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Holt"},{"name":"D. Holz"},{"name":"P. Hopkins"},{"name":"C. Horst"},{"name":"J. Hough"},{"name":"E. Houston"},{"name":"E. Howell"},{"name":"A. Hreibi"},{"name":"Y. Hu"},{"name":"E. Huerta"},{"name":"D. Huet"},{"name":"B. Hughey"},{"name":"S. Husa"},{"name":"S. Huttner"},{"name":"T. Huynh--Dinh"},{"name":"N. Indik"},{"name":"R. Inta"},{"name":"G. Intini"},{"name":"H. N. Isa"},{"name":"J. Isac"},{"name":"M. Isi"},{"name":"B. Iyer"},{"name":"K. Izumi"},{"name":"T. Jacqmin"},{"name":"K. Jani"},{"name":"P. Jaranowski"},{"name":"S. Jawahar"},{"name":"F. Jiménez-Forteza"},{"name":"W. Johnson"},{"name":"D. Jones"},{"name":"R. Jones"},{"name":"R. Jonker"},{"name":"L. Ju"},{"name":"J. Junker"},{"name":"C. Kalaghatgi"},{"name":"V. Kalogera"},{"name":"B. Kamai"},{"name":"S. Kandhasamy"},{"name":"G. Kang"},{"name":"J. Kanner"},{"name":"S. Kapadia"},{"name":"S. Karki"},{"name":"K. Karvinen"},{"name":"M. Kasprzack"},{"name":"M. Katolik"},{"name":"E. Katsavounidis"},{"name":"W. Katzman"},{"name":"S. Kaufer"}],"abstract":"On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ∼ 1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40 − 8 + 8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 M ⊙ . An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ∼ 40 Mpc ) less than 11 hours after the merger by the One-Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ∼10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ∼ 9 and ∼ 16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC 4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta.","source":"Semantic Scholar","year":2019,"language":"en","subjects":["Physics","Political Science"],"doi":"10.3847/2041-8213/AA91C9","url":"https://www.semanticscholar.org/paper/9259e6979f0851e181af209e5dec65972bab71b4","pdf_url":"https://iopscience.iop.org/article/10.3847/2041-8213/aa91c9/pdf","is_open_access":true,"citations":3080,"published_at":"","score":93},{"id":"ss_7617d4015f2521bce6abad3adb8135c272123bc9","title":"The Belle II Physics Book","authors":[{"name":"E. Kou"},{"name":"P. Urquijo"},{"name":"W. Altmannshofer"},{"name":"F. Beaujean"},{"name":"G. Bell"},{"name":"M. Beneke"},{"name":"I. Bigi"},{"name":"F. Blanke"},{"name":"C. Bobeth"},{"name":"M. Bona"},{"name":"N. Brambilla"},{"name":"V. 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Prasanth"},{"name":"E. Prencipe"},{"name":"M. Prim"},{"name":"M. Purohit"},{"name":"A. Rabusov"},{"name":"R. Rasheed"},{"name":"S. Reiter"},{"name":"M. Remnev"},{"name":"P. Resmi"},{"name":"I. Ripp-Baudot"},{"name":"M. Ritter"},{"name":"M. Ritzert"},{"name":"G. Rizzo"},{"name":"L. Rizzuto"},{"name":"S. Robertson"},{"name":"D. R. Perez"},{"name":"J. Roney"},{"name":"C. Rosenfeld"},{"name":"A. Rostomyan"},{"name":"N. Rout"},{"name":"S. Rummel"},{"name":"G. Russo"},{"name":"D. Sahoo"},{"name":"Y. Sakai"},{"name":"M. Salehi"},{"name":"D. Sanders"},{"name":"S. Sandilya"},{"name":"A. Sangal"},{"name":"L. Santelj"},{"name":"J. Sasaki"},{"name":"Y. Sato"},{"name":"V. Savinov"},{"name":"B. Scavino"},{"name":"M. Schram"},{"name":"H. Schreeck"},{"name":"J. Schueler"},{"name":"C. Schwanda"},{"name":"A. Schwartz"},{"name":"R. Seddon"},{"name":"Y. Seino"},{"name":"K. Senyo"},{"name":"O. Seon"},{"name":"I. Seong"},{"name":"M. Sevior"},{"name":"C. Sfienti"},{"name":"M. Shapkin"},{"name":"C. Shen"},{"name":"M. Shimomura"},{"name":"J. Shiu"},{"name":"B. Shwartz"},{"name":"A. Sibidanov"},{"name":"F. Simon"},{"name":"J. Singh"},{"name":"R. Sinha"},{"name":"S. Skambraks"},{"name":"K. Smith"},{"name":"R. Sobie"},{"name":"A. Soffer"},{"name":"A. Sokolov"},{"name":"E. Solovieva"},{"name":"B. Spruck"},{"name":"S. Stanič"},{"name":"M. Starič"},{"name":"N. Starinsky"},{"name":"U. Stolzenberg"},{"name":"Z. Stottler"},{"name":"R. Stroili"},{"name":"J. Strube"},{"name":"J. Stypuła"},{"name":"M. Sumihama"},{"name":"K. Sumisawa"},{"name":"T. Sumiyoshi"},{"name":"D. Summers"},{"name":"W. Sutcliffe"},{"name":"S. Suzuki"},{"name":"M. Tabata"},{"name":"M. Takahashi"},{"name":"M. Takizawa"},{"name":"U. Tamponi"},{"name":"J. Tan"},{"name":"S. Tanaka"},{"name":"K. Tanida"},{"name":"N. Taniguchi"},{"name":"Y. Tao"},{"name":"P. Taras"},{"name":"G. T. Muñoz"},{"name":"F. Tenchini"},{"name":"U. Tippawan"},{"name":"E. Torassa"},{"name":"K. Trabelsi"},{"name":"T. Tsuboyama"},{"name":"M. Uchida"},{"name":"S. Uehara"},{"name":"T. Uglov"},{"name":"Y. Unno"},{"name":"S. Uno"},{"name":"Y. Ushiroda"},{"name":"Y. Usov"},{"name":"S. Vahsen"},{"name":"R. Tonder"},{"name":"G. Varner"},{"name":"K. Varvell"},{"name":"A. Vinokurova"},{"name":"L. Vitale"},{"name":"M. Vos"},{"name":"A. Vossen"},{"name":"E. Waheed"},{"name":"H. Wakeling"},{"name":"K. Wan"},{"name":"M. Wang"},{"name":"X. Wang"},{"name":"B. Wang"},{"name":"A. Warburton"},{"name":"J. Webb"},{"name":"S. Wehle"},{"name":"C. Wessel"}],"abstract":"We present the physics program of the Belle II experiment, located on the intensity frontier SuperKEKB e+e- collider. Belle II collected its first collisions in 2018, and is expected to operate for the next decade. It is anticipated to collect 50/ab of collision data over its lifetime. This book is the outcome of a joint effort of Belle II collaborators and theorists through the Belle II theory interface platform (B2TiP), an effort that commenced in 2014. The aim of B2TiP was to elucidate the potential impacts of the Belle II program, which includes a wide scope of physics topics: B physics, charm, tau, quarkonium, electroweak precision measurements and dark sector searches. It is composed of nine working groups (WGs), which are coordinated by teams of theorist and experimentalists conveners: Semileptonic and leptonic B decays, Radiative and Electroweak penguins, phi_1 and phi_2 (time-dependent CP violation) measurements, phi_3 measurements, Charmless hadronic B decay, Charm, Quarkonium(like), tau and low-multiplicity processes, new physics and global fit analyses. This book highlights \"golden- and silver-channels\", i.e. those that would have the highest potential impact in the field. Theorists scrutinised the role of those measurements and estimated the respective theoretical uncertainties, achievable now as well as prospects for the future. Experimentalists investigated the expected improvements with the large dataset expected from Belle II, taking into account improved