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Summer Students 2013Table of contents: | ||||||||
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StudentsJeff Picard | ||||||||
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> > | ||||||||
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< < | Higgs properties measurement in H → γ γ | |||||||
> > | Higgs properties measurement in H → γ γ | |||||||
After the discovery of a Higgs-like boson around 125 GeV it has become important to measure the properties of the new state. I am determining the expected sensitivity of our measurement of the particle's spin in the LHC run 2 dataset, and how proposed upgrades to CMS will affect the sensitivity. | ||||||||
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Higgs decays using Razor variables | ||||||||
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< < | I will be analyzing H → WW → llνν decays using razor variables for a high mass Higgs. This will then be extended to a boosted di-Higgs analysis in which each Higgs decays to a WW pair. Here the first WW undergoes a leptonic decay while the second WW pair (from the other Higgs) undergoes a fully hadronic decay producing merged jets. | |||||||
> > | I will be analyzing H → WW → llνν decays using razor variables for a high mass Higgs. This will then be extended to a boosted di-Higgs analysis in which each Higgs decays to a WW pair. Here the first WW undergoes a leptonic decay while the second WW pair (from the other Higgs) undergoes a fully hadronic decay producing merged jets. | |||||||
Natalie Harrison | ||||||||
Added: | ||||||||
> > | ||||||||
Dark matter production with the CMS detector at CERN | ||||||||
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High energy particle colliders, like the LHC, are one of three ways proposed to detect dark matter. Dark matter is theorized to be a natural candidate for the lightest supersymmetric particle and is proposed to be a decay product in an event where SUSY sparticles are pair produced and decay into standard model quarks, which are detected in the collider and a neutralino that escapes detection (proposed DM). The other two methods are direct detection, in which we expect dark matter scattering off a nuclei, and indirect detection, in which dark matter annihilates and remnants of this annihilation are studied. Previous collider searches have been done for dark matter produced in association with a single photon or jet. My work looks specifically for events where dark matter particles are produced in association with at least two jets and leave behind a signature of large missing transverse energy (ET) in the detector. Because of the large amount of missing ET, we can utilize the razor variables MR and R2, developed initially for SuperSymmetry searches . My aim is to improve upper limits on the DM production cross section and translate these into the cross section of DM-nucleon interaction to compare with results from direct detection experiments. I also hope to analyze the results for various different theoretical models.
Ian Wessen | ||||||||
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> > | ||||||||
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< < | Higgs physics through two decay channels, H → γ γ and H → WW | |||||||
> > | Higgs physics through two decay channels, H → γ γ and H → WW | |||||||
Changed: | ||||||||
< < | H → γ γ : Superior resolution of ECAL and the clean kinematics of photon final states enable kinematic reconstruction of parent particles with great accuracy. I want to parametrize a fitting function against Monte Carlo Standard Model background processes and then compare this to the data from the photon photon final state. The pulls on the fit parameters suggest how well our standard model and the data from CMS agree. | |||||||
> > | H → γ γ : Superior resolution of ECAL and the clean kinematics of photon final states enable kinematic reconstruction of parent particles with great accuracy. I want to parametrize a fitting function against Monte Carlo Standard Model background processes and then compare this to the data from the photon photon final state. The pulls on the fit parameters suggest how well our standard model and the data from CMS agree. | |||||||
Changed: | ||||||||
< < | H → WW : The decay to two W contains a lot of kinematic information, but there are many challenges is distinguishing our signal from background. Background sources of missing energy and dilepton final states require a series of discriminating cuts. My analysis focuses on vector boson fusion Higgs production with a characteristic 2-jet final state. By carefully choosing events with these signatures, we can then apply kinematic analysis à la razor techniques to learn about the Higgs. | |||||||
> > | H → WW : The decay to two W contains a lot of kinematic information, but there are many challenges is distinguishing our signal from background. Background sources of missing energy and dilepton final states require a series of discriminating cuts. My analysis focuses on vector boson fusion Higgs production with a characteristic 2-jet final state. By carefully choosing events with these signatures, we can then apply kinematic analysis à la razor techniques to learn about the Higgs. | |||||||
