32 results on '"Doebert, Steffen"'
Search Results
2. The AWAKE Run 2 programme and beyond
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Gschwendtner, Edda, Lotov, Konstantin, Muggli, Patric, Wing, Matthew, Agnello, Riccardo, Ahdida, Claudia Christina, Goncalves, Maria Carolina Amoedo, Andrebe, Yanis, Apsimon, Oznur, Apsimon, Robert, Arnesano, Jordan Matias, Bachmann, Anna-Maria, Barrientos, Diego, Batsch, Fabian, Bencini, Vittorio, Bergamaschi, Michele, Blanchard, Patrick, Burrows, Philip Nicholas, Buttenschön, Birger, Caldwell, Allen, Chappell, James, Chevallay, Eric, Chung, Moses, Cooke, David Andrew, Damerau, Heiko, Davut, Can, Demeter, Gabor, Dexter, Amos Christopher, Doebert, Steffen, Elverson, Francesa Ann, Farmer, John, Fasoli, Ambrogio, Fedosseev, Valentin, Fonseca, Ricardo, Furno, Ivo, Gessner, Spencer, Gorn, Aleksandr, Granados, Eduardo, Granetzny, Marcel, Graubner, Tim, Grulke, Olaf, Guran, Eloise Daria, Hafych, Vasyl, Hartin, Anthony, Henderson, James, Hüther, Mathias, Kedves, Miklos, Keeble, Fearghus, Khudiakov, Vadim, Kim, Seong-Yeol, Kraus, Florian, Krupa, Michel, Lefevre, Thibaut, Liang, Linbo, Liu, Shengli, Lopes, Nelson, Calderon, Miguel Martinez, Mazzoni, Stefano, Godoy, David Medina, Moody, Joshua, Moon, Kookjin, Guzmán, Pablo Israel Morales, Moreira, Mariana, Nechaeva, Tatiana, Nowak, Elzbieta, Pakuza, Collette, Panuganti, Harsha, Pardons, Ans, Pepitone, Kevin, Perera, Aravinda, Pucek, Jan, Pukhov, Alexander, Ramjiawan, Rebecca Louise, Rey, Stephane, Scaachi, Adam, Schmitz, Oliver, Senes, Eugenio, Silva, Fernando, Silva, Luis, Stollberg, Christine, Sublet, Alban, Swain, Catherine, Topaloudis, Athanasios, Torrado, Nuno, Tuev, Petr, Turner, Marlene, Velotti, Francesco, Verra, Livio, Verzilov, Victor, Vieira, Jorge, Vincke, Helmut, Weidl, Martin, Welsch, Carsten, Wendt, Manfred, Wiwattananon, Peerawan, Wolfenden, Joseph, Woolley, Benjamin, Wyler, Samuel, Xia, Guoxing, Yarygova, Vlada, Zepp, Michael, and Della Porta, Giovanni Zevi
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Physics - Accelerator Physics ,High Energy Physics - Experiment ,Physics - Plasma Physics - Abstract
Plasma wakefield acceleration is a promising technology to reduce the size of particle accelerators. Use of high energy protons to drive wakefields in plasma has been demonstrated during Run 1 of the AWAKE programme at CERN. Protons of energy 400 GeV drove wakefields that accelerated electrons to 2 GeV in under 10 m of plasma. The AWAKE collaboration is now embarking on Run 2 with the main aims to demonstrate stable accelerating gradients of 0.5-1 GV/m, preserve emittance of the electron bunches during acceleration and develop plasma sources scalable to 100s of metres and beyond. By the end of Run 2, the AWAKE scheme should be able to provide electron beams for particle physics experiments and several possible experiments have already been evaluated. This article summarises the programme of AWAKE Run 2 and how it will be achieved as well as the possible application of the AWAKE scheme to novel particle physics experiments., Comment: 21 pages, 8 figures. Submitted to Symmetry journal
- Published
- 2022
3. Design of the AWAKE Run 2c transfer lines using numerical optimizers
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Ramjiawan, Rebecca, Bencini, Vittorio, Doebert, Steffen, Farmer, John, Gschwendtner, Edda, Velotti, Francesco, Verra, Livio, and Della Porta, Giovanni Zevi
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Physics - Accelerator Physics - Abstract
The Advanced Wakefield (AWAKE) Experiment is a proof-of-principle experiment demonstrating the acceleration of electron beams via proton-driven plasma wakefield acceleration. AWAKE Run 1 achieved acceleration of electron beams to 2 GeV and the intention for Run 2 is to build on these results by achieving acceleration to ~10 GeV with a higher beam quality. As part of the upgrade to Run 2, the existing proton and electron beamlines will be adapted and a second plasma cell and new 150 MeV electron beamline will be added. This new beamline will be required to inject electron bunches with micron-level beam size and stability into the second plasma cell from within the 1 m gap between the two plasma cells. In this paper we describe the techniques used (e.g. numerical optimizers and genetic algorithms) to produce the design of the 150 MeV electron line in order to meet the challenging experimental specifications. Operational techniques are also studied for both electron transfer lines including steering and alignment methods utilising numerical optimizers and beam measurement techniques employing neural networks.
