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4 search hits
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- Measurement of charged jet suppression in Pb-Pb collisions at √sNN = 2.76 TeV (2014)
- B. Abelev J. Adam D. Adamová M. M. Aggarwal G. Aglieri Rinella M. Agnello A.i G. Agocs A. Agostinelli N. Agrawal Z. Ahammed N. Ahmad A. Ahmad Masoodi I. Ahmed S. U. Ahn S. A. Ahn I. Aimo S. Aiola M. Ajaz A. Akindinov D. Aleksandrov B. Alessandro D. Alexandre A. Alici A. Alkin J. Alme T. Alt V. Altini S. Altinpinar I. Altsybeev C. Alves Garcia Prado C. Andrei A. Andronic V. Anguelov J. Anielski T. Antičić F. Antinori P. Antonioli L. Aphecetche Harald Appelshäuser N. Arbor S. Arcelli N. Armesto R. Arnaldi T. Aronsson I. C. Arsene M. Arslandok A. Augustinus R. Averbeck T. C. Awes M. D. Azmi M. Bach A. Badalà Y. W. Baek S. Bagnasco R. Bailhache V. Bairathi R. Bala A. Baldisseri F. Baltasar Dos Santos Pedrosa J. Bán R. C. Baral R. Barbera F. Barile G. G. Barnaföldi L. S. Barnby V. Barret J. Bartke M. Basile N. Bastid S. Basu B. Bathen G. Batigne B. Batyunya P. C. Batzing C. Baumann I. G. Bearden H. Beck C. Bedda N. K. Behera I. Belikov F. Bellini R. Bellwied E. Belmont-Moreno G. Bencedi S. Beole I. Berceanu G. G. Barnaföldi L. S. Barnby V. Barret J. Bartke M. Basile N. Bastid S. Basu B. Bathen G. Batigne B. Batyunya P. C. Batzing C. Baumann I. G. Bearden H. Beck C. Bedda N. K. Behera I. Belikov F. Bellini R. Bellwied E. Belmont-Moreno G. Bencedi S. Beole I. Berceanu M. Bogolyubsky L. Boldizsár M. Bombara J. Book H. Borel A. Borissov J. Bornschein F. Bossú M. Botje E. Botta S. Böttger P. Braun-Munzinger M. Bregant T. Breitner T. A. Broker T. A. Browning M. Broz E. Bruna G. E. Bruno D. Budnikov H. Buesching S. Bufalino P. Buncic O. Busch Z. Buthelezi D. Caffarri X. Cai H. Caines A. Caliva E. Calvo Villar P. Camerini V. Canoa Roman F. Carena W. Carena F. Carminati A. Casanova Díaz J. Castillo Castellanos E. A. R. Casula V. Catanescu C. Cavicchioli C. Ceballos Sanchez J. Cepila P. Cerello B. Chang S. Chapeland J. L. Charvet S. Chattopadhyay S. Chattopadhyay M. Cherney C. Cheshkov B. Cheynis V. Chibante Barroso D. D. Chinellato P. Chochula M. Chojnacki S. Choudhury P. Christakoglou C. H. Christensen P. Christiansen T. Chujo S. U. Chung C. Cicalo L. Cifarelli F. Cindolo J. Cleymans F. Colamaria D. Colella A. Collu M. Colocci G. Conesa Balbastre Z. Conesa del Valle M. E. Connors G. Contin J. G. Contreras T. M. Cormier Y. Corrales Morales P. Cortese I. Cortés Maldonado M. R. Cosentino F. Costa P. Crochet R. Cruz Albino E. Cuautle L. Cunqueiro A. Dainese R. Dang A. Danu D. Das I. Das K. Das S. Das A. Dash S. Dash S. De H. Delagrange A. Deloff E. Dénes G. D’Erasmo G. O. V. de Barros A. De Caro G. de Cataldo J. de Cuveland A. De Falco D. De Gruttola N. De Marco S. De Pasquale R. de Rooij M. A. Diaz Corchero T. Dietel R. Divià D. Di Bari S. Di Liberto A. Di Mauro P. Di Nezza Ø. Djuvsland A. Dobrin T. Dobrowolski D. Domenicis Gimenez B. Dönigus O. Dordic S. Dorheim A. K. Dubey A. Dubla L. Ducroux P. Dupieux A. K. Dutta Majumdar D. Elia H. Engel B. Erazmus H. A. Erdal D. Eschweiler B. Espagnon M. Estienne S. Esumi D. Evans S. Evdokimov G. Eyyubova D. Fabris J. Faivre D. Falchieri