The LAS Trigger. Malte Wilfert. Institut für Kernphysik - Johannes Gutenberg-Universität Mainz. 7. March 2012

Similar documents
Geant4 Electromagnetic Physics for HEP Applications

The MINERνA Experiment

Messy rabbit-hole! TRACK TOP-BOTTOM ASYMMETRY

UK Opportunities in SiD Calorimetry

Yoke Instrumentation: ILD Muon System / Tail Catcher. Valeri Saveliev IAM, RAS, Russia DESY, Germany 3 June, 2016

Scan of Recent high MET events

TPC Report. D. Karlen T2K ND280m meeting December 7, 2004 Rome

PHENIX RPC in China. Xiaomei LI. Science and Technology on Nuclear Data Laboratory China Institute of Atomic Energy

The Transition Radiation Detector of the AMS-02 Experiment

4-3 Rate of Change and Slope. Warm Up. 1. Find the x- and y-intercepts of 2x 5y = 20. Describe the correlation shown by the scatter plot. 2.

arxiv: v1 [physics.ins-det] 16 Aug 2014

Navigate to the golf data folder and make it your working directory. Load the data by typing

Analysis of RPC Performance with Different Gas Mixture

DRAFT SANE Gas Cherenkov General Operation and Safety Manual

Monitored Drift Tubes in ATLAS. Michele LIVAN 1. Dipartimento di Fisica Nucleare e Teorica, Universita di Pavia

TI 176B Flow Rate Audit Calculations

Design and Construction of a GEM-TPC Prototype for R&D Purposes

GIF++ A New Gamma Irradiation Facility

Analysis of Car-Pedestrian Impact Scenarios for the Evaluation of a Pedestrian Sensor System Based on the Accident Data from Sweden

STANDARD SCORES AND THE NORMAL DISTRIBUTION

KINEMATIC ANALYSIS OF SHOT PUT IN ELITE ATHLETES A CASE STUDY

4-3 Rate of Change and Slope. Warm Up Lesson Presentation. Lesson Quiz

Guideline for RMO Key comparison for Air kerma rate in 60 Co gamma radiation

Slide 1 / The distance traveled by a wave in one period is called? Frequency Period Speed of wave Wavelength Amplitude

Waves Multiple Choice

Status of MDT Production and Testing

New experimental techniques: recent developments in particle detectors

Chamber Calibration Data

Gas Leak Measurement of TRT Barrel Module

PSY201: Chapter 5: The Normal Curve and Standard Scores

Section 2C Formulas with Dividing Decimals

Outline Chapter 7 Waves

Status of SuperKEKB Control System. April 25, 2012 Tatsuro NAKAMURA KEKB Control Group, KEK

THE development of more advanced techniques in radiotherapy,

The Changing Hitting Performance Profile In the Major League, September 2007 MIDDLEBURY COLLEGE ECONOMICS DISCUSSION PAPER NO.

Diaphragm pop-pop engine

Today: waves. Exam Results. Wave Motion. What is moving? Motion of a piece of the rope. Energy transport

7.4 Temperature, Salinity and Currents in Jamaica Bay

Engineering Fundamentals final project: Jerry Built

Development of a 1-MW Target and Beam Monitor for NuMI

Performance of a triple-gem detector for high rate charged particle triggering

Implementation of the Different Detector Concepts in Mokka Simulation Framework

THE BALLISTIC PENDULUM

Assembly and measurements of a mechanical prototype of the BIS MDT chamber

HMS/SHMS Drift Chambers Calibration. Carlos Yero June 26, 2017

8th Grade. Data.

Related Rates - Classwork

2019 State Competition Sprint Round Problems 1 30

Lab 12 Standing Waves

Ground Forces Impact on Release of Rotational Shot Put Technique

Outline Physical Basis Aerosol Products Validation Algorithm Improvements. AEROCOM Meeting CNES, Paris, June 2-3, 2003

UAB MATH-BY-MAIL CONTEST, 2004

Variation of Nordic Classic Ski Characteristics from Norwegian national team athletes

Lesson 16: More on Modeling Relationships with a Line

Nortek Technical Note No.: TN-021. Chesapeake Bay AWAC Evaluation

MASSIVE TITANIUM SUBLIMATION PUMPING IN THE CESR INTERACTION REGION *

Massey Method. Introduction. The Process

CVEN Computer Applications in Engineering and Construction. Programming Assignment #4 Analysis of Wave Data Using Root-Finding Methods

Workshop 1: Bubbly Flow in a Rectangular Bubble Column. Multiphase Flow Modeling In ANSYS CFX Release ANSYS, Inc. WS1-1 Release 14.