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- 2022
4. Drive beam sources and longitudinal shaping techniques
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Lemery, Francois, Andonian, Gerard, Doebert, Steffen, Ha, Gwanghui, Lu, Xueying, Power, John, and Wisniewski, Eric
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Physics - Accelerator Physics - Abstract
Linear colliders are an attractive platform to explore high-precision physics of newly discovered particles. The recent significant progress in advanced accelerator technologies has motivated their applications to colliders which has been discussed in the {\sc alegro} workshop. In this paper we discuss one promising scheme, collinear wakefield acceleration. We especially discuss available drive and witness beam sources based on L and S-band radiofrequency technology, and also summarize available and forthcoming longitudinal shaping techniques to improve the overall acceleration efficiency via the transformer ratio.
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- 2022
- Full Text
- View/download PDF
5. Design of an electron source for the FCC-ee with top-up injection capability
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Vostrel, Zdenek and Doebert, Steffen
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- 2024
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6. Simulation Study of an LWFA-based Electron Injector for AWAKE Run 2
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Williamson, Barney, Xia, Guoxing, Doebert, Steffen, Karsch, Stefan, and Muggli, Patric
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Physics - Accelerator Physics ,Physics - Plasma Physics - Abstract
The AWAKE experiment aims to demonstrate preservation of injected electron beam quality during acceleration in proton-driven plasma waves. The short bunch duration required to correctly load the wakefield is challenging to meet with the current electron injector system, given the space available to the beamline. An LWFA readily provides short-duration electron beams with sufficient charge from a compact design, and provides a scalable option for future electron acceleration experiments at AWAKE. Simulations of a shock-front injected LWFA demonstrate a 43 TW laser system would be sufficient to produce the required charge over a range of energies beyond 100 MeV. LWFA beams typically have high peak current and large divergence on exiting their native plasmas, and optimisation of bunch parameters before injection into the proton-driven wakefields is required. Compact beam transport solutions are discussed., Comment: Paper submitted to NIMA proceedings for the 3rd European Advanced Accelerator Concepts Workshop. 4 pages, 3 figures, 1 table Changes after revision: Figure 2: figures 2 and 3 of the previous version collated with plots of longitudinal electric field Line 45: E_0 = 96 GV/m Lines 147- 159: evaluation of beam loading made more accurate Lines 107 - 124: discussion of simulation geometry moved
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- 2017
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7. Design and optimisation of the Compact Linear Collider main LINAC module for micron-level stability and alignment
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Capstick, Matthew, Doebert, Steffen, Aicheler, Markus, and Rossi, Carlo
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- 2022
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8. CLIC X-band technology developments and their use in compact accelerators for research, medicine and industry.
