Monte Carlo samples for CLICdet

A description of Whizard settings for CLICdet along with selected Sindarin examples is provided at this repository: https://gitlab.cern.ch/CLICdp/DetectorSoftware/clic-whizard2-settings

• All samples were generated using WHIZARD2.7.0-2.8.3 unless stated otherwise.
• The detector model is CLIC_o3_v14 unless stated otherwise.
• If not stated otherwise, beam spectra from CIRCE2 and ISR pt from the recoil handler are used.
• Resonance history settings for the Pythia6 interface are:

resonance_on_shell_limit   = 16
resonance_on_shell_turnoff = 8

• Cuts correspond to default Whizard 1 cuts:
  • For ee->qq, ee->qqqq, ee->hqq, ee->qqqqqq samples: m(qq) > 10 GeV
  • For samples with lepton pairs: M(ll) > 4 GeV
  • Q cut between incoming and outgoing e- (e+) (virtual photon): 1 GeV

In Sindarin:

real default_M_cut = 4 GeV
real default_jet_cut = 10 GeV
real default_E_cut = 10 GeV
real default_Q_cut = 4 GeV
alias quarks = u:d:s:c:b:U:D:S:C:B
cuts = all M > default_M_cut [lepton,lepton]
and all M > default_jet_cut [quarks,quarks]
and all M < - default_Q_cut [incoming e1, e1]
and all M < - default_Q_cut [incoming E1, E1]

Caveat for cuts: automatic flavor summation with charge-conjugated final states: https://answers.launchpad.net/whizard/+question/687913: don't sum automatically over lists of particles when applying cuts on part of the list only.

• Parameters: m(u)=m(d)=m(s)=m(c)=m(b)=0
• The column "Events produced" gives the approximate number of produced events. (Obtain the current number with something like dirac-ilc-find-in-FC /ilc/prod/ ProdID=... Datatype=DST | wc)

Samples at 350 GeV

Based on existing Whizard1 generation

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee->hZ, Z->qq, h->π_vπ_v, π_v->bb	14367	240000	240000	93.44*	based on 10945
ee->hZ, Z->qq, h->π_vπ_v, π_v->bb	14369	240000	240000	93.44*	based on 10942
ee -> qqnunu	14371	306500	306500	324.5353	based on 2860

* = assuming BR(h->π_vπ_v) = 100%, BR(π_v->bb) = 100% for the hidden valley pions π_v

WHIZARD samples at 380 GeV

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee -> HZ, Z->mumu	13384	30k	30000	4.0562080E+00	mH=125 GeV, 380 GeV beam spectrum and overlay, no polarisation

WHIZARD samples at 1.5 TeV assuming polarised beams

Beam spectrum and gg->had overlay is taken from 1.4 TeV (scaled to 1.5 TeV).

Various signal and background processes

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee -> ZHH	13338	1000	3250	7.8121091E-02	P(e-) = +80%
ee -> ZHH	13337	3000	3200	1.1231722E-01	P(e-) = -80%
ee -> qq	15300	1M	958700	2.863E+03	P(e-)=-80%
ee -> qq	15301	500k	479300	1.787E+03	P(e-)=+80%
ee->qqqq	13769	2M	1950200	1943.2	P(e-)=-80%
ee->qqqq	13770	2M	1949800	1943.2	P(e-)=-80%
ee->qqqq	13771	3k	1945200	260.3	P(e-)=+80%
ee -> ll	14397	500k	500100	1406	P(e-)=-80%; Q cut 400 GeV
ee -> ll	14398	500k	500000	1406	extension of 14397
ee -> ll	14399	500k	500100	1406	extension of 14397
ee -> ll	14400	500k	500000	1406	extension of 14397
ee -> ll	14401	500k	500000	1213	P(e-)=+80%; Q cut 400 GeV
ee -> qqlnu	14676	500k	499800	7001	P(e-)=-80%
ee -> qqlnu	14677	500k	500000	7001	P(e-)=-80%, extension of 14676
ee -> qqlnu	14678	500k	499900	7001	P(e-)=-80%, extension of 14676
ee -> qqlnu	14679	500k	499900	7001	P(e-)=-80%, extension of 14676
ee -> qqlnu	14680	500k	499900	1687	P(e-)=+80%
qq -> qqll	14692	500k	500000	2715	P(e-)=-80%
qq -> qqll	14693	500k	500000	2715	P(e-)=-80%, extension of 14692
qq -> qqll	14694	500k	500100	2502	P(e-)=+80%
ee -> qqnunu	14885	1M	1000100	1460	P(e-) = -80%
ee -> qqnunu	14886	100k	100100	185	P(e-) = +80%
ee -> qqqqlnu	14970	500k	493300	169	P(e-) = -80%
ee -> qqqqlnu	14971	40k	97900	57.8	P(e-) = +80%
ee -> qqlnununu	15008	500k	492300	66.8	P(e-) = -80%
ee -> qqlnununu	15009	50k	48100	7.6	P(e-) = +80%
ee -> qqlnulnu	14992	100k	97400	14.9	P(e-) = -80%
ee -> qqlnulnu	14993	10k	10000	4.9	P(e-) = +80%