performance from the upgraded detector.","source":"Semantic Scholar","year":2018,"language":"en","subjects":["Physics"],"doi":"10.1093/ptep/ptz106","url":"https://www.semanticscholar.org/paper/7617d4015f2521bce6abad3adb8135c272123bc9","pdf_url":"https://academic.oup.com/ptep/article-pdf/2019/12/123C01/32693980/ptz106.pdf","is_open_access":true,"citations":1020,"published_at":"","score":92},{"id":"ss_e3b0ea7209731c47b582215c6c67f9c691ad9863","title":"Deep Q-learning From Demonstrations","authors":[{"name":"Todd Hester"},{"name":"Matej Vecerík"},{"name":"O. Pietquin"},{"name":"Marc Lanctot"},{"name":"T. Schaul"},{"name":"Bilal Piot"},{"name":"Dan Horgan"},{"name":"John Quan"},{"name":"A. Sendonaris"},{"name":"Ian Osband"},{"name":"Gabriel Dulac-Arnold"},{"name":"J. Agapiou"},{"name":"Joel Z. Leibo"},{"name":"A. Gruslys"}],"abstract":"Deep reinforcement learning (RL) has achieved several high profile successes in difficult decision-making problems. However, these algorithms typically require a huge amount of data before they reach reasonable performance. In fact, their performance during learning can be extremely poor. This may be acceptable for a simulator, but it severely limits the applicability of deep RL to many real-world tasks, where the agent must learn in the real environment. In this paper we study a setting where the agent may access data from previous control of the system. We present an algorithm, Deep Q-learning from Demonstrations (DQfD), that leverages small sets of demonstration data to massively accelerate the learning process even from relatively small amounts of demonstration data and is able to automatically assess the necessary ratio of demonstration data while learning thanks to a prioritized replay mechanism. DQfD works by combining temporal difference updates with supervised classification of the demonstrator’s actions. We show that DQfD has better initial performance than Prioritized Dueling Double Deep Q-Networks (PDD DQN) as it starts with better scores on the first million steps on 41 of 42 games and on average it takes PDD DQN 83 million steps to catch up to DQfD’s performance. DQfD learns to out-perform the best demonstration given in 14 of 42 games. In addition, DQfD leverages human demonstrations to achieve state-of-the-art results for 11 games. Finally, we show that DQfD performs better than three related algorithms for incorporating demonstration data into DQN.","source":"Semantic Scholar","year":2017,"language":"en","subjects":["Computer Science"],"doi":"10.1609/aaai.v32i1.11757","url":"https://www.semanticscholar.org/paper/e3b0ea7209731c47b582215c6c67f9c691ad9863","pdf_url":"https://ojs.aaai.org/index.php/AAAI/article/download/11757/11616","is_open_access":true,"citations":1237,"published_at":"","score":91},{"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_0988b91244ae624209d850ce5094296d52ba73d9","title":"Observation of electron-antineutrino disappearance at Daya Bay.","authors":[{"name":"F. An"},{"name":"J. Bai"},{"name":"A. Balantekin"},{"name":"H. Band"},{"name":"D. Beavis"},{"name":"W. Beriguete"},{"name":"M. Bishai"},{"name":"S. Blyth"},{"name":"K. Boddy"},{"name":"R. Brown"},{"name":"B. Cai"},{"name":"G. Cao"},{"name":"J. Cao"},{"name":"R. Carr"},{"name":"W. Chan"},{"name":"J. Chang"},{"name":"Y. Chang"},{"name":"C. Chasman"},{"name":"H. Chen"},{"name":"H. Chen"},{"name":"S. Chen"},{"name":"S. Chen"},{"name":"X. Chen"},{"name":"X. Chen"},{"name":"X. Chen"},{"name":"Y. Chen"},{"name":"Y. Chen"},{"name":"J. Cherwinka"},{"name":"M. Chu"},{"name":"J. Cummings"},{"name":"Z. Deng"},{"name":"Y. Ding"},{"name":"M. Diwan"},{"name":"L. Dong"},{"name":"E. Draeger"},{"name":"X. Du"},{"name":"D. Dwyer"},{"name":"W. Edwards"},{"name":"S. Ely"},{"name":"S. Fang"},{"name":"J. Fu"},{"name":"Z. Fu"},{"name":"L. Ge"},{"name":"V. Ghazikhanian"},{"name":"R. Gill"},{"name":"J. Goett"},{"name":"M. Gonchar"},{"name":"G. Gong"},{"name":"H. Gong"},{"name":"Y. Gornushkin"},{"name":"L. Greenler"},{"name":"W. Gu"},{"name":"M. Guan"},{"name":"X. Guo"},{"name":"R. Hackenburg"},{"name":"R. Hahn"},{"name":"S. Hans"},{"name":"M. He"},{"name":"Q. He"},{"name":"W. He"},{"name":"K. Heeger"},{"name":"Y. Heng"},{"name":"P. Hinrichs"},{"name":"T. Ho"},{"name":"Y. Hor"},{"name":"Y. Hsiung"},{"name":"B. Hu"},{"name":"T. Hu"},{"name":"H. Huang"},{"name":"H. Huang"},{"name":"P. Huang"},{"name":"X. Huang"},{"name":"X. Huang"},{"name":"P. Huber"},{"name":"Z. Isvan"},{"name":"D. Jaffe"},{"name":"S. Jetter"},{"name":"X. Ji"},{"name":"X. Ji"},{"name":"H. Jiang"},{"name":"W. Jiang"},{"name":"J. Jiao"},{"name":"R. Johnson"},{"name":"L. Kang"},{"name":"S. Kettell"},{"name":"M. Kramer"},{"name":"K. Kwan"},{"name":"M. Kwok"},{"name":"T. Kwok"},{"name":"C. Lai"},{"name":"W. Lai"},{"name":"W. Lai"},{"name":"K. Lau"},{"name":"L. Lebanowski"},{"name":"J. Lee"},{"name":"M. K. Lee"},{"name":"R. Leitner"},{"name":"J. Leung"},{"name":"K. Y. Leung"},{"name":"C. Lewis"},{"name":"B. Li"},{"name":"F. Li"},{"name":"G. Li"},{"name":"J. Li"},{"name":"Q. Li"},{"name":"S. Li"},{"name":"W. Li"},{"name":"X. Li"},{"name":"X. Li"},{"name":"X. Li"},{"name":"Y. Li"},{"name":"Z. Li"},{"name":"H. Liang"},{"name":"J. Liang"},{"name":"C. Lin"},{"name":"G. Lin"},{"name":"S. Lin"},{"name":"S. X. Lin"},{"name":"Y. Lin"},{"name":"J. Ling"},{"name":"J. Link"},{"name":"L. Littenberg"},{"name":"B. Littlejohn"},{"name":"B. Liu"},{"name":"C. Liu"},{"name":"D. W. Liu"},{"name":"H. Liu"},{"name":"J. Liu"},{"name":"J. Liu"},{"name":"S. Liu"},{"name":"X. Liu"},{"name":"Y. Liu"},{"name":"C. Lu"},{"name":"H. Lu"},{"name":"A. Luk"},{"name":"K. Luk"},{"name":"T. Luo"},{"name":"X. Luo"},{"name":"L. Ma"},{"name":"Q. Ma"},{"name":"X. Ma"},{"name":"X. Ma"},{"name":"Y. Ma"},{"name":"B. Mayes"},{"name":"K. McDonald"},{"name":"M. McFarlane"},{"name":"R. Mckeown"},{"name":"Y. Meng"},{"name":"D. Mohapatra"},{"name":"J. Morgan"},{"name":"Y. Nakajima"},{"name":"J. Napolitano"},{"name":"D. Naumov"},{"name":"I. Nemchenok"},{"name":"C. Newsom"},{"name":"H. Ngai"},{"name":"W. Ngai"},{"name":"Y. Nie"},{"name":"Z. Ning"},{"name":"J. Ochoa-Ricoux"},{"name":"D. Oh"},{"name":"A. Olshevski"},{"name":"A. Pagac"},{"name":"S. Patton"},{"name":"C. Pearson"},{"name":"V. Pěč"},{"name":"J. C. Peng"},{"name":"L. Piilonen"},{"name":"L. Pinsky"},{"name":"C. Pun"},{"name":"F. Qi"},{"name":"M. Qi"},{"name":"X. Qian"