Overall feature |
Signature |
Benchmark Points |
I. Exotic decay of Higgses |
Neutral Higgs to neutral Higgs + Z |
H->AZ |
bbll, tautaull |
BP1_D, BP2_2, BP2_3, BP2_4 |
A->HZ |
bbll, tautaull, WWZ, ZZZ |
BP2_1, BP2_8, BP3_A1, BP3_A2, BP3_B1, BP3_B2 |
A->hZ |
bbll, tautaull, gagall, WWll, ZZll |
BP1_B, BP2_9, BP2_10 |
|
comment |
The heavy CP-even Higgs H being the 125 GeV SM-like Higgs or non-alignment |
h->ZA |
Zmumu, Ztautau, Zbb |
BP4_ABCD |
|
comment |
SM Higgs decay |
Neutral Higgs to neutral Higgs + neutral Higgs |
H->AA |
bbbb, 4tau, bbtautau, bbgaga |
BP2_3, BP2_3, BP2_5 |
H->hh |
bbbb, bbtautau, bbWW, bbZZ, bbgaga |
BP1_A, BP2_9 |
|
comment |
The heavy CP-even Higgs H being the 125 GeV SM-like Higgs or non-alignment |
Neutral Higgs to Hpm Wmp |
H->Hpm Wmp |
tblnu |
BP1_D, BP2_6, BP2_8 |
A->Hpm Wmp |
tblnu, taunulnu |
BP1_D, BP2_6, BP2_7, BP3_A2, BP3_B2 |
Neutral Higgs to H+H- |
H->H+H- |
ttbb |
BP2_8 |
Hpm to neutral Higgs + Wpm, Hpm produced with tbHpm channel |
Hpm->AW |
bbbbWW, tautaubbWW |
BP1_D, BP2_2, BP2_3, BP2_4, BP2_5 |
Hpm->HW |
bbbbWW, tautaubbWW |
BP2_1 |
Hpm->hW |
bbbbWW, tautaubbWW,bbZZWW, bbWWWW, bbgagaWW |
BP2_9, BP2_10 |
|
comment |
The heavy CP-even Higgs H being the 125 GeV SM-like Higgs |
Long cascade |
Hpm->AW->HZW |
bbWZ, tautauWZ |
BP1_E |
A->Hpm Wmp ->WWH |
bbWW, tautauWW |
BP1_E |
|
comment |
Small branching fraction, <5% |
II. Decay of Higgses to WW, ZZ, gaga, bb, tautau |
Fermiophobic heavy H, produced via H+H-, HA, H+A, H+H |
H+->HW, A->HZ |
H->WW,ZZ, multigauge boson final states |
BP6 |
|
comment |
Small production cross section, difficult to search, a rather light, yet very elusive, non-SM scalar. |
Non-alignment/H being the SM-like 125 GeV Higgs/mA~mh~125/flipped Yukawa/MSSM-like |
H/h to SM final states |
usual SM-like Higgs search channel, higher mass |
BP1_A, BP1_B, BP1_C, BP1_F, BP1_G |
III. One neutral Higgs being MET |
H in the Inert Doublet Model, produced via H+H-, HA, H+A, H+H |
H+->HW (or AW), A->HZ |
W/Z/WW/WZ+MET final states |
BP5 |
|
comment |
Small production cross section for some benchmarks [masses > 300 GeV], H is dark matter candidate [mass> 50 GeV], unique signal of MET. W,Z decays as in SM.. SM gauge couplings and kinematics determine production cross sections and decays |
This is the working page for the discussion on CP-conserving 2HDM benchmarks. Note that the list of submitted proposals below is not necessarily (yet) complete.
Phenomenological benchmarks for the CP-conserving 2HDM with softly-broken Z_2-symmetry.
Benchmark points for exotic Higgs decays.
We attach our 2HDM benchmarks for LHC searches, based on our recent work
1405.5537, together with some discussion on their salient features and motivation.
Here in attach a brief note explaining the benchmark scenarios we chose (.pdf and .tex), together with a file with the definition of the benchmarks in terms of 2HDM parameter.
We are still working on other benchmark scenarios mentioned in a previous mail (higgs-to-2-Higgs topologies) and we will provide them shortly.
Please find attached a short writeup containing benchmarks for the IDM. This note should be seen as a preview of a full publication which should then be used as a reference.
Following your call for 2HDM benchmark suggestions, I'd like to contribute with one of the scenarios we devised for our Higgs pair study [arXiv:1407.0281]. Please find attached all the details, hopefully complying with the indications given in your email.
