This menu appears on the screen just after construction of
Feynman diagrams and together with the information about numbers of diagrams and
subprocesses generated.
The first function of this menu (Squaring) is the instruction
for CompHEP to create squared diagrams. CompHEP uses the squared diagram
technique for evaluation of squared matrix elements. See Section
for details.
The View diagrams function gives you a tool
to view a graphic representation of generated Feynman diagrams,
to remove some diagrams before the squaring and to create
the LATEX output for undeleted diagrams.
If a few subprocesses have been generated then the subprocess menu appears
after an activation of the View diagrams menu function. There is a
possibility to remove all diagrams in the highlighted subprocess by
pressing the F7 button. In its turn the F8 key restores all
diagrams of the highlighted subprocess deleted before.
When you choose a subprocess the diagram graphic viewer is
launched. See Section
for details
or use the
and
functional keys for online help.
Here we would like to note some peculiarities of constructed diagrams.
- Incoming particles are drawn on the left side of diagrams,
whereas the outgoing ones are shown on the right.
- Particles with spins
are represented
by the dotted, solid, and dashed line correspondingly.
- Charged particles are represented by arrow lines.
The arrow indicates the direction of particle (not anti-particle)
propagation.
- Incoming and outgoing particles are labeled by
relevant names in the end of the line. Virtual particles are labeled
by their names at the mid-line. If a particle is not self-conjugated,
the particle's name is used for the labeling (not the anti-particle's one).
- In the case of collision process a first colliding particle is
disposed in the top part of picture, whereas the second one is drawn
in the bottom part.
- CompHEP produces only one representative of a set of diagrams
which can be transformed one to another by replacing the identical
outgoing particles. For example, CompHEP creates only one diagram for
the
->
process, whereas all textbooks present two diagrams
in this case. In other words, momenta are not assigned to the outgoing
particles on the step of diagrams generation.
- CompHEP does not generate diagrams with Faddeev-Popov and
Goldstone ghosts1. Such diagrams are restored on the step of
squared diagram evaluation. Any ghost has a real particle as a prototype
(see Section
). As a rule, a diagram with ghosts has got
the parent diagram where ghosts are replaced by real particles.
During the
calculation of these parent diagrams the contributions of the corresponding
ghost diagrams are also calculated and added to the contribution of the parent
one (see Section
). There exist some exceptions
from this rule. For example, the
Standard Model contains the vertex with four Goldstone bosons associated
with the
-boson, however the
vertex is absent in the theory.
To provide a possibility to take into account the ghost diagrams with a
four-Goldstone vertex CompHEP generates false diagrams with
interaction.
- Vertices with a complicated color structure, for example,
the four-gluon one, are implemented by means of unphysical tensor field.
This field is treated by CompHEP as a special gluon ghost and
does not appear in the constructed diagrams.
A contribution of the four-gluon vertex is restored when
squared diagrams are evaluated, in the same manner as the contribution of
Faddeev-Popov and Goldstone ghosts.
See Sections
,
,
for further
explanations.
Footnote
- 1
In the following text we use Goldstone ghost
instead of commonly used Goldstone boson. For our convenience we
name both of these two kinds of fields and the auxiliary tensor field as
ghosts.