A. Fantoni M. Fasel D. Fehlker L. Feldkamp D. Felea A. Feliciello G. Feofilov J. Ferencei A. Fernández Téllez E. G. Ferreiro A. Ferretti A. Festanti J. Figiel M. A. S. Figueredo S. Filchagin D. Finogeev F. M. Fionda E. M. Fiore E. Floratos M. Floris S. Foertsch P. Foka S. Fokin E. Fragiacomo A. Francescon U. Frankenfeld U. Fuchs C. Furget M. Fusco Girard J. J. Gaardhøje M. Gagliardi M. Gallio D. R. Gangadharan P. Ganoti C. Garabatos E. Garcia-Solis C. Gargiulo I. Garishvili J. Gerhard M. Germain A. Gheata M. Gheata B. Ghidini P. Ghosh S.K. Ghosh P. Gianotti P. Giubellino E. Gladysz-Dziadus P. Glässel R. Gomez P. González-Zamora S. Gorbunov L. Görlich S. Gotovac L. K. Graczykowski R. Grajcarek A. Grelli A. Grigoras C. Grigoras V. Grigoriev A. Grigoryan S. Grigoryan B. Grinyov N. Grion J. F. Grosse-Oetringhaus J.-Y. Grossiord R. Grosso F. Guber R. Guernane B. Guerzoni M. Guilbaud K. Gulbrandsen H. Gulkanyan T. Gunji A. Gupta R. Gupta K. H. Khan R. Haake Ø. Haaland C. Hadjidakis M. Haiduc H. Hamagaki G. Hamar L. D. Hanratty A. Hansen John W. Harris H. Hartmann A. Harton D. Hatzifotiadou S. Hayashi A. Hayrapetyan S. T. Heckel M. Heide H. Helstrup A. Herghelegiu G. Herrera Corral B. A. Hess K. F. Hetland B. Hicks B. Hippolyte J. Hladky P. Hristov M. Huang T. J. Humanic D. Hutter D. S. Hwang J.-C. Ianigro R. Ilkaev I. Ilkiv M. Inaba E. Incani G. M. Innocenti C. Ionita M. Ippolitov M. Irfan M. Ivanov V. Ivanov O. Ivanytskyi A. Jacholkowski C. Jahnke H. J. Jang M. A. Janik P. H. S. Y. Jayarathna S. Jena R. T. Jimenez Bustamante P. G. Jones H. Jung A. Jusko S. Kalcher P. Kalinak A. Kalweit J. Kamin J. H. Kang V. Kaplin S. Kar A. Karasu Uysal O. Karavichev T. Karavicheva E. Karpechev U. Kebschull R. Keidel B. Ketzer M. Mohisin Khan P. Khan S. A. Khan A. Khanzadeev Y. Kharlov B. Kileng B. Kim D. W. Kim D. J. Kim J. S. Kim M. Kim M. Kim S. Kim T. Kim S. Kirsch I. Kisel S. Kiselev A. Kisiel G. Kiss J. L. Klay J. Klein C. Klein-Bösing A. Kluge M. L. Knichel A. G. Knospe C. Kobdaj M. K. Köhler Thorsten Kollegger A. Kolojvari V. Kondratiev N. Kondratyeva A. Konevskikh V. Kovalenko M. Kowalski S. Kox G. Koyithatta Meethaleveedu J. Kral I. Králik F. Kramer A. Kravčáková M. Krelina M. Kretz M. Krivda F. Krizek M. Krus E. Kryshen M. Krzewicki V. Kučera Y. Kucheriaev T. Kugathasan C. Kuhn P. G. Kuijer I. Kulakov J. Kumar P. Kurashvili A. Kurepin A. B. Kurepin A. Kuryakin S. Kushpil V. Kushpil M. J. Kweon Y. Kwon P. Ladron de Guevara C. Lagana Fernandes I. Lakomov R. Langoy C. Lara A. Lardeux A. Lattuca S. L. La Pointe P. La Rocca R. Lea G. R. Lee I. Legrand J. Lehnert R. C. Lemmon M. Lenhardt V. Lenti E. Leogrande M. Leoncino I. León Monzón P. Lévai S. Li J. Lien R. Lietava S. Lindal V. Lindenstruth C. Lippmann M. A. Lisa H. M. Ljunggren D. F. Lodato P. I. Loenne V. R. Loggins V. Loginov D. Lohner C. Loizides X. Lopez E. López Torres X.