Inert Doublet Model at 1.5 TeV

Benchmark Point	ProdID	Events planned	Events produced	σ [fb]	Comments
bp21	14321	50k	50k	8.093	P(e-)=-80%
bp23	14322	50k	50k	12.497	P(e-)=-80%
hp17	14323	50k	50k	2.435	P(e-)=-80%
hp20	14324	50k	50k	1.323	P(e-)=-80%
hp3	14325	50k	50k	0.6294	P(e-)=-80%

Samples compatible with ttbar fully hadronic at 1.5 TeV

• For all samples: mH = 10 TeV; m(qq) > 10 GeV; alphas = 0
• "y" = d, s, b
• "x" = u, c

=> Compatible with ttbar means all combinations of yyxyyx because the top decays both always give down-type quarks.

The processes ee -> bbcbbc, ee->bbubbu, ee->ddcyyc, ee->dduyyu, ee->sscbbc, ee->sscssc, ee->ssussu, ee->ssubbu, ee->yyccyyu, ee->yyuyyc are defined in such a way that they are mutually exclusive and cover all flavor combinations for 6-quark final states.

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee->bbcbbc		300		1.297E-02	P(e-)=-80%
ee->bbcbbc		100		4.429E-03	P(e-)=+80%
ee->bbubbu		300		1.285E-02	P(e-)=-80%
ee->bbubbu		100		4.382E-03	P(e-)=+80%
ee->ddcyyc		45000		1.794E+00	P(e-)=-80%
ee->ddcyyc		6100		2.473E-01	P(e-)=+80%
ee->dduyyu		720000		2.886E+01	P(e-)=-80%
ee->dduyyu		300000		1.157E+01	P(e-)=+80%
ee->sscbbc		650000		2.568E+01	P(e-)=-80%
ee->sscbbc		300000		1.185E+01	P(e-)=+80%
ee->sscssc		35000		1.493E+00	P(e-)=-80%
ee->sscssc		4000		1.761E-01	P(e-)=+80%
ee->ssubbu		3000		1.209E-01	P(e-)=-80%
ee->ssubbu		1200		5.108E-02	P(e-)=+80%
ee->ssussu		500		1.726E-02	P(e-)=-80%
ee->ssussu		200		4.895E-03	P(e-)=+80%
ee->yycyyu		800000		3.195E+01	P(e-)=-80%
ee->yycyyu		300000		1.270E+01	P(e-)=+80%
ee->yyuyyc		800000		3.179E+01	P(e-)=-80%
ee->yyuyyc		300000		1.272E+01	P(e-)=+80%

WHIZARD samples at 3 TeV assuming polarised beams

Various signal and background processes (Standard Model)

