Efficiencies of the BSC Detector at CDF Experiment

Slides:



Advertisements
Similar presentations
We provide 3 slides, not for students, to separate the activities. 1. Rolling for Rutherford Classroom PPT.
Advertisements

ATLAS Experiment at CERN. Why Build ATLAS? Before the LHC there was LEP (large electron positron collider) the experiments at LEP had observed the W and.
Measurement of the Top Quark mass using data from CDF experiment at Tevatron Fedor Prokoshin.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
The new Silicon detector at RunIIb Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96.
A. Bay Beijing October Accelerators We want to study submicroscopic structure of particles. Spatial resolution of a probe ~de Broglie wavelength.
Particle Accelerators and Detectors
MARS flux simulations - update Sergei Striganov Fermilab August 12, 2009.
The Diffractive Structure Function: ξ dependence Christina Mesropian The Rockefeller University.
welcome undergraduate physicists High Energy
Compton Scattering Experiment John Klumpp And Ainsley Niemkiewicz.
Forward Detectors and Measurement of Proton-Antiproton Collision Rates by Zachary Einzig, Mentor Michele Gallinaro INTRODUCTION THE DETECTORS EXPERIMENTAL.
Evidence for high mass exclusive dijet production in the D0 experiment Zdenek Hubacek Czech Technical University in Prague (on behalf of D0 Collaboration)
Measuring the Mass of the Top Quark An Educational Resource from Fermilab, where the top quark was discovered in 1995.
My Chapter 30 Lecture.
Particle Accelerators
Joseph Haley Joseph Haley Overview Review of the Standard Model and the Higgs boson Creating Higgs bosons The discovery of a “Higgs-like” particle.
Chapter 2 Particle accelerators: From basic to applied research Rüdiger Schmidt (CERN) – Version E1.0.
Incoherent pair background processes with full polarizations at the ILC Anthony Hartin JAI, Oxford University Physics, Denys Wilkinson Building, Keble.
Announcements Homework returned now 9/19 Switching to more lecture-style class starting today Good luck on me getting powerpoint lectures ready every day.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
Collider Detector at Fermilab Sung-hyun chang High Energy Physics lab. KNU.
4 th International Workshop on VHMP, Alushta 2 June 2003 Carmine Elvezio Pagliarone A j u m p i n t o t h e F u t u r e !
Working Together Scientific Collaboration or Conspiracy?
April 23, 2008 Workshop on “High energy photon collisions at the LHC 1 Cem Güçlü İstanbul Technical University Physics Department Physics of Ultra-Peripheral.
June 15, 2002David Finley to Aspen PAC Slide 1 Report on 132 nsec Operation Report to the Fermilab.
2011 JINR, DUBNA Student Practice.  Vaclav Kosar Czech Technical University in Prague  Viktor Burian Czech Technical University in Prague  Andra-Georgia.
Feasibility of Detecting Leptoquarks With the CDF Detector Althea Moorhead Mentor: Darin Acosta.
1 On the total charm production cross section in hadronic interactions at high energies √s > 1 TeV Yu.F. Novoseltsev, G.M. Vereshkov Institute for Nuclear.
1 Experience at CERN with luminosity monitoring and calibration, ISR, SPS proton antiproton collider, LEP, and comments for LHC… Werner Herr and Rüdiger.
Searching for New Matter with the D0 Experiment Todd Adams Department of Physics Florida State University September 19, 2004.
Interactions Kihyeon Cho September 6, People have long asked, What is world made of? and What holds it together?
High Energy Accelerators Dennis Silverman Physics and Astronomy U. C. Irvine.
Ivan Vitev & The First Precise Determination of Quark Energy Loss in Nuclei Ivan Vitev (PI), Ming Liu (Co-PI), Patrick McGaughey, Benwei Zhang T-16 and.
accelerator centers worldwide
Particle Physics Particle Physics Chris Parkes April/May 2003  Hydrogen atom Quantum numbers Electron intrinsic spin  Other atoms More electrons! Pauli.
1 Experimental Particle Physics PHYS6011 Fergus Wilson, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2) 3.Collider Experiments.
1 CMS Sensitivity to Quark Contact Interactions with Dijets Selda Esen (Brown) Robert M. Harris (Fermilab) DPF Meeting Nov 1, 2006.
Kinematics of Top Decays in the Dilepton and the Lepton + Jets channels: Probing the Top Mass University of Athens - Physics Department Section of Nuclear.
Energy Loss Simulation for the CDF Run II W Mass Measurement Tom Riddick University College London.
Feasibility study of Higgs pair creation in gamma-gamma collider Hiroshima University Nozomi Maeda 19.April 2009.
Search for a Standard Model Higgs Boson in the Diphoton Final State at the CDF Detector Karen Bland [ ] Department of Physics,
A Precision Measurement of the Mass of the Top Quark Abazov, V. M. et al. (D0 Collaboration). Nature 429, (2004) Presented by: Helen Coyle.
Study of the Differential Luminosity Spectrum Measurement using Bhabha Events in 350GeV WANG Sicheng 王 思丞 Supervisor: André Sailer.
E+/e- Backgrounds at BEPCII/BESIII JIN Dapeng Aug. 22, 2011.
CERN’s Large Hadron Collider
Michael Carrigan Advisors: Kevin Black & Lidia Dell’Asta
Alessandro Bettini Introduction to Elementary Particle Physics
First data from TOTEM experiment at LHC
A.Smirnov, A.Sidorin, D.Krestnikov
Emmanuel Tsesmelis TS/LEA 26 January 2007
Physics Section 6.2 Calculate the momentum of collisions
Trang Hoang Florida State University - Dzero
PARTICLE FLUX CALCULATION-III
Physics: Concepts and Connections, 4th ed
Conservation of Momentum in 1-D and collisions
Other issues and concepts under study Conclusions References
Particle physics.
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 6th May 2009 Fergus Wilson, RAL.
THE GOD PARTICLE 1 Shashwat Mandal & Christian Bach 5
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 28th April 2008 Fergus Wilson. RAL.
Nuclear Reactions.
Experimental Particle Physics PHYS6011 Joel Goldstein, RAL
The Measurement of Forward Particle Production in LHC
Perspectives on Physics and on CMS at Very High Luminosity
PYTHIA 6.2 “Tunes” for Run II
Parton Density Functions
The Top Quark Search Joey Foley.
b-Quark Production at the Tevatron
IR/MDI requirements for the EIC
Presentation transcript:

