Probing Higgs in Type III Seesaw at the Large Hadron Collider

Transcription

1 Probing Higgs in Type III Seesaw at the Large Hadron Collider Priyotosh Bandyopadhyay Korea Institute for Advanced Study, Seoul The 1st KIAS Phenomenology Workshop, KIAS, Seoul, South Korea Work done with Prof. Eung Jin Chun, Prof. Suyong Choi arxiv:1111.xxxx [hep-ph] November 19, 2011

2 Plan 1 Neutrino Mass 2 Seesaw Mechanism 3 Type III Seesaw 4 Triplet fermions and Decay modes 5 Phenomenology at the LHC 2b + 3l 2b + SSD 6 Conclusion

3 Neutrino Mass Dirac & Majorana If neutrinos are of only Dirac type Possible mass term is y ν LHν

4 Neutrino Mass Dirac & Majorana If neutrinos are of only Dirac type Possible mass term is y ν LHν How do you have small ν mass O(0.1) ev) By having y ν O(10 12 ) unnatural

5 Neutrino Mass Dirac & Majorana If neutrinos are of only Dirac type Possible mass term is y ν LHν How do you have small ν mass O(0.1) ev) By having y ν O(10 12 ) unnatural Is there other way to get small neutrino mass? If neutrinos are Majorana!

6 Majorana Neutrino 1 ν c = ν, self-conjugate under the charge conjugation. 2 We can have a mass term L = 1 2 m L(ψ L ) c ψ L m R(ψ R ) c ψ R + h.c 3 This kind of mass can be naturally generated by Seesaw Mechanism.

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8 Seesaw Mechanism Seesaw mechanism is one where the smallness of neutrino mass is explained by a large scale. There are different versions of this seesaw mechanism but have a basic structure: M ν < v >2 M seesaw MeV2 TeV ev Introduces two scales: very high scale and a moderate scale to get the very small scale.

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10 Type III Seesaw Mechanism SU(2) L triplet fermions with Y = 0, Σ = (Σ +,Σ 0,Σ ). The matrix form of the triplet; ( ) Σ 0 2Σ + Σ = 2Σ Σ 0 where Σ + is the antiparticle state of Σ : Σ + (Σ ) c. Then the gauge invariant Yukawa terms are L = [ y i Hε ΣP L l i + h.c. ] Tr [ ΣΣ ] where l i is the lepton doublet and H is the Higgs doublet: l = (ν i,e i ) L and H = (H +,H 0 ).

11 Neutrino mass and mixing The neutrinos get a seesaw mass m ν,ij y i y j v 2 /M which becomes O 0.1 ev for y i 10 6 and M 1 TeV. The neutrino Dirac mass, y i v, induces mixing between l and Σ. The mixing angles for the neutral and charged part are respectively. θ νi y iv M and θ l i 2 y iv M

12 Gauge interaction Due to the l Σ mixing, we get the mixed gauge interaction as follows; [ ] 1 L mixed = gθ νi W µ + 2 Σ0 γ µ P L e i + ν i γ µ R R Σ [ ] 1 gθ νi Wµ 2 ē i γ µ P L Σ 0 + Σ γ µ P R ν i + gθ ν i 2c W Z µ [ 2 Σ γ µ P L e i + 2ē i γ µ P L Σ Σ 0 γ µ γ 5 ν i ]

13 Phenomenology Thus, we have the electroweak production of the triplets at the LHC, pp Σ ± Σ 0, Σ ± Σ The triplet decays as follows: Σ ± l ± h l ± Z 0 νw ± Σ 0 π ± Σ 0 νh νz 0 l ± W We can see the final states with multi-leptons could be interesting. 1 1 Aguila08

14 Cross-section of the triplet 14 TeV LHC Cross-section is very low for higher triplet mass 2. 2 Hambye et al. 08, Aguila et al. 08

15 Decay branching of the triplet fermions Σ - -> H l Σ - -> Z l Σ - -> W - ν Σ - -> π - Σ 0, Σ 0 -> H ν Σ 0 -> Z Σ Σ 0 -> W + l m ~ ν =10 mev 0.5 f π =130 MeV 0.6 Branching fraction m ~ ν =10 mev Branching fraction /- m Σ M Γ in GeV

16 Decay widths of the triplet fermions 1.4e-11 Γ(Σ 0 ) Γ(Σ +/- ) 1.2e-11 1e-11 Decay widths in GeV 8e-12 6e-12 m ~ ν =10 mev 4e-12 2e m Σ in GeV

17 Plan Neutrino Mass Seesaw Mechanisms Triplet fermion Collider Phenomenology Decay length of the triplet fermions mν in mev M in GeV

18 Benchmark Points for the collider simulation For the collider simulation we took m Σ = 250,400 GeV and m = 10 mev as benchmark points Production cross-sections (fb) m Σ 250 GeV 400 GeV Σ + Σ Σ + Σ Σ Σ Table: Production cross-sections for the benchmark points.

19 Decay branching fraction for the Benchmark Points Decay modes Branching fractions m Σ 250 GeV 400 GeV Σ 0 hν Σ 0 Zν Σ 0 W ± l Σ ± hl ± Σ ± Zl ± Σ ± W ± ν Σ ± Σ 0 π ± Table: Branching fractions for the triplets with m ν = 10 mev.