Da An | ||||||||
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> > | ||||||||
Future analysis for CMS Phase II Upgrade | ||||||||
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Future analysis for CMS Phase II Upgrade | ||||||||
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< < | My project is focused on the possible measurement of the trilinear Higgs self-coupling at 14 TeV. This will be done through an analysis of diHiggs production. I will be looking at the potential of analyzing the HH -> bbgammagamma decay channel in order to determine a significant value for the self-coupling. | |||||||
> > | My project is focused on the possible measurement of the trilinear Higgs self-coupling at 14 TeV. This will be done through an analysis of diHiggs production. I will be looking at the potential of analyzing the HH -> bbgammagamma decay channel in order to determine a significant value for the self-coupling. | |||||||
Valère Lambert | ||||||||
Added: | ||||||||
> > | ||||||||
Changed: | ||||||||
< < | HH → bbγγ decay | |||||||
> > | HH → bbγγ decay | |||||||
Changed: | ||||||||
< < | With the upgrade of the CMS detector in 2020 to a luminosity of 14 TeV there will be the potential to measure the self-coupling constant of the Higgs boson, which has applications to measuring the Higgs potential. In order to better understand the significance of various backgrounds for di-Higgs events we will characterize the potential background channels for the HH → bbγγ decay. My three areas of interest will be events containing two fake photons produced with two real bottom jets, two mistagged charm jets, or two mistagged light jets. By determining the efficiency rates for these various faking events and normalizing by their cross sections, we may weight events in these background channels and produce the expected distributions and number of events for each channel. | |||||||
> > | With the upgrade of the CMS detector in 2020 to a luminosity of 14 TeV there will be the potential to measure the self-coupling constant of the Higgs boson, which has applications to measuring the Higgs potential. In order to better understand the significance of various backgrounds for di-Higgs events we will characterize the potential background channels for the HH → bbγγ decay. My three areas of interest will be events containing two fake photons produced with two real bottom jets, two mistagged charm jets, or two mistagged light jets. By determining the efficiency rates for these various faking events and normalizing by their cross sections, we may weight events in these background channels and produce the expected distributions and number of events for each channel. | |||||||
Gautam Upadhya | ||||||||
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> > | ||||||||
Razor variable analysis of simple SUSY models | ||||||||
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I will be studying simple SUSY models using the razor variables. In particular I will be trying to distinguish between these models and the common ttbar background process, but using a multi-b-jet analysis. Some of the models of interest include RPV-gluino-gluino, T2bw, T2tt dna T6ttHH.
Cedric Flamant | ||||||||
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< < | ||||||||
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Four Dimensional Shower Profiling for Time-of-Flight-Based Vertex Reconstruction | ||||||||
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SUSY Searches | ||||||||
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< < | I am currently working on generating collision events for the Simplified Model Spectra (SMS) models T1ttbb and T2tb with the objective of narrowing the search for SUSY particles. His primary work involves the optimization of code utilized by event generating and analysis software, such as MadGraph and Pythia, and the interpretation of incoming data to ensure that observations correspond with the pertinent models." | |||||||
> > | I am currently working on generating collision events for the Simplified Model Spectra (SMS) models T1ttbb and T2tb with the objective of narrowing the search for SUSY particles. His primary work involves the optimization of code utilized by event generating and analysis software, such as MadGraph and Pythia, and the interpretation of incoming data to ensure that observations correspond with the pertinent models." | |||||||
Added: | ||||||||
> > | Karla Peña | |||||||
Changed: | ||||||||
< < | Karla Peña | |||||||
> > | ||||||||
Dustin Anderson | ||||||||
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> > | ||||||||
Associated production of W/Z bosons and jets | ||||||||
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The production of a massive vector boson alongside one or more jets is an important background for Higgs and SUSY searches. I will analyze this background using the full CMS dataset, examining the scaling of the number of events as a function of jet multiplicity. | ||||||||
