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As the heaviest known fundamental particle, the top quark has taken a central role in the study of fundamental interactions. The top quark mass is a fundamental parameter of the standard model which places constraints on the Higgs boson…

High Energy Physics - Phenomenology · Physics 2012-10-03 Michele Gallinaro

Recent advances in measuring and interpreting cosmic rays from the spectral ankle to the highest energies are briefly reviewed. A knee of heavy primaries and an ankle of light primaries have been observed at about 10^{17} eV. The light…

High Energy Astrophysical Phenomena · Physics 2014-04-28 Karl-Heinz Kampert

We discuss theoretical issues and experimental data that brought the ultra high energy cosmic rays in the list of Nature's greatest puzzles. After many years of research we still do not know how astrophysical acceleration processes can…

Astrophysics · Physics 2016-08-30 Todor Stanev

From direct observations of the longitudinal development of ultra-high energy air showers performed with the Pierre Auger Observatory, upper limits of 3.8%, 2.4%, 3.5% and 11.7% (at 95% c.l.) are obtained on the fraction of cosmic-ray…

High Energy Astrophysical Phenomena · Physics 2011-12-21 The Pierre Auger Collaboration , J. Abraham , P. Abreu , M. Aglietta , C. Aguirre , E. J. Ahn , D. Allard , I. Allekotte , J. Allen , P. Allison , J. Alvarez-Muñiz , M. Ambrosio , L. Anchordoqui , S. Andringa , A. Anzalone , C. Aramo , S. Argiró , K. Arisaka , F. Arneodo , F. Arqueros , T. Asch , H. Asorey , P. Assis , J. Aublin , M. Ave , G. Avila , T. Bäcker , D. Badagnani , K. B. Barber , A. F. Barbosa , S. L. C. Barroso , B. Baughman , P. Bauleo , J. J. Beatty , T. Beau , B. R. Becker , K. H. Becker , A. Bellétoile , J. A. Bellido , S. BenZvi , C. Berat , P. Bernardini , X. Bertou , P. L. Biermann , P. Billoir , O. Blanch-Bigas , F. Blanco , C. Bleve , H. Blümer , M. Boháčová , C. Bonifazi , R. Bonino , J. Brack , P. Brogueira , W. C. Brown , R. Bruijn , P. Buchholz , A. Bueno , R. E. Burton , N. G. Busca , K. S. Caballero-Mora , L. Caramete , R. Caruso , W. Carvalho , A. Castellina , O. Catalano , L. Cazon , R. Cester , J. Chauvin , A. Chiavassa , J. A. Chinellato , A. Chou , J. Chudoba , J. Chye , R. W. Clay , E. Colombo , R. Conceição , B. Connolly , F. Contreras , J. Coppens , A. Cordier , U. Cotti , S. Coutu , C. E. Covault , A. Creusot , A. Criss , J. Cronin , A. Curutiu , S. Dagoret-Campagne , K. Daumiller , B. R. Dawson , R. M. de Almeida , M. De Domenico , C. De Donato , S. J. de Jong , G. De La Vega , W. J. M. de Mello Junior , J. R. T. de Mello Neto , I. De Mitri , V. de Souza , G. Decerprit , L. del Peral , O. Deligny , A. Della Selva , C. Delle Fratte , H. Dembinski , C. Di Giulio , J. C. Diaz , P. N. Diep , C. Dobrigkeit , J. C. D'Olivo , P. N. Dong , D. Dornic , A. Dorofeev , J. C. dos Anjos , M. T. Dova , D. D'Urso , I. Dutan , M. A. DuVernois , R. Engel , M. Erdmann , C. O. Escobar , A. Etchegoyen , P. Facal San Luis , H. Falcke , G. Farrar , A. C. Fauth , N. Fazzini , F. Ferrer , A. Ferrero , B. Fick , A. Filevich , A. Filipçiç , I. Fleck , S. Fliescher , C. E. Fracchiolla , E. D. Fraenkel , W. Fulgione , R. F. Gamarra , S. Gambetta , B. García , D. García Gámez , D. Garcia-Pinto , X. Garrido , G. Gelmini , H. Gemmeke , P. L. Ghia , U. Giaccari , M. Giller , H. Glass , L. M. Goggin , M. S. Gold , G. Golup , F. Gomez Albarracin , M. Gómez Berisso , P. Gonçalves , M. Gonçalves do Amaral , D. Gonzalez , J. G. Gonzalez , D. Góra , A. Gorgi , P. Gouffon , S. Grebe , M. Grigat , A. F. Grillo , Y. Guardincerri , F. Guarino , G. P. Guedes , J. Gutiérrez , J. D. Hague , V. Halenka , P. Hansen , D. Harari , S. Harmsma , J. L. Harton , A. Haungs , M. D. Healy , T. Hebbeker , G. Hebrero , D. Heck , C. Hojvat , V. C. Holmes , P. Homola , J. R. Hörandel , A. Horneffer , M. Hrabovský , T. Huege , M. Hussain , M. Iarlori , A. Insolia , F. Ionita , A. Italiano , S. Jiraskova , M. Kaducak , K. H. Kampert , T. Karova , P. Kasper , B. Kégl , B. Keilhauer , E. Kemp , R. M. Kieckhafer , H. O. Klages , M. Kleifges , J. Kleinfeller , R. Knapik , J. Knapp , D. -H. Koang , A. Krieger , O. Krömer , D. Kruppke , D. Kuempel , N. Kunka , A. Kusenko , G. La Rosa , C. Lachaud , B. L. Lago , M. S. A. B. Leão , D. Lebrun , P. Lebrun , J. Lee , M. A. Leigui de Oliveira , A. Lemiere , A. Letessier-Selvon , M. Leuthold , I. Lhenry-Yvon , R. López , A. Lopez Agüera , J. Lozano Bahilo , A. Lucero , R. Luna García , M. C. Maccarone , C. Macolino , S. Maldera , D. Mandat , P. Mantsch , A. G. Mariazzi , I. C. Maris , H. R. Marquez Falcon , D. Martello , J. Martínez , O. Martínez Bravo , H. J. Mathes , J. Matthews , J. A. J. Matthews , G. Matthiae , D. Maurizio , P. O. Mazur , M. McEwen , R. R. McNeil , G. Medina-Tanco , M. Melissas , D. Melo , E. Menichetti , A. Menshikov , R. Meyhandan , M. I. Micheletti , G. Miele , W. Miller , L. Miramonti , S. Mollerach , M. Monasor , D. Monnier Ragaigne , F. Montanet , B. Morales , C. Morello , J. C. Moreno , C. Morris , M. Mostafá , S. Mueller , M. A. Muller , R. Mussa , G. Navarra , J. L. Navarro , S. Navas , P. Necesal , L. Nellen , C. Newman-Holmes , D. Newton , P. T. Nhung , N. Nierstenhoefer , D. Nitz , D. Nosek , L. Nožka , J. Oehlschläger , A. Olinto , V. M. Olmos-Gilbaja , M. Ortiz , F. Ortolani , N. Pacheco , D. Pakk Selmi-Dei , M. Palatka , J. Pallotta , G. Parente , E. Parizot , S. Parlati , S. Pastor , M. Patel , T. Paul , V. Pavlidou , K. Payet , M. Pech , J. Pȩkala , R. Pelayo , I. M. Pepe , L. Perrone , R. Pesce , E. Petermann , S. Petrera , P. Petrinca , A. Petrolini , Y. Petrov , J. Petrovic , C. Pfendner , A. Pichel , R. Piegaia , T. Pierog , M. Pimenta , T. P into , V. Pirronello , O. Pisanti , M. Platino , J. Pochon , V. H. Ponce , M. Pontz , P. Privitera , M. Prouza , E. J. Quel , J. Rautenberg , D. Ravignani , A. Redondo , S. Reucroft , B. Revenu , F. A. S. Rezende , J. Ridky , S. Riggi , M. Risse , C. Riviére , V. Rizi , C. Robledo , G. Rodriguez , J. Rodriguez Martino , J. Rodriguez Rojo , I. Rodriguez-Cabo , M. D. Rodríguez-Frías , G. Ros , J. Rosado , M. Roth , B. Rouillé-d'Orfeuil , E. Roulet , A. C. Rovero , F. Salamida , H. Salazar , G. Salina , F. Sánchez , M. Santander , C. E. Santo , E. M. Santos , F. Sarazin , S. Sarkar , R. Sato , N. Scharf , V. Scherini , H. Schieler , P. Schiffer , A. Schmidt , F. Schmidt , T. Schmidt , O. Scholten , H. Schoorlemmer , J. Schovancova , P. Schovánek , F. Schroeder , S. Schulte , F. Schüssler , D. Schuster , S. J. Sciutto , M. Scuderi , A. Segreto , D. Semikoz , M. Settimo , R. C. Shellard , I. Sidelnik , B. B. Siffert , N. Smetniansky De Grande , A. Smiałkowski , R. Šmída , B. E. Smith , G. R. Snow , P. Sommers , J. Sorokin , H. Spinka , R. Squartini , E. Strazzeri , A. Stutz , F. Suarez , T. Suomijärvi , A. D. Supanitsky , M. S. Sutherland , J. Swain , Z. Szadkowski , A. Tamashiro , A. Tamburro , T. Tarutina , O. Taşcǎu , R. Tcaciuc , D. Tcherniakhovski , N. T. Thao , D. Thomas , R. Ticona , J. Tiffenberg , C. Timmermans , W. Tkaczyk , C. J. Todero Peixoto , B. Tomé , A. Tonachini , I. Torres , P. Travnicek , D. B. Tridapalli , G. Tristram , E. Trovato , V. Tuci , M. Tueros , R. Ulrich , M. Unger , M. Urban , J. F. Valdés Galicia , I. Valiño , L. Valore , A. M. van den Berg , R. A. Vázquez , D. Veberič , A. Velarde , T. Venters , V. Verzi , M. Videla , L. Villaseñor , S. Vorobiov , L. Voyvodic , H. Wahlberg , P. Wahrlich , O. Wainberg , D. Warner , A. A. Watson , S. Westerhoff , B. J. Whelan , G. Wieczorek , L. Wiencke , B. Wilczyńska , H. Wilczyński , C. Wileman , M. G. Winnick , H. Wu , B. Wundheiler , P. Younk , G. Yuan , E. Zas , D. Zavrtanik , M. Zavrtanik , I. Zaw , A. Zepeda , M. Ziolkowski