},{"name":"N. Raper"},{"name":"R. Rosero"},{"name":"B. Roskovec"},{"name":"X. Ruan"},{"name":"B. Seilhan"},{"name":"B. Shao"},{"name":"K. Shih"},{"name":"H. Steiner"},{"name":"P. Stoler"},{"name":"G. Sun"},{"name":"J. Sun"},{"name":"Y. Tam"},{"name":"H. Tanaka"},{"name":"X. Tang"},{"name":"H. Themann"},{"name":"Y. Torun"},{"name":"S. Trentalange"},{"name":"O. Tsai"},{"name":"K. Tsang"},{"name":"R. Tsang"},{"name":"C. Tull"},{"name":"B. Viren"},{"name":"S. Virostek"},{"name":"V. Vorobel"},{"name":"C. Wang"},{"name":"L. Wang"},{"name":"L. Wang"},{"name":"L. Wang"},{"name":"M. Wang"},{"name":"N. Wang"},{"name":"R. Wang"},{"name":"T. Wang"},{"name":"W. Wang"},{"name":"X. Wang"},{"name":"Y. Wang"},{"name":"Z. Wang"},{"name":"Z. Wang"},{"name":"D. Webber"},{"name":"Y. Wei"},{"name":"L. Wen"},{"name":"D. Wenman"},{"name":"K. Whisnant"},{"name":"C. White"},{"name":"L. Whitehead"},{"name":"C. Whitten"},{"name":"J. Wilhelmi"},{"name":"T. Wise"},{"name":"H. Wong"},{"name":"H. Wong"},{"name":"J. Wong"},{"name":"E. Worcester"},{"name":"F. F. Wu"},{"name":"Q. Wu"},{"name":"D. Xia"},{"name":"S. Xiang"},{"name":"Q. Xiao"},{"name":"Z. Xing"},{"name":"G. Xu"},{"name":"J. Xu"},{"name":"J. Xu"},{"name":"W. Xu"},{"name":"Y. Xu"},{"name":"T. Xue"},{"name":"C. Yang"},{"name":"L. Yang"},{"name":"M. Ye"},{"name":"M. Yeh"},{"name":"Y. Yeh"},{"name":"K. Yip"},{"name":"B. Young"},{"name":"Z. Yu"},{"name":"L. Zhan"},{"name":"C. Zhang"},{"name":"F. Zhang"},{"name":"J. Zhang"},{"name":"Q. Zhang"},{"name":"K. Zhang"},{"name":"Q. Zhang"},{"name":"S. Zhang"},{"name":"Y. C. Zhang"},{"name":"Y. Zhang"},{"name":"Y. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zhang"},{"name":"Z. Zhang"},{"name":"J. Zhao"},{"name":"Q. Zhao"},{"name":"Y. Zhao"},{"name":"L. Zheng"},{"name":"W. Zhong"},{"name":"L. Zhou"},{"name":"Z. Zhou"},{"name":"H. Zhuang"},{"name":"J. Zou"}],"abstract":"The Daya Bay Reactor Neutrino Experiment has measured a nonzero value for the neutrino mixing angle θ(13) with a significance of 5.2 standard deviations. Antineutrinos from six 2.9 GWth reactors were detected in six antineutrino detectors deployed in two near (flux-weighted baseline 470 m and 576 m) and one far (1648 m) underground experimental halls. With a 43,000 ton-GWth-day live-time exposure in 55 days, 10,416 (80,376) electron-antineutrino candidates were detected at the far hall (near halls). The ratio of the observed to expected number of antineutrinos at the far hall is R=0.940±0.011(stat.)±0.004(syst.). A rate-only analysis finds sin(2)2θ(13)=0.092±0.016(stat.)±0.005(syst.) in a three-neutrino framework.","source":"Semantic Scholar","year":2012,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1103/PhysRevLett.108.171803","url":"https://www.semanticscholar.org/paper/0988b91244ae624209d850ce5094296d52ba73d9","pdf_url":"https://link.aps.org/accepted/10.1103/PhysRevLett.108.171803","is_open_access":true,"citations":2132,"published_at":"","score":86},{"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. Aguilar-Saavedra"},{"name":"M. Agustoni"},{"name":"M. Aharrouche"},{"name":"S. Ahlen"},{"name":"F. Ahles"},{"name":"A. Ahmad"},{"name":"M. Ahsan"},{"name":"G. Aielli"},{"name":"T. Akdogan"},{"name":"T. P. A°kesson"},{"name":"G. Akimoto"},{"name":"A. Akimov"},{"name":"M. Alam"},{"name":"M. A. Alam"},{"name":"J. Albert"},{"name":"S. Albrand"},{"name":"M. Aleksa"},{"name":"I. Aleksandrov"},{"name":"F. Alessandria"},{"name":"C. Alexa"},{"name":"G. Alexander"},{"name":"G. Alexandre"},{"name":"T. Alexopoulos"},{"name":"M. Alhroob"},{"name":"M. Aliev"},{"name":"G. Alimonti"},{"name":"J. Alison"},{"name":"B. Allbrooke"},{"name":"P. Allport"},{"name":"S. Allwood-Spiers"},{"name":"J. Almond"},{"name":"A. Aloisio"},{"name":"R. Alon"},{"name":"A. Alonso"},{"name":"F. Alonso"},{"name":"A. Altheimer"},{"name":"B. Gonzalez"},{"name":"M. Alviggi"},{"name":"K. Amako"},{"name":"C. Amelung"},{"name":"V. Ammosov"},{"name":"S. D. Santos"},{"name":"A. Amorim"},{"name":"N. Amram"},{"name":"C. Anastopoulos"},{"name":"L. Ancu"},{"name":"N. Andari"},{"name":"T. Andeen"},{"name":"C. Anders"},{"name":"G. Anders"},{"name":"K. Anderson"},{"name":"A. Andreazza"},{"name":"V. Andrei"},{"name":"M. Andrieux"},{"name":"X. Anduaga"},{"name":"S. Angelidakis"},{"name":"P. Anger"},{"name":"A. Angerami"},{"name":"F. Anghinolfi"},{"name":"A. Anisenkov"},{"name":"N. Anjos"},{"name":"A. Annovi"},{"name":"A. Antonaki"},{"name":"M. Antonelli"},{"name":"A. Antonov"},{"name":"J. Antoš"},{"name":"F. Anulli"},{"name":"M. Aoki"},{"name":"S. Aoun"},{"name":"L. A. Bella"},{"name":"R. Apolle"},{"name":"R. Apolle"},{"name":"G. Arabidze"},{"name":"I. Aracena"},{"name":"Y. Arai"},{"name":"A. Arce"},{"name":"S. Arfaoui"},{"name":"J. Arguin"},{"name":"E. Arik"},{"name":"M. Arık"},{"name":"A. Armbruster"},{"name":"O. Arnaez"},{"name":"V. Arnal"},{"name":"C. Arnault"},{"name":"A. Artamonov"},{"name":"G. Artoni"},{"name":"D. Arutinov"},{"name":"S. Asai"},{"name":"S. Ask"},{"name":"B. A°sman"},{"name":"L. Asquith"},{"name":"K. Assamagan"},{"name":"A. Astbury"},{"name":"M. Atkinson"},{"name":"B. Aubert"},{"name":"É. Augé"},{"name":"K. Augsten"},{"name":"M. Aurousseau"},{"name":"G. Avolio"},{"name":"R. Avramidou"},{"name":"D. Axen"},{"name":"G. Azuelos"},{"name":"G. Azuelos"},{"name":"Y. Azuma"},{"name":"M. Baak"},{"name":"G. Baccaglioni"},{"name":"C. Bacci"},{"name":"A. Bach"},{"name":"H. Bachacou"},{"name":"K. Bachas"},{"name":"M. Backes"},{"name":"M. Backhaus"},{"name":"J. B. Mayes"},{"name":"E. Badescu"},{"name":"P. Bagnaia"},{"name":"S. Bahinipati"},{"name":"Yuting Bai"},{"name":"D. Bailey"},{"name":"T. Bain"},{"name":"J. Baines"},{"name":"O. Baker"},{"name":"M. Baker"},{"name":"S. Baker"},{"name":"P. Balek"},{"name":"E. Banas"},{"name":"P. Banerjee"},{"name":"S. Banerjee"},{"name":"D. Banfi"},{"name":"A. Bangert"},{"name":"V. Bansal"},{"name":"H. S. Bansil"},{"name":"L. Barak"},{"name":"S. Baranov"},{"name":"A. B. Galtieri"},{"name":"T. Barber"},{"name":"E. Barberio"},{"name":"D. Barberis"},{"name":"M. Barbero"},{"name":"D. Bardin"},{"name":"T. Barillari"},{"name":"M. Barisonzi"},{"name":"T. Barklow"},{"name":"N. Barlow"},{"name":"B. Barnett"},{"name":"R. Barnett"},{"name":"A. Baroncelli"},{"name":"G. Barone"},{"name":"A. Barr"},{"name":"F. Barreiro"},{"name":"J. Costa"},{"name":"P. Barrillon"},{"name":"R. Bartoldus"},{"name":"A. Barton"},{"name":"V. Bartsch"},{"name":"A. Basye"},{"name":"R. Bates"},{"name":"L. Báťková"},{"name":"J. Batley"},{"name":"A. Battaglia"},{"name":"M. Battistin"},{"name":"F. Bauer"},{"name":"H. Bawa"},{"name":"H. Bawa"},{"name":"S. Beale"},{"name":"T. Beau"},{"name":"P. Beauchemin"},{"name":"R. Beccherle"},{"name":"P. Bechtle"},{"name":"H. Beck"},{"name":"A. Becker"},{"name":"S. Becker"},{"name":"M. Beckingham"},{"name":"K. Becks"},{"name":"A. Beddall"},{"name":"A. 