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Doebert, Steffen, primary
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- 2024
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9. Development of the AWAKE Stripline BPM Electronics
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Liu, Shengli, Verzilov, Victor, Farabolini, Wilfrid, Doebert, Steffen, Schmidt, Janet S., and Liu, Zhen-An, editor
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- 2018
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10. Work on PETS Developed at CIEMAT
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Sanchez, Laura, Aragon, Fernando, Calero, Jesus, Carrillo, David, Gavela, Daniel, Gutierrez, Jose Luis, Lara, Alvaro, Rodriguez, Enrique, Toral, Fernando, Doebert, Steffen, Riddone, Germana, and Samoshkin, Alexandre
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Physics - Accelerator Physics - Abstract
CIEMAT has been working on the RF power extractor so-called PETS (Power Extraction and Transfer Structure) for the CLIC Test Facility 3 (CTF3) since 2007. The first contribution has been installed at the Test Beam Line (TBL). Additionally, a new PETS configuration is presently under fabrication at CIEMAT and will be installed in the Test Module at CTF3. This paper describes the PETS prototypes design, fabrication and assembly techniques. The characterization of the devices with low RF power is also described., Comment: 9 pages, 9 figures, 3 tables, 10 references. Work presented in the LCWS11
- Published
- 2012
11. AWAKE status report 2022
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Bencini, Vittorio, Caldwell, Allen, Doebert, Steffen, Farmer, John, Granados, Eduardo, Gschwendtner, Edda, Guran, Eloise, Mazzoni, Stefano, Muggli, Patric, Pukhov, Alexander, Sublet, Alban, Wing, Matthew, and Zevi Della Porta, Giovanni
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Detectors and Experimental Techniques - Abstract
2022 Status Report of the Advanced Wakefield Experiment AWAKE
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- 2022
12. The AWAKE Run 2 Programme and Beyond
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Gschwendtner, Edda, primary, Lotov, Konstantin, additional, Muggli, Patric, additional, Wing, Matthew, additional, Agnello, Riccardo, additional, Ahdida, Claudia Christina, additional, Amoedo Goncalves, Maria Carolina, additional, Andrebe, Yanis, additional, Apsimon, Oznur, additional, Apsimon, Robert, additional, Arnesano, Jordan Matias, additional, Bachmann, Anna-Maria, additional, Barrientos, Diego, additional, Batsch, Fabian, additional, Bencini, Vittorio, additional, Bergamaschi, Michele, additional, Blanchard, Patrick, additional, Burrows, Philip Nicholas, additional, Buttenschön, Birger, additional, Caldwell, Allen, additional, Chappell, James, additional, Chevallay, Eric, additional, Chung, Moses, additional, Cooke, David Andrew, additional, Damerau, Heiko, additional, Davut, Can, additional, Demeter, Gabor, additional, Dexter, Amos Christopher, additional, Doebert, Steffen, additional, Elverson, Francesa Ann, additional, Farmer, John, additional, Fasoli, Ambrogio, additional, Fedosseev, Valentin, additional, Fonseca, Ricardo, additional, Furno, Ivo, additional, Gessner, Spencer, additional, Gorn, Aleksandr, additional, Granados, Eduardo, additional, Granetzny, Marcel, additional, Graubner, Tim, additional, Grulke, Olaf, additional, Guran, Eloise Daria, additional, Hafych, Vasyl, additional, Hartin, Anthony, additional, Henderson, James, additional, Hüther, Mathias, additional, Kedves, Miklos, additional, Keeble, Fearghus, additional, Khudiakov, Vadim, additional, Kim, Seong-Yeol, additional, Kraus, Florian, additional, Krupa, Michel, additional, Lefevre, Thibaut, additional, Liang, Linbo, additional, Liu, Shengli, additional, Lopes, Nelson, additional, Martinez Calderon, Miguel, additional, Mazzoni, Stefano, additional, Medina Godoy, David, additional, Moody, Joshua, additional, Moon, Kookjin, additional, Morales Guzmán, Pablo Israel, additional, Moreira, Mariana, additional, Nechaeva, Tatiana, additional, Nowak, Elzbieta, additional, Pakuza, Collette, additional, Panuganti, Harsha, additional, Pardons, Ans, additional, Pepitone, Kevin, additional, Perera, Aravinda, additional, Pucek, Jan, additional, Pukhov, Alexander, additional, Ramjiawan, Rebecca Louise, additional, Rey, Stephane, additional, Scaachi, Adam, additional, Schmitz, Oliver, additional, Senes, Eugenio, additional, Silva, Fernando, additional, Silva, Luis, additional, Stollberg, Christine, additional, Sublet, Alban, additional, Swain, Catherine, additional, Topaloudis, Athanasios, additional, Torrado, Nuno, additional, Tuev, Petr, additional, Turner, Marlene, additional, Velotti, Francesco, additional, Verra, Livio, additional, Verzilov, Victor, additional, Vieira, Jorge, additional, Vincke, Helmut, additional, Weidl, Martin, additional, Welsch, Carsten, additional, Wendt, Manfred, additional, Wiwattananon, Peerawan, additional, Wolfenden, Joseph, additional, Woolley, Benjamin, additional, Wyler, Samuel, additional, Xia, Guoxing, additional, Yarygova, Vlada, additional, Zepp, Michael, additional, and Zevi Della Porta, Giovanni, additional
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- 2022
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13. Drive Beam Sources and Longitudinal Shaping Techniques for Beam Driven Accelerators