BP3_A1 |
Main Features |
Type I-II 2HDM in alignment limit, decay of non-SM Higgses: A -> HZ, Hpm -> HW |
Spectrum/input parameters |
mh (SM-like) = 125 GeV, mH=180 GeV, mA=420 GeV, mHpm=420 GeV, SBA=1, TB=3, m12=100 GeV |
sigma(gg->A)*Br(A->HZ) |
Type I: 2.795*0.843 [pb] Type II: 2.837*0.838 [pb] |
sigma(tbHpm)*Br(Hpm->HW) |
Type I: sigma(tbHpm)*0.857 Type II: sigma(tbHpm)*0.854 |
Relevant H decay branching fraction(s) |
Type I: Br(H ->bb) = 0.711 Type II: Br(H ->bb) = 0.899 |
comment |
BP3_A1_Bis |
Main Features |
Type I-II 2HDM in alignment limit, decay of non-SM Higgses: A -> HZ |
Spectrum/input parameters |
mh (SM-like) = 125 GeV, mH=400 GeV, mA=550 GeV, mHpm=550 GeV, SBA=1, TB=3, m12=210 GeV |
sigma(gg->A)*Br(A->HZ) |
Type I: 0.657*0.498 [pb] Type II: 0.684*0.486 [pb] |
Relevant H decay branching fraction(s) |
Type I: Br(H ->tt) = 0.992 Type II: Br(H ->tt) = 0.866, Br(H ->bb) = 0.115 |
comment |
Benchmark similar to BP3_A1 (sizable A-H mass splitting), but higher mH |
|
Dominant H -> tt makes H discovery challenging via direct (ggH) production |
|
Width_H < 1 GeV |
BP3_B1 |
Main Features |
Type I 2HDM away from alignment, decay of non-SM Higgses: A -> HZ |
Spectrum/input parameters |
mh (SM-like) = 125 GeV, mH=180 GeV, mA=400 GeV, mHpm=400 GeV, SBA=0.95, TB=2, m12=100 GeV |
sigma(gg->A)*Br(A->HZ) |
8.158*0.584 [pb] |
Relevant H decay branching fraction(s) |
Type I: Br(H ->WW) = 0.715 Type II: Br(H ->ZZ) = 0.285 |
comment |
Multilepton (2,3,4) Final State |
|
Direct H Production (ggH) suppressed for CBA>0 |
|
4-lepton Final State: m_4l does not reconstruct mH -> Heavy Higgs di-boson searches not as sensitive |
BP4_A |
Main Features |
Type I 2HDM, Decay of SM Higgses into Z boson and light A=20 GeV |
Spectrum/input parameters(A) |
mh (SM-like) = 125.97 GeV, mH=165.50 GeV, mA=20.25 GeV, mHpm=444.72 GeV, SBA=-0.99, TB=1.86, m12=62.38 GeV |
|
sigma(gg->h1)*Br(h1->ZA) |
38.82*0.0971 [pb] |
Br(A->mumu) |
0.0002101 |
Br(A->tautau) |
0.0585 |
Br(A->bb) |
0.8496 |
BP4_B |
Main Features |
Type I 2HDM, Decay of SM Higgses into Z boson and light A=63 GeV |
Spectrum/input parameters(A) |
mh (SM-like) = 125.93 GeV, mH=153.37 GeV, mA=63.42 GeV, mHpm=444.72 GeV, SBA=-0.85, TB=6.20, m12=52.85 GeV |
|
sigma(gg->h1)*Br(h1->ZA) |
26.59*0.0268 [pb] |
Br(A->mumu) |
0.0002318 |
Br(A->tautau) |
0.0655 |
Br(A->bb) |
0.7908 |
BP4_C |
Main Features |
Type II 2HDM, Decay of SM Higgses into Z boson and light A=6 GeV |
Spectrum/input parameters(A) |
mh (SM-like) = 125.85 GeV, mH=263.67 GeV, mA=6.28 GeV, mHpm=308.25 GeV, SBA=0.99, TB=1.89, m12=52.32 GeV |
|
sigma(gg->h1)*Br(h1->ZA) |
52.32*0.3063 [pb] |
Br(A->mumu) |
0.003348 |
Br(A->tautau) |
0.7813 |
Br(A->bb) |
0 |
BP4_D |
Main Features |
Type II 2HDM, Decay of SM Higgses into Z boson and light A=25 GeV |
Spectrum/input parameters(A) |
mh (SM-like) = 126.27 GeV, mH=227.08 GeV, mA=24.71GeV, mHpm=226.80 GeV, SBA=0.99, TB=1.76, m12=58.37 GeV |
|
sigma(gg->h1)*Br(h1->ZA) |
52.46*0.1526 [pb] |
Br(A->mumu) |
0.000224 |
Br(A->tautau) |
0.0627 |
Br(A->bb) |
0.9175 |
BP4_E |
Main Features |
Type II 2HDM, Decay of SM Higgses into Z boson and light A=63 GeV |
Spectrum/input parameters(A) |
mh (SM-like) = 125.19 GeV, mH=210.20 GeV, mA=63.06 GeV, mHpm=333.50 GeV, SBA=0.78, TB=2.38, m12=69.22 GeV |
|
sigma(gg->h1)*Br(h1->ZA) |
53.46*0.03818 [pb] |
Br(A->mumu) |
0.000265 |
Br(A->tautau) |
0.0747 |
Br(A->bb) |
