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## Kinematics and Cross Section for a Two-body Process

In this section we begin the description of kinematics selection and cross-section calculation. The example is for the case of a process, with final-state masses assumed to be vanishing. Later on we will expand to finite fixed masses, and to resonances.

Consider two incoming beam particles in their c.m. frame, each with energy . The total squared c.m. energy is then . The two partons that enter the hard interaction do not carry the total beam momentum, but only fractions and , respectively, i.e. they have four-momenta

 (67)

There is no reason to put the incoming partons on the mass shell, i.e. to have time-like incoming four-vectors, since partons inside a particle are always virtual and thus space-like. These space-like virtualities are introduced as part of the initial-state parton-shower description, see section , but do not affect the formalism of this section, wherefore massless incoming partons is a sensible ansatz. The one example where it would be appropriate to put a parton on the mass shell is for an incoming lepton beam, but even here the massless kinematics description is adequate as long as the c.m. energy is correctly calculated with masses.

The squared invariant mass of the two partons is defined as

 (68)

Instead of and , it is often customary to use and either or :
 (69) (70) (71)

In addition to and , two additional variables are needed to describe the kinematics of a scattering . One corresponds to the azimuthal angle of the scattering plane around the beam axis. This angle is always isotropically distributed for unpolarized incoming beam particles, and so need not be considered further. The other variable can be picked as , the polar angle of parton 3 in the c.m. frame of the hard scattering. The conventional choice is to use the variable

 (72)

with defined as above. In the following, we will make use of both and . It is also customary to define ,
 (73)

but is not an independent variable since
 (74)

If the two outgoing particles have masses and , respectively, then the four-momenta in the c.m. frame of the hard interaction are given by

 (75)

where
 (76)

Then and are modified to
 (77)

with
 (78)

The cross section for the process may be written as

 (79)

The choice of scale is ambiguous, and several alternatives are available in the program. For massless outgoing particles the default is the squared transverse momentum

 (80)

which is modified to
 (81)

when masses are introduced in the final state. The mass term is selected such that, for , the expression reduces to the squared transverse mass, . For cases with spacelike virtual incoming photons, of virtuality , a further generalization to
 (82)

is offered.

The expresses the differential cross section for a scattering, as a function of the kinematical quantities , and . It is in this function that the physics of a given process resides.

The performance of a machine is measured in terms of its luminosity , which is directly proportional to the number of particles in each bunch and to the bunch crossing frequency, and inversely proportional to the area of the bunches at the collision point. For a process with a as given by eq. (), the differential event rate is given by , and the number of events collected over a given period of time

 (83)

The program does not calculate the number of events, but only the integrated cross sections.

Next: Resonance Production Up: Process Generation Previous: Equivalent photon flux in   Contents
Stephen Mrenna 2005-07-11