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee -> qq	13399	400k	404350	1269 (*)	P(e-) = -80%, mH=125 GeV, q=u,d,s,c,b
ee -> qq	13400	400k	404325	1269 (*)	extension of 13399
ee -> qq	13401	400k	404575	1269 (*)	extension of 13399
ee -> qq	13402	400k	404325	1269 (*)	extension of 13399
ee -> qq	13398	400k	404475	786 (*)	P(e-) = +80%, mH=125 GeV, q=u,d,s,c,b
ee -> qq	13425	400k	397600	170.8	P(e-) = -80%, mH=125 GeV, q=u,d,s,c,b; m(qq)>1 TeV
ee -> qq	13426	400k	397875	170.8	extension of 13425
ee -> qq	13427	400k	397575	170.8	extension of 13425
ee -> qq	13428	400k	397750	170.8	extension of 13425
ee -> qq	13429	400k	398400	73.5	P(e-) = +80%, mH=125 GeV, q=u,d,s,c,b; m(qq)>1 TeV
ee -> qqqq	13394	500k	499000	902	P(e-) = -80%, mH = 10 TeV, q=u,d,s,c,b; with ISR PT recoil
ee -> qqqq	13395	500k	498725	902	extension of 13394
ee -> qqqq	13396	500k	498975	902	extension of 13394
ee -> qqqq	13397	500k	499050	902	extension of 13394
ee -> qqqq	13393	500k	498700	120	P(e-) = +80%, mH = 10 TeV, q=u,d,s,c,b; with ISR PT recoil
ee -> qqqq	13696	400k	399300	369.8	P(e-) = -80%, mH = 10 TeV, q=u,d,s,c,b; m(qqqq)> 2000 GeV
ee -> qqqq	13697	400k	399450	369.8	extension of 13696
ee -> qqqq	13698	400k	399250	369.8	extension of 13696
ee -> qqqq	13699	400k	399125	369.8	extension of 13696
ee -> qqqq	13700	400k	399025	49.2	P(e-) = +80%, mH = 10 TeV, q=u,d,s,c,b; m(qqqq)> 2000 GeV
ee -> hqq	13391	120k	121250	3.83	P(e-)=-80%, q=udscb, mH=125 GeV, mqq>10!GeV; with ISR PT recoil
ee -> hqq	13392	30k	30250	2.67	P(e-)=+80%, q=udscb, mH=125 GeV, mqq>10!GeV; with ISR PT recoil
ee -> hZ, Z->ll	13389	12k	12000	3.7966586E-01	P(e-)=-80%, l=e,mu, mH=125 GeV, m(ll) > 4 GeV
ee -> hZ, Z->ll	13390	3k	3000	2.6364074E-01	P(e-)=+80%, l=e,mu, mH=125 GeV, m(ll) > 4 GeV
ee -> ZHH	14343	10k	10000	6.06E-02	P(e-) = -80%
ee -> ZHH	14344	10k	10000	4.23E-02	P(e-) = +80%
ee -> qqHH	14364	40k	40000	4.18E-02	P(e-) = -80%
ee -> qqHH	14365	40k	39950	2.898E-02	P(e-) = +80%
gg -> had only	13903	125k	125k	-	no "signal", only the gamma gamma -> hadrons at 3 TeV (30 BX)
gg -> had only	13904	125k	125k	-	extension of 13903
gg -> had only	13927	125k	125k	-	extension of 13903
gg -> had only	13930	125k	125k	-	extension of 13903
gg -> had only	13933	125k	125k	-	extension of 13903
gg -> had only	13936	125k	125k	-	extension of 13903
gg -> had only	13939	125k	125k	-	extension of 13903
gg -> had only	13942	125k	125k	-	extension of 13903
gg -> had only	13945	125k	125k	-	extension of 13903
gg -> had only	13948	125k	125k	-	extension of 13903
ee -> ll	14382	500k	499725	1664.9796	P(e-)=-80%; Q cut 400 GeV
ee -> ll	14383	500k	499775	1664.9796	extension of 14382
ee -> ll	14384	500k	499600	1664.9796	extension of 14382
ee -> ll	14385	500k	499750	1664.9796	extension of 14382
ee -> ll	14386	500k	499450	1439.0744	P(e-)=+80%; Q cut 400 GeV
ee->qqlnu	14545	250k	244875	8672	P(e-)=-80%, default cuts, (**)
ee->qqlnu	14546	250k	245175	8672	extension of 14545, (**)
ee->qqlnu	14547	250k	244875	8672	extension of 14545, (**)
ee->qqlnu	14548	250k	244850	8672	extension of 14545, (**)
ee->qqlnu	14549	250k	244700	8672	extension of 14545, (**)
ee->qqlnu	14550	250k	245050	8672	extension of 14545, (**)
ee->qqlnu	14551	250k	245200	8672	extension of 14545, (**)
ee->qqlnu	14552	250k	245025	8672	extension of 14545, (**)
ee->qqlnu	14553	250k	245050	8672	extension of 14545, (**)
ee->qqlnu	14554	250k	245225	8672	extension of 14545, (**)
ee->qqlnu	14555	250k	244675	8672	extension of 14545, (**)
ee->qqlnu	14556	250k	244825	8672	extension of 14545, (**)
ee->qqlnu	14557	250k	245500	8672	extension of 14545, (**)
ee->qqlnu	14558	250k	245025	8672	extension of 14545, (**)
ee->qqlnu	14559	250k	245050	8672	extension of 14545, (**)
ee->qqlnu	14560	250k	245000	8672	extension of 14545, (**)
ee->qqlnu	14561	250k	247050	2291.6	P(e-)=+80%, default cuts, (**)
ee->qqlnu	14562	250k	246875	2291.6	extension of 14561, (**)
ee -> qqll	14654	250k	248125	3.180E+03	P(e-)=-80%, (**)
ee -> qqll	14655	250k	247750	3.180E+03	P(e-)=-80%, extension of 14654, (**)
ee -> qqll	14656	250k	247825	3.180E+03	P(e-)=-80%, extension of 14654, (**)
ee -> qqll	14657	250k	248450	3.180E+03	P(e-)=-80%, extension of 14654, (**)
ee -> qqll	14658	250k	248150	3.020E+03	P(e-)=+80%, (**)
ee -> qqll	14659	250k	248475	3.020E+03	P(e-)=+80%, extension of 14658, (**)
ee -> ZZH -> qqqqH	14726	6000	6025	1.3943515E-01	P(e-) = -80%
ee -> ZZH -> qqqqH	14727	3000	3025	7.1648198E-02	P(e-) = +80%
ee -> WWH -> qqqqH	14734	100k	99775	4.116E+00	P(e-) = -80%
ee -> WWH -> qqqqH	14735	2500	2525	5.176E-01	P(e-) = +80%
ee -> qqnunu	14869	500k	499950	2.3335039E+03	P(e-) = -80%
ee -> qqnunu	14870	500k	499850	2.3335039E+03	P(e-) = -80%, extension of 14869
ee -> qqnunu	14871	500k	499925	2.3335039E+03	P(e-) = -80%, extension of 14869
ee -> qqnunu	14872	500k	499850	2.3335039E+03	P(e-) = -80%, extension of 14869
ee -> qqnunu	14873	500k	499900	2.7006587E+02	P(e-) = +80%
ee -> qqnunu	14874	500k	500000	2.7006587E+02	P(e-) = +80%, extension of 14873
ee -> qqqqlnu	14960	300k	291200	148	P(e-) = -80%
ee -> qqqqlnu	14961	300k	290250	148	P(e-) = -80%, extension of 14960
ee -> qqqqlnu	14962	50k	49675	42.2	P(e-) = +80%
ee -> qqlnununu	15018	250k	247350	96.8	P(e-) = -80%
ee -> qqlnununu	15019	250k	247700	14.0	P(e-) = -80%, extension of 15018
ee -> qqlnununu	15020	50k	49650		P(e-) = +80%
ee -> qqlnulnu	15028	120k	118625	20.4	P(e-) = -80%
ee -> qqlnulnu	15029	20k	19750	7.0	P(e-) = +80%