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Lemery, Francois, Andonian, Gerard, Doebert, Steffen, Ha, Gwanghui, Lu, Xueying, Power, John, and Wisniewski, Eric
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particle source [electron] ,Beam dynamics ,longitudinal [beam profile] ,beam profile: longitudinal ,technology [accelerator] ,RF system ,collinear ,wake field [acceleration] ,Accelerators and Storage Rings ,electron: particle source ,Wake-field acceleration (laser-driven, electron-driven) ,acceleration: wake field ,efficiency ,Accelerator modelling and simulations (multi-particle dynamics, single-particle dynamics) ,Physics::Accelerator Physics ,ddc:610 ,accelerator: technology ,linear collider ,Instrumentation ,Mathematical Physics ,physics.acc-ph - Abstract
Journal of Instrumentation 17(05), P05036 (2022). doi:10.1088/1748-0221/17/05/P05036, Linear colliders are an attractive platform to explore high-precision physics of newly discovered particles. The recent significant progress in advanced accelerator technologies has motivated their applications to colliders which has been discussed in the alegro workshop. In this paper we discuss structure wakefield acceleration, namely collinear wakefield acceleration and two-beam acceleration. We especially discuss available drive and witness beam sources based on L and S-band radiofrequency technology, and also summarize available and forthcoming longitudinal shaping techniques to improve the overall acceleration efficiency via the transformer ratio., Published by Inst. of Physics, London
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- 2022
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14. Flux Concentrator Optimization for Future Positron Sources
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Bajas, Hugo, primary, Doebert, Steffen, additional, Latina, Andrea, additional, and Zhao, Yongke, additional
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- 2022
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15. Electron source and pre-injector design for the FCC-ee
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Brezina, Tomas and Doebert, Steffen
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FCC,FCC-ee injector,CHART - Abstract
This report describes the electron pre-injector of the FCC-ee injector chain. There are two main options for electron sources for such a machine, an RF-photo injector or a thermionic gun. The study comprises the source itself and a linear accelerator to accelerate the electrons up to 200 MeV.
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- 2021
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16. Proposal for the ILC Preparatory Laboratory (Pre-lab)
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Nakada, T., Michizono, S., Murayama, H., Lankford, A., Taylor, G., Stapnes, S., Okada, Y., Collier, Paul, Dunham, Bruce, Elsen, Eckhard, Foster, Brian, Fuster, Juan, Henderson, Stuart, Kruecken, Reiner, Lykken, Joseph D., Titov, Maksym, Yamashita, Satoru, Belomestnykh, Sergey, Buesser, Karsten, Burrows, Philip, Catalán-Lasheras, Nuria, Cenni, Enrico, Clarke, Jim, Delikaris, Dimitri, Doebert, Steffen, Faus-Golfe, Angeles, García-Tabarés, Luis, Geng, Rongli, Grames, Joseph, Hayano, Hitoshi, Kubo, Kiyoshi, Kuriki, Masao, Latina, Andrea, Laxdal, Robert, Liepe, Matthias, List, Benno, List, Jenny, Markiewicz, Thomas, McIntosh, Peter, Michizono, Shinichiro, Monaco, Laura, Moortgat-Pick, Gudrid, Napoly, Olivier, Okugi, Toshiyuki, Omori, Tsunehiko, Osborne, John Andrew, Parker, Brett, Podadera, Ivan, Posen, Sam, Riemann, Sabine, Rimmer, Robert, Ross, Marc C., Rubin, David L., Sanuki, Tomoyuki, Sievers, Peter, Solyak, Nikolay, Takahashi, Tohru, Terunuma, Nobuhiro, Umemori, Kensei, Weise, Hans, White, Glen, Yamamoto, Akira, Yamamoto, Yasuchika, Yokoya, Kaoru, Zobov, Mikhail, Murayama, Hitoshi, Vallée, Claude, Behnke, Ties, Brau, James, Denisov, Dmitri, Forti, Francesco, Fujii, Keisuke, Gao, Yuanning, Mazumdar, Kajari, McBride, Patricia, Nelson, Timothy, Nojiri, Mihoko, Simon, Frank, Urquijo, Phillip, White, Andrew, Żarnecki, Aleksander Filip, Bellerive, Alain, Božović-Jelisavčić, Ivanka, Kawagoe, Kiyotomo, Pöschl, Roman, Sugimoto, Yasuhiro, Krüger, Katja, Merkel, Petra, Miller, David, Vos, Marcel, Gaede, Frank, Jeans, Daniel, Strube, Jan, Peskin, Michael, Robson, Aidan, and Tian, Junping
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Accelerator Physics (physics.acc-ph) ,hep-ex ,FOS: Physical sciences ,hep-ph ,nucl-ex ,Accelerators and Storage Rings ,High Energy Physics - Experiment ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Physics - Accelerator Physics ,Nuclear Physics - Experiment ,Nuclear Experiment (nucl-ex) ,Nuclear Experiment ,Particle Physics - Experiment ,Particle Physics - Phenomenology ,physics.acc-ph - Abstract
During the preparatory phase of the International Linear Collider (ILC) project, all technical development and engineering design needed for the start of ILC construction must be completed, in parallel with intergovernmental discussion of governance and sharing of responsibilities and cost. The ILC Preparatory Laboratory (Pre-lab) is conceived to execute the technical and engineering work and to assist the intergovernmental discussion by providing relevant information upon request. It will be based on a worldwide partnership among laboratories with a headquarters hosted in Japan. This proposal, prepared by the ILC International Development Team and endorsed by the International Committee for Future Accelerators, describes an organisational framework and work plan for the Pre-lab. Elaboration, modification and adjustment should be introduced for its implementation, in order to incorporate requirements arising from the physics community, laboratories, and governmental authorities interested in the ILC., 48 pages, 5 figures