Deleted: | ||||||||
< < | ||||||||
Thomas Arnold | ||||||||
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< < | ||||||||
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Machine Learning for the LHC Grid | ||||||||
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< < | Phase 2 Analysis of WW → 2l 2ν with high pileup With the luminosity upgrades to the LHC in the next decade, the pileup in events will be approximately 3x larger than those seen at the end of Run 1. With this expectation, I'm currently working on analysis of these Phase 2 events, specifically looking at lepton detection efficiencies and MET in simulated Drell-Yan -> ee and WW -> 2l2nu events at 14TeV and 140 pileup. These channels are of particular interest to the continued study of the properties of the Higgs-like boson. | |||||||
> > | Phase 2 Analysis of WW → 2l 2ν with high pileup | |||||||
Added: | ||||||||
> > | With the luminosity upgrades to the LHC in the next decade, the pileup in events will be approximately 3x larger than those seen at the end of Run 1. With this expectation, I'm currently working on analysis of these Phase 2 events, specifically looking at lepton detection efficiencies and MET in simulated Drell-Yan -> ee and WW -> 2l2nu events at 14TeV and 140 pileup. These channels are of particular interest to the continued study of the properties of the Higgs-like boson. | |||||||
Marco Cruz-Heredia | ||||||||
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General Information | ||||||||
Added: | ||||||||
> > | Summer Student Index | |||||||
Information from Summer 2012 | ||||||||
Changed: | ||||||||
< < | Check last years twiki for further logistical info : https://twiki.hep.caltech.edu/twiki/bin/view/Main/Summer2012 Summer2012 | |||||||
> > | Check last years twiki for further logistical info : https://twiki.hep.caltech.edu/twiki/bin/view/Main/Summer2012 Summer2012 | |||||||
Projects and Final Reports from previous SURF students | ||||||||
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Thomas Arnold | ||||||||
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Machine Learning for the LHC Grid | ||||||||
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Summer Students 2013Table of contents: | ||||||||
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Natalie Harrison | ||||||||
Added: | ||||||||
> > | Dark matter production with the CMS detector at CERN High energy particle colliders, like the LHC, are one of three ways proposed to detect dark matter. Dark matter is theorized to be a natural candidate for the lightest supersymmetric particle and is proposed to be a decay product in an event where SUSY sparticles are pair produced and decay into standard model quarks, which are detected in the collider and a neutralino that escapes detection (proposed DM). The other two methods are direct detection, in which we expect dark matter scattering off a nuclei, and indirect detection, in which dark matter annihilates and remnants of this annihilation are studied. Previous collider searches have been done for dark matter produced in association with a single photon or jet. My work looks specifically for events where dark matter particles are produced in association with at least two jets and leave behind a signature of large missing transverse energy (ET) in the detector. Because of the large amount of missing ET, we can utilize the razor variables MR and R2, developed initially for SuperSymmetry searches . My aim is to improve upper limits on the DM production cross section and translate these into the cross section of DM-nucleon interaction to compare with results from direct detection experiments. I also hope to analyze the results for various different theoretical models. | |||||||
Ian Wessen |
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Summer Students 2013Table of contents: | ||||||||
Line: 83 to 83 | ||||||||
Karla PeñaDustin Anderson | ||||||||
Added: | ||||||||
> > | Associated production of W/Z bosons and jets The production of a massive vector boson alongside one or more jets is an important background for Higgs and SUSY searches. I will analyze this background using the full CMS dataset, examining the scaling of the number of events as a function of jet multiplicity. | |||||||
Thomas ArnoldMachine Learning for the LHC Grid | ||||||||
Line: 90 to 97 | ||||||||
My research will focus on exploring how machine learning, specifically reinforcement learning, can be used to better handle matching of the workflows of the LHC experiments with LHC Grid resources. I will be using the RLPypackage (written in Python) developed at MIT to facilitate the investigation into reinforcement learning by implementing my own simulations of computer systems. The aim is to understand which learning systems better fit with a distributed system as the LHC Grid as well as to evaluate the speed with which such systems can be learned.
