Indian Participation in LHC and a Glimpse of the Road Ahead**
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A Thermionic Electron Gun for the Preliminary Phase of Ctf3 G
Proceedings of EPAC 2002, Paris, France A THERMIONIC ELECTRON GUN FOR THE PRELIMINARY PHASE OF CTF3 G. Bienvenu, M. Bernard, J. Le Duff, LAL, Orsay, France H. Hellgren, R. Pittin, L. Rinolfi, CERN, Geneva, Switzerland Abstract A dedicated electron gun has been designed and built Table 1: Beam parameters at gun exit for the preliminary phase of the CLIC Test Facility 3 Nominal beam energy 90 keV (CTF3). The gun is based on a thermionic gridded Pulse width 2 to 10 ns cathode and operates at 90 kV in the intensity range of Intensity 0.05 to 2 A 50 mA to 2A. The specific time structure of the beam is Number of pulses 1 to 7 characterized by a burst of up to seven pulses of variable Repetition rate 50 Hz pulse width (4 to 10 ns) each separated by 420 ns, the revolution time of the former EPA (Electron Positron Emittance (rms) <15 mm.mrd Accumulator) ring. The mechanical conception was specifically designed to be compatible with the existing 2.1 Mechanical design front-end of the former LIL (LEP Injector Linac). We will The vacuum chamber of the CLIO gun has been designed describe the experimental results obtained with the beam to fit existing CERN equipment, in particular the gun is on CTF3. fully compatible with the «CERN plug-in system» and an existing pair of ion pumps. All inner elements have been 1 INTRODUCTION baked under vacuum (400 ºC, 10-5 mbar, 12 h) and assembled under clean laminar airflow. With these The Compact Linear Collider (CLIC) scheme is based precautions a pressure of 10-9 mbar was obtained very on the production of a 30 GHz RF pulse that requires quickly and the HV processing reduced to a few hours. -
HERA Collisions CERN LHC Magnets
The Gallex (gallium-based) solar neutrino experiment in the Gran Sasso underground Laboratory in Italy has seen evidence for neutrinos from the proton-proton fusion reaction deep inside the sun. A detailed report will be published in our next edition. again, with particles taken to 26.5 aperture models are also foreseen to GeV and initial evidence for electron- CERN test coil and collar assemblies and a proton collisions being seen. new conductor distribution will further Earlier this year, the big Zeus and LHC magnets improve multipole components. H1 detectors were moved into A number of other models and position to intercept the first HERA With test magnets for CERN's LHC prototypes are being built elsewhere collisions, and initial results from this proton-proton collider regularly including a twin-aperture model at new physics frontier are eagerly attaining field strengths which show the Japanese KEK Laboratory and awaited. that 10 Tesla is not forbidden terri another in the Netherlands (FOM-UT- tory, attention turns to why and NIHKEF). The latter will use niobium- where quenches happen. If 'training' tin conductor, reaching for an even can be reduced, superconducting higher field of 11.5 T. At KEK, a magnets become easier to commis single aperture configuration was sion. Tests have shown that successfully tested at 4.3 K, reaching quenches occur mainly at the ends of the short sample limit of the cable the LHC magnets. This should be (8 T) in three quenches. This magnet rectifiable, and models incorporating was then shipped to CERN for HERA collisions improvements will soon be reassem testing at the superfluid helium bled by the industrial suppliers. -
Trigger and Data Acquisition
