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2. The Compact Linear Collider (CLIC) - 2018 Summary Report

Author

CLIC, The, collaborations, CLICdp, Charles, T. K., Giansiracusa, P. J., Lucas, T. G., Rassool, R. P., Volpi, M., Balazs, C., Afanaciev, K., Makarenko, V., Patapenka, A., Zhuk, I., Collette, C., Boland, M. J., Hoffman, A. C. Abusleme, Diaz, M. A., Garay, F., Chi, Y., He, X., Pei, G., Pei, S., Shu, G., Wang, X., Zhang, J., Zhao, F., Zhou, Z., Chen, H., Gao, Y., Huang, W., Kuang, Y. P., Li, B., Li, Y., Meng, X., Shao, J., Shi, J., Tang, C., Wang, P., Wu, X., Zha, H., Ma, L., Han, Y., Fang, W., Gu, Q., Huang, D., Huang, X., Tan, J., Wang, Z., Zhao, Z., Uggerhøj, U. I., Wistisen, T. N., Aabloo, A., Aare, R., Kuppart, K., Vigonski, S., Zadin, V., Aicheler, M., Baibuz, E., Brücken, E., Djurabekova, F., Eerola, P., Garcia, F., Haeggström, E., Huitu, K., Jansson, V., Kassamakov, I., Kimari, J., Kyritsakis, A., Lehti, S., Meriläinen, A., Montonen, R., Nordlund, K., Österberg, K., Saressalo, A., Väinölä, J., Veske, M., Farabolini, W., Mollard, A., Peauger, F., Plouin, J., Bambade, P., Chaikovska, I., Chehab, R., Delerue, N., Davier, M., Faus-Golfe, A., Irles, A., Kaabi, W., LeDiberder, F., Pöschl, R., Zerwas, D., Aimard, B., Balik, G., Blaising, J. -J., Brunetti, L., Chefdeville, M., Dominjon, A., Drancourt, C., Geoffroy, N., Jacquemier, J., Jeremie, A., Karyotakis, Y., Nappa, J. M., Serluca, M., Vilalte, S., Vouters, G., Bernhard, A., Bründermann, E., Casalbuoni, S., Hillenbrand, S., Gethmann, J., Grau, A., Huttel, E., Müller, A. -S., Peiffer, P., Perić, I., de Jauregui, D. Saez, Emberger, L., Graf, C., Simon, F., Szalay, M., van der Kolk, N., Brass, S., Kilian, W., Alexopoulos, T., Apostolopoulos, T., Gazis, E. N., Gazis, N., Kostopoulos, V., Kourkoulis, S., Heilig, B., Lichtenberger, J., Shrivastava, P., Dayyani, M. K., Ghasem, H., Hajari, S. S., Shaker, H., Ashkenazy, Y., Popov, I., Engelberg, E., Yashar, A., Abramowicz, H., Benhammou, Y., Borysov, O., Borysova, M., Levy, A., Levy, I., Alesini, D., Bellaveglia, M., Buonomo, B., Cardelli, A., Diomede, M., Ferrario, M., Gallo, A., Ghigo, A., Giribono, A., Piersanti, L., Stella, A., Vaccarezza, C., de Blas, J., Franceschini, R., D'Auria, G., Di Mitri, S., Abe, T., Aryshev, A., Fukuda, M., Furukawa, K., Hayano, H., Higashi, Y., Higo, T., Kubo, K., Kuroda, S., Matsumoto, S., Michizono, S., Naito, T., Okugi, T., Shidara, T., Tauchi, T., Terunuma, N., Urakawa, J., Yamamoto, A., Raboanary, R., Luiten, O. J., Stragier, X. F. D., Hart, R., van der Graaf, H., Eigen, G., Adli, E., Lindstrøm, C. A., Lillestøl, R., Malina, L., Pfingstner, J., Sjobak, K. N., Ahmad, A., Hoorani, H., Khan, W. A., Bugiel, S., Bugiel, R., Firlej, M., Fiutowski, T. A., Idzik, M., Moroń, J., Świentek, K. P., de Renstrom, P. Brückman, Krupa, B., Kucharczyk, M., Lesiak, T., Pawlik, B., Sopicki, P., Turbiarz, B., Wojtoń, T., Zawiejski, L. K., Kalinowski, J., Nowak, K., Żarnecki, A. F., Firu, E., Ghenescu, V., Neagu, A. T., Preda, T., Zgura, I. S., Aloev, A., Azaryan, N., Boyko, I., Budagov, J., Chizhov, M., Filippova, M., Glagolev, V., Gongadze, A., Grigoryan, S., Gudkov, D., Karjavine, V., Lyablin, M., Nefedov, Yu., Olyunin, A., Rymbekova, A., Samochkine, A., Sapronov, A., Shelkov, G., Shirkov, G., Soldatov, V., Solodko, E., Trubnikov, G., Tyapkin, I., Uzhinsky, V., Vorozhtov, A., Zhemchugov, A., Levichev, E., Mezentsev, N., Piminov, P., Shatilov, D., Vobly, P., Zolotarev, K., Jelisavčić, I. Božović, Kačarević, G., Dumbelović, G. Milutinović, Pandurović, M., Radulović, M., Stevanović, J., Vukasinović, N., Lee, D. -H., Ayala, N., Benedetti, G., Guenzel, T., Iriso, U., Marti, Z., Perez, F., Pont, M., Trenado, J., Ruiz-Jimeno, A., Vila, I., Calero, J., Dominguez, M., Garcia-Tabares, L., Gavela, D., Lopez, D., Toral, F., Gutierrez, C. Blanch, Boronat, M., Esperante, D., Fullana, E., Fuster, J., García, I., Gimeno, B., Lopez, P. Gomis, González, D., Perelló, M., Ros, E., Villarejo, M. A., Vnuchenko, A., Vos, M., Borgmann, Ch., Brenner, R., Ekelöf, T., Jacewicz, M., Olvegård, M., Ruber, R., Ziemann, V., Aguglia, D., Gonzalvo, J. Alabau, Leon, M. Alcaide, Tehrani, N. Alipour, Anastasopoulos, M., Andersson, A., Andrianala, F., Antoniou, F., Apyan, A., Arominski, D., Artoos, K., Assly, S., Atieh, S., Baccigalupi, C., Sune, R. Ballabriga, Caballero, D. Banon, Barnes, M. J., Garcia, J. Barranco, Bartalesi, A., Bauche, J., Bayar, C., Belver-Aguilar, C., Morell, A. Benot, Bernardini, M., Bett, D. R., Bettoni, S., Bettencourt, M., Bielawski, B., Garcia, O. Blanco, Kraljevic, N. Blaskovic, Bolzon, B., Bonnin, X. A., Bozzini, D., Branger, E., Brondolin, E., Brunner, O., Buckland, M., Bursali, H., Burkhardt, H., Caiazza, D., Calatroni, S., Campbell, M., Lasheras, N. Catalan, Cassany, B., Castro, E., Soares, R. H. Cavaleiro, Bastos, M. Cerqueira, Cherif, A., Chevallay, E., Cilento, V., Corsini, R., Costa, R., Cure, B., Curt, S., Gobbo, A. Dal, Dannheim, D., Daskalaki, E., Deacon, L., Degiovanni, A., De