Christopher Hayes | ||||||||
Added: | ||||||||
> > | Phase 2 Analysis of WW → 2l 2ν with high pileup With the luminosity upgrades to the LHC in the next decade, the pileup in events will be approximately 3x larger than those seen at the end of Run 1. With this expectation, I'm currently working on analysis of these Phase 2 events, specifically looking at lepton detection efficiencies and MET in simulated Drell-Yan -> ee and WW -> 2l2nu events at 14TeV and 140 pileup. These channels are of particular interest to the continued study of the properties of the Higgs-like boson. | |||||||
Marco Cruz-Heredia | ||||||||
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Summer Students 2013Table of contents: | ||||||||
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StudentsJeff Picard | ||||||||
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> > | Higgs properties measurement in H → γ γ After the discovery of a Higgs-like boson around 125 GeV it has become important to measure the properties of the new state. I am determining the expected sensitivity of our measurement of the particle's spin in the LHC run 2 dataset, and how proposed upgrades to CMS will affect the sensitivity. | |||||||
Ann Wang | ||||||||
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Da An | ||||||||
Added: | ||||||||
> > | Future analysis for CMS Phase II Upgrade My project is focused on the possible measurement of the trilinear Higgs self-coupling at 14 TeV. This will be done through an analysis of diHiggs production. I will be looking at the potential of analyzing the HH -> bbgammagamma decay channel in order to determine a significant value for the self-coupling. | |||||||
Valère Lambert | ||||||||
Changed: | ||||||||
< < | ||||||||
> > | HH → bbγγ decay With the upgrade of the CMS detector in 2020 to a luminosity of 14 TeV there will be the potential to measure the self-coupling constant of the Higgs boson, which has applications to measuring the Higgs potential. In order to better understand the significance of various backgrounds for di-Higgs events we will characterize the potential background channels for the HH → bbγγ decay. My three areas of interest will be events containing two fake photons produced with two real bottom jets, two mistagged charm jets, or two mistagged light jets. By determining the efficiency rates for these various faking events and normalizing by their cross sections, we may weight events in these background channels and produce the expected distributions and number of events for each channel. | |||||||
Gautam Upadhya | ||||||||
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I will be studying simple SUSY models using the razor variables. In particular I will be trying to distinguish between these models and the common ttbar background process, but using a multi-b-jet analysis. Some of the models of interest include RPV-gluino-gluino, T2bw, T2tt dna T6ttHH.
Cedric Flamant | ||||||||
Changed: | ||||||||
< < | ||||||||
> > | Four Dimensional Shower Profiling for Time-of-Flight-Based Vertex Reconstruction Following the planned Phase II upgrade to the CMS detector, high event pile-up will be common. Associating detections with their proper vertices will be a challenging task, so it has been proposed to use timing systems to help in vertex reconstruction. In order to implement a time-based vertex reconstruction algorithm, it is necessary to define time of flight in a statistically precise and meaningful way. The current scope of my project is to investigate the time and space characteristics of hits in order to assign a proper time of flight to each detection in ECAL, and to see what additional difficulties arise in high pile-up. | |||||||
Anthony Lutz | ||||||||
Added: | ||||||||
> > | SUSY Searches I am currently working on generating collision events for the Simplified Model Spectra (SMS) models T1ttbb and T2tb with the objective of narrowing the search for SUSY particles. His primary work involves the optimization of code utilized by event generating and analysis software, such as MadGraph and Pythia, and the interpretation of incoming data to ensure that observations correspond with the pertinent models." | |||||||
Karla PeñaDustin Anderson | ||||||||
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Summer Students 2013Table of contents: | ||||||||
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Georges Obied | ||||||||
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> > | Higgs decays using Razor variables I will be analyzing H → WW → llνν decays using razor variables for a high mass Higgs. This will then be extended to a boosted di-Higgs analysis in which each Higgs decays to a WW pair. Here the first WW undergoes a leptonic decay while the second WW pair (from the other Higgs) undergoes a fully hadronic decay producing merged jets. | |||||||
Natalie HarrisonIan Wessen |
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Summer Students 2013Table of contents: | ||||||||
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Ian Wessen | ||||||||