Trigger and data acquisition N. Ellis CERN, Geneva, Switzerland Abstract The lectures address some of the issues of triggering and data acquisition in large high-energy physics experiments. Emphasis is placed on hadron-collider experiments that present a particularly challenging environment for event se- lection and data collection. However, the lectures also explain how T/DAQ systems have evolved over the years to meet new challenges. Some examples are given from early experience with LHC T/DAQ systems during the 2008 single-beam operations. 1 Introduction These lectures concentrate on experiments at high-energy particle colliders, especially the general- purpose experiments at the Large Hadron Collider (LHC) [1]. These experiments represent a very chal- lenging case that illustrates well the problems that have to be addressed in state-of-the-art high-energy physics (HEP) trigger and data-acquisition (T/DAQ) systems. This is also the area in which the author is working (on the trigger for the ATLAS experiment at LHC) and so is the example that he knows best. However, the lectures start with a more general discussion, building up to some examples from LEP [2] that had complementary challenges to those of the LHC. The LEP examples are a good reference point to see how HEP T/DAQ systems have evolved in the last few years. Students at this school come from various backgrounds — phenomenology, experimental data analysis in running experiments, and preparing for future experiments (including working on T/DAQ systems in some cases). These lectures try to strike a balance between making the presentation accessi- ble to all, and going into some details for those already familiar with T/DAQ systems. -
India-CMS Newsletter Member Institutes/ Universities of India-CMS
India-CMS Newsletter Member Institutes/ Universities of India-CMS Vol 1. No. 1, July 2015 1. Nuclear Physics Division (NPD) Bhabha Atomic Research Center (BARC) Mumbai http://www.barc.gov.in/ First volume produced at: 2. Indian Institute of Science Education and Research (IISER) Department of Physics Pune http://www.iiserpune.ac.in Panjab University Sector 14 Chandigarh - 160014 3. Indian Institute of Technology (IIT), Bhubaneswar Bhubaneswar http:// www.iitbbs.ac.in 4. Department of Physics Indian Institute of Technology (IIT), Bombay Mumbai http://www.iitb.ac.in/en/education/academic-divisions 5. Indian Institute of Technology (IIT), Madras Chennai https://www.iitm.ac.in 6. School of Physical Sciences National Institute of Science Education and Research (NISER), Edited and Compiled by: Bhubaneswar http://physics.niser.ac.in/ Manjit Kaur Department of Physics 7. Department of Physics Panjab University Panjab University Chandigarh Chandigarh http://physics.puchd.ac.in/ [email protected] 8. Division of High Energy Nuclear and Particle Physics Ajit Mohanty Saha Institute of Nuclear Physics (SINP) Director Kolkata http://www.saha.ac.in/web/henppd-home Saha Institute of Nuclear Physics (SINP) Kolkatta 9. Department of High Energy Physics [email protected] Tata Institute of Fundamental Research (TIFR), Mumbai http://www.tifr.res.in/ ~dhep/ Abhimanyu Chawla Department of Physics 10. Department of Physics & Astrophysics Panjab University University of Delhi Chandigarh Delhi http://www.du.ac.in/du/index.php?page=physics-astrophysics [email protected] 11. Visva Bharti Santiniketan, West Bengal 731204 http://www.visvabharati.ac.in/Address.html 1 2 Contents Message ........................................................................................................................................................ 3 Message ....................................................................................................................................................... -
Status of the Ctf3 Commissioning
Proceedings of EPAC 2002, Paris, France STATUS OF THE CTF3 COMMISSIONING R. Corsini, B. Dupuy, L. Rinolfi, P. Royer, F. Tecker, CERN, Geneva, Switzerland A. Ferrari∗, Uppsala University, Sweden Abstract In this paper, we describe the present status of the fa- cility as well as the results of the first beam measurements The Preliminary Phase of the new CLIC Test Facility performed during the commissioning [4, 5]. These results CTF3 consists of a low-charge demonstration of the elec- are compared to beam dynamics predictions [6]. Finally, tron bunch train combination process on which the CLIC the next steps towards the completion of the experiment drive beam generation scheme is