Gilson Aqua-Check Moisture Tester MA-26X

Gears Ratios and Speed / Problem Solving

Thomas Lykke Andersen, Morten Kramer, Peter Frigaard November 2003

Measurements of the Cross Section for e 1 e 2! Hadrons at Center-of-Mass Energies from 2 to 5 GeV

SUMMARY AND RESULTS OF THE CRYOPLANT OPERATION FOR HERA

Tex-1001-S, Operating Inertial Profilers and Evaluating Pavement Profiles. Chapter 10 Special Procedures. Overview

Chapter 3 Tex-1001-S, Operating Inertial Profilers and Evaluating Pavement Profiles

Improving the Accuracy and Reliability of ACS Estimates for Non-Standard Geographies Used in Local Decision Making

Grade: 8. Author(s): Hope Phillips

Effects of transglottal pressure on fundamental frequency of phonation: Study with a rubber model

Lesson 14: Modeling Relationships with a Line

CR Series. Special doors for clean room application

Student Population Projections By Residence. School Year 2016/2017 Report Projections 2017/ /27. Prepared by:

PHYS 102 Quiz Problems Chapter 16 : Waves I Dr. M. F. Al-Kuhaili

Long term stability tests of INO RPC prototypes

Quantitative Literacy: Thinking Between the Lines

Dario Barberis Curriculum Vitae

A Study of Spatial Resolution of GEM TPC with Ar-CF 4 -ic 4 H 10 Gas Mixtures

Yasuyuki Hirose 1. Abstract

LINEAR AND ANGULAR KINEMATICS Readings: McGinnis Chapters 2 and 6 DISTANCE, DISPLACEMENT, SPEED, VELOCITY, AND ACCELERATION:

4.1 Why is the Equilibrium Diameter Important?

Lab 7 Rotational Equilibrium - Torques

2011 Canadian Intermediate Mathematics Contest

Lesson 6: The Distance Between Two Rational Numbers

DIFFRACTION 05 MAY 2014

BUBBLE CHAMBERS, TECHNOLOGY AND IMPACT ON HIGH ENERGY PHYSICS Gert G. Harigel

Experimental Procedure

EFFECTS OF OCEAN THERMAL STUCTURE ON FISH FINDING WITH SONAR

Students will use two different methods to determine the densities of a variety of materials and objects.

ANALYSIS OF TURBULENCE STRUCTURE IN THE URBAN BOUNDARY LAYER. Hitoshi Kono and Kae Koyabu University of Hyogo, Japan

[A] 7 4 [B] 7 45 [C] 7 14 [D] [1] p. [3] 4. Solve. 2 x = 8 [B] 1 3

Air Ball! LabQuest Vernier Gas Pressure Sensor Vernier Motion Detector basketball stopper with needle, stopper stem and tubing attached meter stick

FLUKA Simulations of Radiation Field in Second Accelerator Tunnel

Modelling and Simulation of Environmental Disturbances

Re: ENSC 440 Functional Specification for the Wall Climbing Robot. Dear Mr. Leung,

HEIDRUN TLP MODEL TESTS Summary of results (Pictures and figures are partly prepared by Marintek personel)

A Longterm Aging Study of the Honeycomb Drift Tubes of HERA-B Using a Circulated and Purified CF -Gas Mixture

Validation Study of the Lufft Ventus Wind Sensor

TARGET SCORING. WRAS Targets

How to Make, Interpret and Use a Simple Plot

Quadratic Word Problems

Transcription:

The LAS Trigger Malte Wilfert Institut für Kernphysik - Johannes Gutenberg-Universität Mainz 7. March 212 Malte Wilfert (KPH Mainz) LAST 7. March 212 1 / 18

Outline 1 LAS Trigger 2 Observations 3 Multiplicity 4 Summary Malte Wilfert (KPH Mainz) LAST 7. March 212 2 / 18