Michele, G., De Oliveira, L., Romano, V. Del Pozo, Delahaye, J. P., Delikaris, D., de Almeida, P. G. Dias, Dobers, T., Doebert, S., Doytchinov, I., Draper, M., Ramos, F. Duarte, Duquenne, M., Plaja, N. Egidos, Elsener, K., Esberg, J., Esposito, M., Evans, L., Fedosseev, V., Ferracin, P., Fiergolski, A., Foraz, K., Fowler, A., Friebel, F., Fuchs, J-F., Gaddi, A., Gamba, D., Fajardo, L. Garcia, Morales, H. Garcia, Garion, C., Gasior, M., Gatignon, L., Gayde, J-C., Gerbershagen, A., Gerwig, H., Giambelli, G., Gilardi, A., Goldblatt, A. N., Anton, S. Gonzalez, Grefe, C., Grudiev, A., Guerin, H., Guillot-Vignot, F. G., Gutt-Mostowy, M. L., Lutz, M. Hein, Hessler, C., Holma, J. K., Holzer, E. B., Hourican, M., Hynds, D., Ikarios, E., Levinsen, Y. Inntjore, Janssens, S., Jeff, A., Jensen, E., Jonker, M., Kamugasa, S. W., Kastriotou, M., Kemppinen, J. M. K., Khan, V., Kieffer, R. B., Klempt, W., Kokkinis, N., Kossyvakis, I., Kostka, Z., Korsback, A., Platia, E. Koukovini, Kovermann, J. W., Kozsar, C-I., Kremastiotis, I., Kröger, J., Kulis, S., Latina, A., Leaux, F., Lebrun, P., Lefevre, T., Leogrande, E., Linssen, L., Liu, X., Cudie, X. Llopart, Magnoni, S., Maidana, C., Maier, A. A., Durand, H. Mainaud, Mallows, S., Manosperti, E., Marelli, C., Lacoma, E. Marin, Marsh, S., Martin, R., Martini, I., Martyanov, M., Mazzoni, S., Mcmonagle, G., Mether, L. M., Meynier, C., Modena, M., Moilanen, A., Mondello, R., Cabral, P. B. Moniz, Irazabal, N. Mouriz, Munker, M., Muranaka, T., Nadenau, J., Navarro, J. G., Quirante, J. L. Navarro, Del Busto, E. Nebo, Nikiforou, N., Ninin, P., Nonis, M., Nisbet, D., Nuiry, F. X., Nürnberg, A., Ögren, J., Osborne, J., Ouniche, A. C., Pan, R., Papadopoulou, S., Papaphilippou, Y., Paraskaki, G., Pastushenko, A., Passarelli, A., Patecki, M., Pazdera, L., Pellegrini, D., Pepitone, K., Codina, E. Perez, Fontenla, A. Perez, Persson, T. H. B., Petrič, M., Pitman, S., Pitters, F., Pittet, S., Plassard, F., Popescu, D., Quast, T., Rajamak, R., Redford, S., Remandet, L., Renier, Y., Rey, S. F., Orozco, O. Rey, Riddone, G., Castro, E. Rodriguez, Roloff, P., Rossi, C., Rossi, F., Rude, V., Ruehl, I., Rumolo, G., Sailer, A., Sandomierski, J., Santin, E., Sanz, C., Bedolla, J. Sauza, Schnoor, U., Schmickler, H., Schulte, D., Senes, E., Serpico, C., Severino, G., Shipman, N., Sicking, E., Simoniello, R., Skowronski, P. K., Mompean, P. Sobrino, Soby, L., Sollander, P., Solodko, A., Sosin, M. P., Spannagel, S., Sroka, S., Stapnes, S., Sterbini, G., Stern, G., Ström, R., Stuart, M. J., Syratchev, I., Szypula, K., Tecker, F., Thonet, P. A., Thrane, P., Timeo, L., Tiirakari, M., Garcia, R. Tomas, Tomoiaga, C. I., Valerio, P., Vaňát, T., Vamvakas, A. L., Van Hoorne, J., Viazlo, O., Pinto, M. Vicente Barreto, Vitoratou, N., Vlachakis, V., Weber, M. A., Wegner, R., Wendt, M., Widorski, M., Williams, O. E., Williams, M., Woolley, B., Wuensch, W., Wulzer, A., Uythoven, J., Xydou, A., Yang, R., Zelios, A., Zhao, Y., Zisopoulos, P., Benoit, M., Sultan, D M S, Riva, F., Bopp, M., Braun, H. H., Craievich, P., Dehler, M., Garvey, T., Pedrozzi, M., Raguin, J. Y., Rivkin, L., Zennaro, R., Guillaume, S., Rothacher, M., Aksoy, A., Nergiz, Z., Yavas, Ö., Denizli, H., Keskin, U., Oyulmaz, K. Y., Senol, A., Ciftci, A. K., Baturin, V., Karpenko, O., Kholodov, R., Lebed, O., Lebedynskyi, S., Mordyk, S., Musienko, I., Profatilova, Ia., Storizhko, V., Bosley, R. R., Price, T., Watson, M. F., Watson, N. K., Winter, A. G., Goldstein, J., Green, S., Marshall, J. S., Thomson, M. A., Xu, B., You, T., Gillespie, W. A., Spannowsky, M., Beggan, C., Martin, V., Zhang, Y., Protopopescu, D., Robson, A., Apsimon, R. J., Bailey, I., Burt, G. C., Dexter, A. C., Edwards, A. V., Hill, V., Jamison, S., Millar, W. L., Papke, K., Casse, G., Vossebeld, J., Aumeyr, T., Bergamaschi, M., Bobb, L., Bosco, A., Boogert, S., Boorman, G., Cullinan, F., Gibson, S., Karataev, P., Kruchinin, K., Lekomtsev, K., Lyapin, A., Nevay, L., Shields, W., Snuverink, J., Towler, J., Yamakawa, E., Boisvert, V., West, S., Jones, R., Joshi, N., Bett, D., Bodenstein, R. M., Bromwich, T., Burrows, P. N., Christian, G. B., Gohil, C., Korysko, P., Paszkiewicz, J., Perry, C., Ramjiawan, R., Roberts, J., Coates, T., Salvatore, F., Bainbridge, A., Clarke, J. A., Krumpa, N., Shepherd, B. J. A., Walsh, D., Chekanov, S., Demarteau, M., Gai, W., Liu, W., Metcalfe, J., Power, J., Repond, J., Weerts, H., Xia, L., Zupan, J., Wells, J. D., Zhang, Z., Adolphsen, C., Barklow, T., Dolgashev, V., Franzi, M., Graf, N., Hewett, J., Kemp, M., Kononenko, O., Markiewicz, T., Moffeit, K., Neilson, J., Nosochkov, Y., Oriunno, M., Phinney, N., Rizzo, T., Tantawi, S., Wang, J., Weatherford, B., White, G., and Woodley, M.

