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Wong"},{"name":"C. Woody"},{"name":"L. Xia"},{"name":"B. Xiao"},{"name":"J. Xie"},{"name":"H. Xing"},{"name":"Q. Xu"},{"name":"J. Zhang"},{"name":"S. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zhao"},{"name":"Y. Zhao"},{"name":"L. Zheng"},{"name":"Y. Zhou"},{"name":"P. Zurita"}],"abstract":"This report describes the physics case, the resulting detector requirements, and the evolving detector concepts for the experimental program at the Electron-Ion Collider (EIC). The EIC will be a powerful new high-luminosity facility in the United States with the capability to collide high-energy electron beams with high-energy proton and ion beams, providing access to those regions in the nucleon and nuclei where their structure is dominated by gluons. Moreover, polarized beams in the EIC will give unprecedented access to the spatial and spin structure of the proton, neutron, and light ions. The studies leading to this document were commissioned and organized by the EIC User Group with the objective of advancing the state and detail of the physics program and developing detector concepts that meet the emerging requirements in preparation for the realization of the EIC. The effort aims to provide the basis for further development of concepts for experimental equipment best suited for the science needs, including the importance of two complementary detectors and interaction regions. This report consists of three volumes. Volume I is an executive summary of our findings and developed concepts. In Volume II we describe studies of a wide range of physics measurements and the emerging requirements on detector acceptance and performance. Volume III discusses general-purpose detector concepts and the underlying technologies to meet the physics requirements. These considerations will form the basis for a world-class experimental program that aims to increase our understanding of the fundamental structure of all visible matter","source":"Semantic Scholar","year":2021,"language":"en","subjects":["Physics","Computer Science"],"doi":"10.1016/j.nuclphysa.2022.122447","url":"https://www.semanticscholar.org/paper/00de2899a07eff345e3b2ed8ad91993336426bd6","pdf_url":"http://arxiv.org/pdf/2103.05419","is_open_access":true,"citations":1033,"published_at":"","score":95},{"id":"ss_1aa57fd9f06e73c5fb05f070cc88b2f7cc3aa6d3","title":"Offloading in Mobile Edge Computing: Task Allocation and Computational Frequency Scaling","authors":[{"name":"T. Dinh"},{"name":"Jianhua Tang"},{"name":"Q. La"},{"name":"Tony Q. S. Quek"}],"abstract":"","source":"Semantic Scholar","year":2017,"language":"en","subjects":["Computer Science"],"doi":"10.1109/TCOMM.2017.2699660","url":"https://www.semanticscholar.org/paper/1aa57fd9f06e73c5fb05f070cc88b2f7cc3aa6d3","is_open_access":true,"citations":842,"published_at":"","score":86.25999999999999},{"id":"ss_f36ae623f8aec8910e78ae6712569549e15b9f14","title":"Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC","authors":[{"name":"G. Aad"},{"name":"T. Abajyan"},{"name":"B. Abbott"},{"name":"J. Abdallah"},{"name":"S. Khalek"},{"name":"A. Abdelalim"},{"name":"O. Abdinov"},{"name":"R. Aben"},{"name":"B. Abi"},{"name":"M. Abolins"},{"name":"O. AbouZeid"},{"name":"H. Abramowicz"},{"name":"H. Abreu"},{"name":"B. Acharya"},{"name":"L. Adamczyk"},{"name":"D. Adams"},{"name":"T. Addy"},{"name":"J. Adelman"},{"name":"S. Adomeit"},{"name":"P. Adragna"},{"name":"T. Adye"},{"name":"S. Aefsky"},{"name":"J. A. 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Yin"},{"name":"Z. You"},{"name":"B. Yu"},{"name":"C. Yu"},{"name":"J. Yu"},{"name":"C. Yuan"},{"name":"X. Yuan"},{"name":"Y. Yuan"},{"name":"A. Yuncu"},{"name":"A. Zafar"},{"name":"Y. Zeng"},{"name":"B. Zhang"},{"name":"B. Zhang"},{"name":"C. Zhang"},{"name":"D. Zhang"},{"name":"H. Zhang"},{"name":"H. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"K. Zhang"},{"name":"L. Zhang"},{"name":"S. Zhang"},{"name":"T. Zhang"},{"name":"X. Zhang"},{"name":"Y. Zhang"},{"name":"Y. Zhang"},{"name":"Y. Zhang"},{"name":"Y. Zhang"},{"name":"Yao Zhang"},{"name":"Yi. Zhang"},{"name":"Yu Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zhang"},{"name":"G. Zhao"},{"name":"J. Zhao"},{"name":"J. Zhao"},{"name":"J. Zhao"},{"name":"Lei Zhao"},{"name":"Ling Zhao"},{"name":"M. Zhao"},{"name":"Q. Zhao"},{"name":"S. Zhao"},{"name":"T. Zhao"},{"name":"Y. Zhao"},{"name":"Z. Zhao"},{"name":"A. Zhemchugov"},{"name":"B. Zheng"},{"name":"J. Zheng"},{"name":"Y. Zheng"},{"name":"Y. Zheng"},{"name":"B. Zhong"},{"name":"L. Zhou"},{"name":"L. Zhou"},{"name":"Q. Zhou"},{"name":"X. Zhou"},{"name":"X. Zhou"},{"name":"X. Zhou"},{"name":"Xiaoyu Zhou"},{"name":"Xu Zhou"},{"name":"A. Zhu"},{"name":"J. Zhu"},{"name":"K. Zhu"},{"name":"K. Zhu"},{"name":"S. Zhu"},{"name":"W. Zhu"},{"name":"X. Zhu"},{"name":"Y. Zhu"},{"name":"Y. Zhu"},{"name":"Z. Zhu"},{"name":"J. Zhuang"},{"name":"B. Zou"},{"name":"J. Zou"}],"abstract":"There has recently been a dramatic renewal of interest in hadron spectroscopy and charm physics. This renaissance has been driven in part by the discovery of a plethora of charmonium-like XYZ states at BESIII and B factories, and the observation of an intriguing proton-antiproton threshold enhancement and the possibly related X(1835) meson state at BESIII, as well as the threshold measurements of charm mesons and charm baryons. We present a detailed survey of the important topics in tau-charm physics and hadron physics that can be further explored at BESIII during the remaining operation period of BEPCII. This survey will help in the optimization of the data-taking plan over the coming years, and provides physics motivation for the possible upgrade of BEPCII to higher luminosity.","source":"Semantic Scholar","year":2019,"language":"en","subjects":["Physics"],"doi":"10.1088/1674-1137/44/4/040001","url":"https://www.semanticscholar.org/paper/1cc50536e9f3c0d0d3056beb5eadb9cce2309a20","pdf_url":"https://iopscience.iop.org/article/10.1088/1674-1137/44/4/040001/pdf","is_open_access":true,"citations":474,"published_at":"","score":77.22},{"id":"ss_315d41aae1d8f6bf57d22be0ea0445913ce61e03","title":"Direct detection of a break in the teraelectronvolt cosmic-ray spectrum of electrons and positrons","authors":[{"name":"G. Ambrosi"},{"name":"Q. An"},{"name":"R. Asfandiyarov"},{"name":"P. Azzarello"},{"name":"P. Bernardini"},{"name":"B. Bertucci"},{"name":"M. Cai"},{"name":"J. Chang"},{"name":"D. Chen"},{"name":"H. Chen"},{"name":"J. Chen"},{"name":"W. Chen"},{"name":"M. Cui"},{"name":"T. Cui"},{"name":"A. D’Amone"},{"name":"A. Benedittis"},{"name":"I. Mitri"},{"name":"M. D. Santo"},{"name":"J. N. Dong"},{"name":"T. Dong"},{"name":"Y. Dong"},{"name":"Z. Dong"},{"name":"G. Donvito"},{"name":"D. Droz"},{"name":"K. Duan"},{"name":"J. Duan"},{"name":"M. Duranti"},{"name":"D. D’Urso"},{"name":"R. Fan"},{"name":"Y. Fan"},{"name":"F. Fang"},{"name":"C. Feng"},{"name":"L. Feng"},{"name":"P. Fusco"},{"name":"V. Gallo"},{"name":"F. Gan"},{"name":"M. Gao"},{"name":"S. Gao"},{"name":"F. Gargano"},{"name":"S. Garrappa"},{"name":"K. Gong"},{"name":"Y. Gong"},{"name":"D. Guo"},{"name":"J. Guo"},{"name":"Y. Hu"},{"name":"G. Huang"},{"name":"Y. -. Huang"},{"name":"M. Ionica"},{"name":"D. Jiang"},{"name":"W. Jiang"},{"name":"X. Jin"},{"name":"J. Kong"},{"name":"S. Lei"},{"name":"S. Li"},{"name":"X. Li"},{"name":"W. Li"},{"name":"Y. Li"},{"name":"Y. Liang"},{"name":"Y. Liang"},{"name":"N. Liao"},{"name":"H. Liu"},{"name":"J. Liu"},{"name":"S. Liu"},{"name":"W. Liu"},{"name":"Y. Liu"},{"name":"F. Loparco"},{"name":"M. Ma"},{"name":"P. Ma"},{"name":"S. Ma"},{"name":"T. Ma"},{"name":"X. Ma"},{"name":"X. Ma"},{"name":"G. Marsella"},{"name":"M. Mazziotta"},{"name":"D. Mo"},{"name":"X. Niu"},{"name":"X. Peng"},{"name":"W. Peng"},{"name":"R. Qiao"},{"name":"J. Rao"},{"name":"M. Salinas"},{"name":"G. Shang"},{"name":"W. Shen"},{"name":"Z. Shen"},{"name":"Z. Shen"},{"name":"J. Song"},{"name":"H. Su"},{"name":"M. Su"},{"name":"Z. Sun"},{"name":"A. Surdo"},{"name":"X. Teng"},{"name":"X. Tian"},{"name":"A. Tykhonov"},{"name":"V. Vagelli"},{"name":"S. Vitillo"},{"name":"C. Wang"},{"name":"H. Wang"},{"name":"H. Wang"},{"name":"J. Wang"},{"name":"L. Wang"},{"name":"Q. Wang"},{"name":"S. Wang"},{"name":"X. H. Wang"},{"name":"X. Wang"},{"name":"Y. Wang"},{"name":"Y. Wang"},{"name":"Yu