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> > | Higgs physics through two decay channels, H → γ γ and H → WW H → γ γ : Superior resolution of ECAL and the clean kinematics of photon final states enable kinematic reconstruction of parent particles with great accuracy. I want to parametrize a fitting function against Monte Carlo Standard Model background processes and then compare this to the data from the photon photon final state. The pulls on the fit parameters suggest how well our standard model and the data from CMS agree. H → WW : The decay to two W contains a lot of kinematic information, but there are many challenges is distinguishing our signal from background. Background sources of missing energy and dilepton final states require a series of discriminating cuts. My analysis focuses on vector boson fusion Higgs production with a characteristic 2-jet final state. By carefully choosing events with these signatures, we can then apply kinematic analysis à la razor techniques to learn about the Higgs. | |||||||
Da AnValère Lambert | ||||||||
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Christopher HayesMarco Cruz-Heredia | ||||||||
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> > | ||||||||
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> > | Muon Test Lab I will be analyzing the data from the muon test in the Lauristen laboratory. In particular, at this first stage I will be using the ROOT physics analysis framework to get the spectrum of energy deposited by cosmic muons in a LYSO crystal as well as the rise time and decay time of such a device. | |||||||
Michaelangelo Lucas |
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Christopher HayesMarco Cruz-Heredia | ||||||||
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Michaelangelo Lucas | ||||||||
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Summer Students 2013Table of contents: | ||||||||
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Ann Wang | ||||||||
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> > | Razor variables and applications on searches for new physics at the LHC: SUSY scenarios My research will focus on exploring both R-parity conserving and RPV MFV SUSY in detail. I hope to develop an analytical method to detect certain signal SUSY events with ttbar background, such as a RPV gluino decay to a top, bottom, and strange quark. This involves implementing a new razor-like analysis and developing various fit models, which will help us set new limits for SUSY models such as RPV Gtbs, T2bw, and T2tt. | |||||||
Georges ObiedNatalie Harrison |
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Summer Students 2013Table of contents: | ||||||||
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Gautam Upadhya | ||||||||
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< < | Razor variable analysis of simple SUSY models: I will be studying simple SUSY models using the razor variables. In particular I will be trying to distinguish between these models and the common ttbar background process, but using a multi-b-jet analysis. Some of the models of interest include RPV-gluino-gluino, T2bw, T2tt dna T6ttHH. | |||||||
> > | Razor variable analysis of simple SUSY models I will be studying simple SUSY models using the razor variables. In particular I will be trying to distinguish between these models and the common ttbar background process, but using a multi-b-jet analysis. Some of the models of interest include RPV-gluino-gluino, T2bw, T2tt dna T6ttHH. | |||||||
Cedric FlamantAnthony Lutz | ||||||||
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Dustin AndersonThomas Arnold | ||||||||
Added: | ||||||||
> > | Machine Learning for the LHC Grid My research will focus on exploring how machine learning, specifically reinforcement learning, can be used to better handle matching of the workflows of the LHC experiments with LHC Grid resources. I will be using the RLPypackage (written in Python) developed at MIT to facilitate the investigation into reinforcement learning by implementing my own simulations of computer systems. The aim is to understand which learning systems better fit with a distributed system as the LHC Grid as well as to evaluate the speed with which such systems can be learned. | |||||||
Christopher HayesMarco Cruz-HerediaMichaelangelo Lucas | ||||||||
Added: | ||||||||
> > | Python for Reinforcement Machine Learning Machine learning has found wide applications in systems where decisions have to be made based on data. This includes control systems, computer systems, data analysis, etc. One of the tools of choice is often the python programming language, due to the very large amount of existing python libraries as well as to the general popularity of the language itself. During my FSRI research I plan to write python modules and programs that implement machine learning scenarios in the context of simple computer systems. | |||||||
Proposals | ||||||||
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Valère LambertGautam Upadhya | ||||||||
Added: | ||||||||
> > | Razor variable analysis of simple SUSY models: I will be studying simple SUSY models using the razor variables. In particular I will be trying to distinguish between these models and the common ttbar background process, but using a multi-b-jet analysis. Some of the models of interest include RPV-gluino-gluino, T2bw, T2tt dna T6ttHH. | |||||||
Cedric FlamantAnthony LutzKarla PeñaDustin Anderson | ||||||||
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> > | ||||||||
Thomas ArnoldChristopher HayesMarco Cruz-Heredia | ||||||||
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> > | StudentsJeff PicardAnn WangGeorges ObiedNatalie HarrisonIan WessenDa AnValère LambertGautam UpadhyaCedric FlamantAnthony LutzKarla PeñaDustin AndersonThomas ArnoldChristopher HayesMarco Cruz-HerediaMichaelangelo Lucas | ||||||||||||||||
ProposalsProcedure