Subjects
Physics - Accelerator Physics
Abstract

The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^-$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively. CLIC uses a two-beam acceleration scheme, in which 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept has been refined using improved software tools. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations and parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25-30 years., Comment: 112 pages, 59 figures; published as CERN Yellow Report Monograph Vol. 2/2018; corresponding editors: Philip N. Burrows, Nuria Catalan Lasheras, Lucie Linssen, Marko Petri\v{c}, Aidan Robson, Daniel Schulte, Eva Sicking, Steinar Stapnes

Published
2018
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3. Updated baseline for a staged Compact Linear Collider

Author

CLIC, The, collaborations, CLICdp, Boland, M. J., Felzmann, U., Giansiracusa, P. J., Lucas, T. G., Rassool, R. P., Balazs, C., Charles, T. K., Afanaciev, K., Emeliantchik, I., Ignatenko, A., Makarenko, V., Shumeiko, N., Patapenka, A., Zhuk, I., Hoffman, A. C. Abusleme, Gutierrez, M. A. Diaz, Gonzalez, M. Vogel, Chi, Y., He, X., Pei, G., Pei, S., Shu, G., Wang, X., Zhang, J., Zhao, F., Zhou, Z., Chen, H., Gao, Y., Huang, W., Kuang, Y. P., Li, B., Li, Y., Shao, J., Shi, J., Tang, C., Wu, X., Ma, L., Han, Y., Fang, W., Gu, Q., Huang, D., Huang, X., Tan, J., Wang, Z., Zhao, Z., Laštovička, T., Uggerhoj, U., Wistisen, T. N., Aabloo, A., Eimre, K., Kuppart, K., Vigonski, S., Zadin, V., Aicheler, M., Baibuz, E., Brücken, E., Djurabekova, F., Eerola, P., Garcia, F., Haeggström, E., Huitu, K., Jansson, V., Karimaki, V., Kassamakov, I., Kyritsakis, A., Lehti, S., Meriläinen, A., Montonen, R., Niinikoski, T., Nordlund, K., Österberg, K., Parekh, M., Törnqvist, N. A., Väinölä, J., Veske, M., Farabolini, W., Mollard, A., Napoly, O., Peauger, F., Plouin, J., Bambade, P., Chaikovska, I., Chehab, R., Davier, M., Kaabi, W., Kou, E., LeDiberder, F., Pöschl, R., Zerwas, D., Aimard, B., Balik, G., Baud, J. -P., Blaising, J. -J., Brunetti, L., Chefdeville, M., Drancourt, C., Geoffroy, N., Jacquemier, J., Jeremie, A., Karyotakis, Y., Nappa, J. M., Vilalte, S., Vouters, G., Bernard, A., Peric, I., Gabriel, M., Simon, F., Szalay, M., van der Kolk, N., Alexopoulos, T., Gazis, E. N., Gazis, N., Ikarios, E., Kostopoulos, V., Kourkoulis, S., Gupta, P. D., Shrivastava, P., Arfaei, H., Dayyani, M. K., Ghasem, H., Hajari, S. S., Shaker, H., Ashkenazy, Y., Abramowicz, H., Benhammou, Y., Borysov, O., Kananov, S., Levy, A., Levy, I., Rosenblat, O., D'Auria, G., Di Mitri, S., Abe, T., Aryshev, A., Higo, T., Makida, Y., Matsumoto, S., Shidara, T., Takatomi, T., Takubo, Y., Tauchi, T., Toge, N., Ueno, K., Urakawa, J., Yamamoto, A., Yamanaka, M., Raboanary, R., Hart, R., van der Graaf, H., Eigen, G., Zalieckas, J., Adli, E., Lillestøl, R., Malina, L., Pfingstner, J., Sjobak, K. N., Ahmed, W., Asghar, M. I., Hoorani, H., Bugiel, S., Dasgupta, R., Firlej, M., Fiutowski, T. A., Idzik, M., Kopec, M., Kuczynska, M., Moron, J., Swientek, K. P., Daniluk, W., Krupa, B., Kucharczyk, M., Lesiak, T., Moszczynski, A., Pawlik, B., Sopicki, P., Wojtoń, T., Zawiejski, L., Kalinowski, J., Krawczyk, M., Żarnecki, A. F., Firu, E., Ghenescu, V., Neagu, A. T., Preda, T., Zgura, I-S., Aloev, A., Azaryan, N., Budagov, J., Chizhov, M., Filippova, M., Glagolev, V., Gongadze, A., Grigoryan, S., Gudkov, D., Karjavine, V., Lyablin, M., Olyunin, A., Samochkine, A., Sapronov, A., Shirkov, G., Soldatov, V., Solodko, A., Solodko, E., Trubnikov, G., Tyapkin, I., Uzhinsky, V., Vorozhtov, A., Levichev, E., Mezentsev, N., Piminov, P., Shatilov, D., Vobly, P., Zolotarev, K., Jelisavcic, I. Bozovic, Kacarevic, G., Lukic, S., Milutinovic-Dumbelovic, G., Pandurovic, M., Iriso, U., Perez, F., Pont, M., Trenado, J., Aguilar-Benitez, M., Calero, J., Garcia-Tabares, L., Gavela, D., Gutierrez, J. L., Lopez, D., Toral, F., Moya, D., Jimeno, A. Ruiz, Vila, I., Argyropoulos, T., Gutierrez, C. Blanch, Boronat, M., Esperante, D., Faus-Golfe, A., Fuster, J., Martinez, N. Fuster, Muñoz, N. Galindo, García, I., Navarro, J. Giner, Ros, E., Vos, M., Brenner, R., Ekelöf, T., Jacewicz, M., Ögren, J., Olvegård, M., Ruber, R., Ziemann, V., Aguglia, D., Tehrani, N. Alipour, Andersson, A., Andrianala, F., Antoniou, F., Artoos, K., Atieh, S., Sune, R. Ballabriga, Barnes, M. J., Garcia, J. Barranco, Bartosik, H., Belver-Aguilar, C., Morell, A. Benot, Bett, D. R., Bettoni, S., Blanchot, G., Garcia, O. Blanco, Bonnin, X. A., Brunner, O., Burkhardt, H., Calatroni, S., Campbell, M., Lasheras, N. Catalan, Bastos, M. Cerqueira, Cherif, A., Chevallay, E., Constance, B., Corsini, R., Cure, B., Curt, S., Dalena, B., Dannheim, D., De Michele, G., De Oliveira, L., Deelen, N., Delahaye, J. P., Dobers, T., Doebert, S., Draper, M., Ramos, F. Duarte, Dubrovskiy, A., Elsener, K., Esberg, J., Esposito, M., Fedosseev, V., Ferracin, P., Fiergolski, A., Foraz, K., Fowler, A., Friebel, F., Fuchs, J-F., Rojas, C. A. Fuentes, Gaddi, A., Fajardo, L. Garcia, Morales, H. Garcia, Garion, C., Gatignon, L., Gayde, J-C., Gerwig, H., Goldblatt, A. N., Grefe, C., Grudiev, A., Guillot-Vignot, F. G., Gutt-Mostowy, M. L., Hauschild, M., Hessler, C., Holma, J. K., Holzer, E., Hourican, M., Hynds, D., Levinsen, Y. Inntjore, Jeanneret, B., Jensen, E., Jonker, M., Kastriotou, M., Kemppinen, J. M. K., Kieffer, R. B., Klempt, W., Kononenko, O., Korsback, A., Platia, E. Koukovini, Kovermann, J. W., Kozsar, C-I., Kremastiotis, I., Kulis, S., Latina, A., Leaux, F., Lebrun, P., Lefevre, T., Linssen, L., Cudie, X. Llopart, Maier, A. A., Durand, H. Mainaud, Manosperti, E., Marelli, C., Lacoma, E. Marin, Martin, R., Mazzoni, S., Mcmonagle, G., Mete, O., Mether, L. M., Modena, M., Münker, R. M., Muranaka, T., Del Busto, E. Nebot, Nikiforou, N., Nisbet, D., Nonglaton, J-M., Nuiry, F. X., Nürnberg, A., Olvegard, M., Osborne, J., Papadopoulou, S., Papaphilippou, Y., Passarelli, A., Patecki, M., Pazdera, L., Pellegrini, D., Pepitone, K., Codina, E. Perez, Fontenla, A. Perez, Persson, T. H. B., Petrič, M., Pitters, F., Pittet, S., Plassard, F., Rajamak, R., Redford, S., Renier, Y., Rey, S. F., Riddone, G., Rinolfi, L., Castro, E. Rodriguez, Roloff, P., Rossi, C., Rude, V., Rumolo, G., Sailer, A., Santin, E., Schlatter, D., Schmickler, H., Schulte, D., Shipman, N., Sicking, E., Simoniello, R., Skowronski, P. K., Mompean, P. Sobrino, Soby, L., Sosin, M. P., Sroka, S., Stapnes, S., Sterbini, G., Ström, R., Syratchev, I., Tecker, F., Thonet, P. A., Timeo, L., Timko, H., Garcia, R. Tomas, Valerio, P., Vamvakas, A. L., Vivoli, A., Weber, M. A., Wegner, R., Wendt, M., Woolley, B., Wuensch, W., Uythoven, J., Zha, H., Zisopoulos, P., Benoit, M., Pinto, M. Vicente Barreto, Bopp, M., Braun, H. H., Divall, M. Csatari, Dehler, M., Garvey, T., Raguin, J. Y., Rivkin, L., Zennaro, R., Aksoy, A., Nergiz, Z., Pilicer, E., Tapan, I., Yavas, O., Baturin, V., Kholodov, R., Lebedynskyi, S., Miroshnichenko, V., Mordyk, S., Profatilova, I., Storizhko, V., Watson, N., Winter, A., Goldstein, J., Green, S., Marshall, J. S., Thomson, M. A., Xu, B., Gillespie, W. A., Pan, R., Tyrk, M. A, Protopopescu, D., Robson, A., Apsimon, R., Bailey, I., Burt, G., Constable, D., Dexter, A., Karimian, S., Lingwood, C., Buckland, M. D., Casse, G., Vossebeld, J., Bosco, A., Karataev, P., Kruchinin, K., Lekomtsev, K., Nevay, L., Snuverink, J., Yamakawa, E., Boisvert, V., Boogert, S., Boorman, G., Gibson, S., Lyapin, A., Shields, W., Teixeira-Dias, P., West, S., Jones, R., Joshi, N., Bodenstein, R., Burrows, P. N., Christian, G. B., Gamba, D., Perry, C., Roberts, J., Clarke, J. A., Collomb, N. A., Jamison, S. P., Shepherd, B. J. A., Walsh, D., Demarteau, M., Repond, J., Weerts, H., Xia, L., Wells, J. D., Adolphsen, C., Barklow, T., Breidenbach, M., Graf, N., Hewett, J., Markiewicz, T., McCormick, D., Moffeit, K., Nosochkov, Y., Oriunno, M., Phinney, N., Rizzo, T., Tantawi, S., Wang, F., Wang, J., White, G., and Woodley, M.

