Tests of Photos operability for very heavy intermediate states or at very high energies
note that versions of PHOTOS (until may 2004) did not have worked well
for such heavy, TeV range, objects
| GENERATOR |
Branching ratio |
Maximum SDP |
T1 |
T2 |
Booklet |
|
test1 |
test2 |
test1 |
test2 |
test1 |
test2 |
test1 |
test2 |
test1 |
test2 |
| (n photons) -> |
0 |
1 |
0 |
1 |
2 |
0 |
1 |
0 |
1 |
2 |
| Comparison no 1 - older: Z -> mumu at 2 TeV |
| E_test=10.0, older |
| KK |
|
|
71.79 |
23.97 |
4.24 |
|
| PHOTOS O(4) |
|
|
72.31 |
22.41 |
5.27 |
|
|
0 |
0.0012 |
0.0375 |
|
3.113 |
|
0.202 |
|
 |
| Comparison no 1-NEW: Z -> mumu , highly virtual Z/gamma* state at 2 TeV , 4M events |
| E_test=10.0 |
| KK |
71.80 |
28.20 |
71.80 |
23.97 |
4.23 |
|
| PHOTOS O(2) |
72.32 |
27.68 |
72.32 |
22.42 |
5.26 |
0 |
0.0052 |
0 |
0.004 |
0.032 |
1.039 |
3.094 |
0.146 |
0.240 |
 |
 |
| PHOTOS O(4) |
72.29 |
27.71 |
72.29 |
22.43 |
5.28 |
0 |
0.0055 |
0 |
0.0007 |
0.0292 |
0.986 |
3.07 |
0.154 |
0.150 |
 |
 |
| PHOTOS EXP(7) |
71.71 |
28.29 |
71.71 |
24.03 |
4.26 |
0 |
0 |
0 |
0 |
0 |
0.174 |
0.166 |
0 |
0 |
 |
 |
| E_test=20.0 |
| KK |
76.17 |
23.82 |
76.16 |
20.92 |
2.92 |
|
| PHOTOS O(2) |
76.46 |
23.54 |
76.46 |
20.04 |
3.50 |
0 |
0.0023 |
0 |
0.0019 |
0.0198 |
0.567 |
1.752 |
0.052 |
0.091 |
 |
 |
| PHOTOS O(4) |
76.42 |
23.58 |
76.42 |
20.07 |
3.50 |
0 |
0.002 |
0 |
0.0005 |
0.015 |
0.498 |
1.689 |
0.047 |
0.053 |
 |
 |
| PHOTOS EXP(7) |
76.10 |
23.90 |
76.10 |
20.96 |
2.94 |
0 |
0 |
0 |
0 |
0 |
0.138 |
0.119 |
0 |
0 |
 |
 |
| Comparison no 2: Z -> e+ e-, highly virtual Z/gamma* state at 2 TeV |
In construction of the plots we have used "muons of electron mass"
(therefore description of plots and tables may be wrong, even though the results are OK.
Plots will be replaced) |
| E_test=10.0 |
| KK |
59.19 |
40.81 |
59.19 |
31.39 |
9.42 |
|
| PHOTOS EXP |
59.23 |
40.77 |
59.23 |
31.32 |
9.45 |
0 |
0.002 |
0 |
0.002 |
0.0003 |
0.079 |
0.129 |
0.080 |
0.080 |
 |
 |
|
| Comparison no 3: Z -> mumu at LHC energies (pp at 14TeV), Z is close to its resonance peak |
| E_test=10.0 |
| PYTHIA w/FSR |
87.98 |
12.02 |
87.98 |
11.21 |
0.81 |
|
| PHOTOS EXP |
89.21 |
10.78 |
89.21 |
10.12 |
0.67 |
0 |
0.0240 |
0 |
0.025 |
0.003 |
2.468 |
2.453 |
0.278 |
0.263 |
 |
 |
| Comparison no 4: W+ -> mu+ nu_mu at LHC energies (pp at 14TeV), W is close to its resonance peak |
| E_test=10.0 |
| WINHAC (EXP) |
95.449 |
4.551 |
95.449 |
4.441 |
0.110 |
|
| WINHAC+PHOTOS (EXP) |
95.424 |
4.576 |
95.424 |
4.454 |
0.121 |
0 |
0.0003 |
0 |
0.0003 |
0.0018 |
0.046 |
0.035 |
0.0013 |
0.0013 |
 |
 |
| PYTHIA (FSR ON) |
94.707 |
5.293 |
94.707 |
5.147 |
0.146 |
|
| PYHIA+PHOTOS (EXP) |
95.416 |
4.584 |
95.416 |
4.463 |
0.121 |
0 |
0.0562 |
0 |
0.055 |
0.024 |
1.416 |
1.391 |
0.269 |
0.263 |
 |
 |
The purpose of these tests is to present the performance of PHOTOS at different sophistication levels,
and how it compares with the matix element generator: KKMC, widely used PYTHIA and WINHAC.
As one can see, adding third and fourth order in PHOTOS improves agreement with the baseline, i.e. KKMC.
However, only PHOTOS EXP has a good agreement with KKMC. In case of W decays, we perform comparison
with PHOTOS EXP only. Agreement is not as perfect as in case of KKMC and Z decays, this is of no surprise,
the quality of the single-photon emission kernel is not as good;
see reference: Acta Phys.Polon.B34:4561-4570,2003. It will be relatively easy to improve, if necessary.
One can be surprised why we call these comparisons at very high energies,
as the scale of most of the plots do not exceed 150 GeV. This is because W or Z, which decays
were studies, are ultra-relativistic (as in LHC). From physics point of view, this does not
provide much of importance, but in this way we test the algorithm's numerical stability in
real working conditions.
The tests are being defined in the laboratory frame
(the 4-momenta of leptons and photons are defined in this frame), that is why
Etest=10/20 GeV should be compared to average W/Z energy and not its mass.
The tests on momenta from the rest-frame of decaying particle are collected in the
antenna algorithm studies page.
Note: In practical applications, problems with numerical stability
may occur. These problems result in PHOTOS "STOP" messages, e.g.
"Too much bremsstrahlung, PRSOFT=...", at least if PHOTOS runs with
default settings.
For explanation of built-in solutions (to be activated by the user) and comments
on their applicability,
please refer to our stability studies page.
Last modification: Piotr Golonka, 24 August 2004, 17:35