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Tutt"},{"name":"J. Ulbricht"},{"name":"T. Urban"},{"name":"V. Vagelli"},{"name":"E. Valente"},{"name":"C. Vannini"},{"name":"E. Valtonen"},{"name":"M. Vargas Treviño"},{"name":"S. Vaurynovich"},{"name":"M. Vecchi"},{"name":"M. Vergain"},{"name":"B. Verlaat"},{"name":"C. Vescovi"},{"name":"J. Vialle"},{"name":"G. Viertel"},{"name":"G. Volpini"},{"name":"D. Wang"},{"name":"N. Wang"},{"name":"Q. Wang"},{"name":"R. Wang"},{"name":"X. Wang"},{"name":"Z. Wang"},{"name":"W. Wallraff"},{"name":"Z. Weng"},{"name":"M. Willenbrock"},{"name":"M. Wlochal"},{"name":"H. Wu"},{"name":"K. Y. Wu"},{"name":"Z. S. Wu"},{"name":"W. Xiao"},{"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":"Z. Zhang"},{"name":"M. M. Zhang"},{"name":"Z. Zheng"},{"name":"H. Zhuang"},{"name":"V. Zhukov"},{"name":"A. Zichichi"},{"name":"P. Zuccon"},{"name":"C. Zurbach"}],"abstract":"","source":"Semantic Scholar","year":2013,"language":"en","subjects":null,"url":"https://www.semanticscholar.org/paper/2bfd0eecdc3c95c4f9fb47271d9765eb18f3c75f","is_open_access":true,"citations":827,"published_at":"","score":81.81},{"id":"ss_be50b7c7107cd48e83ff43d7497f4ca5bf004f71","title":"Monolithic ultra-high-Q lithium niobate microring resonator","authors":[{"name":"Mian Zhang"},{"name":"Cheng Wang"},{"name":"Rebecca Cheng"},{"name":"A. Shams-Ansari"},{"name":"M. Lončar"}],"abstract":"We demonstrate an ultralow loss monolithic integrated lithium niobate photonic platform consisting of dry-etched subwavelength waveguides with extracted propagation losses as low as 2.7 dB/m and microring resonators with quality factors up to 107.","source":"Semantic Scholar","year":2017,"language":"en","subjects":["Materials Science","Physics"],"doi":"10.1364/OPTICA.4.001536","url":"https://www.semanticscholar.org/paper/be50b7c7107cd48e83ff43d7497f4ca5bf004f71","pdf_url":"https://doi.org/10.1364/optica.4.001536","is_open_access":true,"citations":666,"published_at":"","score":80.98},{"id":"ss_261d98443d5f6452c3bc7a3f3ec735ac7ce19e25","title":"Direct evidence for neutrino flavor transformation from neutral-current interactions in the Sudbury Neutrino Observatory.","authors":[{"name":"Q. Ahmad"},{"name":"R. C. Allen"},{"name":"T. Andersen"},{"name":"J. Anglin"},{"name":"J. C. Barton"},{"name":"E. Beier"},{"name":"M. Bercovitch"},{"name":"J. Bigu"},{"name":"S. 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Radcliffe"},{"name":"A. Roberge"},{"name":"B. Robertson"},{"name":"R. Robertson"},{"name":"R. Robertson"},{"name":"S. Rosendahl"},{"name":"J. K. Rowley"},{"name":"V. Rusu"},{"name":"E. Saettler"},{"name":"K. Schaffer"},{"name":"M. Schwendener"},{"name":"A. Schulke"},{"name":"H. Seifert"},{"name":"H. Seifert"},{"name":"H. Seifert"},{"name":"M. Shatkay"},{"name":"J. Simpson"},{"name":"C. Sims"},{"name":"D. Sinclair"},{"name":"D. Sinclair"},{"name":"P. Skensved"},{"name":"A. Smith"},{"name":"M. Smith"},{"name":"T. Spreitzer"},{"name":"N. Starinsky"},{"name":"T. D. Steiger"},{"name":"R. Stokstad"},{"name":"L. Stonehill"},{"name":"R. S. Storey"},{"name":"B. Sur"},{"name":"B. Sur"},{"name":"R. Tafirout"},{"name":"N. Tagg"},{"name":"N. Tagg"},{"name":"N. Tanner"},{"name":"R. Taplin"},{"name":"M. Thorman"},{"name":"P. Thornewell"},{"name":"P. Trent"},{"name":"Y. Tserkovnyak"},{"name":"R. Berg"},{"name":"R. D. Water"},{"name":"R. D. Water"},{"name":"C. Virtue"},{"name":"C. Waltham"},{"name":"J. Wang"},{"name":"D. Wark"},{"name":"D. Wark"},{"name":"D. Wark"},{"name":"N. West"},{"name":"J. Wilhelmy"},{"name":"J. Wilkerson"},{"name":"J. Wilkerson"},{"name":"J. Wilson"},{"name":"P. Wittich"},{"name":"J. Wouters"},{"name":"M. Yeh"}],"abstract":"Observations of neutral-current nu interactions on deuterium in the Sudbury Neutrino Observatory are reported. Using the neutral current (NC), elastic scattering, and charged current reactions and assuming the standard 8B shape, the nu(e) component of the 8B solar flux is phis(e) = 1.76(+0.05)(-0.05)(stat)(+0.09)(-0.09)(syst) x 10(6) cm(-2) s(-1) for a kinetic energy threshold of 5 MeV. The non-nu(e) component is phi(mu)(tau) = 3.41(+0.45)(-0.45)(stat)(+0.48)(-0.45)(syst) x 10(6) cm(-2) s(-1), 5.3sigma greater than zero, providing strong evidence for solar nu(e) flavor transformation. The total flux measured with the NC reaction is phi(NC) = 5.09(+0.44)(-0.43)(stat)(+0.46)(-0.43)(syst) x 10(6) cm(-2) s(-1), consistent with solar models.","source":"Semantic Scholar","year":2002,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1103/PhysRevLett.89.011301","url":"https://www.semanticscholar.org/paper/261d98443d5f6452c3bc7a3f3ec735ac7ce19e25","pdf_url":"http://link.aps.org/pdf/10.1103/PhysRevLett.89.011301","is_open_access":true,"citations":2622,"published_at":"","score":80},{"id":"ss_1492a4f3d45da9da40ed9c742957bf8fb7f342f2","title":"Belle Collaboration","authors":[{"name":"N. Satoyama"},{"name":"K. Abe"},{"name":"I. Adachi"},{"name":"H. Aihara"},{"name":"D. Anipko"},{"name":"A. Bakich"},{"name":"E. Barberio"},{"name":"I. Bedny"},{"name":"K. Belous"},{"name":"U. Bitenc"},{"name":"I. Bizjak"},{"name":"A. Bondar"},{"name":"A. Bozek"},{"name":"M. Bračko"},{"name":"T. Browder"},{"name":"Ming-Chuan Chang"},{"name":"P. Chang"},{"name":"A. Chen"},{"name":"W. Chen"},{"name":"B. Cheon"},{"name":"R. Chistov"},{"name":"Y. Choi"},{"name":"Y. Choi"},{"name":"S. Cole Ap"},{"name":"J. Dalseno"},{"name":"M. Dash"},{"name":"A. Drutskoy"},{"name":"S. Eidelman"},{"name":"S. Fratina"},{"name":"N. Gabyshev"},{"name":"T. Gershon"},{"name":"A. Go"},{"name":"G. Gokhroo"},{"name":"H. Ha"},{"name":"J. Haba"},{"name":"Y. Hasegawa"},{"name":"K. Hayasaka"},{"name":"D. Heffernan"},{"name":"T. Hokuue"},{"name":"Y. Hoshi"},{"name":"S. Hou"},{"name":"W. Hou"},{"name":"T. Iijima"},{"name":"K. Ikado"},{"name":"K. Inami"},{"name":"A. Ishikawa"},{"name":"R. Itoh"},{"name":"M. Iwasaki"},{"name":"Y. Iwasaki"},{"name":"J. H. Kang Ba"},{"name":"S. Kataoka"},{"name":"N. Katayama"},{"name":"H. Kawai"},{"name":"T. Kawasaki"},{"name":"H. Khan"},{"name":"H. Kichimi"},{"name":"H. Kim"},{"name":"S. Kim"},{"name":"Y. Kim"},{"name":"K. Kinoshita"},{"name":"S. Korpar"},{"name":"P. Križan"},{"name":"P. Krokovny"},{"name":"R. Kumar"},{"name":"C. Kuo"},{"name":"A. Kuzmin"},{"name":"Y.