Wang"},{"name":"S. Wen"},{"name":"Z. Wang"},{"name":"D. Wei"},{"name":"J. Wei"},{"name":"Y. F. Wei"},{"name":"D. Wu"},{"name":"J. Wu"},{"name":"L. Wu"},{"name":"S. Wu"},{"name":"X. Wu"},{"name":"K. Xi"},{"name":"Z. Xia"},{"name":"Y. Xin"},{"name":"H. Xu"},{"name":"Z. L. Xu"},{"name":"Z. Xu"},{"name":"G. Xue"},{"name":"H. Yang"},{"name":"P. Yang"},{"name":"Y. Q. Yang"},{"name":"Z. L. Yang"},{"name":"H. Yao"},{"name":"Y. Yu"},{"name":"Q. Yuan"},{"name":"C. Yue"},{"name":"J. Zang"},{"name":"C. Zhang"},{"name":"D. L. Zhang"},{"name":"F. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"L. Zhang"},{"name":"P. Zhang"},{"name":"S. X. Zhang"},{"name":"W. Zhang"},{"name":"Y. Zhang"},{"name":"Y. Zhang"},{"name":"Y. Zhang"},{"name":"Y. Zhang"},{"name":"Y. P. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zhang"},{"name":"H. Zhao"},{"name":"H. Zhao"},{"name":"X. Zhao"},{"name":"C. Zhou"},{"name":"Y. Zhou"},{"name":"X. Zhu"},{"name":"Y. Zhu"},{"name":"S. Zimmer"}],"abstract":"High-energy cosmic-ray electrons and positrons (CREs), which lose energy quickly during their propagation, provide a probe of Galactic high-energy processes and may enable the observation of phenomena such as dark-matter particle annihilation or decay. The CRE spectrum has been measured directly up to approximately 2 teraelectronvolts in previous balloon- or space-borne experiments, and indirectly up to approximately 5 teraelectronvolts using ground-based Cherenkov γ-ray telescope arrays. Evidence for a spectral break in the teraelectronvolt energy range has been provided by indirect measurements, although the results were qualified by sizeable systematic uncertainties. Here we report a direct measurement of CREs in the energy range 25 gigaelectronvolts to 4.6 teraelectronvolts by the Dark Matter Particle Explorer (DAMPE) with unprecedentedly high energy resolution and low background. The largest part of the spectrum can be well fitted by a ‘smoothly broken power-law’ model rather than a single power-law model. The direct detection of a spectral break at about 0.9 teraelectronvolts confirms the evidence found by previous indirect measurements, clarifies the behaviour of the CRE spectrum at energies above 1 teraelectronvolt and sheds light on the physical origin of the sub-teraelectronvolt CREs.","source":"Semantic Scholar","year":2017,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1038/nature24475","url":"https://www.semanticscholar.org/paper/315d41aae1d8f6bf57d22be0ea0445913ce61e03","pdf_url":"https://arxiv.org/pdf/1711.10981","is_open_access":true,"citations":516,"published_at":"","score":76.48},{"id":"ss_6bb3cff588226c5a50823dc33653e8d72f9490a5","title":"Observation of the rare Bs0 →µ+µ− decay from the combined analysis of CMS and LHCb data","authors":[{"name":"The Cms"},{"name":"LHCb Collaborations V. Khachatryan"},{"name":"A. Sirunyan"},{"name":"A. Tumasyan"},{"name":"W. Adam"},{"name":"T. Bergauer"},{"name":"M. Dragicevic"},{"name":"J. Ero"},{"name":"M. Friedl"},{"name":"R. Fruhwirth"},{"name":"V. Ghete"},{"name":"C. Hartl"},{"name":"N. Hormann"},{"name":"J. Hrubec"},{"name":"M. Jeitler"},{"name":"W. Kiesenhofer"},{"name":"V. Knunz"},{"name":"M. Krammer"},{"name":"I. Kratschmer"},{"name":"D. Liko"},{"name":"I. Mikulec"},{"name":"D. Rabady"},{"name":"B. Rahbaran"},{"name":"H. Rohringer"},{"name":"R. Schofbeck"},{"name":"J. Strauss"},{"name":"W. Treberer-treberspurg"},{"name":"W. Waltenberger"},{"name":"C. Wulz"},{"name":"V. Mossolov"},{"name":"N. Shumeiko"},{"name":"J. Gonzalez"},{"name":"S. Alderweireldt"},{"name":"S. Bansal"},{"name":"T. Cornelis"},{"name":"E. Wolf"},{"name":"X. Janssen"},{"name":"A. Knutsson"},{"name":"J. Lauwers"},{"name":"S. Luyckx"},{"name":"S. Ochesanu"},{"name":"R. Rougny"},{"name":"M. Klundert"},{"name":"H. Haevermaet"},{"name":"P. Mechelen"},{"name":"N. Remortel"},{"name":"A. Spilbeeck"},{"name":"F. Blekman"},{"name":"S. Blyweert"},{"name":"J. D’Hondt"},{"name":"N. Daci"},{"name":"N. Heracleous"},{"name":"J. Keaveney"},{"name":"S. Lowette"},{"name":"M. Maes"},{"name":"A. Olbrechts"},{"name":"Q. Python"},{"name":"D. Strom"},{"name":"S. Tavernier"},{"name":"W. Doninck"},{"name":"P. Mulders"},{"name":"G. Onsem"},{"name":"I. Villella"},{"name":"C. Caillol"},{"name":"B. Clerbaux"},{"name":"G. Lentdecker"},{"name":"D. Dobur"},{"name":"L. Favart"},{"name":"A. Gay"},{"name":"A. Grebenyuk"},{"name":"A. L'eonard"},{"name":"A. Mohammadi"},{"name":"L. Perniè"},{"name":"A. Randle-conde"},{"name":"T. Reis"},{"name":"T. Ševa"},{"name":"L. Thomas"},{"name":"C. Velde"},{"name":"P. Vanlaer"},{"name":"J. Wang"},{"name":"F. Zenoni"},{"name":"V. Adler"},{"name":"K. Beernaert"},{"name":"L. Benucci"},{"name":"A. Cimmino"},{"name":"S. Costantini"},{"name":"S. Crucy"},{"name":"S. Dildick"},{"name":"A. Fagot"},{"name":"G. Garcia"},{"name":"J. Mccartin"},{"name":"A. A. O. Rios"},{"name":"D. Ryckbosch"},{"name":"S. S. Diblen"},{"name":"M. Sigamani"},{"name":"N. Strobbe"},{"name":"F. Thyssen"},{"name":"M. Tytgat"},{"name":"E. Yazgan"},{"name":"N. Zaganidis"},{"name":"S. Başeğmez"},{"name":"C. Beluffi"},{"name":"G. Bruno"},{"name":"R. Castello"},{"name":"A. Caudron"},{"name":"L. Ceard"},{"name":"G. G. Silveira"},{"name":"C. Delaere"},{"name":"T. Pree"},{"name":"D. Favart"},{"name":"L. Forthomme"},{"name":"A. Giammanco"},{"name":"J. Hollar"},{"name":"A. Jafari"},{"name":"P. Jež"},{"name":"M. Komm"},{"name":"V. Lemaitre"},{"name":"C. Nuttens"},{"name":"D. Pagano"},{"name":"L. Perrini"},{"name":"A. Pin"},{"name":"K. Piotrzkowski"},{"name":"A. Popov"},{"name":"L. Quertenmont"},{"name":"M. Selvaggi"},{"name":"M. Marono"},{"name":"J. M. Garcia"},{"name":"N. Beliy"},{"name":"T. Caebergs"},{"name":"E. Daubie"},{"name":"G. Hammad"},{"name":"W. L. A. J'unior"},{"name":"G. Alves"},{"name":"L. Brito"},{"name":"M. M. Junior"},{"name":"T. Martins"},{"name":"C. M. Herrera"},{"name":"M. Pol"},{"name":"P. Teles"},{"name":"W. Carvalho"},{"name":"J. Chinellato"},{"name":"A. Cust'odio"},{"name":"E. Costa"},{"name":"D. Damiao"},{"name":"C. Martins"},{"name":"S. F. Souza"},{"name":"H. Malbouisson"},{"name":"D. Figueiredo"},{"name":"L. Mundim"},{"name":"H. Nogima"},{"name":"W. D. Silva"},{"name":"J. Santaolalla"},{"name":"A. Santoro"},{"name":"A. Sznajder"},{"name":"E. Manganote"},{"name":"A. Pereira"},{"name":"C. Bernardes"},{"name":"S. Dogra"},{"name":"T. Tomei"},{"name":"E. Gregores"},{"name":"P. Mercadante"},{"name":"S. Novaes"},{"name":"S. Padula"},{"name":"A. Aleksandrov"},{"name":"V. Genchev"},{"name":"R. Hadjiiska"},{"name":"P. Iaydjiev"},{"name":"A. Marinov"},{"name":"S. Piperov"},{"name":"M. Rodozov"},{"name":"G. Sultanov"},{"name":"M. Vutova"},{"name":"A. Dimitrov"},{"name":"I. Glushkov"},{"name":"L. Litov"},{"name":"B. Pavlov"},{