- Published
- 2021
17. Optimisation of the CLIC positron source at the 1.5 TeV and 3 TeV stages
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Zhao, Yongke, Latina, Andrea, Doebert, Steffen, Schulte, Daniel, and Ma, Lianliang
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Astrophysics::High Energy Astrophysical Phenomena ,Physics::Accelerator Physics ,Accelerators and Storage Rings - Abstract
Positron source is very important for many accelerator experiments. The optimisation of positron source is therefore a crucial problem to be solved. In this report, a new simple, general and effective optimisation strategy is proposed, based on iterations of scan of free parameters, which has the advantage of easily handling realistic parametric problems. The new strategy in principle can be 25 times faster than the old optimisation method. The optimisation of the CLIC positron source at the 3 TeV and 1.5 TeV stages with the new strategy is presented. Positron yield is improved by 43% compared with previous studies, mainly due to the removal of the distance between the targets. The validation of the simulation code is carried out with a cross-check with the ILC positron source results. In addition, studies on mesh grid size for PEDD estimation and matching of positron beam to the latest design of the injector linac are also presented. Positrons can be transported in the matched injector linac almost without losses, with a final accepted yield of 2.14 e+/e-.
- Published
- 2020
18. Thermal control for the two-beam module of the compact linear collider with computational fluid dynamics simulations of conjugate heat transfer problems, with subsidiary finite-element simulations
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Lam, Cheuk Wing Edmond, Vamvakas, Alex, Aicheler, Markus, Vainola, Jukka Ilmari, and Doebert, Steffen
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Physics::Accelerator Physics ,Accelerators and Storage Rings - Abstract
Conjugate heat transfer simulations were performed for the two-beam module of the Compact Linear Collider (CLIC). A full approach using ANSYS Fluent is presented for the determination of heat dissipation values from the main beam portion of the module to the cooling air and water. A transient model for heat dissipated through the tunnel to the outside soil is presented as well. Structural stress-strain simulations and modal analyses were performed for the adjustable supports with the finite-element method using ANSYS Mechanical. The operating range of the adjustable supports was determined.
- Published
- 2018
19. AWAKE++: The AWAKE Acceleration Scheme for New Particle Physics Experiments at CERN
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Gschwendtner, Edda, Bartmann, Wolfgang, Caldwell, Allen Christopher, Calviani, Marco, Chappell, James Anthony, Crivelli, Paolo, Damerau, Heiko, Depero, Emilio, Doebert, Steffen, Gall, Jonathan, Gninenko, Sergei, Goddard, Brennan, Hessler, Christoph, Hartin, Anthony, Keeble, Fearghus Robert, Osborne, John Andrew, Pardons, Ans, Petrenko, Alexey, Scaachi, Adam, and Wing, Matthew
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Physics::Accelerator Physics ,Accelerators and Storage Rings - Abstract
The AWAKE experiment reached all planned milestones during Run 1 (2016-18), notably the demonstration of strong plasma wakes generated by proton beams and the acceleration of externally injected electrons to multi-GeV energy levels in the proton driven plasma wakefields. During Run~2 (2021 - 2024) AWAKE aims to demonstrate the scalability and the acceleration of electrons to high energies while maintaining the beam quality. Assuming continued success of the AWAKE program, AWAKE will be in the position to use the AWAKE scheme for particle physics applications such as fixed target experiments for dark photon searches and also for future electron-proton or electron-ion colliders. With strong support from the accelerator and high energy physics community, these experiments could be installed during CERN LS3; integration and beam line design studies show the feasibility of a fixed target experiment in the AWAKE facility, downstream of the AWAKE experiment in the former CNGS area. The expected electrons on target for fixed target experiments exceeds the electrons on target by three to four orders of magnitude with respect to the current NA64 experiment, making it a very promising experiment in the search for new physics. Studies show that electrons can be accelerated to 70 GeV in a 130 m long plasma cell installed in an extended TI 2 extraction tunnel from SPS to the LHC and transported to collision with protons/ions from the LHC. The experiment would focus on studies of the structure of matter and QCD in a new kinematic domain. The AWAKE scheme offers great potential for future high energy physics applications and it is the right moment now to support further development of this technology leading to unique facilities.