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Full event kinematics in H to ZgammaCMS data collected at pp collisions at 7 and 8 TeV in LHC Run1gave an observation for a Higgs-like boson with mass 126 GeV. The decay channel of this boson to a Z boson and a photon has unique sensitivity to probe for heavy new particles that are not predicted by the Standard Model. The student will study a number of possible improvements to the sensitivity of the search including the use of the full event kinematics and the use of event by event mass resolution. In addition, the student will study the possibility to use the full event kinematics to characterize additional properties of the Higgs-like boson. | |||||||||||||||||
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< < | StudentsJeff PicardEinsteinBohr | ||||||||||||||||
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EinsteinBohrGeneral Information | ||||||||
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< < | Information from Summer 2013 | |||||||
> > |
Information from Summer 2012 | |||||||
Check last years twiki for further logistical info : https://twiki.hep.caltech.edu/twiki/bin/view/Main/Summer2012 | ||||||||
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CMS data collected at pp collisions at 7 and 8 TeV in LHC Run1 gave an observation for a Higgs-like boson with mass 126 GeV. The golden mode in terms of sensitivity to the Higgs mass is H -> ZZ -> 4 leptons final state. The student will study the applications of the full kinematics available in this channel to characterize the properties of a possible signal for a resonance in the still allowed mass range to distinguish a Standard Model Higgs boson from Higgs "look-alikes". He will also contribute to the experimental analysis using at best the information on lepton momentum determination to improve the determination of the mass of the new particle. Artur ApresyanAlex Mott | ||||||||
Added: | ||||||||
> > | Higgs properties measurement in H to gamma gamma | |||||||
CMS data collected in the LHC run 1 has established the existence of a new boson with a mass near 125 GeV, which (among other modes) decays into two photons. Because of the extremely high resolution of the CMS Electromagnetic Calorimeter (ECAL) and relatively high signal yields in this channel, it is ideal to study the properties of this newly discovered particle. The student will study the properties of this boson with the existing LHC run 1 dataset and the expected sensitivity for precision measurement with the expected LHC run 2 dataset. The student will also measure the expected improvement in sensitivity for properties measurement from various proposed upgrades to the CMS detector, which will provide an important input to CMS upgrade planning.
Yi Chen | ||||||||
Changed: | ||||||||
< < | HCAL noise | |||||||
> > | HCAL noise | |||||||
After LS1 there is a good chance we will collect data at 25ns spacing as opposed to 50ns bunch spacing with high pileup. This poses an interesting challenge for the sub-detectors to develop efficient noise filters/algorithms designed for short bunch spacing. Hadronic calorimeter is important for most physics we want to do at the LHC. As we didn't have physics runs with 25ns bunch spacing, not much has been developed so far in terms of filters. In this project we will probe different possibilities of the noise-signal rejection algorithms using collision data collected in 2012 at both 50ns bunch spacing and 25ns bunch spacing, as well as mixed samples from data to emulate condition of high pileup and short bunch spacing. It's a nice chance to do important pioneering work that will affect the way we reject noise in the next run period.
Javier Duarte | ||||||||
Added: | ||||||||
> > | Razoy SUSYSi XieFull event kinematics in H to Zgamma | |||||||
Changed: | ||||||||
< < | Razoy SUSY | |||||||
> > | CMS data collected at pp collisions at 7 and 8 TeV in LHC Run1 gave an observation for a Higgs-like boson with mass 126 GeV. The decay channel of this boson to a Z boson and a photon has unique sensitivity to probe for heavy new particles that are not predicted by the Standard Model. The student will study a number of possible improvements to the sensitivity of the search including the use of the full event kinematics and the use of event by event mass resolution. In addition, the student will study the possibility to use the full event kinematics to characterize additional properties of the Higgs-like boson. | |||||||
StudentsJeff PicardEinstein |
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Artur ApresyanAlex Mott | ||||||||
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> > | CMS data collected in the LHC run 1 has established the existence of a new boson with a mass near 125 GeV, which (among other modes) decays into two photons. Because of the extremely high resolution of the CMS Electromagnetic Calorimeter (ECAL) and relatively high signal yields in this channel, it is ideal to study the properties of this newly discovered particle. The student will study the properties of this boson with the existing LHC run 1 dataset and the expected sensitivity for precision measurement with the expected LHC run 2 dataset. The student will also measure the expected improvement in sensitivity for properties measurement from various proposed upgrades to the CMS detector, which will provide an important input to CMS upgrade planning. | |||||||
Yi ChenHCAL noise |
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General InformationInformation from Summer 2013 | ||||||||
