The information is divided into several areas covering the major themes. A basic introduction can be found at the Reception, a more detailed introduction to the physics is in the Theory area, while the Accelerators and Detectors areas introduce the tools of the trade. Each area has a number of sub-headings, and the information is structured in such a way that the further you delve into each area, the deeper you dig into the subject.
The core of the CD-ROM is in the Projects area. Here you will find real physics analysis projects using real data for your students to do. They will need to be familiar with the information contained in the first pages of each of the preceeding chapters before embarking on these projects. A 'Briefing Room' at the entrance to the Projects area will allow your students to test their knowledge before starting the projects.
Care has been taken to make the CD-ROM easily navigable. It is based on the metaphor of a visit to the CERN site. The menu bar on the left will take you to wherever you want to go. A pop-up index can take you to any term you wish to return to, and clicking on the top left window will take you back to the CERN sitemap, which can also be used as an entry point to any area you wish to visit.
The authors would be very glad to see the results of your students' analyses. This will help us to improve this CD-ROM for future versions. If you are willing to share your results with us, please send them to us using the contact details below.
The Z particle is neutral. This means that it can decay into pairs of oppositely charged particles like an electron-positron pair, or a muon-antimuon pair, or a tau-antitau pair, or a quark and an antiquark. It can also decay into pairs of neutral particles, neutrinos and antineutrinos. Neutrinos don't leave any traces in the detector, meaning that the Z branching ratio into neutrinos cannot be measured directly. It is, however, these "invisible" decays of the Z that allow us to work out what the Universe is made of. We'll come back to them later.
To measure the Z branching ratios into visible particles, students will look at reconstructed Z particle decays. Using what they have learned from the introduction about what different decays look like, they will identify the decays and add up the number of times the Z decays into an electron and a positron, a muon and an antimuon, a tau and an antitau, or a quark and an antiquark.
The more events your students study, the more precise their result will be. Consequently the best way to approach the task is to split the class up into teams, each with responsibility for analyzing one file of 100 events. Each group should prepare a table, like the one shown below, in which they can record their observations. An event can only be one of the four possibilities. When they have finished, they can calculate the Z branching ratios into each particle type by dividing the number of each kind of event by the total number of events they looked at.
#Event | e+e- | mu+mu- | tau+tau- | quark-antiquark |
1 | X | - | - | - |
2 | - | - | - | X |
3 | - | - | - | X |
4 | - | - | X | - |
Sum | ||||
4 evts | 1 | 0 | 1 | 2 |
When each analysis team has finished you can ask them to present their branching ratios. If you plot the results from each group on the board you will find that they are not all the same, but they scatter around a central value. The next step of the analysis will be to combine all the results in a statistically meaningful way to arrive at your class' final answer, which you can then compare with CERN's published results.
After the project, there is a discussion of the significance of the branching ratio measurement, and its implications for the composition of matter in the Universe.
Click here to open the "Z branching ratio" project
As you may notice, identifying the events is not always easy. In fact, nature is such that it is not always possible to say what an event is with 100% certainty. However, to help you we have put together lists with the most probable answer for each decay. The files below correspond to each file of events:
The reason for this is that quarks and antiquarks can radiate gluons, the carriers of the strong force, which go on to generate jets of their own. The probability that a quark or antiquark will radiate a gluon is directly related to the strength of the strong interaction. This means that by counting up the numbers of two, three, and four or more jet events, we can measure the strength of the strong interaction. That is the goal of this project, which is followed by a discussion of the relative strengths of all the interactions of nature.
The events are the same as for the previous project, but the tables that your students should keep are slightly different:
#Event | 2-jets | 3-jets | >3-jets | |
1 | X | - | - | |
2 | - | X | - | |
3 | X | - | - | |
4 | - | - | X | |
Sum | ||||
4 evts | 2 | 1 | 1 |
Since the data sets are the same for projects 1 and 2, if the students have enough time there is nothing to stop them from doing both projects at once.
Click here to open the "Strong Coupling Constant" Project
Since Z decays into electron-positron pairs, muon-antimuon pairs, and tau-antitau pairs are relatively rare, one file contains just such events.
Click here to open the "Rare Events with W and Z Particles
The following general tips should help you get the most out of this CD-ROM:
James Gillies CERN 1211 Geneva 23 Switzerland E-mail: James.Gillies@cern.ch
Telephone: + 41 22 767 63 33 |
Richard Jacobsson CERN 1211 Geneva 23 Switzerland E-mail: Richard.Jacobsson@cern.ch
Telephone: + 41 22 767 36 19 |