- Published
- 2018
20. Finite Element Model for Thermal-Structural analysis of CLIC Lab Module type 0#2
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Moilanen, Antti, Aicheler, Markus, Vamvakas, Alex, Vainola, Jukka Ilmari, and Doebert, Steffen
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Physics::Accelerator Physics ,Accelerators and Storage Rings - Abstract
Temperature changes lead to unwanted thermo-mechanical deformations in the components of the Compact Linear Collider (CLIC) module. There are several sources and sinks of heat around the CLIC two-beam module. Heat is generated in the components that produce, transfer, and extract radio frequency (RF) power. Excess heat is removed from the components by cooling water as well as dissipated to air by convection from the outer surfaces of the components. The ambient temperature might also vary along the tunnel during the operation of CLIC. Due to tight assembling and alignment tolerances, it is necessary to minimize the thermo-mechanical deformations in the components. In this paper, the steps of thermal-structural Finite Element Analysis (FEA) of CLIC lab module type 0#2 are described from geometry model simplification to setting up the simulation. The description is accompanied by useful hints for CATIA and ANSYS users performing similar modelling tasks. A reliable computer simulation is important for studying the effects of different operational parameters as well as evaluating future two-beam module designs.
- Published
- 2017
21. Commissioning of beam instrumentation at the CERN AWAKE facility after integration of the electron beam line
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Gorgisyan, Ishkhan, primary, Mazzoni, Stefano, additional, Burger, Stephane, additional, Jensen, Lars, additional, Jensen, Steen, additional, Medina, David, additional, Wendt, Manfred, additional, Soby, Lars, additional, Gschwendtner, Edda, additional, Gessner, Spencer, additional, Doebert, Steffen, additional, Pepitone, Kevin, additional, Bracco, Chiara, additional, Velotti, Francesco, additional, Keeble, Fearghus, additional, Wing, Matthew, additional, Jolly, Simon, additional, Cascella, Michele, additional, and Verzilov, Victor, additional
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- 2018
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22. Towards TeV-scale electron-positron collisions: the Compact Linear Collider (CLIC)
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Doebert, Steffen, primary and Sicking, Eva, additional
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- 2018
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23. Low-level feedback control for the phase regulation of CLIC Drive Beam Klystrons
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Daskalaki, Eleni and Doebert, Steffen
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Accelerators and Storage Rings - Abstract
The requirement of luminosity loss below 1% raises tight tolerances for the phase and power stability of the CLIC drive beam (DB) klystrons and consequently for the high voltage pulse ripple of the modulators. A low-level RF (LLRF) feedback system needs to be developed and combined with the modulator in order to guarantee the phase and amplitude tolerances. To this aim, three feedback control strategies were investigated, i) Proportional Integral (PI) controller, ii) Linear Quadratic Integral Regulator (LQI) and iii) Model Predictive Controller (MPC). The klystron, as well as the incident phase noise were modelled and used for the design and evaluation of the controllers. First simulation results are presented along with future steps and directions.