-J Kwon Ba"},{"name":"J. Lange"},{"name":"G. Leder"},{"name":"M. Lee"},{"name":"T. Lesiak"},{"name":"A. Limosani"},{"name":"S. Lin"},{"name":"D. Liventsev"},{"name":"G. Majumder"},{"name":"T. Matsumoto"},{"name":"S. Mconie"},{"name":"H. Miyake"},{"name":"H. Miyata"},{"name":"Y. Miyazaki"},{"name":"R. Mizuk"},{"name":"T. Mori"},{"name":"T. Nagamine"},{"name":"I. Nakamura"},{"name":"E. Nakano"},{"name":"M. Nakao"},{"name":"H. Nakazawa"},{"name":"Z. Natkaniec"},{"name":"S. Nishida"},{"name":"O. Nitoh"},{"name":"S. Noguchi"},{"name":"T. Nozaki"},{"name":"S. Ogawa"},{"name":"T. Ohshima"},{"name":"S. Okuno"},{"name":"Y. Onuki"},{"name":"H. Ozaki"},{"name":"P. Pakhlov"},{"name":"G. Pakhlova"},{"name":"H. Park"},{"name":"R. Pestotnik"},{"name":"L. E. Piilonen Az"},{"name":"H. Sahoo"},{"name":"Y. Sakai"},{"name":"T. Schietinger"},{"name":"O. Schneider"},{"name":"J. Schümann"},{"name":"C. Schwanda"},{"name":"R. Seidl"},{"name":"K. Senyo"},{"name":"M. Sevior"},{"name":"M. Shapkin"},{"name":"H. Shibuya"},{"name":"B. Shwartz"},{"name":"J. B. Singh"},{"name":"A. Sokolov"},{"name":"A. Somov"},{"name":"N. Soni"},{"name":"S. Stanič"},{"name":"M. Starič"},{"name":"H. Stoeck"},{"name":"K. Sumisawa"},{"name":"T. Sumiyoshi"},{"name":"S. Suzuki"},{"name":"F. Takasaki"},{"name":"K. Tamai"},{"name":"N. Tamura"},{"name":"M. Tanaka"},{"name":"G. Taylor"},{"name":"Y. Teramoto"},{"name":"X. Tian"},{"name":"I. Tikhomirov"},{"name":"T. Tsuboyama"},{"name":"T. Tsukamoto"},{"name":"S. Uehara"},{"name":"T. Uglov"},{"name":"S. Uno"},{"name":"P. Urquijo"},{"name":"G. Varner"},{"name":"S. Villa"},{"name":"C. C. Wang"},{"name":"C. H. Wang"},{"name":"M. Wang"},{"name":"Y. Watanabe"},{"name":"R. Wedd"},{"name":"E. Won"},{"name":"Q. Xie"},{"name":"Yabsley"},{"name":"A. Yamaguchi"},{"name":"Y. Yamashita"},{"name":"M. Yamauchi"},{"name":"Z. Zhang"},{"name":"V. Zhilich"},{"name":"A. Zupanc"}],"abstract":"","source":"Semantic Scholar","year":2001,"language":"en","subjects":null,"url":"https://www.semanticscholar.org/paper/1492a4f3d45da9da40ed9c742957bf8fb7f342f2","is_open_access":true,"citations":2658,"published_at":"","score":80},{"id":"ss_d774fff858e12537b8a1219078a71d7b6f63b495","title":"Assessing heterogeneity in meta-analysis: Q statistic or I2 index?","authors":[{"name":"Tania B. Huedo-Medina"},{"name":"J. Sánchez-Meca"},{"name":"Fulgencio Marín-Martínez"},{"name":"J. Botella"}],"abstract":"","source":"Semantic Scholar","year":2006,"language":"en","subjects":["Psychology","Medicine"],"doi":"10.1037/1082-989X.11.2.193","url":"https://www.semanticscholar.org/paper/d774fff858e12537b8a1219078a71d7b6f63b495","is_open_access":true,"citations":3823,"published_at":"","score":80},{"id":"ss_bf35564bd43f18633e830b1c2cc5783c48196852","title":"The ALEPH Collaboration","authors":[{"name":"A. Heister"},{"name":"S. Schael"},{"name":"R. Barate"},{"name":"R. Brunelì"},{"name":"I. de Bonis"},{"name":"D. Decamp"},{"name":"C. Goy"},{"name":"S. Jézéquel"},{"name":"J. Lees"},{"name":"F. Martin"},{"name":"E. Merle"},{"name":"M. Minard"},{"name":"B. Pietrzyk"},{"name":"B. Trocmé"},{"name":"G. Boix"},{"name":"S. Bravo"},{"name":"M. Casado"},{"name":"M. Chmeissani"},{"name":"J. M. Crespo"},{"name":"E. Fernández"},{"name":"M. Fernandez-Bosman"},{"name":"L. Garrido"},{"name":"E. Grauges"},{"name":"J. López"},{"name":"M. Martínez"},{"name":"G. Merino"},{"name":"A. Pacheco"},{"name":"D. Paneque"},{"name":"H. Ruiz"},{"name":"A. Colaleo"},{"name":"D. Creanza"},{"name":"N. De Filippis"},{"name":"M. De Palma"},{"name":"G. Iaselli"},{"name":"G. Maggi"},{"name":"M. Maggi"},{"name":"S. Nuzzo"},{"name":"A. Ranieri"},{"name":"G. Raso"},{"name":"F. Ruggieri"},{"name":"G. Selvaggi"},{"name":"L. Silvestris"},{"name":"P. Tempesta"},{"name":"A. Tricomi"},{"name":"G. Zito"},{"name":"X. Huang"},{"name":"J. Lin"},{"name":"Q. Ouyang"},{"name":"T. Wang"},{"name":"Y. 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Hansen"},{"name":"J. Hansen"},{"name":"P. Hansen"},{"name":"B. Nilsson"},{"name":"A. Kyriakis"},{"name":"C. Markou"},{"name":"E. Simopoulou"},{"name":"A. Vayaki"},{"name":"K. Zachariadou"},{"name":"A. Blondel"},{"name":"J. Brient"},{"name":"F. Machefert"},{"name":"A. Rougé"},{"name":"M. Swynghedauw"},{"name":"R. Tanaka"},{"name":"H. Videau"},{"name":"V. Ciulli"},{"name":"E. Focardi"},{"name":"G. Parrini"},{"name":"A. Antonelli"},{"name":"M. Antonelli"},{"name":"G. Bencivenni"},{"name":"F. Bossi"},{"name":"G. Capon"},{"name":"V. Chiarella"},{"name":"P. Laurelli"},{"name":"G. Mannocchi"},{"name":"G. Murtas"},{"name":"L. Passalacqua"},{"name":"J. Kennedy"},{"name":"J. Lynch"},{"name":"P. Negus"},{"name":"V. O 'shea"},{"name":"A. Thompson"},{"name":"S. Wasserbaech"},{"name":"R. Cavanaugh"},{"name":"C. Geweniger"},{"name":"P. Hanke"},{"name":"V. Hepp"},{"name":"E. Kluge"},{"name":"G. Leibenguth"},{"name":"A. Putzer"},{"name":"H. Stenzel"},{"name":"K. Tittel"},{"name":"M. 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Ziegler"},{"name":"A. Bonissent"},{"name":"P. Coyle"},{"name":"C. Curtil"},{"name":"A. Ealet"},{"name":"D. Fouchez"},{"name":"P. Payre"},{"name":"A. Tilquin"},{"name":"F. Ragusa"},{"name":"A. David"},{"name":"H. Dietl"},{"name":"G. Ganis"},{"name":"K. Hüttmann"},{"name":"G. Lütjens"},{"name":"W. Männer"},{"name":"H. Moser"},{"name":"R. Settles"},{"name":"G. Wolf"},{"name":"J. Boucrot"},{"name":"O. Callot"},{"name":"M. Davier"},{"name":"L. Duflot"},{"name":"J. Grivaz"},{"name":"A. Heusse"},{"name":"Jacholkowska"},{"name":"L. Serin"},{"name":"J. Veillet"},{"name":"J. De Vivie De