The LAS Trigger Enlarge the trigger acceptance towards large Q 2 Using target pointing in vertical direction Two new hodoscopes in the LAS with a large distance H1 in front of the RICH H2 behind the Muon Filter Problem: High trigger rate Malte Wilfert (KPH Mainz) LAST 7. March 212 3 / 18

H1 and H2 6 H1 Size: 23 192cm 32 elements Rohacell casing In Front of the RICH H2 Size: 5 42cm 2 parts with 32 elements Aluminium frame Behind the muon filter Malte Wilfert (KPH Mainz) LAST 7. March 212 4 / 18

Runs with inclusive LAST 3 runs on 26. August 211 LAST runs as inclusive trigger No solenoid Runs: 93621 (166 Spills) 93622 (15 Spills) 93625 (89 Spills) Malte Wilfert (KPH Mainz) LAST 7. March 212 5 / 18

Hits on H2 Reconstructed tracks from a primary vertex y [cm] 2 15 1 5-5 -1-15 -2-25 -2-15 -1-5 5 1 15 2 25 x [cm] 3 25 2 15 1 5 LAS triggerbit set Last measured position behind the muon filter Time information in corresponding H2 element Increased number of hits next to the hole Malte Wilfert (KPH Mainz) LAST 7. March 212 6 / 18

Hits on H2 y [cm] y [cm] 2 15 1 5-5 -1-15 -2 2 15 1-1 -15-2 q< -25-2 -15-1 -5 5 1 15 2 25 x [cm] q> 5-5 -25-2 -15-1 -5 5 1 15 2 25 x [cm] 3 25 2 15 1 5 18 16 14 12 1 8 6 4 2 Left peak is caused by neg. particles Right peak is caused by pos. particles Which particles are these? look at the momentum distribution p 5GeV/c Using the RICH for particle identification mainly caused by e ± Malte Wilfert (KPH Mainz) LAST 7. March 212 7 / 18

Hits on H2 12 1 q< Left peak is caused by neg. particles 8 6 4 2 7 6 5 4 3 2 1 5 1 15 2 25 3 35 4 45 p [GeV/c] q> 5 1 15 2 25 3 35 4 45 p [GeV/c] Right peak is caused by pos. particles Which particles are these? look at the momentum distribution p 5GeV/c Using the RICH for particle identification mainly caused by e ± Malte Wilfert (KPH Mainz) LAST 7. March 212 7 / 18

Hits on H2 6 5 4 3 2 q< Left peak is caused by neg. particles Right peak is caused by pos. particles 1 22 2 18 16 14 12 1 8 6 4 2 - π K p e µ bg q> - π K p e µ bg Which particles are these? look at the momentum distribution p 5GeV/c Using the RICH for particle identification mainly caused by e ± Malte Wilfert (KPH Mainz) LAST 7. March 212 7 / 18

Hits on H1 H1 y [cm] 1 5-5 4 35 3 25 2 15 1 5 e ± from H2 are not in H1 Hits on H1 in those events Other particle causes the second hit -1-1 -5 5 1 x [cm] Malte Wilfert (KPH Mainz) LAST 7. March 212 8 / 18

New ECAL1 hole in 212 Change of the hole size of ECAL1 2 new columns on the top and bottom of the hole 4 new rows on the left and right side Could this solve the problem with the e ±? Malte Wilfert (KPH Mainz) LAST 7. March 212 9 / 18

Position of the electrons at ECAL1 and HCAL1 y [cm] y [cm] 25 2 15 1 5-5 -1-15 -2 ECAL -25-25 -2-15 -1-5 5 1 15 2 25 x [cm] 25 2 15 1 5-5 -1-15 -2 HCAL -25-25 -2-15 -1-5 5 1 15 2 25 x [cm] 35 3 25 2 15 1 5 25 2 15 1 5 Old ECAL1 hole (red) e ± could pass the hole in ECAL1 Also pass the hole in HCAL1 New ECAL1 hole (green) Seems to solve the problem e ± now in ECAL1 Reduce the trigger rate Malte Wilfert (KPH Mainz) LAST 7. March 212 1 / 18