- Published
- 2015
24. Studies of Cs3Sb cathodes for the CLIC drive beam photo injector option
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Martini, Irene, Chevallay, Eric, Doebert, Steffen, Fedosseev, Valentine, Hessler, Christoph, and Martyanov, Mikhail
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Accelerators and Storage Rings - Abstract
Within the CLIC (Compact Linear Collider) project, feasibility studies of a photo injector option for the drive beam as an alternative to its baseline design using a thermionic electron gun are on-going. This R&D program covers both the laser and the photocathode side. Whereas the available laser pulse energy in ultra-violet (UV) is currently limited by the optical defects in the 4thharmonics frequency conversion crystal induced by the0.14 ms long pulse trains, recent measurements of Cs3Sbphotocathodes sensitive to green light showed their potential to overcome this limitation. Moreover, using visible laser beams leads to better stability of produced electron bunches and one can take advantages of the availability of higher quality optics. The studied Cs3Sbphotocathodes have been produced in the CERN photo emission laboratory using the co-deposition technique and tested in a DC gun set-up. The analysis of data acquired during the cathode production process will be presented in this paper, as well as the results of lifetime measurements in the DC gun
- Published
- 2013
25. Production of long bunch trains with 4.5muC total charge using a photoinjector
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Mete, Oznur, Chevallay, Eric, Csatari, Marta, Dabrowski, Anne, Doebert, Steffen, Egger, Daniel, Fedosseev, Valentine, Olvegaard, Maja, and Petrarca, Massimo
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Accelerators and Storage Rings - Published
- 2012
26. Production of long bunch trains with 4.5 mu C total charge using a photoinjector
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Mete, Oznur, Chevallay, Eric, Csatari, Marta, Dabrowski, Anne, Doebert, Steffen, Egger, Daniel, Fedosseev, Valentine, Olvegaard, Maja, and Petrarca, Massimo
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Injector Design ,Physics::Accelerator Physics ,Laser ,Photo-Injector - Abstract
A photoinjector, PHIN (PHotoINjector), has been realized at CERN by a joint effort of several institutes within the European Coordinated Accelerator Research in Europe program. The test facility has been installed and commissioned at CERN with the aim to demonstrate the beam parameters needed for the CLIC Test Facility 3 (CTF3). This beam is unique with respect to its long bunch train and high average charge per bunch requirements. The nominal beam for CTF3 consists of 1908 bunches each having a 2.33 nC charge and a bunch frequency of 1.5 GHz. Thus, a total charge of similar to 4.4 mu C has to be extracted and accelerated. The stability of the intensity and the beam parameters along this exceptionally high average current train is crucial for the correct functioning of the CLIC drive beam scheme. Consequently, extensive time-resolved measurements of the transverse and longitudinal beam parameters have been developed, optimized, and performed. The shot-to-shot intensity stability has been studied in detail for the electron and the laser beams, simultaneously. The PHIN photoinjector has been commissioned between 2008 and 2010 during intermittent operations. This paper reports on the obtained results in order to demonstrate the feasibility and the stability of the required beam parameters.
- Published
- 2012
27. Results from the CLIC X-BAND structure test program at the NLCTA
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Adolphsen, Chris, Bowden, Gordon, Dolgashev, Valery, Laurent, Lisa, Tantawi, Sami, Wang, Faya, Wang, W Juwen, Doebert, Steffen, Grudiev, Alexej, Riddone, Germana, Wuensh, Walter, Zennaro, Riccardo, Higashi, Yasuo, and Higo, Toshiyasu
- Subjects
Accelerators and Storage Rings - Abstract
As part of a SLAC-CERN-KEK collaboration on high gradient X-band structure research, several prototype structures for the CLIC linear collider study have been tested using two of the high power (300 MW) X-band rf stations in the NLCTA facility at SLAC. These structures differ in terms of their manufacturing (brazed disks and clamped quadrants), gradient profile (amount by which the gradient increases along the structure which optimizes efficiency and maximizes sustainable gradient) and HOM damping (use of slots or waveguides to rapidly dissipate dipole mode energy). The CLIC goal in the next few years is to demonstrate the feasibility of a CLIC-ready baseline design and to investigate alternatives which could bring even higher efficiency. This paper summarizes the high gradient test results from the NLCTA in support of this effort.