(*) Difference between cross sections from previous production for ee->qq is understood: It originates from the improved beam spectrum used now, which better models the low invariant mass region.

(**) Due to the extremely high number of hits for very few events (<0.1% of events) originating from very forward electrons (which most analyses will anyway not consider), a small number of jobs did not finish. The resulting bias is negligible.

Various signal processes (BSM)

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee -> ch1 ch1 -> neu1 pi neu1 pi	13901	50k	50025	13.04	P(e-)=-80%, m(ch1,ch1)>4GeV, pure higgsino, m_ch1=1050 GeV, m_neu1=1049.84, ctau(ch1)=600mm (v2)
ee -> ch1 ch1 -> neu1 pi neu1 pi	13902	50k	50025	3.94	P(e-)=+80%, m(ch1,ch1)>4GeV, pure higgsino, m_ch1=1050 GeV, m_neu1=1049.84, ctau(ch1)=600mm (v2)
ee -> ch1 ch1 -> neu1 pi neu1 pi	14633	50k	50025	8.50	no polarisation, without overlay, m(ch1,ch1)>4GeV, pure higgsino, m_ch1=1050 GeV, m_neu1=1049.84, ctau(ch1)=180mm (v3)
ee -> ch1 ch1 -> neu1 pi neu1 pi	14710	50k	50025	13.0	P(e-)=-80%, no overlay, m(ch1,ch1)>4GeV, pure higgsino, m_ch1=1050 GeV, m_neu1=1049.84, ctau(ch1)= 6.9mm (v4)
ee -> ch1 ch1 -> neu1 pi neu1 pi	14712	50k	50025	3.9	P(e-)=-80%, with overlay, m(ch1,ch1)>4GeV, pure higgsino, m_ch1=1050 GeV, m_neu1=1049.84, ctau(ch1)= 6.9mm (v4)