Regie"},{"name":"C. Yuan"},{"name":"G. Bagliesi"},{"name":"T. Boccali"},{"name":"L. Fo"},{"name":"A. Giammanco"},{"name":"A. Giassi"},{"name":"F. Ligabue"},{"name":"A. Messineo"},{"name":"F. Palla"},{"name":"G. Sanguinetti"},{"name":"A. Sciabà"},{"name":"R. Tenchini"},{"name":"A. Venturi"},{"name":"P. Verdini"},{"name":"O. Awunor"},{"name":"G. Blair"},{"name":"G. Cowan"},{"name":"A. Garcia-Bellido"},{"name":"M. Green"},{"name":"L. T. Jones"},{"name":"T. Medcalf"},{"name":"A. Misiejuk"},{"name":"J. Strong"},{"name":"P. Teixeira-Dias"},{"name":"R. Clifft"},{"name":"T. Edgecock"},{"name":"P. Norton"},{"name":"I. Tomalin"},{"name":"B. Bloch-Devaux"},{"name":"D. Boumediene"},{"name":"P. Colas"},{"name":"B. Fabbro"},{"name":"E. Lançon"},{"name":"M. Lemaire"},{"name":"E. Locci"},{"name":"P. Pérez"},{"name":"J. Rander"},{"name":"P. Seager"},{"name":"B. Tuchming"},{"name":"B. Vallage"},{"name":"N. Konstantinidis"},{"name":"A. Litke"},{"name":"G. Taylor"},{"name":"C. Booth"},{"name":"S. Cartwright"},{"name":"F. Combley"},{"name":"P. Hodgson"},{"name":"M. Lehto"},{"name":"L. Thompson"},{"name":"A. Böhrer"},{"name":"S. Brandt"},{"name":"C. Grupen"},{"name":"J. Hess"},{"name":"A. Ngac"},{"name":"G. Prange"},{"name":"U. Sieler"},{"name":"C. Borean"},{"name":"G. Giannini"},{"name":"H. He"},{"name":"J. Putz"},{"name":"J. Rothberg"},{"name":"S. Armstrong"},{"name":"K. Berkelman"},{"name":"K. Cranmer"},{"name":"D. Ferguson"},{"name":"Y. Gao"},{"name":"S. Gonzalez"},{"name":"O. Hayes"},{"name":"H. Hu"},{"name":"S. Jin"},{"name":"J. Kile"},{"name":"P. A. McNamara III"},{"name":"J. Nielsen"},{"name":"Y. Pan"},{"name":"J. V. von Wimmersperg-Toeller"},{"name":"W. Wiedenmann"},{"name":"J. Wu"},{"name":"Sau Wu"},{"name":"X. Wu"},{"name":"G. Zobernig"},{"name":"G. Dissertori"}],"abstract":"","source":"Semantic Scholar","year":1997,"language":"en","subjects":null,"url":"https://www.semanticscholar.org/paper/bf35564bd43f18633e830b1c2cc5783c48196852","is_open_access":true,"citations":1328,"published_at":"","score":80},{"id":"ss_64dff102734bc7e1596898934507a37d8f9c9094","title":"Precision Measurement of the Proton Flux in Primary Cosmic Rays from Rigidity 1 GV to 1.8 TV with the Alpha Magnetic Spectrometer on the International Space Station.","authors":[{"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":"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":"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":"E. Cortina Gil"},{"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":"L. Di Masso"},{"name":"F. Dimiccoli"},{"name":"C. Díaz"},{"name":"P. von Doetinchem"},{"name":"F. Donnini"},{"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. 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Papi"},{"name":"M. Pauluzzi"},{"name":"E. Pedreschi"},{"name":"S. Pensotti"},{"name":"R. Pereira"},{"name":"N. Picot-Clemente"},{"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":"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":"C. Sbarra"},{"name":"S. Schael"},{"name":"S. M. Schmidt"},{"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":"S. Vitillo"},{"name":"L. Wang"},{"name":"N. 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. 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":"A precise measurement of the proton flux in primary cosmic rays with rigidity (momentum/charge) from 1 GV to 1.8 TV is presented based on 300 million events. Knowledge of the rigidity dependence of the proton flux is important in understanding the origin, acceleration, and propagation of cosmic rays. We present the detailed variation with rigidity of the flux spectral index for the first time. The spectral index progressively hardens at high rigidities.","source":"Semantic Scholar","year":2014,"language":"en","subjects":["Physics","Medicine"],"doi":"10.1103/PHYSREVLETT.114.171103","url":"https://www.semanticscholar.org/paper/64dff102734bc7e1596898934507a37d8f9c9094","pdf_url":"http://link.aps.org/pdf/10.1103/PhysRevLett.114.171103","is_open_access":true,"citations":685,"published_at":"","score":78.55},{"id":"ss_1cc50536e9f3c0d0d3056beb5eadb9cce2309a20","title":"Future Physics Programme of BESIII","authors":[{"name":"M. Ablikim"},{"name":"M. Achasov"},{"name":"P. Adlarson"},{"name":"S. Ahmed"},{"name":"M. Albrecht"},{"name":"M. Alekseev"},{"name":"A. Amoroso"},{"name":"F. An"},{"name":"Q. An"},{"name":"Y. Bai"},{"name":"O. Bakina"},{"name":"R. Ferroli"},{"name":"Y. Ban"},{"name":"K. Begzsuren"},{"name":"J. Bennett"},{"name":"N. Berger"},{"name":"M. Bertani"},{"name":"D. Bettoni"},{"name":"F. Bianchi"},{"name":"J. Biernat"},{"name":"J. Bloms"},{"name":"I. Boyko"},{"name":"R. Briere"},{"name":"L. Calibbi"},{"name":"H. Cai"},{"name":"X. Cai"},{"name":"A. Calcaterra"},{"name":"G. Cao"},{"name":"N. Cao"},{"name":"S. Cetin"},{"name":"J. Chai"},{"name":"J. Chang"},{"name":"W. Chang"},{"name":"J. Charles"},{"name":"G. Chelkov"},{"name":"Chen"},{"name":"G. Chen"},{"name":"H. Chen"},{"name":"J. Chen"},{"name":"M. Chen"},{"name":"S. Chen"},{"name":"Y. Chen"},{"name":"H. Y. Cheng"},{"name":"W. Cheng"},{"name":"G. Cibinetto"},{"name":"F. Cossio"},{"name":"X. Cui"},{"name":"H. Dai"},{"name":"J. Dai"},{"name":"X. Dai"},{"name":"A. Dbeyssi"},{"name":"D. Dedovich"},{"name":"Z. Deng"},{"name":"A. Denig"},{"name":"I. Denysenko"},{"name":"M. Destefanis"},{"name":"S. Eidelman"},{"name":"S. Descotes-Genon"},{"name":"F. Mori"},{"name":"Y. Ding"},{"name":"C. Dong"},{"name":"J. Dong"},{"name":"L. Dong"},{"name":"M. Dong"},{"name":"Z. Dou"},{"name":"S. Du"},{"name":"J. Fan"},{"name":"J. Fang"},{"name":"S. Fang"},{"name":"Y. Fang"},{"name":"R. Farinelli"},{"name":"L. Fava"},{"name":"F. Feldbauer"},{"name":"G. Felici"},{"name":"C. Feng"},{"name":"M. Fritsch"},{"name":"C. Fu"},{"name":"Y. Fu"},{"name":"Q. Gao"},{"name":"X. Gao"},{"name":"Y. Gao"},{"name":"Y. Gao"},{"name":"Z. Gao"},{"name":"B. Garillon"},{"name":"I. Garzia"},{"name":"E. Gersabeck"},{"name":"A. Gilman"},{"name":"K. Goetzen"},{"name":"L. Gong"},{"name":"W. Gong"},{"name":"W. Gradl"},{"name":"M. Greco"},{"name":"L. Gu"},{"name":"M. Gu"},{"name":"Y. Gu"},{"name":"A. Guo"},{"name":"F. Guo"},{"name":"L. Guo"},{"name":"R. Guo"},{"name":"Y. Guo"},{"name":"A. Guskov"},{"name":"S. Han"},{"name":"X. Hao"},{"name":"F. Harris"},{"name":"K. He"},{"name":"F. Heinsius"},{"name":"T. Held"},{"name":"Y. Heng"},{"name":"Y. Hou"},{"name":"Z. Hou"},{"name":"H. Hu"},{"name":"J. Hu"},{"name":"T. Hu"},{"name":"Y. Hu"},{"name":"G. Huang"},{"name":"J. Huang"},{"name":"X. Huang"},{"name":"X. Huang"},{"name":"Z. Huang"},{"name":"N. Huesken"},{"name":"T. Hussain"},{"name":"W. Andersson"},{"name":"W. Imoehl"},{"name":"M. Irshad"},{"name":"Q. Ji"},{"name":"Q. Ji"},{"name":"X. Ji"},{"name":"X. Ji"},{"name":"H. Jiang"},{"name":"X. Jiang"},{"name":"X. Jiang"},{"name":"J. Jiao"},{"name":"Z. Jiao"},{"name":"D. Jin"},{"name":"S. Jin"},{"name":"Y. Jin"},{"name":"T. Johansson"},{"name":"N. Kalantar-Nayestanaki"},{"name":"X. Kang"},{"name":"R. Kappert"},{"name":"M. Kavatsyuk"},{"name":"B. Ke"},{"name":"I. Keshk"},{"name":"T. Khan"},{"name":"A. Khoukaz"},{"name":"P. Kiese"},{"name":"R. Kiuchi"},{"name":"R. Kliemt"},{"name":"L. Koch"},{"name":"O. B. Kolcu"},{"name":"B. Kopf"},{"name":"M. Kuemmel"},{"name":"M. Kuessner"},{"name":"A. Kupsc"},{"name":"M. Kurth"},{"name":"M. Kurth"},{"name":"W. Kuehn"},{"name":"J. Lange"},{"name":"P. Larin"},{"name":"L. Lavezzi"},{"name":"H. Leithoff"},{"name":"T. Lenz"},{"name":"C. Li"},{"name":"Cheng