0.9191 |
BP5 |
Main Features |
IDM, Two Higgs doublet model with dark matter candidate (labelled H) |
Benchmark planes |
Floating parameters |
masses of scalars mH,mA, mH+ |
|
mH > 50 GeV, mass degeneracy (see plots) |
Fixed parameters |
mh=125 GeV |
Irrelevant parameters |
lambda2; lambda345 (if kept within allowed ranges, ~ [0.02;0.02]) |
BR (A -> ZH) |
1 |
BR (H+ -> W+ H) |
dominant |
comment |
only pair-production of H,A,H+ possible |
|
signature: always missing ET from HH in final states |
|
Z,W decay as in SM |
|
production and decay modes determined by SM gauge couplings and kinematics |
|
for mH< mh/2: lam345 becomes important; parameter space extremely constrained |
BP5_A |
Main Features |
Low mass H [mH < mh/2] |
Spectrum/input parameters |
mh (SM-like) = 125.1 GeV, mH=57.5 GeV, mA=113.0 GeV, mH+=123.0 GeV, abs(lambda345) in [0.002,0.015] |
sigma(pp->HA) |
0.371(4) [pb] |
sigma(pp->H+H-) |
0.097(1) [pb] |
Br(H+->W+H) |
>0.99 |
Br(H+->W+A) |
<0.01 |
BP5_B |
Main Features |
Low mass H [mh/2 < mH < mh] |
Spectrum/input parameters |
mh (SM-like) = 125.1 GeV, mH=85.5 GeV, mA=111.0 GeV, mH+=140.0 GeV, abs(lambda345) < 0.015 |
sigma(pp->HA) |
0.226(2) [pb] |
sigma(pp->H+H-) |
0.0605(9) [pb] |
Br(H+->W+H) |
~0.96 |
Br(H+->W+A) |
~0.04 |
BP5_C |
Main Features |
Intermediate mass H [mH ~ mh] |
Spectrum/input parameters |
mh (SM-like) = 125.1 GeV, mH=128.0 GeV, mA=134.0 GeV, mH+=176.0 GeV, abs(lambda345) < 0.05 |
sigma(pp->HA) |
0.0765(7) [pb] |
sigma(pp->H+H-) |
0.0259(3) [pb] |
Br(H+->W+H) |
~0.66 |
Br(H+->W+A) |
~0.34 |
BP5_D |
Main Features |
High mass H [mH>mh]; degeneracy |
Spectrum/input parameters |
mh (SM-like) = 125.1 GeV, mH=363.0 GeV, mA=374.0 GeV, mH+=374.0 GeV, abs(lambda345) <0.25] |
sigma(pp->HA) |
0.00122(1) [pb] |
sigma(pp->H+H-) |
0.00124(1) [pb] |
Br(H+->W+H) |
1.0 |
BP5_E |
Main Features |
High mass H [mH>mh] |
Spectrum/input parameters |
mh (SM-like) = 125.1 GeV, mH=311.0 GeV, mA=415.0 GeV, mHpm=447.0 GeV, abs(lambda345) <0.19 |
sigma(pp->HA) |
0.00129(1) [pb] |
sigma(pp->H+H-) |
0.000553(7) [pb] |
Br(H+->W+H) |
>0.99 |
Br(H+->W+A) |
<0.01 |
production cross sections produced using Madgraph5 with a manually inserted ggh vertex in the EFT description [UFO model from
BP6 |
Main Features |
Fermiophobic heavy Higgs |
Reference point |
Spectrum/input parameters |
mh0 (SM-like) = 125 GeV, MHH=200 GeV, MA0=500 GeV, MHp=500 GeV, SA = 0, TB=20, m12=2000 GeV |
Leading Signatures/Rates |
|
sigma(pp->HA)*Br(H->VV) |
sigma(HA) = 1.91 fb |
sigma(pp->Hpm H)*Br(H->VV) |
sigma(Hpm H) = 0.88 fb |
GammaH |
3.39 E-03 GeV |
Br(H -> ZZ) |
0.742 |
Br(H -> WW) |
0.258 |
Br(H -> gaga) |
< 10^{-4} |
Br(H -> ga Z) |
< 10^{-4} |
Br(H -> ff) |
0 |
comment |
Sharp resonance into WW/ZZ |
|
Relatively light, yet very elusive Higgs companion |
|
Warning sign: lack of signal should not rule out the model too early |
Benchmark planes |
Floating parameters |
CP--even heavy Higgs mass [MHH], Mass splitting [DeltaM] |
Fixed parameters |
Neutral Higgs mixing SA=0 (by construction) |
|
CP--odd Higgs mass MA0 = MHH + DeltaM |
|
Charged Higgs mass MHp = MA0 + DeltaM |
|
Z2 Soft-breaking mass $m_{12}^2 = MHH^2/Tan[b] |
Fiducial TB choices |
(by increasing departure from alignment) |
|
TB=40 (small departure) |
|
TB=20 (moderate departure) |
|
TB=10 (large departure) |
comment |
fermiophobic.pdf: Detailed description of parameter plane. |