"name":"P. Petkov"},{"name":"J. Bian"},{"name":"G. Chen"},{"name":"H. Chen"},{"name":"M. Chen"},{"name":"T. Cheng"},{"name":"R. Du"},{"name":"C. Jiang"},{"name":"R. Plestina"},{"name":"F. Romeo"},{"name":"J. Tao"},{"name":"Z. Wang"},{"name":"C. Asawatangtrakuldee"},{"name":"Y. Ban"},{"name":"Q. Li"},{"name":"S. Liu"},{"name":"Y. Mao"},{"name":"S. Qian"},{"name":"D. Wang"},{"name":"Z. Xu"},{"name":"W. Zou"},{"name":"C. Avila"},{"name":"A. Cabrera"},{"name":"L. Sierra"},{"name":"C. Florez"},{"name":"J. Gomez"},{"name":"B. Moreno"},{"name":"J. Sanabria"},{"name":"N. Godinovic"},{"name":"D. Lelas"},{"name":"D. Polic"},{"name":"I. Puljak"},{"name":"Z. Antunović"},{"name":"M. Kovač"},{"name":"V. Brigljevic"},{"name":"K. Kadija"},{"name":"J. Luetić"},{"name":"D. Mekterović"},{"name":"L. Sudić"},{"name":"A. Attikis"},{"name":"G. Mavromanolakis"},{"name":"J. Mousa"},{"name":"C. Nicolaou"},{"name":"F. Ptochos"},{"name":"P. Razis"},{"name":"M. Bodlák"},{"name":"M. Finger"},{"name":"M. Finger"},{"name":"Y. Assran"},{"name":"A. Kamel"},{"name":"M. Mahmoud"},{"name":"A. Radi"},{"name":"M. Kadastik"},{"name":"M. Murumaa"},{"name":"M. Raidal"},{"name":"A. Tiko"},{"name":"P. Eerola"},{"name":"G. Fedi"},{"name":"M. Voutilainen"},{"name":"J. Harkonen"},{"name":"V. Karimaki"},{"name":"R. Kinnunen"},{"name":"M. Kortelainen"},{"name":"T. Lamp'en"},{"name":"K. Lassila-Perini"},{"name":"S. Lehti"},{"name":"T. Lind'en"},{"name":"P. Luukka"},{"name":"T. Maenpaa"},{"name":"T. Peltola"},{"name":"E. Tuominen"},{"name":"J. Tuominiemi"},{"name":"E. Tuovinen"},{"name":"L. Wendland"},{"name":"J. Talvitie"},{"name":"T. Tuuva"},{"name":"M. Besançon"},{"name":"F. Couderc"},{"name":"M. Dejardin"},{"name":"D. Denegri"},{"name":"B. Fabbro"},{"name":"J. Faure"},{"name":"C. Favaro"},{"name":"F. Ferri"},{"name":"S. Ganjour"},{"name":"A. Givernaud"},{"name":"P. Gras"},{"name":"G. H. Monchenault"},{"name":"P. Jarry"},{"name":"E. Locci"},{"name":"J. Malcles"},{"name":"J. Rander"},{"name":"A. Rosowsky"},{"name":"M. Titov"},{"name":"S. Baffioni"},{"name":"F. Beaudette"},{"name":"P. Busson"},{"name":"C. Charlot"},{"name":"T. Dahms"},{"name":"M. Dalchenko"},{"name":"L. Dobrzyński"},{"name":"N. Filipovic"},{"name":"A. Florent"},{"name":"R. G. Cassagnac"},{"name":"L. Mastrolorenzo"},{"name":"P. Min'e"},{"name":"C. Mironov"},{"name":"I. Naranjo"},{"name":"M. Nguyen"},{"name":"C. Ochando"},{"name":"G. Ortona"},{"name":"P. Paganini"},{"name":"S. Regnard"},{"name":"R. Salerno"},{"name":"J. Sauvan"},{"name":"Y. Sirois"},{"name":"C. Veelken"},{"name":"Y. Yilmaz"},{"name":"A. Zabi"},{"name":"J. Agram"},{"name":"J. Andrea"},{"name":"A. Aubin"},{"name":"D. Bloch"},{"name":"J. Brom"},{"name":"E. Chabert"},{"name":"C. Collard"},{"name":"É. Conte"},{"name":"J. Fontaine"},{"name":"D. Gel'e"},{"name":"U. Goerlach"},{"name":"C. Goetzmann"},{"name":"A. Bihan"},{"name":"K. Skovpen"},{"name":"P. Hove"},{"name":"S. Gadrat"},{"name":"S. Beauceron"},{"name":"N. Beaupere"},{"name":"G. Boudoul"},{"name":"E. Bouvier"},{"name":"S. Brochet"},{"name":"C. Montoya"},{"name":"J. Chasserat"},{"name":"R. Chierici"},{"name":"D. Contardo"},{"name":"P. Depasse"},{"name":"H. Mamouni"},{"name":"J. Fan"},{"name":"J. Fay"},{"name":"S. Gascon"},{"name":"M. Gouzevitch"},{"name":"B. Ille"},{"name":"T. Kurca"},{"name":"M. Lethuillier"},{"name":"L. Mirabito"},{"name":"S. Perriès"},{"name":"J. D. R. Alvarez"},{"name":"D. Sabes"},{"name":"L. Sgandurra"},{"name":"V. Sordini"},{"name":"M. Donckt"},{"name":"P. Verdier"},{"name":"S. Viret"},{"name":"H. Xiao"},{"name":"Z. Tsamalaidze"},{"name":"C. Autermann"},{"name":"S. Beranek"},{"name":"M. Bontenackels"},{"name":"M. Edelhoff"},{"name":"L. Feld"},{"name":"A. Heister"},{"name":"O. Hindrichs"},{"name":"K. Klein"},{"name":"A. Ostapchuk"},{"name":"F. Raupach"},{"name":"J. Sammet"},{"name":"S. Schael"},{"name":"J. Schulte"},{"name":"H. Weber"},{"name":"B. Wittmer"},{"name":"V. Zhukov"},{"name":"M. Ata"},{"name":"M. Brodski"},{"name":"E. Dietz-Laursonn"},{"name":"D. Duchardt"},{"name":"M. Erdmann"},{"name":"R. Fischer"},{"name":"A. Guth"},{"name":"T. Hebbeker"},{"name":"C. Heidemann"},{"name":"K. Hoepfner"},{"name":"D. Klingebiel"},{"name":"S. Knutzen"},{"name":"P. Kreuzer"},{"name":"M. Merschmeyer"},{"name":"A. Meyer"},{"name":"P. Millet"},{"name":"M. Olschewski"},{"name":"K. Padeken"},{"name":"P. Papacz"},{"name":"H. Reithler"},{"name":"S. Schmitz"},{"name":"L. Sonnenschein"},{"name":"D. Teyssier"},{"name":"S. Thuer"},{"name":"M. Weber"},{"name":"V. Cherepanov"},{"name":"Y. Erdogan"},{"name":"G. Flugge"},{"name":"H. Geenen"},{"name":"M. Geisler"},{"name":"W. H. Ahmad"},{"name":"F. Hoehle"},{"name":"B. Kargoll"},{"name":"T. Kress"},{"name":"Y. Kuessel"},{"name":"A. Kunsken"},{"name":"J. Lingemann"},{"name":"A. Nowack"},{"name":"I. Nugent"},{"name":"O. Pooth"},{"name":"A. Stahl"},{"name":"M. Martin"},{"name":"I. Asin"},{"name":"N. Bartosik"},{"name":"J. Behr"},{"name":"U. Behrens"},{"name":"A. Bell"},{"name":"A. Bethani"},{"name":"K. Borras"},{"name":"A. Burgmeier"},{"name":"A. Cakir"},{"name":"L. Calligaris"},{"name":"A. Campbell"},{"name":"S. Choudhury"},{"name":"F. Costanza"},{"name":"C. Pardos"},{"name":"G. Dolinska"},{"name":"S. Dooling"},{"name":"T. Dorland"},{"name":"G. Eckerlin"},{"name":"D. Eckstein"},{"name":"T. Eichhorn"},{"name":"G. Flucke"},{"name":"J. García"},{"name":"A. Geiser"},{"name":"P. Gunnellini"},{"name":"J. Hauk"},{"name":"M. Hempel"},{"name":"H. Jung"},{"name":"A. Kalogeropoulos"},{"name":"M. Kasemann"},{"name":"P. Katsas"},{"name":"J. Kieseler"},{"name":"C. Kleinwort"},{"name":"I. Korol"},{"name":"D. Krucker"},{"name":"W. Lange"},{"name":"J. Leonard"},{"name":"K. Lipka"},{"name":"A. Lobanov"},{"name":"W. Lohmann"},{"name":"B. Lutz"},{"name":"R. Mankel"},{"name":"I. Marfin"},{"name":"I. Melzer-Pellmann"},{"name":"A. Meyer"},{"name":"G. Mittag"},{"name":"J. Mnich"},{"name":"A. Mussgiller"},{"name":"S. Naumann-Emme"},{"name":"A. Nayak"},{"name":"E. Ntomari"},{"name":"H. Perrey"},{"name":"D. Pitzl"},{"name":"R. Plačakytė"},{"name":"A. Raspereza"},{"name":"P. Cipriano"},{"name":"B. Roland"},{"name":"E. Ron"},{"name":"M. Sahin"},{"name":"J. Salfeld-Nebgen"},{"name":"P. Saxena"},{"name":"T. Schoerner-Sadenius"},{"name":"M. Schroder"},{"name":"C. Seitz"},{"name":"S. Spannagel"},{"name":"A. Treviño"},{"name":"R. Walsh"},{"name":"C. Wissing"},{"name":"V. Blobel"},{"name":"M. Vignali"},{"name":"A. Draeger"},{"name":"J. Erfle"},{"name":"E. Garutti"},{"name":"K. Goebel"},{"name":"M. Gorner"},{"name":"J. Haller"},{"name":"M. Hoffmann"},{"name":"R. Hoing"},{"name":"A. Junkes"},{"name":"H. Kirschenmann"},{"name":"R. Klanner"},{"name":"R. Kogler"},{"name":"J. Lange"},{"name":"T. Lapsien"},{"name":"T. Lenz"},{"name":"I. Marchesini"},{"name":"J. Ott"},{"name":"T. Peiffer"},{"name":"A. Perieanu"},{"name":"N. Pietsch"},{"name":"J. Poehlsen"},{"name":"T. Poehlsen"},{"name":"D. Rathjens"},{"name":"C. Sander"},{"name":"H. Schettler"},{"name":"P. Schleper"},{"name":"E. Schlieckau"},{"name":"A. Schmidt"},{"name":"M. Seidel"},{"name":"V. Sola"},{"name":"H. Stadie"},{"name":"G. Steinbruck"},{"name":"D. Troendle"}],"abstract":"The standard model of particle physics describes the fundamental particles and their interactions via the strong, electromagnetic and weak forces. It provides precise predictions for measurable quantities that can be tested experimentally. The probabilities, or branching fractions, of the strange B meson () and the B0 meson decaying into two oppositely charged muons (μ+ and μ−) are especially interesting because of their sensitivity