
to Kagan and Kilcup anonymously using the comment box.
Return to Contents
- Course title:
- Physics 880.02: Particle Physics
- Texts:
- Quarks and Leptons by Halzen and Martin
- Topics to be covered:
Last term:
Symmetries
C, P and T
Isospin, SU(3), SU(6)
Hadrons
Constituent Quark Model
Quark Parton Model
Deep Inelastic Scattering
This term:
Fermi Theory, V-A, PCAC, CVC etc.
Detectors
GSW Standard Model
- Meeting Schedule:
- Tuesday and Thursday, 4.30pm - 6pm
- Smith 4079
- Assigments:
- Homework (every other week)
- Final Project
- Instructors:
- Prof. Gregory Kilcup
office: 4048 Smith Lab
email: kilcup@mps.ohio-state.edu
phone: 292-3224 (office) or 297-1152 (home)
- Prof. Harris Kagan
office: 2083 Smith Lab
email: kagan@mps.ohio-state.edu
phone: 292-2314 (office)
Return to Contents
Last Term's Final Project: Heavy flavor production
To calibrate your first programs you will need
the "official" answer for the e+e- problems.
- For (300 MeV, 300 MeV) at DAØNE: 2.57M events/day
- For (2.0 GeV, 2.0 GeV) at DAØNE: 57.8K events/day
- For (3.5 GeV, 8.0 GeV) at KEKB: 545K events/day
Note that to have a useful event we need to have both
muons in the detector.
Statement of the Problem
Compute the total and the visible cross-section for b-anti-b
production at two future colliders. Compare the rate at Fermilab
after its upgrade to that for the LHC. Take FNAL to
have 1.0 TeV proton and anti-proton beams at the promised
luminosity of 200. Take the LHC to deliver two 7.0 TeV
proton beams at L=10000. Assume the detector sees all
b-quarks aimed at it, and that it covers the region
20<theta<160 as before. Only count events where both
quarks are detected.
Starting Point
You will need the parton distributions, as given
in a subroutine of this Fortran code or
this C code.
The driver there just integrates the up and down
distributions, verifying that these distributions
are for a proton. The distributions are each given
in terms of a set of six Q**2 dependent parameters.
For efficiency you may prefer to extract these parameters
(and the functional form) for the particular distributions
you need. Or you may prefer to pick a set of bins in
x-space and use the sample program to dump out a table.
Sample valence up-quark and gluon distributions
from this particular set are plotted above.
Note the dependence on the scale (Q**2). To get
sensible results, you should pick Q**2 to be typical of
the process you are considering.
You will also find it handy to have the QCD cross-sections,
as available in this PS file.
Note that these depend on Q**2 as well, in the form of alpha(Q**2).
To be consistent you need to pick the same Q**2 here, and
use the value Lamba = 231 MeV (which was used in determining
the distributions).
Extensions
Aside from the straight comparison of the proton-proton
and proton-antiproton machines, each group should pick
some further direction to explore. These might include
- Map the cross-section as a function of beam energy
- Include the quark-mass dependence and compute the top-quark
production cross-section
- Investigate the dependence of the result on the choice
of factorization scale (Q**2).
Return to Contents
Lifetime of the Muon
A sample writeup can be found in
this PostScript file.
It was obtained using this TeX file,
which also needs this figure and
this style file, taken from a typical
international HEP conference.
Return to Contents
Your comments and
suggestions are appreciated.
[OSU Physics]
[Math and Physical Sciences]
[Ohio State University]
Physics 880.02. Created 6-Jan-97.
kilcup@mps.ohio-state.edu