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Programs, Calculations, Proposal for parameters, Documentation

Programs

The known event generators for single top quark production include: ONETOP, PYTHIA, COMPHEP, MADGRAPH.

ONETOP

Author(s): C.P.Yuan, D. Carlson, S. Mrenna, Barringer, B. Pineiro, R. Brock

This is a stand-alone event generator which calculates weighted and unweighted events for the 2->2; 2->3; s-channel signal processes. It also calculates LO W+bbar background and ttbar background events. The unique feature about ONETOP is due to the matrix element calculation within the helicity basis. The complete density matrix is preserved in the signal and ttbar background events.

As used in ATLAS: the initial and final state partons are passed to PYTHIA for partlcle generation, including ISR and FSR. Standard PYTHIA and/or HEP COMMON records can be written. PYTHIA common is passed to ATLFAST for detector simulation.

Beatirz Pineiro has prepared documentation on the use of the ntuples produced with ONETOP.

PYTHIA

Author: Torbjörn Sjöstrand

Pythia has its own version of single top quark production.

Implementation in ATLAS:

Dubna:

 

Protvino

 

COMPHEP

Author(s): P.A.Baikov et al., Physical Results by means of CompHEP,in Proc.of X Workshop on High Energy Physics and Quantum Field Theory (QFTHEP-95), ed.by B.Levtchenko, V.Savrin, Moscow, 1996, p.101 , hep-ph/9701412

 

MADGRAPH

Authors: T. Stelzer and W.F. Long, Comp. Phys. Comm. 81, 357 (1994).

This is not an event generator, but rather a program for calculating the matrix elements of user-defined processes.

 

Calculations

11/17 We have been attempting to compare cross section calculations, This is a compilation to date:


Calculations of cross sections from various sources - no branching ratios included. In all cases, first number is for t, second is for tbar ... for W b bbar, first is W +, second is W -. All are in picobarns. Extensive footnotes are located below table. (In most cases, rounded to nearest pb.)

Updated 11/17/98 2050h

GROUP 2->2 2->3 s-channel Wt W bbar ttbar
Dubnaa 123 /        ? e  675 f
Protvino1 157 / 96   3.3 / 2.0 2 69 / 67 3 284 / 191 4 ~600 5
MSU10 111 / 11   4.1 / 12 59 / 59 13 no radiation:
85.5 /
14
596 15
Victoria         no radiation:
19
23
w raidation
312 24
 
Willenbrock etal.30   (t+tb) 244  (t+tb)10 62 / 62  (W+&W-) 318  803 36
Boos, et al. 40  (t+tb) 88 (t+tb) 154 41 (t+tb)10  (t+tr) 98  can't figure out  can't figure out

footnotes.

a 2->2 process passed to pythia; pdf-CTEQ2L

e bbbar content not yet filtered. Totals are:

f specifically the process g g & q qbar -> t(->b W(->e nubar)) tbar(->b W(->q qbar))

1 private calculation pdf-CTEQ2? ; QCD scales in pdf, mt or MW ; mb = 4.5 GeV/c2 ;

2 specifically the process

3 specifically the process g b -> W(->e nu) t(->b W(->e nu))

4 specifically the process

back to table

5 specifically the process g g & q qbar -> t(->b W(->e nubar)) tbar(->b W(->q qbar))

10 ONETOP pdf-CTEQ2L ;

11 specifically the process u b -> d t(->b W(->e nu))

12 specifically the process u dbar -> b t(->b W(->e nu))

back to table

13 specifically the process g b -> W(->e nu) t(->b W(->e nu))

14 specifically the process u dbar -> W(->e nu) g(->b bbar) (2 graphs)

15 specifically the process g g & q qbar -> t(->b W(->e nubar)) tbar(->b W(->ebar nu))

23 From Dugan's mail message of 11/17: generated Wplus jets without ISR or FSR in pythia and filtered results for bbbar final states got

1.85e4pb * (35 events with bbbar/300000 total events) = 2.16pb where W->e,nu

24 with radiation for both graphs:

3.26e4pb * (319 events with bbbar/300000 total events) = 34.7pb where W->e,nu

30 analytic calculations ; pdf CTEQ4L ; scale in g-f -SQRT(pT^2 + mb^2) - NLO calculations - k-factors at work!

36 NLO - so should not agree with LO calculations

40 comphep calculation...almost imposible to unambiguously figure out what they are doing.

41 cross section taken from Willenbrock

 

back to table


Proposal for calculational parameters:

We agreed that I would make a proposal for everyone for common parameters to be used in the MC calculations. I'm late, but here they are:

The 2-2 Process - use MW

     
    Use s-hat
     
     
    Use MW
     
     
    Use m t
     
     
    Use MW
     
       AL4 = QCDL                          (lambda)
       AL5=AL4*(AL4/AXMBOT)**(2./23.)
AL6=AL5*(AL5/XMTOP)**(2./21.)
XRATMIN=5.
B0=12.D0*3.14159/(33.-8.)
B1=6.D0*(153.-19.*4.)/(33.-8.)**2
ISTART=.FALSE.
END IF
XRAT=QQ**2
IF(XRAT.LT.XRATMIN)XRAT=XRATMIN
IF(SQRT(XRAT).GT.XMTOP)THEN
RAT=LOG(XRAT/AL6**2)
B0=12.D0*3.14159/21.
B1=6.D0*(153.-19.*6.)/21.**2
ELSEIF(SQRT(XRAT).GT.AXMBOT)THEN
RAT=LOG(XRAT/AL5**2)
B0=12.D0*3.14159/23.
B1=6.D0*(153.-19.*5.)/23.**2
ELSE
RAT=LOG(XRAT/AL4**2)
B0=12.D0*3.14159/25.
B1=6.D0*(153.-19.*4.)/25.**2
END IF
ALPHAS=B0/RAT

last modified: Thursday, December 10, 1998

Maintained by Chip Brock
Raymond Brock, Professor of Physics and Chairperson, Department of Physics and Astronomy, Michigan State University, East Lansing, MI 48824,