Subjects
Physics - Accelerator Physics, High Energy Physics - Experiment
Abstract

The Compact Linear Collider (CLIC) is a multi-TeV high-luminosity linear e+e- collider under development. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in a staged approach with three centre-of-mass energy stages ranging from a few hundred GeV up to 3 TeV. The first stage will focus on precision Standard Model physics, in particular Higgs and top-quark measurements. Subsequent stages will focus on measurements of rare Higgs processes, as well as searches for new physics processes and precision measurements of new states, e.g. states previously discovered at LHC or at CLIC itself. In the 2012 CLIC Conceptual Design Report, a fully optimised 3 TeV collider was presented, while the proposed lower energy stages were not studied to the same level of detail. This report presents an updated baseline staging scenario for CLIC. The scenario is the result of a comprehensive study addressing the performance, cost and power of the CLIC accelerator complex as a function of centre-of-mass energy and it targets optimal physics output based on the current physics landscape. The optimised staging scenario foresees three main centre-of-mass energy stages at 380 GeV, 1.5 TeV and 3 TeV for a full CLIC programme spanning 22 years. For the first stage, an alternative to the CLIC drive beam scheme is presented in which the main linac power is produced using X-band klystrons., Comment: 57 pages, 27 figures, 12 tables, published as CERN Yellow Report. Updated version: Minor layout changes for print version

Published
2016
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4. Pressure-induced high-Tc superconducting phase in FeSe: correlation between anion height and Tc

Author

Okabe, H., Takeshita, N., Horigane, K., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Strongly Correlated Electrons
Abstract

In this study, we performed high-pressure electrical resistivity measurements of polycrystalline FeSe in the pressure range of 1-16.0 GPa at temperatures of 4-300 K. A precise evaluation of Tc from zero-resistivity temperatures revealed that Tc shows a slightly distorted dome-shaped curve, with maximum Tc (30 K) at 6 GPa, which is lower than a previously reported Tc value (~37 K). With the application of pressure, the temperature dependence of resistivity above Tc changes dramatically to a linear dependence; a non-Fermi-liquid-like "high-Tc" phase appears above 3 GPa. We found a striking correlation between Tc and the Se height: the lower the Se height, the more enhanced is Tc. Moreover, this relation is broadly applicable to other iron pnictides, strongly indicating that high-temperature superconductivity can appear only around the optimum anion height (~1.38A). On the basis of these results, we suggest that the anion height should be considered as a key determining factor of Tc of iron-based superconductors containing various anions., Comment: 6 pages, 6 figures

Published
2010
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5. AC susceptibility study of superconducting aluminium-doped silicon carbide

Author

Kriener, M., Muranaka, T., Akimitsu, J., and Maeno, Y.

Subjects
Condensed Matter - Superconductivity
Abstract

In 2007, type-I superconductivity in heavily boron-doped silicon carbide was discovered. The question arose, if it is possible to achieve a superconducting phase by introducing dopants different from boron. Recently, aluminum-doped silicon carbide was successfully found to superconduct by means of resistivity and DC magnetization measurements. In contrast to boron-doped silicon carbide, the aluminum doped system is treated as a type-II superconductor because of the absence of an hysteresis in data measured upon decreasing and increasing temperature in finite magnetic fields. In this paper, results of a recent AC susceptibility study on aluminum-doped silicon carbide are presented. In higher applied DC magnetic fields and at low temperatures, a weak indication of supercooling with a width of a few mK is found. This supports the conclusion that aluminum-doped silicon carbide is located near to the border between type-I and type-II superconductivity, as pointed out in a recent theoretical work, too., Comment: 2 pages, 1 figure

Published
2009
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6. Specific heat of aluminium-doped superconducting silicon carbide

Author

Kriener, M., Muranaka, T., Kikuchi, Y., Akimitsu, J., and Maeno, Y.

Subjects
Condensed Matter - Superconductivity
Abstract

The discoveries of superconductivity in heavily boron-doped diamond, silicon and silicon carbide renewed the interest in the ground states of charge-carrier doped wide-gap semiconductors. Recently, aluminium doping in silicon carbide successfully yielded a metallic phase from which at high aluminium concentrations superconductivity emerges. Here, we present a specific-heat study on superconducting aluminium-doped silicon carbide. We observe a clear jump anomaly at the superconducting transition temperature 1.5 K indicating that aluminium-doped silicon carbide is a bulk superconductor. An analysis of the jump anomaly suggests BCS-like phonon-mediated superconductivity in this system., Comment: 4 pages, 2 figures

Published
2009
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7. Superconductivity in heavily boron-doped silicon carbide

Author

Kriener, M., Muranaka, T., Kato, J., Ren, Z. A., Akimitsu, J., and Maeno, Y.