based. The principle of are described. the combination relies on the injection of short electron bunches into an isochronous ring using RF deflecting cavi- ties. The commissioning of this facility started in Septem- 2 COMMISSIONING WITH BEAM ber 2001, with alternating periods of installation work and 2.1 The Front-End and the Linac beam studies. In this paper, we present the status of the facility, the first beam measurements and the next steps to- The new thermionic gun built by LAL (“Laboratoire wards the completion of the experiment. de l’Acc´el´erateur Lin´eaire d’Orsay”) was successfully in- stalled and commissioned [7]. This triode gun produces a train of up to seven pulses at a repetition rate of 50 Hz. The 1 INTRODUCTION pulse length can be varied between 2 ns and 10 ns FWHM and the pulses are spaced by 420 ns, corresponding to the The Compact Linear Collider (CLIC) [1] RF power revolution period of the ring, as required for the bunch fre- source scheme is based on the production of a 30 GHz quency multiplication process. -
Hep-Ph/0609102
CERN-PH-TH/2006-175 September 2006 Physics Opportunities with Future Proton Accelerators at CERN A. Blondel a, L. Camilleri b, A. Ceccucci b, J. Ellis b , M. Lindroos b , M. Mangano b , G. Rolandi b a University of Geneva CH-1211 Geneva 4, SWITZERLAND b CERN, CH-1211 Geneva 23, SWITZERLAND Abstract We analyze the physics opportunities that would be made possible by upgrades of CERN’s proton accelerator complex. These include the new physics possible with luminosity or energy upgrades of the LHC, options for a possible future neutrino complex at CERN, and opportunities in other physics including rare kaon decays, other fixed-target experiments, nuclear physics and antiproton physics, among other possibilities. We stress the importance of inputs from initial LHC running and planned neutrino experiments, and summarize the principal detector R&D issues. 1 Introduction and summary In our previous report [1], we presented an initial survey of the physics opportunities that could be provided by possible developments and upgrades of the present CERN Proton Accelerator Complex [2,3]. These topics have subsequently been discussed by the CERN Council Strategy Group [4]. In this report, we amplify and update some physics points from our initial report and identify detector R&D priorities for the preferred experimental programme from 2010 onwards. We consider experimentation at the high-energy frontier to be the top priority in choosing a strategy for upgrading CERN's proton accelerator complex. This experimentation includes the upgrade to optimize the useful LHC luminosity integrated over the lifetime of the accelerator, through both a consolidation of the LHC injector chain and a possible luminosity upgrade project we term the SLHC. -
CLIC Status Compact Linear Collider
CLIC Status Compact Linear Collider IAS Program - HEP Plenary, 21 January 2019 Andrea Latina, CERN on behalf of the CLIC and CLICdp Collaborations 1 CLIC Status Compact Linear Collider Project overview Physics reach Accelerator technologies Outlook Compact Linear Collider e+e– collisions up to 3TeV http://clic.cern/ IAS Program - HEP Plenary, 21 January 2019 Andrea Latina, CERN on behalf of the CLIC and CLICdp Collaborations 2 Collaborations http://clic.cern/ • CLIC accelerator design and development • CLIC physics prospects & simulation studies • (Construction and operation of CTF3) • Detector optimization + R&D for CLIC CLIC accelerator collaboration CLIC detector and physics ~60 institutes from 28 countries (CLICdp) 30 institutes from 18 countries IAS HEP 2019 Andrea Latina 3 CLIC IAS HEP 2019 Andrea Latina 4 CLIC layout and power generation Baseline electron polarisation ±80% IAS HEP 2019 Andrea Latina 5 CLIC layout – 3TeV Baseline electron polarisation ±80% IAS HEP 2019 Andrea Latina 6 CLIC CDR 2012 Updated Staging Project Implementation https://cds.cern.ch/record/1500095 Baseline 2016 Plan 2018 https://cds.cern.ch/record/1425915 https://cds.cern.ch/record/1475225 