Li"},{"name":"D. Li"},{"name":"F. Li"},{"name":"F. Li"},{"name":"G. Li"},{"name":"H. Li"},{"name":"H. Li"},{"name":"J. Li"},{"name":"J. Li"},{"name":"Kenneth K. Li"},{"name":"L. Li"},{"name":"Lei Li"},{"name":"P. Li"},{"name":"P. Li"},{"name":"Q. Li"},{"name":"W. Li"},{"name":"W. Li"},{"name":"X. Li"},{"name":"X. Li"},{"name":"X. Li"},{"name":"X. Li"},{"name":"Z. Li"},{"name":"H. Liang"},{"name":"Y. Liang"},{"name":"Y. Liang"},{"name":"G. Liao"},{"name":"L. Liao"},{"name":"J. Libby"},{"name":"C. Lin"},{"name":"D. Lin"},{"name":"Y. Lin"},{"name":"B. Liu"},{"name":"B. Liu"},{"name":"C. Liu"},{"name":"D. Liu"},{"name":"D. Liu"},{"name":"F. Liu"},{"name":"F. Liu"},{"name":"Feng. Liu"},{"name":"H. Liu"},{"name":"H. Liu"},{"name":"Huanhuan Liu"},{"name":"Huihui Liu"},{"name":"J. Liu"},{"name":"J. Liu"},{"name":"Li-Yu Daisy Liu"},{"name":"Li-Yu Daisy Liu"},{"name":"Q. Liu"},{"name":"S. Liu"},{"name":"T. Liu"},{"name":"X. Liu"},{"name":"X. Liu"},{"name":"Y. Liu"},{"name":"Z. Liu"},{"name":"Zhiqing Liu"},{"name":"Y. Long"},{"name":"X. Lou"},{"name":"H. Lu"},{"name":"J. Lu"},{"name":"J. Lu"},{"name":"Y. Lu"},{"name":"Y. Lu"},{"name":"C. Luo"},{"name":"M. Luo"},{"name":"P. Luo"},{"name":"T. Luo"},{"name":"X. Luo"},{"name":"S. Lusso"},{"name":"X. Lyu"},{"name":"F. Ma"},{"name":"H. Ma"},{"name":"L. Ma"},{"name":"M. Ma"},{"name":"Q. Ma"},{"name":"X. Ma"},{"name":"X. Ma"},{"name":"X. Ma"},{"name":"Y. Ma"},{"name":"F. Maas"},{"name":"M. Maggiora"},{"name":"S. Maldaner"},{"name":"S. Malde"},{"name":"Q. A. Malik"},{"name":"A. Mangoni"},{"name":"Y. Mao"},{"name":"Z. Mao"},{"name":"S. Marcello"},{"name":"Z. Meng"},{"name":"J. Messchendorp"},{"name":"G. Mezzadri"},{"name":"J. Min"},{"name":"T. Min"},{"name":"R. Mitchell"},{"name":"X. Mo"},{"name":"Y. Mo"},{"name":"C. Morales"},{"name":"N. Muchnoi"},{"name":"H. Muramatsu"},{"name":"A. Mustafa"},{"name":"S. Nakhoul"},{"name":"Y. Nefedov"},{"name":"F. Nerling"},{"name":"I. Nikolaev"},{"name":"Z. Ning"},{"name":"S. Nisar"},{"name":"S. Niu"},{"name":"S. Olsen"},{"name":"Q. Ouyang"},{"name":"S. Pacetti"},{"name":"Y. Pan"},{"name":"M. Papenbrock"},{"name":"P. Patteri"},{"name":"M. Pelizaeus"},{"name":"H. Peng"},{"name":"K. Peters"},{"name":"A. Petrov"},{"name":"J. Pettersson"},{"name":"J. Ping"},{"name":"R. Ping"},{"name":"A. Pitka"},{"name":"R. Poling"},{"name":"V. Prasad"},{"name":"M. Qi"},{"name":"T. Qi"},{"name":"S. Qian"},{"name":"C. Qiao"},{"name":"N. Qin"},{"name":"X. Qin"},{"name":"X. Qin"},{"name":"Z. Qin"},{"name":"J. Qiu"},{"name":"S. Qu"},{"name":"K. H. Rashid"},{"name":"C. Redmer"},{"name":"M. Richter"},{"name":"M. Ripka"},{"name":"A. Rivetti"},{"name":"V. Rodin"},{"name":"M. Rolo"},{"name":"G. Rong"},{"name":"J. Rosner"},{"name":"C. Rosner"},{"name":"M. Rump"},{"name":"A. Sarantsev"},{"name":"M. Savrié"},{"name":"K. Schoenning"},{"name":"W. Shan"},{"name":"X. Shan"},{"name":"M. Shao"},{"name":"C. Shen"},{"name":"P. Shen"},{"name":"X. Shen"},{"name":"H. Sheng"},{"name":"X. Shi"},{"name":"X. Shi"},{"name":"J. Song"},{"name":"Q. Song"},{"name":"X. Song"},{"name":"S. Sosio"},{"name":"C. Sowa"},{"name":"S. Spataro"},{"name":"F. Sui"},{"name":"G. Sun"},{"name":"J. Sun"},{"name":"L. Sun"},{"name":"S. Sun"},{"name":"X. Sun"},{"name":"Y. Sun"},{"name":"Y. Sun"},{"name":"Y. Sun"},{"name":"Z. Sun"},{"name":"Z. Sun"},{"name":"Y. Tan"},{"name":"C. Tang"},{"name":"G. Tang"},{"name":"X. Tang"},{"name":"V. Thorén"},{"name":"B. Tsednee"},{"name":"I. Uman"},{"name":"B. Wang"},{"name":"B. Wang"},{"name":"C. Wang"},{"name":"D. Wang"},{"name":"H. H. Wang"},{"name":"K. Wang"},{"name":"L. Wang"},{"name":"L. Wang"},{"name":"M. Wang"},{"name":"M. Wang"},{"name":"Meng Wang"},{"name":"P. Wang"},{"name":"R. Wang"},{"name":"W. Wang"},{"name":"X. Wang"},{"name":"X. Wang"},{"name":"X. Wang"},{"name":"Y. Wang"},{"name":"Y. Wang"},{"name":"Z. Wang"},{"name":"Z. Wang"},{"name":"Z. Wang"},{"name":"Zongyuan Wang"},{"name":"T. Weber"},{"name":"D. Wei"},{"name":"P. Weidenkaff"},{"name":"H. Wen"},{"name":"S. Wen"},{"name":"U. Wiedner"},{"name":"G. Wilkinson"},{"name":"M. Wolke"},{"name":"L. Wu"},{"name":"L. Wu"},{"name":"Z. Wu"},{"name":"L. Xia"},{"name":"Y. Xia"},{"name":"S. Xiao"},{"name":"Y. Xiao"},{"name":"Z. Xiao"},{"name":"Y. Xie"},{"name":"Y. Xie"},{"name":"T. Xing"},{"name":"X. Xiong"},{"name":"Q. L. Xiu"},{"name":"G. Xu"},{"name":"L. Xu"},{"name":"Q. Xu"},{"name":"W. Xu"},{"name":"X. Xu"},{"name":"F. Yan"},{"name":"L. Yan"},{"name":"W. Yan"},{"name":"W. Yan"},{"name":"Y. Yan"},{"name":"H. Yang"},{"name":"H. Yang"},{"name":"L. Yang"},{"name":"R. Yang"},{"name":"S. Yang"},{"name":"Y. Yang"},{"name":"Y. Yang"},{"name":"Yifan Yang"},{"name":"Z. Q. Yang"},{"name":"M. Ye"},{"name":"M. Ye"},{"name":"J. 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":"crossref_10.1016/j.biortech.2026.134117","title":"Hydrodeoxygenation of lignin-derived bio-oil over NiMn/NC catalyst for bio-based liquid fuel","authors":[{"name":"Xiaomeng Yang"},{"name":"Jianping Li"},{"name":"Yuandong Xu"},{"name":"Dan Wu"},{"name":"He Liu"},{"name":"Yongsheng Zhang"},{"name":"Chunbao Xu"}],"abstract":"","source":"CrossRef","year":2026,"language":"en","subjects":null,"doi":"10.1016/j.biortech.2026.134117","url":"https://doi.org/10.1016/j.biortech.2026.134117","is_open_access":true,"published_at":"","score":70},{"id":"arxiv_2601.00466","title":"Rogue Variable Theory: A Quantum-Compatible Cognition Framework with a Rosetta Stone Alignment Algorithm","authors":[{"name":"Jacek Małecki"},{"name":"Alexander Mathiesen-Ohman"}],"abstract":"Many of the most consequential dynamics in human cognition occur \\emph{before} events become explicit: before decisions are finalized, emotions are labeled, or meanings stabilize into narrative form. These pre-event states are