-G. Lu P. Luettig M. Lunardon J. Luo G. Luparello C. Luzzi A. M. Gago P. M. Jacobs R. Ma A. Maevskaya M. Mager D. P. Mahapatra A. Maire M. Malaev I. Maldonado Cervantes L. Malinina D. Mal’Kevich P. Malzacher A. Mamonov L. Manceau V. Manko F. Manso V. Manzari M. Marchisone J. Mareš G. V. Margagliotti A. Margotti A. Marín C. Markert M. Marquard I. Martashvili N. A. Martin P. Martinengo M. I. Martínez G. Martínez García J. Martin Blanco Y. Martynov A. Mas S. Masciocchi M. Masera A. Masoni L. Massacrier A. Mastroserio A. Matyja C. Mayer J. Mazer R. Mazumder M. A. Mazzoni F. Meddi A. Menchaca-Rocha J. Mercado Pérez M. Meres Y. Miake K. Mikhaylov L. Milano J. Milosevic A. Mischke A. N. Mishra Dariusz Miśkowiec C. M. Mitu J. Mlynarz B. Mohanty L. Molnar L. Montaño Zetina E. Montes M. Morando D. A. Moreira De Godoy S. Moretto A. Morreale A. Morsch V. Muccifora E. Mudnic S. Muhuri M. Mukherjee H. Müller M. G. Munhoz S. Murray L. Musa J. Musinsky B. K. Nandi R. Nania E. Nappi C. Nattrass T. K. Nayak S. Nazarenko A. Nedosekin M. Nicassio M. Niculescu B. S. Nielsen S. Nikolaev S. Nikulin V. Nikulin B. S. Nilsen F. Noferini P. Nomokonov G. Nooren A. Nyanin A. Nyatha J. Nystrand Helmut Oeschler S. Oh S. K. Oh A. Okatan L. Olah J. Oleniacz A. C. Oliveira Da Silva J. Onderwaater C. Oppedisano A. Ortiz Velasquez A. Oskarsson J. Otwinowski K. Oyama Y. Pachmayer M. Pachr P. Pagano G. Paić F. Painke C. Pajares S. K. Pal A. Palmeri D. Pant V. Papikyan G. S. Pappalardo W. J. Park A. Passfeld D. I. Patalakha V. Paticchio B. Paul T. Pawlak T. Peitzmann H. Pereira Da Costa E. Pereira De Oliveira Filho D. Peresunko C. E. Pérez Lara W. Peryt A. Pesci Y. Pestov V. Petráček M. Petran M. Petris M. Petrovici C. Petta S. Piano M. Pikna P. Pillot O. Pinazza L. Pinsky D. B. Piyarathna M. Ploskon M. Planinic J. Pluta S. Pochybova P. L. M. Podesta-Lerma M. G. Poghosyan E. H. O. Pohjoisaho B. Polichtchouk N. Poljak A. Pop S. Porteboeuf-Houssais J. Porter V. Pospisil B. Potukuchi S. K. Prasad R. Preghenella F. Prino C. A. Pruneau I. Pshenichnov G. Puddu P. Pujahari V. Punin J. Putschke H. Qvigstad A. Rachevski S. Raha J. Rak A. Rakotozafindrabe L. Ramello R. Raniwala S. Raniwala S. S. Räsänen B. T. Rascanu D. Rathee A. W. Rauf V. Razazi K. F. Read J. S. Real K. Redlich R. J. Reed A. Rehman P. Reichelt M. Reicher F. Reidt Rainer Ernst Arno Renfordt A. R. Reolon A. Reshetin F. Rettig J.-P. Revol K. Reygers V. Riabov R. A. Ricci T. Richert M. Richter P. Riedler W. Riegler F. Riggi A. Rivetti E. Rocco M. Rodríguez Cahuantzi A. Rodriguez Manso K. Røed E. Rogochaya S. Rohni D. Rohr D. Röhrich R. Romita F. Ronchetti L. Ronflette P. Rosnet S. Rossegger A. Rossi A. Roy C. Roy P. Roy A. J. Rubio Montero R. Rui R. Russo E. Ryabinkin Y. Ryabov A. Rybicki S. Sadovsky K. Šafařík B. Sahlmuller R. Sahoo P. K. Sahu J. Saini C. A. Salgado J. Salzwedel S. Sambyal V. Samsonov X. Sanchez Castro F. J. Sánchez Rodríguez L. Šándor Andres Sandoval M. Sano G. Santagati D. Sarkar E. Scapparone F. Scarlassara R. P. Scharenberg C. Schiaua R. Schicker C. Schmidt H. R. Schmidt S. Schuchmann J. Schukraft M. Schulc T. Schuster Y. Schutz K. Schwarz K. Schweda G. Scioli E. Scomparin P. A. Scott R. Scott G. Segato J. E. Seger I. Selyuzhenkov J. Seo E. Serradilla A. Sevcenco A. Shabetai G. Shabratova R. Shahoyan A. Shangaraev N. Sharma S. Sharma K. Shigaki K. Shtejer Y. Sibiriak S. Siddhanta T. Siemiarczuk D. Silvermyr C. Silvestre G. Simatovic R. Singaraju R. Singh S. Singha V. Singhal B. C. Sinha T. Sinha B. Sitar M. Sitta T. B. Skaali K. Skjerdal R. Smakal N. Smirnov R. J. M. Snellings