http://dx.doi.org/10.5170/CERN-2016-004 IAS HEP 2019 Andrea Latina 7 CLIC Key technologies have been demonstrated CLIC is now a mature project, ready to be built IAS HEP 2019 Andrea Latina 8 Updated CLIC Staging New! increased from 0.5+0.1ab–1 1.5ab–1 3ab–1 Electron polarisation enhances Higgs production at high- energy stages and provides additional observables Baseline polarisation scenario adopted: electron beam (–80%, +80%) polarised in ratio (50:50) at √s=380GeV ; (80:20) at √s=1.5 and 3TeV γγ collider using laser scattering also possible Upgrades using novel accelerator techniques also possible Staging and live-time assumptions following guidelines consistent with other future projects: Machine Parameters and Projected Luminosity Performance of Proposed Future Colliders at CERN arXiv:1810.13022, Bordry et al. -
QCD Studies at L3
QCD Studies at L3 Swagato Banerjee Tata Institute of Fundamental Research Mumbai 400 005 2002 QCD Studies at L3 Swagato Banerjee Tata Institute of Fundamental Research Mumbai 400 005 A Thesis submitted to the University of Mumbai for the degree of Doctor of Philosophy in Physics March, 2002 To my parents Acknowledgement It has been an extremely enlightening and enriching experience working with Sunanda Banerjee, supervisor of this thesis. I would like to thank him for his forbearance and encouragement and for teaching me the different aspects of the subject with lots of patience. I thank all the members of the Department of High Energy Physics of Tata Institute of Fundamental Research (TIFR) for providing various facilities and support, and ideal ambiance for research. In particular, I would like to thank B.S. Acharya, T. Aziz, Sudeshna Banerjee, B.M. Bellara, P.V. Deshpande, S.T. Divekar, S.N. Ganguli, A. Gurtu, M.R. Krishnaswamy, K. Mazumdar, M. Maity, N.K. Mondal, V.S. Narasimham, P.M. Pathare, K. Sudhakar and S.C. Tonwar. Asesh Dutta, Dilip Ghosh, S. Gupta, Krishnendu Mukherjee, Sreerup Ray Chaudhuri, D.P. Roy, Sourov Roy, Gavin Salam and K. Sridhar provided valuable theoretical insight on various occasions. My heartfelt thanks to them. I thank the European Organisation for Nuclear Research (CERN) for its kind hospitality and all the members of the Large Electron Positron (LEP) accelerator group for successful operation over the last decade. The members of the L3 collaboration and the LEP QCD Working Group provided me a stim- ulating working environment. In particular, I thank Pedro Abreu, Satyaki Bhattacharya, Gerard Bobbink, Ingrid Clare, Robert Clare, Glen Cowan, Aaron Dominguez, Dominique Duchesneau, John Field, Ian Fisk, Roger Jones, Mehnaz Hafeez, Stephan Kluth, Wolfgang Lohmann, Wes- ley Metzger, Peter Molnar, Oliver Passon, Martin Pohl, Subir Sarkar, Chris Tully and Micheal Unger. -
2.15 CTF3 Status, Progress and Plans
165 2.15 CTF3 Status, Progress and Plans R. Corsini, P. Skowroński, F. Tecker, CERN, CH-1211 Geneva 23, Switzerland Mail to: [email protected] 2.15.1 Introduction The aim of the CLIC Test Facility CTF3 (see Fig. 1.1), built at CERN by the CLIC International Collaboration, is to prove the main feasibility issues of the two-beam acceleration technology [1]. CTF3 consists of a 150 MeV electron linac followed by a 42 m long Delay Loop and a 84 m Combiner Ring. The beam current from the linac is first doubled in the delay loop and then multiplied again by a factor of four in the combiner ring by interleaving bunches using transverse RF deflecting cavities. The high current beam can then be sent in the CLIC experimental area (CLEX) where it can be decelerated to extract 12 GHz RF power to be used for high gradient acceleration. In the same area a 200 MeV injector (CALIFES) generates a Probe Beam for two-beam experiments. Figure 1.1: CTF3 overall layout. CTF3 was built in order to demonstrate the following two main issues [2]: 1. Drive Beam Generation: efficient generation of a high-current electron beam with the time structure needed to generate 12 GHz RF power. CLIC relies on a novel scheme of fully loaded acceleration in normal conducting travelling wave structures, followed by beam current and bunch frequency multiplication by funneling techniques in a series of delay lines and rings, using injection by RF deflectors. CTF3 is meant to use such a technique to produce a 30 A Drive Beam with 12 GHz bunch repetition frequency. -