to theories that extend the standard model. The standard model predicts that the and decays are very rare, with about four of the former occurring for every billion mesons produced, and one of the latter occurring for every ten billion B0 mesons. A difference in the observed branching fractions with respect to the predictions of the standard model would provide a direction in which the standard model should be extended. Before the Large Hadron Collider (LHC) at CERN started operating, no evidence for either decay mode had been found. Upper limits on the branching fractions were an order of magnitude above the standard model predictions. The CMS (Compact Muon Solenoid) and LHCb (Large Hadron Collider beauty) collaborations have performed a joint analysis of the data from proton–proton collisions that they collected in 2011 at a centre-of-mass energy of seven teraelectronvolts and in 2012 at eight teraelectronvolts. Here we report the first observation of the µ+µ− decay, with a statistical significance exceeding six standard deviations, and the best measurement so far of its branching fraction. Furthermore, we obtained evidence for the µ+µ− decay with a statistical significance of three standard deviations. Both measurements are statistically compatible with standard model predictions and allow stringent constraints to be placed on theories beyond the standard model. The LHC experiments will resume taking data in 2015, recording proton–proton collisions at a centre-of-mass energy of 13 teraelectronvolts, which will approximately double the production rates of and B0 mesons and lead to further improvements in the precision of these crucial tests of the standard model.","source":"Semantic Scholar","year":2014,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1038/nature14474","url":"https://www.semanticscholar.org/paper/6bb3cff588226c5a50823dc33653e8d72f9490a5","pdf_url":"https://www.nature.com/articles/nature14474.pdf","is_open_access":true,"citations":499,"published_at":"","score":72.97},{"id":"ss_e653bb084261812d177cf7459fbde0baf2a45a0b","title":"First evidence that non-metricity f(Q) gravity could challenge ΛCDM","authors":[{"name":"Fotios Anagnostopoulos"},{"name":"S. Basilakos"},{"name":"E. Saridakis"}],"abstract":"Fotios K. Anagnostopoulos, Spyros Basilakos, 3 and Emmanuel N. Saridakis 4, 5 Department of Physics, National \u0026 Kapodistrian University of Athens, Zografou Campus GR 157 73, Athens, Greece National Observatory of Athens, Lofos Nymfon, 11852 Athens, Greece Academy of Athens, Research Center for Astronomy and Applied Mathematics, Soranou Efesiou 4, 11527, Athens, Greece CAS Key Laboratory for Researches in Galaxies and Cosmology, Department of Astronomy, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China School of Astronomy, School of Physical Sciences, University of Science and Technology of China, Hefei 230026, P.R. China","source":"Semantic Scholar","year":2021,"language":"en","subjects":["Physics"],"doi":"10.1016/j.physletb.2021.136634","url":"https://www.semanticscholar.org/paper/e653bb084261812d177cf7459fbde0baf2a45a0b","pdf_url":"https://doi.org/10.1016/j.physletb.2021.136634","is_open_access":true,"citations":265,"published_at":"","score":72.95},{"id":"ss_ff5f1698354c661d18bd73a28bedf798b99eff38","title":"High statistics measurement of the positron fraction in primary cosmic rays of 0.5-500 GeV with the alpha magnetic spectrometer on the international space station.","authors":[{"name":"L. Accardo"},{"name":"M. Aguilar"},{"name":"D. Aisa"},{"name":"B. Alpat"},{"name":"A. Alvino"},{"name":"G. Ambrosi"},{"name":"K. Andeen"},{"name":"L. Arruda"},{"name":"N. Attig"},{"name":"P. Azzarello"},{"name":"A. Bachlechner"},{"name":"F. Barão"},{"name":"A. Barrau"},{"name":"L. Barrin"},{"name":"A. Bartoloni"},{"name":"L. Basara"},{"name":"M. Battarbee"},{"name":"R. Battiston"},{"name":"J. Bazo"},{"name":"U. Becker"},{"name":"M. Behlmann"},{"name":"B. Beischer"},{"name":"J. Berdugo"},{"name":"B. Bertucci"},{"name":"G. Bigongiari"},{"name":"V. Bindi"},{"name":"S. Bizzaglia"},{"name":"M. Bizzarri"},{"name":"G. Boella"},{"name":"W. de Boer"},{"name":"K. Bollweg"},{"name":"V. Bonnivard"},{"name":"B. Borgia"},{"name":"S. Borsini"},{"name":"M. Boschini"},{"name":"M. Bourquin"},{"name":"J. Burger"},{"name":"F. Cadoux"},{"name":"X. Cai"},{"name":"M. Capell"},{"name":"S. Caroff"},{"name":"G. Carosi"},{"name":"J. Casaus"},{"name":"V. Cascioli"},{"name":"G. Castellini"},{"name":"I. Cernuda"},{"name":"D. Cerreta"},{"name":"F. Cervelli"},{"name":"M. Chae"},{"name":"Y. H. Chang"},{"name":"A. Chen"},{"name":"H. Chen"},{"name":"G. Cheng"},{"name":"H. Chen"},{"name":"L. Cheng"},{"name":"A. Chikanian"},{"name":"H. Chou"},{"name":"E. Choumilov"},{"name":"V. Choutko"},{"name":"C. Chung"},{"name":"F. Cindolo"},{"name":"C. Clark"},{"name":"R. Clavero"},{"name":"Nicolas Produit"},{"name":"C. Consolandi"},{"name":"A. Contin"},{"name":"C. Corti"},{"name":"B. Coste"},{"name":"Z. Cui"},{"name":"M. Dai"},{"name":"C. Delgado"},{"name":"S. Della Torre"},{"name":"M. Demirköz"},{"name":"L. Derome"},{"name":"S. Di Falco"},{"name":"L. Di Masso"},{"name":"F. Dimiccoli"},{"name":"C. Díaz"},{"name":"P. von Doetinchem"},{"name":"W. Du"},{"name":"M. Duranti"},{"name":"D. D’Urso"},{"name":"A. Eline"},{"name":"F. J. Eppling"},{"name":"T. Eronen"},{"name":"Y. Y. Fan"},{"name":"L. Farnesini"},{"name":"J. Feng"},{"name":"E. Fiandrini"},{"name":"A. Fiasson"},{"name":"E. Finch"},{"name":"P. Fisher"},{"name":"Y. Galaktionov"},{"name":"G. Gallucci"},{"name":"B. Garcia"},{"name":"R. García-López"},{"name":"H. Gast"},{"name":"I. Gebauer"},{"name":"M. Gervasi"},{"name":"A. Ghelfi"},{"name":"W. Gillard"},{"name":"F. Giovacchini"},{"name":"P. Goglov"},{"name":"J. Gong"},{"name":"C. Goy"},{"name":"V. Grabski"},{"name":"D. Grandi"},{"name":"M. Graziani"},{"name":"C. Guandalini"},{"name":"I. Guerri"},{"name":"K. Guo"},{"name":"D. Haas"},{"name":"M. Habiby"},{"name":"S. Haino"},{"name":"K. Han"},{"name":"Z. H. He"},{"name":"M. Heil"},{"name":"R. Henning"},{"name":"J. Hoffman"},{"name":"T. Hsieh"},{"name":"Z. Huang"},{"name":"C. Huh"},{"name":"M. Incagli"},{"name":"M. Ionica"},{"name":"W. Jang"},{"name":"H. Jinchi"},{"name":"K. Kanishev"},{"name":"G. Kim"},{"name":"K. Kim"},{"name":"T. Kirn"},{"name":"R. Kossakowski"},{"name":"O. Kounina"},{"name":"A. Kounine"},{"name":"V. Koutsenko"},{"name":"Matthew Scott Krafczyk"},{"name":"S. Kunz"},{"name":"G. La Vacca"},{"name":"E. Laudi"},{"name":"G. Laurenti"},{"name":"I. Lazzizzera"},{"name":"A. Lebedev"},{"name":"H. T. Lee"},{"name":"S. Lee"},{"name":"C. Leluc"},{"name":"G. Levi"},{"name":"H. L. Li"},{"name":"J. Li"},{"name":"Q. Li"},{"name":"Q. Li"},{"name":"T. X. Li"},{"name":"W. Li"},{"name":"Y. Li"},{"name":"Z. Li"},{"name":"Z. Li"},{"name":"S. Lim"},{"name":"C. H. Lin"},{"name":"P. Lipari"},{"name":"T. Lippert"},{"name":"D. Liu"},{"name":"H. Liu"},{"name":"M. Lolli"},{"name":"T. Lomtadze"},{"name":"M. Lu"},{"name":"Y. Lu"},{"name":"K. Luebelsmeyer"},{"name":"F. Luo"},{"name":"J. Luo"},{"name":"S. Lv"},{"name":"R. Majka"},{"name":"A. Malinin"},{"name":"C. Mañá"},{"name":"J. Marin"},{"name":"T. Martin"},{"name":"G. Martinez"},{"name":"N. Masi"},{"name":"F. Massera"},{"name":"D. Maurin"},{"name":"A. Menchaca-Rocha"},{"name":"Q. Meng"},{"name":"D. Mo"},{"name":"B. Monreal"},{"name":"L. Morescalchi"},{"name":"P. Mott"},{"name":"M. Müller"},{"name":"J. Ni"},{"name":"N. Nikonov"},{"name":"F. Nozzoli"},{"name":"P. Nunes"},{"name":"A. Obermeier"},{"name":"A. Oliva"},{"name":"M. Orcinha"},{"name":"Federico