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> > | Check last years twiki for further logistical info : https://twiki.hep.caltech.edu/twiki/bin/view/Main/Summer2012 | |||||||
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Yi ChenHCAL noise | ||||||||
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> > | After LS1 there is a good chance we will collect data at 25ns spacing as opposed to 50ns bunch spacing with high pileup. This poses an interesting challenge for the sub-detectors to develop efficient noise filters/algorithms designed for short bunch spacing. Hadronic calorimeter is important for most physics we want to do at the LHC. As we didn't have physics runs with 25ns bunch spacing, not much has been developed so far in terms of filters. In this project we will probe different possibilities of the noise-signal rejection algorithms using collision data collected in 2012 at both 50ns bunch spacing and 25ns bunch spacing, as well as mixed samples from data to emulate condition of high pileup and short bunch spacing. It's a nice chance to do important pioneering work that will affect the way we reject noise in the next run period. | |||||||
Javier DuarteRazoy SUSY |
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< < | Adi BornheimEmanuele Di Marco | |||||||
> > | Adi Bornheim :A high precision time-of-flight detector for CMS(Adi, Artur, Javier, Cristian)A time-of-flight (TOF) detector with a timing resolution of order a few pico seconds is discussed for the CMS Phase II upgrade for the high luminosity LHC (HL-LHC). A major challenge at HL-LHC will be the number of simultaneous interactions per bunch crossing (pile-up, PU). An average of 140 PU interactions is expected with the accelerator desing currently envisioned for HL-LHC. Based on toy MC studies and fully simulated events algorithms have to be developed which allow to associate a vertex location to a physics object such as a Photon or a Jet. Filtering techniques need to be developed which allow to suppress energy deposits from pile-up interactions in the object reconstruction. The goal of the project is to work on the development of these algorithms, test them on simulated events as well as on real CMS data. Geant simulation for a high precision time-of-flight detector for CMS(Cristian, Adi, Artur, Emanuele)A time-of-flight (TOF) detector with a timing resolution of order a few pico seconds is discussed for the CMS Phase II upgrade for the high luminosity LHC (HL-LHC). A major challenge is to develop radiation hard detector technology which allows the time of flight of all relevant final state particles produced in LHC proton-proton collisions. A fundamental question is how the physical size of a calorimetric device limits the achievable timing measurement precision. The goal of this project is to carry out Geant as well as ray tracing simulation based on the existing CMS ECAL crystals as well as proposed upgrade options such as a crystal sampling calorimeter. ECAL calibration and performance in the presence of radiation induce noise(Adi, Emanuele)The noise in the CMS electromagnetic calorimeter (ECAL) increases due to effects of the radiation environment in LHC. This degrades the resolution performance and has an impact of the isolation criterion which is used to distinguish electrons and photons from jets. The increased noise also has an adverse effect on the ability to select isolated low energy photons, which are used to calibrate the ECAL. The goal of this project is to measure precisely the impact of the noise on the ECAL performance and calibration procedure and develop a strategy to mitigate the effect of the noise. Emanuele Di Marco :H->WW->2l2nu with full decay kinematicsCMS data collected at pp collisions at 7 and 8 TeV in LHC Run1gave an observation for a Higgs-like boson with mass 126 GeV. For this mass, due to the large BR and very clean final state, one the most sensitive channel at CMS is H->WW->2l2nu. The problem with this decay mode is the absence of a clear mass peak due to two undetected neutrinos. The student should develop an alternative strategy for the usage of available decay kinematics, in order to separate the signal from non-resonant WW production and give access to the mass also in this channel. If this is achieved, the other informations of the opening angle of the leptons can be used to determine the spin/parity of the new particle. H -> ZZ-> 4 leptons property measurementCMS data collected at pp collisions at 7 and 8 TeV in LHC Run1 gave an observation for a Higgs-like boson with mass 126 GeV. The golden mode in terms of sensitivity to the Higgs mass is H -> ZZ -> 4 leptons final state. The student will study the applications of the full kinematics available in this channel to characterize the properties of a possible signal for a resonance in the still allowed mass range to distinguish a Standard Model Higgs boson from Higgs "look-alikes". He will also contribute to the experimental analysis using at best the information on lepton momentum determination to improve the determination of the mass of the new particle. | |||||||
Artur ApresyanAlex Mott | ||||||||
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Yi ChenHCAL noiseJavier DuarteRazoy SUSY | |||||||
StudentsJeff Picard | ||||||||
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Summer Students 2013Table of contents:ProposalsProcedure
Adi BornheimEmanuele Di MarcoArtur ApresyanAlex MottStudentsJeff Picard2General InformationInformation from Summer 2012Summer2012 |