20 Final state topologies for collider simulation Dominant decay modes are final states with Higgs and/or Gauge bosons associated with leptons. Higgs searches with multi-lepton final state could be interesting. We analyse all plausible leptonic final states. Here we discuss only 2b + 3l and 2b + SSD at the LHC at 14 TeV.

21 Collider simulation We generate the events with MadGraph Generated events thus interfaced with PYTHIA via LHEF Hadronization, ISR/FSR effects and Jet formation (PYCELL) are done inside PYTHIA CTEQ6L is used parton distribution function (PDF) The renormalization/factorization scale is set at ŝ.

22 Status of 2b + Typically hlzl,hlwl,zlzl,zlwl dominantly contribute to the final state. In particular final state with Higgs, i.e., hlzl,hlwl are interesting. b pair can come from h and Z Strategically we try to construct 2b + 3l final state Invariant mass of b-jet pair could give the Higgs peak we are interested in Invariant mass of b b l where b-jets are from the Z and h window can give rise to Σ mass peak.

23 Status of 2b + With the ISR/FSR, jet formation and b mis-tagging other decay modes also could contribute. We define the signal by following cuts: p jet T,min = 20 GeV and jets are ordered in p T leptons (l = e, µ) are selected with p T 20 GeV and η 2.5 no jet should match with a hard lepton in the event ( R j,l 0.4, R l,l 0.2) Considering the b and lepton final state the main SM backgrounds are: t t, t tz, t tw,t th, t tb b, WW, ZZ, WZ

24 2b+ 3l The numbers for the signal and the background for the final topology 2b+ 3l Signal 2b jet + 3l Backgrounds BP1 BP2 t t t tb b t tz t th VV t tw The dominant background is t tz as expected

25 Higgs peak in 2b + 3l final state 12 Total Background Total Background 10 4 BP2, m Σ =400 GeV Number of events BP1, m Σ =250 GeV Number of events m b-b-jets in GeV m b-b-jets in GeV Figure: Invariant mass distributions of b-jet pair from 2b+ 3l final states for BP1, BP2 and SM background.

26 Higgs peak in 2b + 3l final state The number of events in the window 95GeV m b b 145GeV 95GeV m b b 145GeV Signal Backgrounds BP1 BP2 t t t tb b t tz t th VV t tw

27 Sigma peak in 2b + 3l final state Total Background Total Background BP2, m Σ =400 GeV Number of events BP1, m Σ =250 GeV Number of events m b-b-l in GeV m b-b-l in GeV Figure: Invariant mass distributions of b-jet pair plus a charge lepton from 2b + 3l final state for BP1, BP2 and SM background.

28 Sigma peak in 2b + 3l final state The number of events in the window m b b l within 250(400) ± 50 GeV. m b b l Signal Backgrounds t t t tb b t tz t th VV t tw BP BP

29 Results for 2b + 3l final state For 2b+ 3l at 10 fb 1 integrated luminosity the reach for BP1 is 9σ, where as for BP2 4σ Higgs peak reconstructed with m bb a 5σ signal significance for BP1 will require 13 fb 1 integrated luminosity and for BP2, couple of 100 fb 1. m bbl at 10 fb 1 integrated luminosity the reach for BP1 is 7σ Thus the significance drops very fast as we increase the triplet mass. Harder lepton p T cuts and lepton invariant mass veto cut near Z peak will reduce the background further.

30 Status of 2b+ Same-sign di-lepton 2b jet + SSD Signal Backgrounds BP1 BP2 t t t tb b t tz t th VV t tw

31 Status of 2b+ Same-sign di-lepton 25 BP1, m Σ =250 GeV Total Background Total Background 20 Number of events Number of events BP2, m Σ =400 GeV m b-b-jets in GeV m b-b-jets in GeV Figure: Invariant mass for b-jet pair from 2b + SSD final state for BP1, BP2 and SM backgrounds.

32 2b+ Same-sign di-lepton 95GeV m b b 145GeV Signal Backgrounds BP1 BP2 t t t tb b t tz t th VV t tw

33 Status of 2b+ Same-sign di-lepton 25 Total Background 2.5 Total Background Number of events BP1, m Σ =250 GeV Number of events BP2, m Σ =400 GeV m b-b-l in GeV m b-b-l in GeV Figure: Invariant mass for b-jet pair plus a charged lepton from 2b + SSD final state for BP1, BP2 and SM backgrounds.

34 2b+ Same-sign di-lepton m b b l Signal Backgrounds t t t tb b t tz t th VV t tw BP BP

35 Result for 2b+ Same-sign di-lepton For 2b + SSD at 10 fb 1 integrated luminosity the reach for BP1 is 8σ, where as for BP2 2σ Higgs peak reconstructed with m bb have a significance of 6σ for BP1 at 10 fb 1 integrated luminosity and for BP2 it is 1.5σ. m bbl at 10 fb 1 integrated luminosity the reach is 10σ for BP1, and 3σ for BP2. Thus the significance drops very fast as we increase the triplet mass. Harder lepton p T cuts and lepton invariant mass veto cut near Z peak will reduce the background further.

36 Conclusions Higgs searches from triplet fermions decay could be interesting at the LHC For low seesaw scale the reach could be possible at early data of LHC For higher seesaw mass scale as the production cross-section drops down the reach is possible only at higher luminosity. Triplet decay to relatively harder leptons is a good handle to kill the standard model backgrounds. In particular multi-lepton scenarios are good for mass measurements; Higgs and the triplet fermions. 4l, 5l scenarios are also possible but cross-sections are very small.

37 Thank you