Palmonari"},{"name":"C. Palomares"},{"name":"M. Paniccia"},{"name":"A. Papi"},{"name":"M. Pauluzzi"},{"name":"E. Pedreschi"},{"name":"S. Pensotti"},{"name":"R. Pereira"},{"name":"R. Pilastrini"},{"name":"F. Pilo"},{"name":"A. Piluso"},{"name":"C. Pizzolotto"},{"name":"V. Plyaskin"},{"name":"M. Pohl"},{"name":"V. Poireau"},{"name":"E. Postaci"},{"name":"A. Putze"},{"name":"L. Quadrani"},{"name":"X. Qi"},{"name":"P. Rancoita"},{"name":"D. Rapin"},{"name":"J. Ricol"},{"name":"I. Rodríguez"},{"name":"S. Rosier-Lees"},{"name":"L. Rossi"},{"name":"A. Rozhkov"},{"name":"D. Rozza"},{"name":"G. Rybka"},{"name":"R. Sagdeev"},{"name":"J. Sandweiss"},{"name":"P. Saouter"},{"name":"C. Sbarra"},{"name":"S. Schael"},{"name":"S. M. Schmidt"},{"name":"D. Schuckardt"},{"name":"A. Schulz von Dratzig"},{"name":"G. Schwering"},{"name":"G. Scolieri"},{"name":"E. Seo"},{"name":"B. Shan"},{"name":"Y. Shan"},{"name":"J. Shi"},{"name":"X. Shi"},{"name":"Y. Shi"},{"name":"T. Siedenburg"},{"name":"D. Son"},{"name":"F. Spada"},{"name":"F. Spinella"},{"name":"W. Sun"},{"name":"W. Sun"},{"name":"M. Tacconi"},{"name":"C. P. Tang"},{"name":"X. Tang"},{"name":"Z. Tang"},{"name":"L. Tao"},{"name":"D. Tescaro"},{"name":"S. Ting"},{"name":"S. Ting"},{"name":"N. Tomassetti"},{"name":"J. Torsti"},{"name":"C. Türkoğlu"},{"name":"T. Urban"},{"name":"V. Vagelli"},{"name":"E. Valente"},{"name":"C. Vannini"},{"name":"E. Valtonen"},{"name":"S. Vaurynovich"},{"name":"M. Vecchi"},{"name":"M. Velasco"},{"name":"J. Vialle"},{"name":"V. Vitale"},{"name":"G. Volpini"},{"name":"L. Wang"},{"name":"Q. Wang"},{"name":"R. Wang"},{"name":"X. Wang"},{"name":"Z. Wang"},{"name":"Z. Weng"},{"name":"K. Whitman"},{"name":"J. Wienkenhöver"},{"name":"H. Wu"},{"name":"K. Y. Wu"},{"name":"X. Xia"},{"name":"M. Xie"},{"name":"S. Xie"},{"name":"R. Xiong"},{"name":"G. Xin"},{"name":"N. Xu"},{"name":"W. Xu"},{"name":"Qi Yan"},{"name":"J. Yang"},{"name":"M. Yang"},{"name":"Q. Ye"},{"name":"H. Yi"},{"name":"Y. Yu"},{"name":"Z. Yu"},{"name":"S. Zeissler"},{"name":"J. Zhang"},{"name":"M. Zhang"},{"name":"X. B. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zheng"},{"name":"F. Zhou"},{"name":"H. Zhuang"},{"name":"V. Zhukov"},{"name":"A. Zichichi"},{"name":"N. Zimmermann"},{"name":"P. Zuccon"},{"name":"C. Zurbach"}],"abstract":"","source":"Semantic Scholar","year":2014,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1103/PHYSREVLETT.113.121101","url":"https://www.semanticscholar.org/paper/ff5f1698354c661d18bd73a28bedf798b99eff38","pdf_url":"https://link.aps.org/accepted/10.1103/PhysRevLett.113.121101","is_open_access":true,"citations":463,"published_at":"","score":71.89},{"id":"ss_2729f673328b6fc0c147ea95232aad6c5628e634","title":"Electron and Positron Fluxes in Primary Cosmic Rays Measured with the Alpha Magnetic Spectrometer on the International Space Station","authors":[{"name":"M. Aguilar"},{"name":"D. Aisa"},{"name":"A. Alvino"},{"name":"G. Ambrosi"},{"name":"K. Andeen"},{"name":"L. Arruda"},{"name":"N. Attig"},{"name":"P. Azzarello"},{"name":"A. Bachlechner"},{"name":"F. Barão"},{"name":"A. Barrau"},{"name":"L. Barrin"},{"name":"A. Bartoloni"},{"name":"L. Basara"},{"name":"M. Battarbee"},{"name":"R. Battiston"},{"name":"J. Bazo"},{"name":"U. Becker"},{"name":"M. Behlmann"},{"name":"B. Beischer"},{"name":"J. Berdugo"},{"name":"B. Bertucci"},{"name":"G. Bigongiari"},{"name":"V. Bindi"},{"name":"S. Bizzaglia"},{"name":"M. Bizzarri"},{"name":"G. Boella"},{"name":"W. de Boer"},{"name":"K. Bollweg"},{"name":"V. Bonnivard"},{"name":"B. Borgia"},{"name":"S. Borsini"},{"name":"M. Boschini"},{"name":"M. Bourquin"},{"name":"J. Burger"},{"name":"F. Cadoux"},{"name":"X. Cai"},{"name":"M. Capell"},{"name":"S. Caroff"},{"name":"J. Casaus"},{"name":"V. Cascioli"},{"name":"G. Castellini"},{"name":"I. Cernuda"},{"name":"F. Cervelli"},{"name":"M. Chae"},{"name":"Y. H. Chang"},{"name":"A. Chen"},{"name":"H. Chen"},{"name":"G. Cheng"},{"name":"H. Chen"},{"name":"L. Cheng"},{"name":"A. Chikanian"},{"name":"H. Chou"},{"name":"E. Choumilov"},{"name":"V. Choutko"},{"name":"C. Chung"},{"name":"C. Clark"},{"name":"R. Clavero"},{"name":"Nicolas Produit"},{"name":"C. Consolandi"},{"name":"A. Contin"},{"name":"C. Corti"},{"name":"B. Coste"},{"name":"Z. Cui"},{"name":"M. Dai"},{"name":"C. Delgado"},{"name":"S. Della Torre"},{"name":"M. Demirköz"},{"name":"L. Derome"},{"name":"S. Di Falco"},{"name":"L. Di Masso"},{"name":"F. Dimiccoli"},{"name":"C. Díaz"},{"name":"P. von Doetinchem"},{"name":"W. Du"},{"name":"M. Duranti"},{"name":"D. D’Urso"},{"name":"A. Eline"},{"name":"F. J. Eppling"},{"name":"T. Eronen"},{"name":"Y. Y. Fan"},{"name":"L. Farnesini"},{"name":"J. Feng"},{"name":"E. Fiandrini"},{"name":"A. Fiasson"},{"name":"E. Finch"},{"name":"P. Fisher"},{"name":"Y. Galaktionov"},{"name":"G. Gallucci"},{"name":"B. Garcia"},{"name":"R. García-López"},{"name":"H. Gast"},{"name":"I. Gebauer"},{"name":"M. Gervasi"},{"name":"A. Ghelfi"},{"name":"W. Gillard"},{"name":"F. Giovacchini"},{"name":"P. Goglov"},{"name":"J. Gong"},{"name":"C. Goy"},{"name":"V. Grabski"},{"name":"D. Grandi"},{"name":"M. Graziani"},{"name":"C. Guandalini"},{"name":"I. Guerri"},{"name":"K. Guo"},{"name":"M. Habiby"},{"name":"S. Haino"},{"name":"K. Han"},{"name":"Z. H. He"},{"name":"M. Heil"},{"name":"J. Hoffman"},{"name":"T. Hsieh"},{"name":"Z. Huang"},{"name":"C. Huh"},{"name":"M. Incagli"},{"name":"M. Ionica"},{"name":"W. Jang"},{"name":"H. Jinchi"},{"name":"K. Kanishev"},{"name":"G. Kim"},{"name":"K. Kim"},{"name":"T. Kirn"},{"name":"R. Kossakowski"},{"name":"O. Kounina"},{"name":"A. Kounine"},{"name":"V. Koutsenko"},{"name":"Matthew Scott Krafczyk"},{"name":"S. Kunz"},{"name":"G. La Vacca"},{"name":"E. Laudi"},{"name":"G. Laurenti"},{"name":"I. Lazzizzera"},{"name":"A. Lebedev"},{"name":"H. T. Lee"},{"name":"S. Lee"},{"name":"C. Leluc"},{"name":"H. L. Li"},{"name":"J. Li"},{"name":"Q. Li"},{"name":"Q. Li"},{"name":"T. X. Li"},{"name":"W. Li"},{"name":"Y. Li"},{"name":"Z. Li"},{"name":"Z. Li"},{"name":"S. Lim"},{"name":"C. H. Lin"},{"name":"P. Lipari"},{"name":"T. Lippert"},{"name":"D. Liu"},{"name":"H. Liu"},{"name":"T. Lomtadze"},{"name":"M. Lu"},{"name":"Y. Lu"},{"name":"K. Luebelsmeyer"},{"name":"F. Luo"},{"name":"J. Luo"},{"name":"S. Lv"},{"name":"R. Majka"},{"name":"A. Malinin"},{"name":"C. Mañá"},{"name":"J. Marin"},{"name":"T. Martin"},{"name":"G. Martinez"},{"name":"N. Masi"},{"name":"D. Maurin"},{"name":"A. Menchaca-Rocha"},{"name":"Q. Meng"},{"name":"D. Mo"},{"name":"L. Morescalchi"},{"name":"P. Mott"},{"name":"M. Müller"},{"name":"J. Ni"},{"name":"N. Nikonov"},{"name":"F. Nozzoli"},{"name":"P. Nunes"},{"name":"A. Obermeier"},{"name":"A. Oliva"},{"name":"M. Orcinha"},{"name":"Federico Palmonari"},{"name":"C. Palomares"},{"name":"M. Paniccia"},{"name":"A. Papi"},{"name":"E. Pedreschi"},{"name":"S. Pensotti"},{"name":"R. Pereira"},{"name":"F. Pilo"},{"name":"A. Piluso"},{"name":"C. Pizzolotto"},{"name":"V. Plyaskin"},{"name":"M. Pohl"},{"name":"V. Poireau"},{"name":"E. Postaci"},{"name":"A. Putze"},{"name":"L. Quadrani"},{"name":"X. Qi"},{"name":"P. Rancoita"},{"name":"D. Rapin"},{"name":"J. Ricol"},{"name":"I. Rodríguez"},{"name":"S. Rosier-Lees"},{"name":"A. Rozhkov"},{"name":"D. Rozza"},{"name":"R. Sagdeev"},{"name":"J. Sandweiss"},{"name":"P. Saouter"},{"name":"C. Sbarra"},{"name":"S. Schael"},{"name":"S. M. Schmidt"},{"name":"D. Schuckardt"},{"name":"A. Schulz von Dratzig"},{"name":"G. Schwering"},{"name":"G. Scolieri"},{"name":"E. Seo"},{"name":"B. Shan"},{"name":"Y. Shan"},{"name":"J. Shi"},{"name":"X. Shi"},{"name":"Y. Shi"},{"name":"T. Siedenburg"},{"name":"D. Son"},{"name":"F. Spada"},{"name":"F. Spinella"},{"name":"W. Sun"},{"name":"W. Sun"},{"name":"M. Tacconi"},{"name":"C. P. Tang"},{"name":"X. Tang"},{"name":"Z. Tang"},{"name":"L. Tao"},{"name":"D. Tescaro"},{"name":"S. Ting"},{"name":"S. Ting"},{"name":"N. Tomassetti"},{"name":"J. Torsti"},{"name":"C. Türkoğlu"},{"name":"T. Urban"},{"name":"V. Vagelli"},{"name":"E. Valente"},{"name":"C. Vannini"},{"name":"E. Valtonen"},{"name":"S. Vaurynovich"},{"name":"M. Vecchi"},{"name":"M. Velasco"},{"name":"J. Vialle"},{"name":"L. Wang"},{"name":"Q. Wang"},{"name":"R. Wang"},{"name":"X. Wang"},{"name":"Z. Wang"},{"name":"Z. Weng"},{"name":"K. Whitman"},{"name":"J. Wienkenhöver"},{"name":"H. Wu"},{"name":"X. Xia"},{"name":"M. Xie"},{"name":"S. Xie"},{"name":"R. Xiong"},{"name":"G. Xin"},{"name":"N. Xu"},{"name":"W. Xu"},{"name":"Qi Yan"},{"name":"J. Yang"},{"name":"M. Yang"},{"name":"Q. Ye"},{"name":"H. Yi"},{"name":"Y. Yu"},{"name":"Z. Yu"},{"name":"S. Zeissler"},{"name":"J. Zhang"},{"name":"M. Zhang"},{"name":"X. B. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zheng"},{"name":"H. Zhuang"},{"name":"V. Zhukov"},{"name":"A. Zichichi"},{"name":"N. Zimmermann"},{"name":"P. Zuccon"},{"name":"C. Zurbach"}],"abstract":"Precision measurements by the Alpha Magnetic Spectrometer on the International Space Station of the primary cosmic-ray electron flux in the range 0.5 to 700 GeV and the positron flux in the range 0.5 to 500 GeV are presented. The electron flux and the positron flux each require a description beyond a single power-law spectrum. Both the electron flux and the positron flux change their behavior at ∼30  GeV but the fluxes are significantly different in their magnitude and energy dependence. Between 20 and 200 GeV the positron spectral index is significantly harder than the electron spectral index. The determination of the differing behavior of the spectral indices versus energy is a new observation and provides important information on the origins of cosmic-ray electrons and positrons.","source":"Semantic Scholar","year":2014,"language":"en","subjects":["Physics"],"doi":"10.1103/PHYSREVLETT.113.121102","url":"https://www.semanticscholar.org/paper/2729f673328b6fc0c147ea95232aad6c5628e634","pdf_url":"https://pos.sissa.it/234/400/pdf","is_open_access":true,"citations":449,"published_at":"","score":71.47},{"id":"ss_3fd8af88df3768abbdaf71574e24e4ff021c0c19","title":"Antiproton Flux, Antiproton-to-Proton Flux Ratio, and Properties of Elementary Particle Fluxes in Primary Cosmic Rays Measured with the Alpha Magnetic Spectrometer on the International Space Station.","authors":[{"name":"M. Aguilar"},{"name":"L. Ali Cavasonza"},{"name":"B. Alpat"},{"name":"G. Ambrosi"},{"name":"L. Arruda"},{"name":"N. Attig"},{"name":"S. Aupetit"},{"name":"P. Azzarello"},{"name":"A. Bachlechner"},{"name":"F. Barão"},{"name":"A. Barrau"},{"name":"L. Barrin"},{"name":"A. Bartoloni"},{"name":"L. Basara"},{"name":"S. Başeğmez-du Pree"},{"name":"M. Battarbee"},{"name":"R. Battiston"},{"name":"J. Bazo"},{"name":"U. Becker"},{"name":"M. Behlmann"},{"name":"B. Beischer"},{"name":"J. Berdugo"},{"name":"B. Bertucci"},{"name":"V. Bindi"},{"name":"G. Boella"},{"name":"W. de Boer"},{"name":"K. Bollweg"},{"name":"V. Bonnivard"},{"name":"B. Borgia"},{"name":"M. Boschini"},{"name":"M. Bourquin"},{"name":"E. Bueno"},{"name":"J. Burger"},{"name":"F. Cadoux"},{"name":"X. Cai"},{"name":"M. Capell"},{"name":"S. Caroff"},{"name":"J. Casaus"},{"name":"G. Castellini"},{"name":"I. Cernuda"},{"name":"F. Cervelli"},{"name":"M. Chae"},{"name":"Y. H. Chang"},{"name":"A. Chen"},{"name":"G. Chen"},{"name":"H. Chen"},{"name":"L. Cheng"},{"name":"H. Chou"},{"name":"E. Choumilov"},{"name":"V. Choutko"},{"name":"C. Chung"},{"name":"C. Clark"},{"name":"R. Clavero"},{"name":"Nicolas Produit"},{"name":"C. Consolandi"},{"name":"A. Contin"},{"name":"C. Corti"},{"name":"B. Coste"},{"name":"W. Creus"},{"name":"M. Crispoltoni"},{"name":"Z. Cui"},{"name":"Y. Dai"},{"name":"C. Delgado"},{"name":"S. Della Torre"},{"name":"M. Demirköz"},{"name":"L. Derome"},{"name":"S. Di Falco"},{"name":"F. Dimiccoli"},{"name":"C. Díaz"},{"name":"P. von Doetinchem"},{"name":"F. Dong"},{"name":"F. Donnini"},{"name":"M. Duranti"},{"name":"D. D’Urso"},{"name":"A. Egorov"},{"name":"A. Eline"},{"name":"T. Eronen"},{"name":"J. Feng"},{"name":"E. Fiandrini"},{"name":"E. Finch"},{"name":"P. Fisher"},{"name":"V. Formato"},{"name":"Y. Galaktionov"},{"name":"G. Gallucci"},{"name":"B. Garcia"},{"name":"R. García-López"},{"name":"C. Gargiulo"},{"name":"H. Gast"},{"name":"I. Gebauer"},{"name":"M. Gervasi"},{"name":"A. Ghelfi"},{"name":"F. Giovacchini"},{"name":"P. Goglov"},{"name":"D. Gómez-Coral"},{"name":"J. Gong"},{"name":"C. Goy"},{"name":"V. Grabski"},{"name":"D. 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Liu"},{"name":"Hu Liu"},{"name":"S. Lu"},{"name":"Y. Lu"},{"name":"K. Luebelsmeyer"},{"name":"F. Luo"},{"name":"J. Luo"},{"name":"S. Lv"},{"name":"R. Majka"},{"name":"C. Mañá"},{"name":"J. Marin"},{"name":"T. Martin"},{"name":"G. Martinez"},{"name":"N. Masi"},{"name":"D. Maurin"},{"name":"A. Menchaca-Rocha"},{"name":"Q. Meng"},{"name":"D. Mo"},{"name":"L. Morescalchi"},{"name":"P. Mott"},{"name":"T. Nelson"},{"name":"J. Ni"},{"name":"N. Nikonov"},{"name":"F. Nozzoli"},{"name":"P. Nunes"},{"name":"A. Oliva"},{"name":"M. Orcinha"},{"name":"Federico Palmonari"},{"name":"C. Palomares"},{"name":"M. Paniccia"},{"name":"M. Pauluzzi"},{"name":"S. Pensotti"},{"name":"R. Pereira"},{"name":"N. Picot-Clemente"},{"name":"F. Pilo"},{"name":"C. Pizzolotto"},{"name":"V. Plyaskin"},{"name":"M. Pohl"},{"name":"V. Poireau"},{"name":"A. Putze"},{"name":"L. Quadrani"},{"name":"X. Qi"},{"name":"X. Qin"},{"name":"Z. Qu"},{"name":"T. Räihä"},{"name":"P. Rancoita"},{"name":"D. Rapin"},{"name":"J. Ricol"},{"name":"I. Rodríguez"},{"name":"S. Rosier-Lees"},{"name":"A. Rozhkov"},{"name":"D. Rozza"},{"name":"R. Sagdeev"},{"name":"J. Sandweiss"},{"name":"P. Saouter"},{"name":"S. Schael"},{"name":"S. M. Schmidt"},{"name":"A. Schulz von Dratzig"},{"name":"G. Schwering"},{"name":"E. Seo"},{"name":"B. Shan"},{"name":"J. Shi"},{"name":"T. Siedenburg"},{"name":"D. Son"},{"name":"J. Song"},{"name":"W. Sun"},{"name":"M. Tacconi"},{"name":"X. Tang"},{"name":"Z. Tang"},{"name":"L. Tao"},{"name":"D. Tescaro"},{"name":"S. Ting"},{"name":"S. Ting"},{"name":"N. Tomassetti"},{"name":"J. Torsti"},{"name":"C. Türkoğlu"},{"name":"T. Urban"},{"name":"V. Vagelli"},{"name":"E. Valente"},{"name":"C. Vannini"},{"name":"E. Valtonen"},{"name":"M. Vazquez Acosta"},{"name":"M. Vecchi"},{"name":"M. Velasco"},{"name":"J. Vialle"},{"name":"V. Vitale"},{"name":"S. Vitillo"},{"name":"L. Wang"},{"name":"N. Wang"},{"name":"Q. Wang"},{"name":"X. Wang"},{"name":"X. Wang"},{"name":"Z. Wang"},{"name":"C. Wei"},{"name":"Z. Weng"},{"name":"K. Whitman"},{"name":"J. Wienkenhöver"},{"name":"M. Willenbrock"},{"name":"H. Wu"},{"name":"X. Wu"},{"name":"X. Xia"},{"name":"R. Xiong"},{"name":"W. Xu"},{"name":"Qi Yan"},{"name":"J. Yang"},{"name":"M. Yang"},{"name":"Y. Yang"},{"name":"H. Yi"},{"name":"Y. Yu"},{"name":"Z. Yu"},{"name":"S. Zeissler"},{"name":"C. Zhang"},{"name":"J. Zhang"},{"name":"J. Zhang"},{"name":"S. Zhang"},{"name":"S. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zheng"},{"name":"Z. Q. Zhu"},{"name":"H. Zhuang"},{"name":"V. Zhukov"},{"name":"A. Zichichi"},{"name":"N. Zimmermann"},{"name":"P. Zuccon"}],"abstract":"A precision measurement by AMS of the antiproton flux and the antiproton-to-proton flux ratio in primary cosmic rays in the absolute rigidity range from 1 to 450 GV is presented based on 3.49×10^{5} antiproton events and 2.42×10^{9} proton events. The fluxes and flux ratios of charged elementary particles in cosmic rays are also presented. In the absolute rigidity range ∼60 to ∼500  GV, the antiproton p[over ¯], proton p, and positron e^{+} fluxes are found to have nearly identical rigidity dependence and the electron e^{-} flux exhibits a different rigidity dependence. Below 60 GV, the (p[over ¯]/p), (p[over ¯]/e^{+}), and (p/e^{+}) flux ratios each reaches a maximum. From ∼60 to ∼500  GV, the (p[over ¯]/p), (p[over ¯]/e^{+}), and (p/e^{+}) flux ratios show no rigidity dependence. These are new observations of the properties of elementary particles in the cosmos.","source":"Semantic Scholar","year":2016,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1103/PhysRevLett.117.091103","url":"https://www.semanticscholar.org/paper/3fd8af88df3768abbdaf71574e24e4ff021c0c19","pdf_url":"http://link.aps.org/pdf/10.1103/PhysRevLett.117.091103","is_open_access":true,"citations":371,"published_at":"","score":71.13},{"id":"crossref_10.1186/s12885-023-11792-4","title":"A randomised phase II trial of temozolomide with or without cannabinoids in patients with recurrent glioblastoma (ARISTOCRAT): protocol for a multi-centre, double-blind, placebo-controlled trial","authors":[{"name":"Divyalakshmi Bhaskaran"},{"name":"Joshua Savage"},{"name":"Amit Patel"},{"name":"Fiona Collinson"},{"name":"Rhys Mant"},{"name":"Florien Boele"},{"name":"Lucy Brazil"},{"name":"Sara Meade"},{"name":"Peter Buckle"},{"name":"Siân Lax"},{"name":"Lucinda Billingham"},{"name":"Susan C. Short"}],"abstract":"Abstract Background Glioblastoma (GBM) is the most common adult malignant brain tumour, with an incidence of 5 per 100,000 per year in England. Patients with tumours showing O6-methylguanine-DNA methyltransferase (MGMT) promoter methylation represent around 40% of newly diagnosed GBM. Relapse/tumour recurrence is inevitable. There is no agreed standard treatment for patients with GBM, therefore, it is aimed at delaying further tumour progression and maintaining health-related quality of life (HRQoL). Limited clinical trial data exist using cannabinoids in combination with temozolomide (TMZ) in this setting, but early phase data demonstrate prolonged overall survival compared to TMZ alone, with few additional side effects. Jazz Pharmaceuticals (previously GW Pharma Ltd.) have developed nabiximols (trade name Sativex®), an oromucosal spray containing a blend of cannabis plant extracts, that we aim to assess for preliminary efficacy in patients with recurrent GBM. Methods ARISTOCRAT is a phase II, multi-centre, double-blind, placebo-controlled, randomised trial to assess cannabinoids in patients with recurrent MGMT methylated GBM who are suitable for treatment with TMZ. Patients who have relapsed ≥ 3 months after completion of initial first-line treatment will be randomised 2:1 to receive either nabiximols or placebo in combination with TMZ. The primary outcome is overall survival time defined as the time in whole days from the date of randomisation to the date of death from any cause. Secondary outcomes include overall survival at 12 months, progression-free survival time, HRQoL (using patient reported outcomes from QLQ-C30, QLQ-BN20 and EQ-5D-5L questionnaires), and adverse events. Discussion Patients with recurrent MGMT promoter methylated GBM represent a relatively good prognosis sub-group of patients with GBM. However, their median survival remains poor and, therefore, more effective treatments are needed. The phase II design of this trial was chosen, rather than phase III, due to the lack of data currently available on cannabinoid efficacy in this setting. A randomised, double-blind, placebo-controlled trial will ensure an unbiased robust evaluation of the treatment and will allow potential expansion of recruitment into a phase III trial should the emerging phase II results warrant this development. Trial registration ISRCTN: 11460478. ClinicalTrials.Gov: NCT05629702.","source":"CrossRef","year":2024,"language":"en","subjects":null,"doi":"10.1186/s12885-023-11792-4","url":"https://doi.org/10.1186/s12885-023-11792-4","pdf_url":"https://link.springer.com/content/pdf/10.1186/s12885-023-11792-4.pdf","is_open_access":true,"citations":22,"published_at":"","score":68.66},{"id":"crossref_10.1007/s11764-024-01572-9","title":"Barriers and facilitators to self-management in people living with a lower-grade glioma","authors":[{"name":"Ben Rimmer"},{"name":"Michelle Balla"},{"name":"Lizzie Dutton"},{"name":"Sophie Williams"},{"name":"Vera Araújo-Soares"},{"name":"Pamela Gallagher"},{"name":"Tracy Finch"},{"name":"Joanne Lewis"},{"name":"Richéal Burns"},{"name":"Fiona Menger"},{"name":"Linda Sharp"},{"name":"on behalf of the Ways Ahead study team"}],"abstract":"Abstract Purpose Self-management can have clinical and quality-of-life benefits. However, people with lower-grade gliomas (LGG) may face chronic tumour- and/or treatment-related symptoms and impairments (e.g. cognitive deficits, seizures), which could influence their ability to self-manage. Our study aimed to identify and understand the barriers and facilitators to self-management in people with LGG. Methods We conducted semi-structured interviews with 28 people with LGG across the United Kingdom, who had completed primary treatment. Sixteen participants were male, mean age was 50.4 years, and mean time since diagnosis was 8.7 years. Interviews were audio-recorded and transcribed. Following inductive open coding, we deductively mapped codes to Schulman-Green et al.’s framework of factors influencing self-management, developed in chronic illness. Results Data suggested extensive support for all five framework categories (‘Personal/lifestyle characteristics’, ‘Health status’, ‘Resources’, ‘Environmental characteristics’, ‘Healthcare system’), encompassing all 18 factors influencing self-management. How people with LGG experience many of these factors appears somewhat distinct from other cancers; participants described multiple, often co-occurring, challenges, primarily with knowledge and acceptance of their incurable condition, the impact of seizures and cognitive deficits, transport difficulties, and access to (in)formal support. Several factors were on a continuum, for example, sufficient knowledge was a facilitator, whereas lack thereof, was a barrier to self-management. Conclusions People with LGG described distinctive experiences with wide-ranging factors influencing their ability to self-manage. Implications for cancer survivors These findings will improve awareness of the potential challenges faced by people with LGG around self-management and inform development of self-management interventions for this population.","source":"CrossRef","year":2024,"language":"en","subjects":null,"doi":"10.1007/s11764-024-01572-9","url":"https://doi.org/10.1007/s11764-024-01572-9","pdf_url":"https://link.springer.com/content/pdf/10.1007/s11764-024-01572-9.pdf","is_open_access":true,"citations":3,"published_at":"","score":68.09},{"id":"ss_714c207bf089d9b4d773fbceaae7e06461a59c3d","title":"Deterministic design of wavelength scale, ultra-high Q photonic crystal nanobeam cavities.","authors":[{"name":"Q. Quan"},{"name":"M. Lončar"}],"abstract":"Photonic crystal nanobeam cavities are versatile platforms of interest for optical communications, optomechanics, optofluidics, cavity