characterized by ambiguity, contextual tension, and competing latent interpretations. Rogue Variable Theory (RVT) formalizes such states as \\emph{Rogue Variables}: structured, pre-event cognitive configurations that influence outcomes while remaining unresolved or incompatible with a system's current representational manifold. We present a quantum-consistent information-theoretic implementation of RVT based on a time-indexed \\emph{Mirrored Personal Graph} (MPG) embedded into a fixed graph Hilbert space, a normalized \\emph{Quantum MPG State} (QMS) constructed from node and edge metrics under context, Hamiltonian dynamics derived from graph couplings, and an error-weighted `rogue operator'' whose principal eigenvectors identify rogue factor directions and candidate Rogue Variable segments. We further introduce a \\emph{Rosetta Stone Layer} (RSL) that maps user-specific latent factor coordinates into a shared reference Hilbert space to enable cross-user comparison and aggregation without explicit node alignment. The framework is fully implementable on classical systems and does not assume physical quantum processes; \\emph{collapse} is interpreted as informational decoherence under interaction, often human clarification.","source":"arXiv","year":2026,"language":"en","subjects":["q-bio.NC"],"url":"https://arxiv.org/abs/2601.00466","pdf_url":"https://arxiv.org/pdf/2601.00466","is_open_access":true,"published_at":"2026-01-01T20:34:09Z","score":70},{"id":"arxiv_2502.06057","title":"Neurophysiological correlates to the human brain complexity through $q$-statistical analysis of electroencephalogram","authors":[{"name":"Dimitri Marques Abramov"},{"name":"Daniel de Freitas Quintanilha"},{"name":"Henrique Santos Lima"},{"name":"Roozemeria Pereira Costa"},{"name":"Carla Kamil-Leite"},{"name":"Vladimir V. Lazarev"},{"name":"Constantino Tsallis"}],"abstract":"The prospects of assessing neural complexity (NC) by $q$-statistics of the systemic organization of different types and levels of brain activity were studied. In 70 adult subjects, NC was assessed via the parameter $q$ of $q$-statistics, applied to the ongoing and EEG and its spectral power of 20 scalp points (channels). The NC were estimated both globally for all channels (AllCh) and locally (for each single channel) in different Functional States (FSs). The values of $q$ was compared among FSs and single channels, as well they were correlated with the power of $θ$ (4-8Hz), $β_1$ (15-25Hz) and others EEG bands, in each FS. The value of $q$ across all FSs was higher for AllCh than for the single channels FSs. Consistently with previous studies, we found a negative correlation between NC and age. The FSs did not influence the $q$ of the EEG in AllCh, although locally the FS modulated $q$ in a consistent manner (e.g., reducing $q$ in posterior sites with eyes closed). The $q$ was correlated positively with the power of the $θ$ and negatively with that of the $β_1$ band in general. These findings support the idea that, as a first approach, $q$-statistics can describe the human NC. The relationship between $q$ and $θ$ power aligns with greater NC during FSs such as listening music and resting with eyes open, which is consistent with high-order representations rather than low-informative attentional tasks (OddBall).","source":"arXiv","year":2025,"language":"en","subjects":["q-bio.NC","cond-mat.stat-mech","physics.med-ph"],"url":"https://arxiv.org/abs/2502.06057","pdf_url":"https://arxiv.org/pdf/2502.06057","is_open_access":true,"published_at":"2025-02-09T22:33:21Z","score":69},{"id":"arxiv_2512.10972","title":"Quantifying the Dynamics of Consciousness using Hierarchical Integration, Organised Complexity and Metastability","authors":[{"name":"Hassan Ugail"},{"name":"Newton Howard"}],"abstract":"Quantifying the neural signatures of consciousness remains a major challenge in neuroscience and AI. Although many theories link consciousness to rich, multiscale, and flexible neural organisation, robust quantitative measures are still lacking. This paper presents a theory-neutral framework that characterises consciousness-related dynamics through three properties: hierarchical integration (H), cross-frequency complexity (D), and metastability (M). Candidate subsystems are identified using predictive information, temporal complexity, and state-space exploration to distinguish structured from unstructured activity. We provide mathematical definitions for all components and implement the framework in a generative model of synthetic EEG, simulating nine brain states ranging from psychedelic and wakeful to dreaming, non-REM sleep, minimally conscious, anaesthetised, and seizure-like regimes. Across single trials and Monte Carlo ensembles, the composite index reliably separates high-consciousness from impaired or non-conscious states. We further validate the framework using real EEG from the Sleep-EDF dataset alongside matched synthetic EEG designed to reproduce state-dependent oscillatory structure. Across Wake, N2, and REM sleep, synthetic data recapitulate the empirical ordering and magnitude of the index, indicating that the index captures stable and biologically meaningful distinctions. This approach provides a principled and empirically grounded tool for quantifying consciousness-related neural organisation with potential applications to both biological and artificial systems.","source":"arXiv","year":2025,"language":"en","subjects":["q-bio.NC"],"url":"https://arxiv.org/abs/2512.10972","pdf_url":"https://arxiv.org/pdf/2512.10972","is_open_access":true,"published_at":"2025-12-01T22:30:08Z","score":69},{"id":"crossref_10.1021/acsabm.4c00186","title":"Electrochemical Behavior of Janus Kinase Inhibitor Ruxolitinib at a Taurine-Electropolymerized Carbon Paste Electrode: Insights into Sensing Mechanisms","authors":[{"name":"Hasret Subak"},{"name":"Pınar Talay Pınar"}],"abstract":"","source":"CrossRef","year":2024,"language":"en","subjects":null,"doi":"10.1021/acsabm.4c00186","url":"https://doi.org/10.1021/acsabm.4c00186","pdf_url":"https://pubs.acs.org/doi/pdf/10.1021/acsabm.4c00186","is_open_access":true,"citations":10,"published_at":"","score":68.3},{"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}],"total":1649062,"page":1,"page_size":20,"sources":["CrossRef","arXiv","Semantic Scholar"],"query":"q-bio.NC"}