Compact Linear Collider (CLIC)
Compact Linear Collider (CLIC) Philip Burrows John Adams Institute Oxford University 1 Outline • Introduction • Linear colliders + CLIC • CLIC project status • 5-year R&D programme + technical goals • Applications of CLIC technologies 2 Large Hadron Collider (LHC) Largest, highest-energy particle collider CERN, Geneva 3 CERN accelerator complex 4 CLIC vision • A proposed LINEAR collider of electrons and positrons • Designed to reach VERY high energies in the electron-positron annihilations: 3 TeV = 3 000 000 000 000 eV • Ideal for producing new heavy particles of matter, such as SUSY particles, in clean conditions 5 CLIC vision • A proposed LINEAR collider of electrons and positrons • Designed to reach VERY high energies in the electron-positron annihilations: 3 TeV = 3 000 000 000 000 eV • Ideal for producing new heavy particles of matter, such as SUSY particles, in clean conditions … should they be discovered at LHC! 6 CLIC Layout: 3 TeV Drive Beam Generation Complex Main Beam Generation Complex 7 CLIC energy staging • An energy-staging strategy is being developed: ~ 500 GeV 1.5 TeV 3 TeV (and realistic for implementation) • The start-up energy would allow for a Higgs boson and top-quark factory 8 2013 Nobel Prize in Physics 9 e+e- Higgs boson factory e+e- annihilations: E > 91 + 125 = 216 GeV E ~ 250 GeV E > 91 + 250 = 341 GeV E ~ 500 GeV European PP Strategy (2013) High-priority large-scale scientific activities: LHC + High Lumi-LHC Post-LHC accelerator at CERN International Linear Collider Neutrinos 11 International Linear Collider (ILC) c. 250 GeV / beam 31 km 12 Kitakami Site 13 ILC Kitakami Site: IP region 14 Global Linear Collider Collaboration 15 European PP Strategy (2013) CERN should undertake design studies for accelerator projects in a global context, with emphasis on proton-proton and electron-positron high energy frontier machines. -
The a to Z of Accelerators
present explanation for this behav The long timescale needed to terparts. But superconductivity iour is that superconductivity exists produce acceptable conductors of above 77K provides a powerful in many discrete regions within niobium-tin (10-12 years) following stimulant to solve the technological the sample but only weak coupling its discovery in 1962 inevitably problems of dealing with brittle exists between these regions. This comes to mind in assessing the materials. The next few months weak coupling is strongly dimin potential timeîscales for developing could give us many more surprises ished by an external field. Electro high field magnets with the new in an area where none were sus magnetic and structural character materials. These new oxides, like pected only a few months ago. izations of these compounds are niobium-tin and the other A15 The discovery of Bednorz and proceeding furiously and we may compounds are inherently brittle Muller has given a profound new soon expect to know whether this and this is bound to affect their stimulus to superconductivity and percolative nature of the supercon application in magnets, just as the last discovery has surely not ductivity is inherent in the material large scale construction of niobium- yet been made. or results from the way present tin magnets has lagged behind samples are being prepared. their ductile niobium-titanium coun The A to Z of accelerators With great skill, the organizers physics but this information was 1965. The attendance of over of the 1987 Particle Accelerator surpassed in volume by reports 1100 was another reflection of Conference arranged a vast pro from the many other areas where the wealth of activity in the field. -
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