yeo woong yoon (konkuk univ.) 2015/6/2, 16 th lhc meeting @ kias based on 1505.00291 in...
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HEAVY HIGGS RESO-NANCE DIP PART I- FORMALISM
Yeo Woong Yoon (Konkuk Univ.)
2015/6/2, 16th LHC meeting @ KIAS
Based on 1505.00291
In collaboration with
Jeonghyeon Song(Konkuk Univ.), Sunghoon Jung (KIAS)
2
INTERLUDE - RESONANCE
๐๏ฟฝฬ๏ฟฝ= 12๐ |โณ๐๐๐๐|
2| 1
๐2โ๐ 2+๐๐ ฮ |2
|โณ๐๐๐|2๐๐๐ถ๐ท
| 1
๐2โ๐ 2+๐๐ ฮ |2
โ ๐๐ ฮ
๐ฟ(๐2โ๐ 2)
Using the Narrow Width Approximation (NWA)
: The area is
Production โข BW2 โข Decay
๐ ( ๐ด๐ตโฮฆโ๐ถ๐ท )=๐๐๐๐๐ โ Br
ฮฆ
๐ต
๐ด ๐ถ
๐ท
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E598, PRL (1974), SLAC, PRL (1974)
Very excited moment in particle physics was when we discover a resonance peak for a new particle
h0
๐ฝ /ฮจ( ฮ๐=3. 0ร10โ 5)
( ฮ๐=3.4ร10โ5)
ATLAS, PLB (2012), CMS, PLB (2012)
What if th
e interference
effect is stro
ng?
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HEAVY HIGGS SEARCH STRATEGY
2๐๐ก
and are promising
dominant region
Small tanbeta region Higgs Production rate is huge Largely con-strained by and ๐๐
Allmost 100% decay into for small tanbeta. reso-nance search is available from 500 GeV. Small tanbeta region is constrained by search.
Large tanbeta region Bottom and lepton Yukawa couplings are much in-hanced. Constrained by . ๐๐
Desert region. Currently, no experimental search for this region is avail-able.
Perturbaive is broken
Interference effect is important
Sizable decay width
For aligned 2HDM
Interference, one of the most striking phenomena in Quantum Mechanics..
ELECTRON GUN
Roger Bach et al, New Journal of Physics (2013)
1 2
5
At the LHC
CONTINUUM RESONANCE
Invariant Mass Distribution
DipNothingPeakPeak-Dip
?
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GENERAL FORMALISM FOR THE INTERFERENCE EFFECT
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CONTINUUM RESONANCE
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BW-Res. Imaginary-partInterference
Real-partInterference
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Interference effectively change
WHAT DOES IT AFFECT PHENOMENOLOGY?
Mainly..
1. Resonance shape changes
2. NWA should be modified
Also we need to consider following subtleties.
โข Kinematic distribution of final state may be changedโข Smearing effect might be significant
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1. RESONANCE SHAPE
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Real-Part Interference ()
1. RESONANCE SHAPE
We meet this case for the 125GeV SM Higgs production with diphoton decay channel
No complex phase in the resonance signalComplex phase in continuum affect beginning at 2loop
Dixon, Siu (2003) PRL
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1. RESONANCE SHAPE
After Gaussian smearing
Real-part Interference is pure odd function:
Interference only S. Martin (2012) PRD
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1. RESONANCE SHAPE
S. Martin (2012) PRD
* The Interference effect is quite small mainly due to the smalldecay width ().
Res. signal onlyRes. signal + Interference
Slight shift (150 MeV)of mass peak
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1. RESONANCE SHAPEImaginary-Part Interference ()
โPure Dipโ
BW-shape is preserved
(1+ 2๐ค๐
๐ ๐)<0
Pure Dip prefers sizable width and small R value (small signal to bg ratio).
๐=โ90โ ,๐ค๐
=0.7
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1. RESONANCE SHAPEImaginary-Part Interference ()
BW-shape is preserved
(1+ 2๐ค๐
๐ ๐)=0
โNothing-nessโ
๐=โ90โ ,๐ค๐
=0.5
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1. RESONANCE SHAPEImaginary-Part Interference ()
BW-shape is preserved
(1+ 2๐ค๐
๐ ๐)>0
๐=๐2,
โPure Peakโ
๐=โ๐2,๐ค๐
<0.5
: enhanced
: suppressed
๐=90โ ,๐ค๐
=0.4
๐=โ90โ ,๐ค๐
=0.4
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2. MODIFIED NWA
Transient Estimated by NWA
๐ถ=(1+ 2๐ค๐
๐ ๐)
We propose modified NWA as
๐ โ Br โ๐ถ
Correction factor, and simple measure of resonance shape
Cross section for production and decays :
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PREVIOUS DISCUSSIONS ON
INTERFERENCE EFFECT1. Photon collider study
Asakawa, Kamoshita, Sugamoto, Watanabe (2000) EPJC
Dixon, Sofianatos (2009) PRD
Niezurawski, Zarnecki, Krawczyk (2002) JHEP
Morris, Truong, Zappala (1994) PLB
Continuum bg is tree-level, Res. signal is loop level, so R is naturally loop suppressed. Dips can arise
Morris, Truong, Zappala (1994) PLB
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PREVIOUS DISCUSSIONS ON
INTERFERENCE EFFECT2. Hadron collider study
Dicus, Willenbrock, (1988) PRD
Glover, Bij (1989) NPB, Kauer, Brien 1502.04113
Campbell, Ellis, Williams (2011) JHEP
Both Res. signal and continuum are loop processes. R is order 1 (quite big) Small Im-part Interference Mostly peak (excess)
Campbell, Ellis, Williams (2011) JHEP
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๐๐โ๐ด /๐ปโ๐พ๐พ
Sizable C factor. Mostly peak shape
Nothingness
Pure Peak
Pure PeakFor aligned 2HDM
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SUMMARYVery simple and powerful parametrization for the in-
terference effect and resonance shape.
Heavy Higgs search with must be a Dip (or deficit) search.
Even nothingness can happen in which Higgs can hide.
Modified NWA: The correction factor must be included for the interference effect.
Detailed resonance shape analyses of ,, Z, , - working in progress
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