C. Søgaard R. Soltz J. Song M. Song F. Soramel S. Sorensen M. Spacek I. Sputowska M. Spyropoulou-Stassinaki B. K. Srivastava J. Stachel I. Stan G. Stefanek M. Steinpreis E. Stenlund G. Steyn J. H. Stiller D. Stocco M. Stolpovskiy P. Strmen A. A. P. Suaide M. A. Subieta Vasquez T. Sugitate C. Suire M. Suleymanov R. Sultanov M. Šumbera T. Susa T. J. M. Symons A. Szanto de Toledo I. Szarka A. Szczepankiewicz M. Szymanski J. Takahashi M. A. Tangaro J. D. Tapia Takaki A. Tarantola Peloni A. Tarazona Martinez A. Tauro G. Tejeda Muñoz A. Telesca C. Terrevoli A. Ter Minasyan J. Thäder D. Thomas R. Tieulent A. R. Timmins A. Toia H. Torii V. Trubnikov W. H. Trzaska T. Tsuji A. Tumkin R. Turrisi T. S. Tveter J. Ulery K. Ullaland J. Ulrich A. Uras G. L. Usai M. Vajzer M. Vala L. Valencia Palomo S. Vallero P. Vande Vyvre L. Vannucci J. W. Van Hoorne M. van Leeuwen A. Vargas R. Varma M. Vasileiou A. Vasiliev V. Vechernin M. Veldhoen M. Venaruzzo E. Vercellin S. Vergara Limón R. Vernet M. Verweij L. Vickovic G. Viesti J. Viinikainen Z. Vilakazi O. Villalobos Baillie A. Vinogradov L. Vinogradov Y. Vinogradov T. Virgili Y. P. Viyogi A. Vodopyanov M. A. Völkl K. Voloshin S. A. Voloshin G. Volpe B. von Haller I. Vorobyev D. Vranic J. Vrláková B. Vulpescu A. Vyushin B. Wagner J. Wagner V. Wagner M. Wang Y. Wang D. Watanabe M. Weber J. P. Wessels U. Westerhoff J. Wiechula J. Wikne M. Wilde G. Wilk J. Wilkinson M. C. S. Williams B. Windelband M. Winn C. Xiang C. G. Yaldo Y. Yamaguchi H. Yang P. Yang S. Yang S. Yano S. Yasnopolskiy J. Yi Z. Yin I.-K. Yoo I. Yushmanov V. Zaccolo C. Zach A. Zaman C. Zampolli S. Zaporozhets A. Zarochentsev P. Závada N. Zaviyalov H. Zbroszczyk I. S. Zgura M. Zhalov F. Zhang H. Zhang X. Zhang Y. Zhang C. Zhao D. Zhou F. Zhou Y. Zhou H. Zhu J. Zhu J. Zhu X. Zhu A. Zichichi A. Zimmermann M. B. Zimmermann G. Zinovjev Y. Zoccarato M. Zynovyev M. Zyzak
- A measurement of the transverse momentum spectra of jets in Pb-Pb collisions at sNN−−−√=2.76 TeV is reported. Jets are reconstructed from charged particles using the anti-kT jet algorithm with jet resolution parameters R of 0.2 and 0.3 in pseudo-rapidity |η|<0.5. The transverse momentum pT of charged particles is measured down to 0.15 GeV/c which gives access to the low pT fragments of the jet. Jets found in heavy-ion collisions are corrected event-by-event for average background density and on an inclusive basis (via unfolding) for residual background fluctuations and detector effects. A strong suppression of jet production in central events with respect to peripheral events is observed. The suppression is found to be similar to the suppression of charged hadrons, which suggests that substantial energy is radiated at angles larger than the jet resolution parameter R=0.3 considered in the analysis. The fragmentation bias introduced by selecting jets with a high pT leading particle, which rejects jets with a soft fragmentation pattern, has a similar effect on the jet yield for central and peripheral events. The ratio of jet spectra with R=0.2 and R=0.3 is found to be similar in Pb-Pb and simulated PYTHIA pp events, indicating no strong broadening of the radial jet structure in the reconstructed jets with R<0.3.
