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Search for the Standard Model Higgs Boson produced in Association - - PowerPoint PPT Presentation

Search for the Standard Model Higgs Boson produced in Association With a W boson Adrian Buzatu, PhD Candidate McGill University, Montreal, Canada Collider Detector At Fermilab The Missing Ingredient Mass represented by surface The origin


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Search for the Standard Model Higgs Boson produced in Association With a W boson

Adrian Buzatu, PhD Candidate

McGill University, Montreal, Canada Collider Detector At Fermilab

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The Missing Ingredient

2 Adrian Buzatu 31 May 11 Mass represented by surface

The origin of mass for elementary particles? Suspect an extra recipe: the Higgs mechanism Suspect an extra elementary particle: the Higgs boson

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Collider Detector at Fermilab

Central Cal Plug Cal Central Tracker Silicon Tracker Muon Detectors

3 Adrian Buzatu 31 May 11

A particle detector (3D digital camera) As big as a huge room Layers of subdetectors Measuring particle type, direction of movement, energy and momentum

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As Heavy as Heavy Atoms!

Adrian Buzatu 31 May 11 4

Higgs boson is characterized only by its mass, However, its mass is not predicted by the theory! Allowed mass interval

In atomic mass units: 123 – 199, in GeV/c^2: 115 – 185!

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The WH Associated Production

5 Adrian Buzatu 31 May 11 Colliding particles Virtual particles Decay products in detector Higgs Particle (H) Elementary particle as massive as heavy atoms

Our search (WH) Our search: a W boson + a Higgs boson The W boson decays to an electron (muon) + neutrino It helps us a lot that we can indentify well electrons and muons in the detector

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Our Improvement

Adrian Buzatu 31 May 11 6

Charged lepton (Electron or Muon) Our contribution to improve the search: More charged leptons, which means More W bosons, which means More WH events, which means More signal selected, which means More precise “microscope”! We introduce a new method to reconstruct electrons and muons that would normally be lost in the non instrumented regions of the detector

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Charged Lepton Improvement

Adrian Buzatu 31 May 11 7

Dark blue, Green – muons Light blue – electrons Red – muons or electrons that would be lost in the non instrumented regions of the detector, but we recover Cylindrical detector rolled

  • n a plane

Y axis: 0-2Pi X axis – 0 for half height

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3 MET + jets triggers

Adrian Buzatu 31 May 11 8

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Trigger specific jet selection

Adrian Buzatu 31 May 11 9

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Novel method to combine triggers

Adrian Buzatu 31 May 11 10

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Our analysis: 3 triggers

Adrian Buzatu 31 May 11 11

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WH115 Signal Yield

Adrian Buzatu 31 May 11 12

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Signal Percentage Increase

Adrian Buzatu 31 May 11 13

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Different Trigger Combination

Adrian Buzatu 31 May 11 14

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Key Analyses Variables

Adrian Buzatu 31 May 11 15

Mass of hypothetical particle decaying to two bottom quarks Output of trained artificial neural network with background peaking at 0 and signal at 1 Red: WH Signal multiplied by 5 times!

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Our Result

Adrian Buzatu 31 May 11 16

Dotted line: how precise our “microscope” is Solid line: what we actually measure with our “microscope” Name of the game: drive the solid line below 1 to exclude the Higgs boson! Black: the WH analysis before my contribution Red: with the addition of my

  • riginal PhD contribution, the

WH analysis improves both the precision of the “microscope” and the actual measurement Y axis: Measurement divided by theory prediction

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Our numeric result

Adrian Buzatu 31 May 11 17

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Tevatron Combination July 10

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Tevatron High Mass March 11

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Latest Allowed Values

Adrian Buzatu 31 May 11 20

Higgs boson is characterized only by its mass, However, its mass is not predicted by the theory! Allowed mass interval

In atomic mass units: 123 – 170 and 186 -199, in GeV/c^2: 115 – 158 and 173 - 185!

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Conclusions

  • Experimental search for the existence of the Higgs boson
  • Tevatron accelerator
  • CDF detector
  • W boson + Higgs boson search
  • Our contribution: reconstruct more electrons and muons; thus more

W bosons; thus more WH signal; thus a better “microscope”

  • Many analyses from CDF and Dzero at Tevatron combined
  • A large interval in the Higgs boson mass has been excluded in July 10
  • In July 2011 the improved Tevatron combination will be released. Stay

tuned!

Adrian Buzatu 31 May 11 21

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Thank you!

Questions? Comments?

abuzatu@fnal.gov

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Backup slides

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Sensitivity improvement

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With more data, the Tevatron collaborations will improve the sensitivity for Higgs particle search even at low mass

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The Recipe for the Universe

The Universe Ingredients (Elementary Particles) Quarks Electrons Other elementary particles Recipe (Interactions) Electromagnetic Strong Weak Gravitational

The Standard Model

25 Adrian Buzatu 31 May 11 Light, radio, radar Nuclear stability Radioactivity

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How Do Particles Get Mass?

Celebrity crossing the room Then s/he attracts people S/he slows down, has inertia As if s/he acquires mass A rumour comes into the room It still attracts people A group is formed and has inertia As if group acquires mass Normal Particle Higgs Particle

26 Adrian Buzatu 31 May 11