Holes at H2 y [cm] 6 4 2 ECAL1 ECAL1n HCAL1 H2 Old ECAL1 and HCAL1 hole slightly larger then H2 hole Hits on the left and right side of H2-2 -4-6 -1-8 -6-4 -2 2 4 6 8 1 x [cm] New ECAL1 hole smaller than H2 hole Reduces the trigger rate Malte Wilfert (KPH Mainz) LAST 7. March 212 11 / 18

Multiplicity Question Is it possible to identify good events by using multiplicities? 2 Samples are needed: Good events LAS triggerbit Primary vertex with incoming and scattered muon Muon track in H1 and H2 Muon has hits in muonwall 1775 Events All events LAS triggerbit 443545 Events (from 2 chunks) Malte Wilfert (KPH Mainz) LAST 7. March 212 12 / 18

Kinematic distribution Kinematic distribution of good events Only high Q 2 and y 1 8 6 4 2-3 1-2 1-1 1 1 xbj 4 1 35 8 3 25 6 2 4 15 1 2 5 1 1 2 1 2 Q2 [GeV ].1.2.3.4.5.6.7.8.9 1 y Malte Wilfert (KPH Mainz) LAST 7. March 212 13 / 18

Hit distribution of the muons H1 y [cm] 1 5 2 18 16 14 12-5 1 8 6 4 2 Hits from good muons on H1 and H2 y [cm] -1 25 2-1 -5 5 1 H2 x [cm] 5 4.5 Hits are mainly on the top and bottom of the holes 15 1 4 3.5 No timing information used 5 3 2.5-5 2-1 1.5-15 1-2.5-25 -25-2 -15-1 -5 5 1 15 2 25 x [cm] Malte Wilfert (KPH Mainz) LAST 7. March 212 14 / 18

Multipicities H1-1 1 µ Sample All events Hit defined by time information on both sides of one element < 5ns t j +t s 2-2 1-3 1-4 1 2 4 6 8 1 12 14 16 18 2 Hits on H1 Good events have higher multipicities No possibility to cut on the multiplicity in H1 as expected Malte Wilfert (KPH Mainz) LAST 7. March 212 15 / 18

Multiplicities H2 1-1 1 µ Sample All events H2Y1 (Jura) Mainly one hit in µ case -2 1 Same dependency in both cases -3 1 1-1 1-2 1-3 1 2 4 6 8 1 Hits on H2Y1 µ Sample All events No possibility to cut on the multiplicity in H2Y1 H2Y2 (Salève) Mainly zero hits Same dependency in both cases No possibility to cut on the multiplicity in H2Y2 2 4 6 8 1 Hits on H2Y2 Malte Wilfert (KPH Mainz) LAST 7. March 212 16 / 18

Statistics Classes of reconstructed events in the sample Has a primary vertex 79.7% Has a scattered muon 2.9% Scattered muon in H1 and H2 7.2 1 3 % Electron / Positron in H2.6% Incoming beam with no primary vertex 14.2% Malte Wilfert (KPH Mainz) LAST 7. March 212 17 / 18

Summary Mainly e ± at the edges of the hole of H2 New ECAL1 hole solves the problem No possibility to identify good events duo to their multiplicity Malte Wilfert (KPH Mainz) LAST 7. March 212 18 / 18

Kinematic distribution II 4 35 3 25 2 15 y distribution with 2 additional hadrons Reduce radiative events 1 5.1.2.3.4.5.6.7.8.9 1 y Malte Wilfert (KPH Mainz) LAST 7. March 212 19 / 18

Correlations between electrons and positrons Anzahl Elektronen 2 1.8 1.6 1.4 1.2 1.8.6.4 3 1 4 35 3 25 2 15 1 Only one electron or positron in H2 No pairs.2 5.2.4.6.8 1 1.2 1.4 1.6 1.8 2 Anzahl Positronen Malte Wilfert (KPH Mainz) LAST 7. March 212 2 / 18

Multiplicity H2 1-1 1-2 1-3 1-4 1-5 1 µ Sample All events Hit defined by time information on both sides of one element < 5ns t j +t s 2 2 4 6 8 1 12 14 16 18 2 Hits on H2 Malte Wilfert (KPH Mainz) LAST 7. March 212 21 / 18