Efficiencies of the BSC Detector at CDF Experiment Aniel Nieves Dimitri Tsybychev, Darin Acosta

This Presentation will get into… Some insight of what is Particle Physics. Proton-antiproton collisions and important concepts related to that subject. Simulations of proton-antiproton collisions. How we did those simulations. Results.

Particle Physics Particle physics focus on fundamental particles and their interactions. Particle physicists are looking for answers to questions like: Are all the forces a manifestation of a single force? Where does mass come from? or Are there more quarks?

Proton-antiproton Collisions We study proton-antiproton (ppbar) interaction with little bias in the type of ppbar interaction. The rate is measured. The rate and the estimated efficiency are used to calculate the Luminosity (L). The Luminosity is used to obtain cross sections of particular processes. K p p p protons antiprotons K K p

Cross Section Is the effective area a target present to a high energy particle. Measured in barns (1barn = 10-24 cm2). Useful to compare the probability of a type of interaction to occur against another.

Some Basic Equations We measure the rate (R): R = dN / dt = (L )s L is Instantaneous luminosity: L = N / (Dt)s The efficiency is given by: e = Ndet / N The integrated Luminosity (L) is obtained:

Fermilab Beam energy is 1 TeV

The CDF Experiment BSC

Simulations ppbar Collisions Our goal was to estimate the efficiencies. To achieve that, we simulate ppbar interactions and the BSC. The BSC are scintillators

How we did the simulations The simulation is divided in two parts: 1st the simulation of the ppbar collision (Pythia and MBR). 2nd the simulation of particles interacting with the material of the detector (GEANT).

But to give you an idea… Particle coming from interaction point and colliding with the detector.

What is coincidence? A special arrangement of the detectors useful to rule out particles that do not came from IP.

Results

Final Remarks and Conclusion Simulations of ppbar collisions were made to estimate efficiency of detector. This is necessary to obtain other physical information. We obtain results that will be useful for Luminosity calculations at Fermilab, that can also tell us how frequent can be a certain type of interaction. This is not over. There is a lot to do, for example: The CLC