QED, etc. In a previous work [Appl. Phys. Lett. 96, 203102 (2010)], we proposed a deterministic method to achieve ultrahigh Q cavities. This follow-up work provides systematic analysis and verifications of the deterministic design recipe and further extends the discussion to air-mode cavities. We demonstrate designs of dielectric-mode and air-mode cavities with Q \u003e 10⁹, as well as dielectric-mode nanobeam cavities with both ultrahigh-Q (\u003e 10⁷) and ultrahigh on-resonance transmissions (T \u003e 95%).","source":"Semantic Scholar","year":2011,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1364/OE.19.018529","url":"https://www.semanticscholar.org/paper/714c207bf089d9b4d773fbceaae7e06461a59c3d","pdf_url":"https://doi.org/10.1364/oe.19.018529","is_open_access":true,"citations":430,"published_at":"","score":67.9},{"id":"crossref_10.1007/s11764-023-01425-x","title":"Identifying and understanding how people living with a lower-grade glioma engage in self-management","authors":[{"name":"Ben Rimmer"},{"name":"Michelle Balla"},{"name":"Lizzie Dutton"},{"name":"Joanne Lewis"},{"name":"Morven C. Brown"},{"name":"Richéal Burns"},{"name":"Pamela Gallagher"},{"name":"Sophie Williams"},{"name":"Vera Araújo-Soares"},{"name":"Tracy Finch"},{"name":"Fiona Menger"},{"name":"Linda Sharp"},{"name":"on behalf of the Ways Ahead study team"}],"abstract":"Abstract Purpose Lower-grade gliomas (LGG) are mostly diagnosed in working-aged adults and rarely cured. LGG patients may face chronic impairments (e.g. fatigue, cognitive deficits). Self-management can improve clinical and psychosocial outcomes, yet how LGG patients self-manage the consequences of their tumour and its treatment is not fully understood. This study, therefore, aimed to identify and understand how LGG patients engage in the self-management of their condition. Methods A diverse group of 28 LGG patients (age range 22–69 years; male n = 16, female n = 12; mean time since diagnosis = 8.7 years) who had completed primary treatment, were recruited from across the United Kingdom. Semi-structured interviews were conducted. Informed by a self-management strategy framework developed in cancer, directed content analysis identified and categorised self-management types and strategies used by patients. Results Overall, 20 self-management strategy types, comprising 123 self-management strategies were reported; each participant detailed extensive engagement in self-management. The most used strategy types were ‘using support’ (n = 28), ‘creating a healthy environment’ (n = 28), ‘meaning making’ (n = 27), and ‘self-monitoring’ (n = 27). The most used strategies were ‘accepting the tumour and its consequences’ (n = 26), ‘receiving support from friends (n = 24) and family’ (n = 24), and ‘reinterpreting negative consequences’ (n = 24). Conclusions This study provides a comprehensive understanding of the strategies used by LGG patients to self-manage their health and wellbeing, with a diverse, and substantial number of self-management strategies reported. Implications for Cancer Survivors The findings will inform the development of a supported self-management intervention for LGG patients, which will be novel for this patient group.","source":"CrossRef","year":2023,"language":"en","subjects":null,"doi":"10.1007/s11764-023-01425-x","url":"https://doi.org/10.1007/s11764-023-01425-x","pdf_url":"https://link.springer.com/content/pdf/10.1007/s11764-023-01425-x.pdf","is_open_access":true,"citations":7,"published_at":"","score":67.21000000000001},{"id":"crossref_10.1007/s11560-023-00657-3","title":"Komplementvermittelte seltene Glomerulonephritis(GN)-Formen","authors":[{"name":"Bernd Hohenstein"}],"abstract":"","source":"CrossRef","year":2023,"language":"en","subjects":null,"doi":"10.1007/s11560-023-00657-3","url":"https://doi.org/10.1007/s11560-023-00657-3","pdf_url":"https://link.springer.com/content/pdf/10.1007/s11560-023-00657-3.pdf","is_open_access":true,"citations":1,"published_at":"","score":67.03},{"id":"arxiv_2310.16439","title":"Genomic regulatory architecture of human embryo retroviral LTR elements affecting evolution, development, and pathophysiology of Modern Humans","authors":[{"name":"Gennadi Glinsky"}],"abstract":"Two distinct families of pan-primate endogenous retroviruses, namely HERVL and HERVH, infected primates germline, colonized host genomes, and evolved into the global retroviral genomic regulatory dominion (GRD) operating during human embryogenesis (HE). HE retroviral GRD constitutes 8839 highly conserved fixed LTR elements linked to 5444 down-stream target genes forged by evolution into a functionally-consonant constellation of 26 genome-wide multimodular genomic regulatory networks (GRNs), each of which is defined by significant enrichment of numerous single gene ontology (GO)-specific traits. Locations of GRNs appear scattered across chromosomes to occupy from 5.5%-15.09% of human genome. Each GRN harbors from 529-1486 retroviral LTRs derived from LTR7, MLT2A1, and MLT2A2 sequences that are quantitatively balanced according to their genome-wide abundance. GRNs integrate activities from 199-805 down-stream target genes, including transcription factors, chromatin-state remodelers, signal-sensing and signal-transduction mediators, enzymatic and receptor binding effectors, intracellular complexes and extracellular matrix elements, and cell-cell adhesion molecules. GRNs compositions consist of several hundred to thousands smaller GO enrichment-defined genomic regulatory modules (GRMs) combining from a dozen to hundreds LTRs and down-stream target genes, which appear to operate on individuals life-span timescale along specific phenotypic avenues to exert profound effects on patterns of transcription, protein-protein interactions, developmental phenotypes, physiological traits, and pathological conditions of Modern Humans. Overall, this study identifies 69,573 statistically significant retroviral LTR-linked GRMs (Binominal FDR q-value threshold of 0.001), including 27,601 GRMs validated by the single GO-specific directed acyclic graph (DAG) analyses across six GO annotations.","source":"arXiv","year":2023,"language":"en","subjects":["q-bio.GN","q-bio.MN","q-bio.NC","q-bio.PE","q-bio.TO"],"doi":"10.20935/AcadMolBioGen7754","url":"https://arxiv.org/abs/2310.16439","pdf_url":"https://arxiv.org/pdf/2310.16439","is_open_access":true,"published_at":"2023-10-25T08:04:58Z","score":67},{"id":"ss_4525199f5edc5aa50b0c8f3b3fc7c25f7a5266a4","title":"Coenzyme Q--biosynthesis and functions.","authors":[{"name":"Magnus Bentinger"},{"name":"M. Tekle"},{"name":"G. Dallner"}],"abstract":"","source":"Semantic Scholar","year":2010,"language":"en","subjects":["Biology","Medicine"],"doi":"10.1016/j.bbrc.2010.02.147","url":"https://www.semanticscholar.org/paper/4525199f5edc5aa50b0c8f3b3fc7c25f7a5266a4","is_open_access":true,"citations":422,"published_at":"","score":66.66},{"id":"ss_9af3a0139c4f9570ef7799fa606fffa42bd7b24b","title":"The antioxidant role of coenzyme Q.","authors":[{"name":"Magnus Bentinger"},{"name":"K. Brismar"},{"name":"G. Dallner"}],"abstract":"","source":"Semantic Scholar","year":2007,"language":"en","subjects":["Biology","Medicine"],"doi":"10.1016/J.MITO.2007.02.006","url":"https://www.semanticscholar.org/paper/9af3a0139c4f9570ef7799fa606fffa42bd7b24b","is_open_access":true,"citations":519,"published_at":"","score":66.57}],"total":1626383,"page":1,"page_size":20,"sources":["arXiv","Semantic Scholar","CrossRef"],"query":"q-bio.GN"}