Subjects
Condensed Matter - Superconductivity
Abstract

The discoveries of superconductivity in heavily boron-doped diamond (C:B) in 2004 and silicon (Si:B) in 2006 renew the interest in the superconducting state of semiconductors. Charge-carrier doping of wide-gap semiconductors leads to a metallic phase from which upon further doping superconductivity can emerge. Recently, we discovered superconductivity in a closely related system: heavily-boron doped silicon carbide (SiC:B). The sample used for that study consists of cubic and hexagonal SiC phase fractions and hence this lead to the question which of them participates in the superconductivity. Here we focus on a sample which mainly consists of hexagonal SiC without any indication for the cubic modification by means of x-ray diffraction, resistivity, and ac susceptibility., Comment: 9 pages, 5 figures

Published
2008
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8. Superconductivity of hexagonal heavily-boron doped silicon carbide

Author

Kriener, M., Muranaka, T., Ren, Z. -A., Kato, J., Akimitsu, J., and Maeno, Y.

Subjects
Condensed Matter - Superconductivity
Abstract

In 2004 the discovery of superconductivity in heavily boron-doped diamond (C:B) led to an increasing interest in the superconducting phases of wide-gap semiconductors. Subsequently superconductivity was found in heavily boron-doped cubic silicon (Si:B) and recently in the stochiometric ''mixture'' of heavily boron-doped silicon carbide (SiC:B). The latter system surprisingly exhibits type-I superconductivity in contrast to the type-II superconductors C:B and Si:B. Here we will focus on the specific heat of two different superconducting samples of boron-doped SiC. One of them contains cubic and hexagonal SiC whereas the other consists mainly of hexagonal SiC without any detectable cubic phase fraction. The electronic specific heat in the superconducting state of both samples SiC:B can be described by either assuming a BCS-type exponentional temperature dependence or a power-law behavior., Comment: 4 pages, 1 figures

Published
2008
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9. Specific heat and electronic states of superconducting boron-doped silicon carbide

Author

Kriener, M., Maeno, Y., Oguchi, T., Ren, Z. -A., Kato, J., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

The discoveries of superconductivity in the heavily-boron doped semiconductors diamond (C:B) in 2004 and silicon (Si:B) in 2006 have renewed the interest in the physics of the superconducting state of doped semiconductors. Recently, we discovered superconductivity in the closely related ''mixed'' system heavily boron-doped silcon carbide (SiC:B). Interestingly, the latter compound is a type-I superconductor whereas the two aforementioned materials are type-II. In this paper we present an extensive analysis of our recent specific-heat study, as well as the band structure and expected Fermi surfaces. We observe an apparent quadratic temperature dependence of the electronic specific heat in the superconducting state. Possible reasons are a nodal gap structure or a residual density of states due to non-superconducting parts of the sample. The basic superconducting parameters are estimated in a Ginzburg-Landau framework. We compare and discuss our results with those reported for C:B and Si:B. Finally, we comment on possible origins of the difference in the superconductivity of SiC:B compared to the two ''parent'' materials C:B and Si:B., Comment: 9 pages, 7 figures, 2 tables, submitted to Phys. Rev. B

Published
2008
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10. Soft-phonon-driven superconductivity in CaAlSi as seen by inelastic x-ray scattering

Author

Kuroiwa, S., Baron, A. Q. R., Muranaka, T., Heid, R., Bohnen, K. -P., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

Inelastic x-ray scattering and $ab$-$initio$ calculation are applied to investigate the lattice dynamics and electron-phonon coupling of the ternary silicide superconductor CaAlSi ($P/bar{6}m2$). A soft c-axis polarized mode is clearly observed along the $/Gamma$-$A$-$L$ symmetry directions. The soft mode is strongly anharmonically broadened at room temperature, but, at 10 K, its linewidth narrows and becomes in good agreement with calculations of linear electron-phonon coupling. This establishes a coherent description of the detailed phonon properties in this system and links them clearly and consistently with the superconductivity., Comment: 4 pages, 4 figures, to be published in Phys. Rev. B (Rapid Communications)

Published
2008
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11. The enhancement of superconducting transition temperature in yttrium sesquicarbide system, Y2C3, with the maximum Tc of Tc=18K

Author

Amano, G., Akutagawa, S., Muranaka, T., Zenitani, Y., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

We discovered the enhancement of superconducting transition temperature, Tc, in yttrium sesquicarbide system with the maximum Tc of Tc=18K and their superconducting properties were discussed. The crystal structure of Y2C3 is the body-centered cubic (Pu2C3-type) structure, and the lattice parameters are varied with the heat treatment conditions. The magnetization (M-H) curves of this compound showed a typical type-II superconducting behavior, and the lower critical field, Hc1(0), is 3.5mT. The Tc-value in this system was changed in the range from 15K to 18K, depending on the sintering conditions. In a previous report by Krupka et al., maximum Tc in Y2C3 was observed at 11.5K by the magnetic measurements. So we successfully synthesized the new high-Tc phase in Y2C3., Comment: 5 pages, 6 figures. Submitted to J. Phys. Soc. Jpn

Published
2003

12. Evidence for High-frequency Phonon Mediated S-wave Superconductivity : 11B-NMR Study of Al-doped MgB2

Author

Kotegawa, H., Ishida, K., Kitaoka, Y., Muranaka, T., Nakagawa, N., Takagiwa, H., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

We report $^{11}$B-NMR study on Al-doped MgB$_2$ that addresses a possible mechanism for a high superconducting (SC) transition temperature ($T_c$) of $\sim 40$ K in recently discovered MgB$_2$. The result of nuclear spin lattice relaxation rate $1/T_1$ in the SC state revealed that the size in the SC gap is not changed by substituting Al for Mg. The reduction on $T_c$ by Al-doping is shown to be due to the decrease of $N(E_F)$. According to the McMillan equation, the experimental relation between $T_c$ and the relative change in $N(E_F)$ allowed us to estimate a characteristic phonon frequency $\omega \sim 700$ K and an electron-phonon coupling constant $\lambda \sim 0.87$. These results suggest that the high-$T_c$ superconductivity in MgB$_2$ is mediated by the strong electron-phonon coupling with high-frequency phonons., Comment: 6pages, 3figures