Inert Doublet Model at 3 TeV

Benchmark Point	ProdID	Events planned	Events produced	σ [fb]	Comments
bp21	14214	50k	50k	4.213	P(e-)=-80%
bp23	14215	50k	50k	5.767	P(e-)=-80%
hp17	14216	50k	50k	1.678	P(e-)=-80%
hp20	14217	50k	50k	1.506	P(e-)=-80%
hp3	14218	50k	50k	1.775	P(e-)=-80%

Samples compatible with ttbar at 3 TeV

• For all samples: mH = 10 TeV; m(qq) > 10 GeV; alphas = 0
• "y" = d, s, b
• "x" = u, c

only fully hadronic decay so far => 6 quarks compatible with ttbar means all combinations of yyxyyx because the top decays both always give down-type quarks.

The processes ee -> bbcbbc, ee->bbubbu, ee->ddcyyc, ee->dduyyu, ee->sscbbc, ee->sscssc, ee->ssussu, ee->ssubbu, ee->yycbbu, ee->yycddu, ee->yycssu, ee->yyubbc, ee->yyuddc, and ee->yyussc are defined in such a way that they are mutually exclusive and cover all flavor combinations for 6-quark final states. For computational reasons, the processes yycyyu and yyuyyc which were used in the previous productions of ttbar samples had to be split up.

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee->bbcbbc	13094	10000	10000	9.2271753E-03	P(e-)=-80%
ee->bbcbbc	13071	10000	9950	2.9986901E-03	P(e-)=+80%
ee->bbubbu	13095	10000	10000	9.1731760E-03	P(e-)=-80%
ee->bbubbu	13072	10000	10000	2.9825397E-03	P(e-)=+80%
ee->ddcyyc	13096	50000	50050	1.3757137E+00	P(e-)=-80%
ee->ddcyyc	13073	15000	14450	1.7824610E-01	P(e-)=+80%
ee->dduyyu	13097	480000	479075	1.4498909E+01	P(e-)=-80%
ee->dduyyu	13074	130000	126275	5.0109474E+00	P(e-)=+80%
ee->sscbbc	13098	350000	350125	1.2499614E+01	P(e-)=-80%
ee->sscbbc	13075	90000	89000	4.8938333E+00	P(e-)=+80%
ee->sscssc	13099	50000	50225	1.1651315E+00	P(e-)=-80%
ee->sscssc	13076	15000	14975	1.3677677E-01	P(e-)=+80%
ee->ssussu	13123	10000	9550	1.2615661E-02	P(e-)=-80%
ee->ssussu	13077	10000	9875	3.3776171E-03	P(e-)=+80%
ee->ssubbu	13292	20000	20250	5.4145233E-02	P(e-)=-80%
ee->ssubbu	13293	10000	10250	2.3216638E-02	P(e-)=+80%
ee->yycbbu	13318	430k	449775	1.3394883E+01	P(e-)=-80%
ee->yycbbu	13322	130k	130075	5.2101109E+00	P(e-)=+80%
ee->yycddu	13326	63k	62675	2.0054737E+00	P(e-)=-80%
ee->yycddu	13319	10k	10225	4.0984879E-01	P(e-)=+80%
ee->yycssu	13323	64k	65025	2.0248353E+00	P(e-)=-80%
ee->yycssu	13327	10k	10250	4.1853929E-01	P(e-)=+80%
ee->yyubbc	13320	430k	449850	1.3330064E+01	P(e-)=-80%
ee->yyubbc	13324	130k	130125	5.2070149E+00	P(e-)=+80%
ee->yyuddc	13328	63k	62575	2.0034170E+00	P(e-)=-80%
ee->yyuddc	13321	10k	10250	4.1203686E-01	P(e-)=+80%
ee->yyussc	13325	64k	65125	2.0189010E+00	P(e-)=-80%
ee->yyussc	13329	10k	10250	4.2245034E-01	P(e-)=+80%
ee->yycyyu	13078	150000	84775	5.5459085E+00	P(e-)=+80% OVERLAP! (*)
ee->yyuyyc	13079	150000	85825	5.5374079E+00	P(e-)=+80% OVERLAP! (*)

(*) The processes ee_yycyyu (13078) and ee_yyuyyc (13079) - only produced for positive polarisation - correspond to ee_yycyyu=ee_yycbbu+ee_yycddu+ee_yycssu and ee_yyuyyc=ee_yyubbc+ee_yyuddc+ee_yyussc. The existing files for 13078 and 13079 can be used to extend the statistics. In the normalisation, keep in mind that they overlap.