- A break in neoliberal ideology? : A critical analysis of Bolivian elite discourse (2006)
- Marión C. Schmidt
- Intercomparing different devices for the investigation of ice nucleating particles using Snomax® as test substance (2014)
- Heike Wex Stefanie Augustin-Bauditz Yvonne Boose Carsten Budke Joachim Curtius Karoline Diehl Axel Dreyer Fabian Frank Susan Hartmann Naruki Hiranuma Evelyn Jantsch Zamin A. Kanji Alexei Kiselev Thomas Koop Ottmar Möhler Dennis Niedermeier Björn Nillius Michael Rösch Diana Rose C. Schmidt Isabelle Steinke Frank Stratmann
- Seven different instruments and measurement methods were used to examine the immersion freezing of bacterial ice nuclei from Snomax® (hereafter Snomax), a product containing ice active protein complexes from non-viable Pseudomonas syringae bacteria. The experimental conditions were kept as similar as possible for the different measurements. Of the participating instruments, some examined droplets which had been made from suspensions directly, and the others examined droplets activated on previously generated Snomax particles, with particle diameters of mostly a few hundred nanometers and up to a few micrometers in some cases. Data were obtained in the temperature range from −2 to −38 °C, and it was found that all ice active protein complexes were already activated above −12 °C. Droplets with different Snomax mass concentrations covering 10 orders of magnitude were examined. Some instruments had very short ice nucleation times down to below 1 s, while others had comparably slow cooling rates around 1 K min−1. Displaying data from the different instruments in terms of numbers of ice active protein complexes per dry mass of Snomax, nm, showed that within their uncertainty the data agree well with each other as well as to previously reported literature results. Two parameterizations were taken from literature for a direct comparison to our results, and these were a time dependent approach based on a contact angle distribution Niedermeier et al. (2014) and a modification of the parameterization presented in Hartmann et~al.~(2013) representing a time independent approach. The agreement between these and the measured data were good, i.e. they agreed within a temperature range of 0.6 K or equivalently a range in nm of a factor of 2. From the results presented herein, we propose that Snomax, at least when carefully shared and prepared, is a suitable material to test and compare different instruments for their accuracy of measuring immersion freezing.
- Intercomparing different devices for the investigation of ice nucleating particles using Snomax® as test substance (2015)
- Heike Wex Stefanie Augustin-Bauditz Yvonne Boose Carsten Budke Joachim Curtius Karoline Diehl Axel Dreyer Fabian Frank Susan Hartmann Naruki Hiranuma Evelyn Jantsch Zamin A. Kanji Alexei Kiselev Thomas Koop Ottmar Möhler Dennis Niedermeier Björn Nillius Michael Rösch Diana Rose C. Schmidt Isabelle Steinke Frank Stratmann
- Seven different instruments and measurement methods were used to examine the immersion freezing of bacterial ice nuclei from Snomax® (hereafter Snomax), a product containing ice-active protein complexes from non-viable Pseudomonas syringae bacteria. The experimental conditions were kept as similar as possible for the different measurements. Of the participating instruments, some examined droplets which had been made from suspensions directly, and the others examined droplets activated on previously generated Snomax particles, with particle diameters of mostly a few hundred nanometers and up to a few micrometers in some cases. Data were obtained in the temperature range from −2 to −38 °C, and it was found that all ice-active protein complexes were already activated above −12 °C. Droplets with different Snomax mass concentrations covering 10 orders of magnitude were examined. Some instruments had very short ice nucleation times down to below 1 s, while others had comparably slow cooling rates around 1 K min−1. Displaying data from the different instruments in terms of numbers of ice-active protein complexes per dry mass of Snomax, nm, showed that within their uncertainty, the data agree well with each other as well as to previously reported literature results. Two parameterizations were taken from literature for a direct comparison to our results, and these were a time-dependent approach based on a contact angle distribution (Niedermeier et al., 2014) and a modification of the parameterization presented in Hartmann et al. (2013) representing a time-independent approach. The agreement between these and the measured data were good; i.e., they agreed within a temperature range of 0.6 K or equivalently a range in nm of a factor of 2. From the results presented herein, we propose that Snomax, at least when carefully shared and prepared, is a suitable material to test and compare different instruments for their accuracy of measuring immersion freezing.
search hits 1 to 4