Published
2002
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13. Manifestation of multiband optical properties of MgB$_2$

Author

Kuz'menko, A. B., Mena, F. P., Molegraaf, H. J. A., van der Marel, D., Gorshunov, B., Dressel, M., Mazin, I. I., Kortus, J., Dolgov, O. V., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

The optical conductivity of MgB$_2$ has been determined on a dense polycrystalline sample in the spectral range 6 meV - 4.6 eV using a combination of ellipsometric and normal incidence reflectivity measurements. $\sigma_{1}(\omega)$ features a narrow Drude peak with anomalously small plasma frequency (1.4 eV) and a very broad "dome" structure, which comprises the bulk of the low-energy spectral weight. This fact can be reconciled with the results of band structure calculations by assuming that charge carriers from the 2D $\sigma$-bands and the 3D $\pi$-bands have principally different impurity scattering rates and negligible interband scattering. This also explains a surprisingly small correlation between the defect concentration and $T_c$, expected for a two-gap superconductor. The large 3D carrier scattering rate suggests their proximity to the localization limit., Comment: RevTeX, 4 pages, 5 figures

Published
2001
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14. Micro-Raman scattering investigation of MgB2 and RB2 (R=Al, Mn, Nb and Ti)

Author

Ogita, N., Kariya, T., Hiraoka, K., Nagamatsu, J., Muranaka, T., Takagiwa, H., Akimitsu, J., and Udagawa, M.

Subjects
Condensed Matter - Superconductivity
Abstract

Phonon spectra have been investigated by micro-Raman scattering from 290 to 20K. New peaks at 500 and 674 cm-1 appear below 250K in MgB2. These peaks are explained by the Fermi resonance, where Raman-active E2g intereacts with the overtone of E1u due to anhamonicity. Raman spectra of the isostructural RB2 (R=Al, Mn, Nb and Ti) have been also measured at 290K. The line width of E2g phonon of the superconductor MgB2 and NbB2 shows the broader than that of the non-superconductors. It is found that the anharmonicity of phonons is important for the superconductivity for MgB2., Comment: 8 pages, 5 figures

Published
2001

15. Bonding Nature in MgB2

Author

Nishibori, E., Takata, M., Sakata, M., Tanaka, H., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Materials Science
Abstract

The accurate charge density of MgB2 was observed at room temperature(R.T.) and 15K by the MEM(Maximum Entropy Method)/Rietveld analysis using synchrotron radiation powder data. The obtained charge density clearly revealed the covalent bonding feature of boron forming the 2D honeycomb network in the basal plane, on the other hand, Mg is found to be in divalent state. A subtle but clear charge concentration was found on boron 2D sheets at 15K, which should be relating to superconductivity., Comment: 4 pages, 3 figures

Published
2001
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16. Electronic structure of MgB$_2$: X-ray emission and absorption studies

Author

Kurmaev, E. Z., Lyakhovskaya, I. I., Kortus, J., Moewes, A., Miyata, N., Demeter, M., Neumann, M., Yanagihara, M., Watanabe, M., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity, Condensed Matter - Materials Science
Abstract

Measurements of x-ray emission and absorption spectra of the constituents of MgB$_2$ are presented. The results obtained are in good agreement with calculated x-ray spectra, with dipole matrix elements taken into account. The comparison of x-ray emission spectra of graphite, AlB$_2$, and MgB$_2$ in the binding energy scale supports the idea of charge transfer from $\sigma$ to $\pi$ bands, which creates holes at the top of the bonding $\sigma$ bands and drives the high-T$_c$, Comment: final version as published in PRB

Published
2001
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17. Optical measurements of the superconducting gap in MgB2

Author

Gorshunov, B., Kuntscher, C. A., Haas, P., Dressel, M., Mena, F. P., Kuz'menko, A. B., van der Marel, D., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

Far-infrared reflectivity studies on the polycrystalline intermetallic compound MgB_2 with a superconducting transition temperature T_c=39 K were performed at temperatures 20 K to 300 K. We observe a significant raise of the superconducting-to-normal state reflectivity ratio below 70 cm^{-1}, with a maximum at about 25-30 cm^{-1}, which gives a lower estimate of the superconducting gap of 2\Delta(0)\approx3-4 meV., Comment: 3 pages, 3 figures, revtex accepted by European Physics Journal B

Published
2001
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18. High-Resolution Photoemission Study of MgB2

Author

Takahashi, T., Sato, T., Souma, S., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Strongly Correlated Electrons, Condensed Matter - Superconductivity
Abstract

We have performed high-resolution photoemission spectroscopy on MgB2 and observed opening of a superconducting gap with a narrow coherent peak. We found that the superconducting gap is s-like with the gap value of 4.5 meV at 15 K. The temperature dependence (15 - 40 K) of gap value follows well the BCS form, suggesting that 2Delta/kBTc at T=0 is about 3. No pseudogap behavior is observed in the normal state. The present results strongly suggest that MgB2 is categorized into a phonon-mediated BCS superconductor in the weak-coupling regime., Comment: 3 pages, 3 figures, accepted in Physical Review Letters

Published
2001
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19. Compressibility of the MgB2 Superconductor

Author

Prassides, K., Iwasa, Y., Ito, T., Chi, D. H., Uehara, K., Nishibori, E., Takata, M., Sakata, S., Ohishi, Y., Shimomura, O., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

Considerable excitement has been caused recently by the discovery that the binary boride system with stoichiometry MgB2 is superconducting at the remarkably high temperature of 39 K (1). This potentially opens the way to even higher Tc values in a new family of superconductors with unexpectedly simple composition and structure. The simplicity in the electronic and crystal structures could allow the understanding of the physics of high-Tc superconductivity without the presence of the multitude of complicated features, associated with the cuprates. Synchrotron X-ray diffraction was used to measure the isothermal compressibility of MgB2, revealing a stiff tightly-packed incompressible solid with only moderate bonding anisotropy between intra- and inter-layer directions. These results, combined with the pressure evolution of the superconducting transition temperature, Tc establish its relation to the B and Mg bonding distances over a broad range of values., Comment: 6 pages, 3 figures

Published
2001
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20. Evidence for Strong-coupling S-wave Superconductivity in MgB2 :11B NMR Study

Author

Kotegawa, H., Ishida, K., Kitaoka, Y., Muranaka, T., and Akimitsu, J.