- Published
- 2011
28. TOWARDS TEV-SCALE ELECTRON-POSITRON COLLISIONS COMPACT LINEAR COLLIDER (CLIC).
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Doebert, Steffen and Sicking, Eva
- Subjects
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ELECTRON-positron interactions , *LINEAR accelerators , *STATISTICAL accuracy , *ENERGY measurement - Abstract
The Compact Linear Collider (CLIC), a future electron-positron collider at the energy frontier, has the potential to change our understanding of the universe. Proposed to follow the Large Hardron Collider (LHC) programme at CERN, it is conceived for precision measurements as well as for searches for new phenomena. [ABSTRACT FROM AUTHOR]
- Published
- 2018
- Full Text
- View/download PDF
29. Production of long bunch trains with4.5 μCtotal charge using a photoinjector
- Author
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Mete, Oznur, primary, Chevallay, Eric, additional, Csatari, Marta, additional, Dabrowski, Anne, additional, Doebert, Steffen, additional, Egger, Daniel, additional, Fedosseev, Valentine, additional, Olvegaard, Maja, additional, and Petrarca, Massimo, additional
- Published
- 2012
- Full Text
- View/download PDF
30. PHIN photo-injector as the CLIC drive beam source
- Author
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Chevallay, Eric, primary, Csatari, Marta, additional, Dabrowski, Anne, additional, Doebert, Steffen, additional, Egger, Daniel, additional, Fedosseev, Valentine, additional, Mete, Oznur, additional, Olvegaard, Maja, additional, and Petrarca, Massimo, additional
- Published
- 2012
- Full Text
- View/download PDF
31. XLS - D3.1: Preliminary assessments and evaluations of the optimum e-gun and injector solution for the CompactLight design
- Author
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Ferrario, Massimo, Alesini, David, Cardelli, Fabio, Castorina, Giovanni, Croia, Michele, Diomede, Marco, Gallo, Alessandro, Giribono, Anna, Scifo, Jessica, Spataro, Bruno, Vaccarezza, Cristina, Vannozzi, Alessandro, Di Mitri, Simone, Rochow, Regina, Latina, Andrea, Kelisani, Mohsen Dayyani, Doebert, Steffen, Angal-Kalinin, Deepa, Clarke, Jim, Gazis, Evangelos, Aksoy, Avni, Luiten, Jom, Rajabi, Ali, Stragier, Xavier, Faus-Golfe, Angeles, Han, Yanliang, Esperante, Daniel, Boronat, Marçà, Blanch, César, Fuster, Juan, Gimeno, Benito, and Gerardo D'Auria
- Subjects
CompactLight ,RF gun photo-injector ,X-ray Free Electron Lasers ,X-band technology ,Compact Accelerators ,7. Clean energy - Abstract
In this deliverable we report an overview of the possible injector options suitable to match the CompactLight X-band high brightness linac able to drive short wavelength FELs user facilities. Different schemes have been investigated including RF gun injectors at different operating frequency (S, C and X band) and a DC gun based design. The electromagnetic and RF designs for all cases are reported and discussed, including a preliminary evaluation of the laser/cathode system requirements. Matchings with the downstream linac are also investigated with beam dynamics simulations. State of the art S-band injectors look appropriate to achieve the required parameters at low repetition rate ( 100 Hz). On the other end a compact C-band (or X-band) RF gun design is expected to have even better performances at low repetition rates and moreover, due to the lower thermal load, could allow higher repetition rates operation, up to 1 kHz, with acceptable performances degradation. DC guns are also very promising solutions for kHz range operation.
32. XLS - D3.1: Preliminary assessments and evaluations of the optimum e-gun and injector solution for the CompactLight design
- Author
-
Ferrario, Massimo, Alesini, David, Cardelli, Fabio, Castorina, Giovanni, Croia, Michele, Diomede, Marco, Gallo, Alessandro, Giribono, Anna, Scifo, Jessica, Spataro, Bruno, Vaccarezza, Cristina, Vannozzi, Alessandro, Di Mitri, Simone, Rochow, Regina, Latina, Andrea, Kelisani, Mohsen Dayyani, Doebert, Steffen, Angal-Kalinin, Deepa, Clarke, Jim, Gazis, Evangelos, Aksoy, Avni, Luiten, Jom, Rajabi, Ali, Stragier, Xavier, Faus-Golfe, Angeles, Han, Yanliang, Esperante, Daniel, Boronat, Marçà, Blanch, César, Fuster, Juan, and Gimeno, Benito
- Subjects
CompactLight ,RF gun photo-injector ,X-ray Free Electron Lasers ,X-band technology ,Compact Accelerators ,7. Clean energy - Abstract
In this deliverable we report an overview of the possible injector options suitable to match the CompactLight X-band high brightness linac able to drive short wavelength FELs user facilities. Different schemes have been investigated including RF gun injectors at different operating frequency (S, C and X band) and a DC gun based design. The electromagnetic and RF designs for all cases are reported and discussed, including a preliminary evaluation of the laser/cathode system requirements. Matchings with the downstream linac are also investigated with beam dynamics simulations. State of the art S-band injectors look appropriate to achieve the required parameters at low repetition rate ( 100 Hz). On the other end a compact C-band (or X-band) RF gun design is expected to have even better performances at low repetition rates and moreover, due to the lower thermal load, could allow higher repetition rates operation, up to 1 kHz, with acceptable performances degradation. DC guns are also very promising solutions for kHz range operation., On behalf of the CompactLight Collaboration
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