Six-Quark Samples other than ttbar at 3 TeV

• For all samples: mH = 10 TeV; m(qq) > 10 GeV; alphas = 0 * "y" = d, s, b
• "x" = u, c

=> Non-ttbar samples with 6 quarks means all combinations of xxyxxy. The combinations xxxyyy and xxxxxy or yyyyyx are not possible as they would require a net W (instead of only WW) i.e. charge is not conserved.

These samples include all combinations of 3 electroweak gauge bosons, but no Higgs bosons.

Type	ProdID	Events planned	Events produced	σ [fb]	Comments
ee->bbxxxx	14601	1800	1825	3.6427E-02	P(e-)=-80%
ee->bbxxxx	14602	600	625	1.1996E-02	P(e-)=+80%
ee->bdxxxx	14603	400	425	7.8948E-03	P(e-)=-80%
ee->bdxxxx	14476	50	75	9.1650E-04	P(e-)=+80%
ee->bsxxxx	14604	400	425	7.8901E-03	P(e-)=-80%
ee->bsxxxx	14478	50	75	9.0803E-04	P(e-)=+80%
ee->dbxxxx	14605	400	425	7.9020E-03	P(e-)=-80%
ee->dbxxxx	14480	50	75	9.1236E-04	P(e-)=+80%
ee->ddxxxx	14481	100000	100050	2.3698E+00	P(e-)=-80%
ee->ddxxxx	14482	14000	14075	2.7583E-01	P(e-)=+80%
ee->dsxxxx	14606	200000	200025	4.3881E+00	P(e-)=-80%
ee->dsxxxx	14607	20000	20025	5.0859E-01	P(e-)=+80%
ee->sbxxxx	14485	400	425	8.0580E-03	P(e-)=-80%
ee->sbxxxx	14608	50	75	9.1615E-04	P(e-)=+80%
ee->sdxxxx	14487	200000	200050	4.4150E+00	P(e-)=-80%
ee->sdxxxx	14488	20000	20075	5.1915E-01	P(e-)=+80%
ee->ssxxxx	14609	120000	119975	2.2316E+00	P(e-)=-80%
ee->ssxxxx	14610	14000	14025	2.6630E-01	P(e-)=+80%

Requests

To request new production samples for CLICdet and Whizard 2, send an e-mail to Ulrike Schnoor. Please provide the following information:

1. If the GEN files already exists:

• What are the prodIDs?
• The default is to produce only DST. Which additional collections are required, if any?
• I will assume you need exactly the same number of events.
• I will assume that the following default settings can be used. Let me know if any of these should be changed:
  • Overlay at the corresponding energy is switched on
  • Conformal tracking
  • detector model CLIC_o3_v14
  • latest installed version of the Software chain
  • Only DST files are kept (no REC)

2. New production

• Do you have a Sindarin file? If yes, please send it to me.
• Process
• Center-of-mass energy
• beam polarisation
• Any non-standard settings for masses, couplings and other parameters
• Number of events (usually about 10*luminosity*sigma, where the luminosity should be scaled by the polarisation fraction for samples with beam polarisation). The feasibility of the sample will be evaluated (normally a few million is the maximum for important processes).
• Cuts in addition to standard cuts
• The following default settings would be assumed unless you request otherwise:
  • Overlay at the corresponding energy is switched on
  • ISR on (except for processes with Matrix-Element photons)
  • Beamspectrum on
  • Pythia is used with the OPAL tune
  • Conformal tracking is used
  • detector model CLIC_o3_v14
  • Latest installed version of Whizard and of the Software chain
  • Only DST files are kept (no REC)
• Is there a corresponding production with the old software chain? If yes, what is the prod ID?

-- UlrikeSchnoor - 2019-02-08