Subjects
Condensed Matter - Superconductivity
Abstract

We have investigated a gap structure in a newly-discovered superconductor, MgB2 through the measurement of 11B nuclear spin-lattice relaxation rate, ^{11}(1/T_1). ^{11}(1/T_1) is proportional to the temperature (T) in the normal state, and decreases exponentially in the superconducting (SC) state, revealing a tiny coherence peak just below T_c. The T dependence of 1/T_1 in the SC state can be accounted for by an s-wave SC model with a large gap size of 2\Delta /k_BT_c \sim 5 which suggests to be in a strong-coupling regime., Comment: 2 pages with 1 figure

Published
2001
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21. Potato 14-3-3 St14f

Author

Taoka, K., primary, Kawahara, I., additional, Shinya, S., additional, Harada, K., additional, Muranaka, T., additional, Furuita, K., additional, Nakagawa, A., additional, Fujiwara, T., additional, Tsuji, H., additional, and Kojima, C., additional

Published
2023
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24. 99P Impact of single-heterozygous UGT1A1 on the clinical outcomes of nano-liposomal irinotecan plus 5-fluorouracil/leucovorin for patients with pancreatic ductal adenocarcinoma

Author

Harada, K., primary, Yamamura, T., additional, Muto, O., additional, Nakamura, M., additional, Sogabe, S., additional, Sawada, K., additional, Nakano, S., additional, Yagisawa, M., additional, Muranaka, T., additional, Dazai, M., additional, Tateyama, M., additional, Kobayashi, Y., additional, Kato, S., additional, Miyagishima, T., additional, Kawamoto, Y., additional, Yuki, S., additional, Sakata, Y., additional, Sakamoto, N., additional, and Komatsu, Y., additional

Published
2022
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29. SO-30 Impact of single-heterozygous UGT1A1 on the clinical outcomes of nano-liposomal irinotecan plus 5-fluorouracil/leucovorin for patients with pancreatic ductal adenocarcinoma

Author

Harada, K., primary, Yamamura, T., additional, Muto, O., additional, Nakamura, M., additional, Sogabe, S., additional, Sawada, K., additional, Nakano, S., additional, Yagisawa, M., additional, Muranaka, T., additional, Dazai, M., additional, Tateyama, M., additional, Ito, K., additional, Saito, R., additional, Kobayashi, Y., additional, Kato, S., additional, Miyagishima, T., additional, Kawamoto, Y., additional, Yuki, S., additional, Sakata, Y., additional, Sakamoto, N., additional, and Komatsu, Y., additional

Published
2022
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37. P-147 Final analysis: phase II trial of Irinotecan/S-1/cetuximab (IRIS/Cet) as second line treatment in patients with KRAS exon2 wild type mCRC: HGCSG0902. -comparison of administration interval in cetuximab treatment

Author

Yuki, S., Komatsu, Y., Nakatsumi, H., Kawamoto, Y., Muranaka, T., Sawada, K., Tsuji, Y., Hosokawa, A., Nakamura, M., Muto, O., Sasaki, T., Iwanaga, I., Hatanaka, K., Sato, A., Eto, K., Furukawa, K., Tateyama, M., Takahashi, Y., Sogabe, S., Honda, T., Sakamoto, N., and Sakata, Y.

Published
2016
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38. P-152 Observational Cohort Study of 1st line Bevacizumab Combined with Chemotherapy in Metastatic Colorectal Cancer (HGCSG0802): Sub-group Analysis by the Glasgow Prognostic Score (GPS)

Author

Miyagishima, T., Yuki, S., Nakatsumi, H., Kawamoto, Y., Muranaka, T., Sawada, K., Kobayashi, Y., Sasaki, T., Nakamura, M., Sato, A., Iwanaga, I., Tateyama, M., Hatanaka, K., Eto, K., Okuda, H., Muto, O., Abe, M., Oba, A., Kato, S., Miyashita, K., Sakata, Y., and Komatsu, Y.

Published
2016
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48. Anti-resorptive agent related osteonecrosis of the jaw (ARONJ) in urological malignancies: Is the risk different between kidney and prostate cancer patients?

Author

Sakai, Y., primary, Sato, S, additional, Shindo, T., additional, Takahashi, A., additional, Kunishima, Y., additional, Kato, R., additional, Ito, N., additional, Okada, M., additional, Tachiki, H., additional, Taguchi, K., additional, Hirose, T., additional, Hotta, H., additional, Horita, H., additional, Matsukawa, M., additional, Muranaka, T., additional, Nishiyama, K., additional, Miyazaki, A., additional, Hashimoto, K., additional, Tanaka, T., additional, and Masumori, N., additional

Published
2020
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49. Flux creep and irreversibility line in superconducting Pb-Bi alloys

Author

Matsuda, A., Muranaka, T., Akune, T., and Sakamoto, N.

Subjects
Flux pinning -- Research, Superconductivity -- Research, Superconductors -- Magnetic properties, Business, Electronics, Electronics and electrical industries
Abstract

A simple low-temperature superconductor Pb-Bi system was used to understand the relationship between the pinning mechanism and the irreversibility field. The low-temperature Pb-Bi superconductor was used because its pinning attributes have been fully examined and are controllable. A discussion of the observed irreversibility field using both pinning characteristics and numerical calculation derived from the flux creep theory is also presented.

Published
1999

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