We have investigated the relationship between the kinematics and mass of young (<3x10^8 years) white dwarfs using proper motions. Our sample is taken from the colour selected catalogues of SDSS (Eisenstein et al. 2006) and the Palomar-Green…

Astrophysics of Galaxies · Physics 2015-06-05 Christopher Wegg , E. Sterl Phinney

By comparing the observed orbital decay of the binary pulsars PSRB1913+16 and PSRB1534+12 to that predicted by general relativity due to gravitational-wave emission, we are able to bound the mass of the graviton to be less than…

General Relativity and Quantum Cosmology · Physics 2009-11-07 Patrick J. Sutton , Lee Samuel Finn

Particles are accelerated to very high, non-thermal energies in space, solar, and astrophysical plasma environments. In cosmic ray physics, the "Hillas limit" is often used as a rough estimate (or the necessary condition) of the maximum…

High Energy Astrophysical Phenomena · Physics 2024-12-03 Mitsuo Oka , Kazuo Makishima , Toshio Terasawa

Quantum gravity may lead to an energy dependence in the speed of light. The high energy radiation from gamma-ray pulsars can be used to place limits on such effects. We find that emission from the Crab pulsar at energies above 2 GeV trails…

Astrophysics · Physics 2007-05-23 Philip Kaaret

Gas giants are thought to form by runaway accretion: an instability driven by the self-gravity of growing atmospheres that causes accretion rates to rise super-linearly with planet mass. Why runaway should stop at a Jupiter or any other…

Earth and Planetary Astrophysics · Physics 2019-05-29 Sivan Ginzburg , Eugene Chiang

The shape of the two gas giants, Jupiter and Saturn, is determined primarily by their rotation rate, and interior density distribution. It is also affected by their zonal winds, causing an anomaly of O(10 km) at low latitudes. However,…

Earth and Planetary Astrophysics · Physics 2023-05-05 Eli Galanti , Yohai Kaspi , Tristan Guillot

A simple symmetric random walk is considered on a spider that is a collection of half lines (we call them legs) joined at the origin. We establish a strong approximation of this random walk by the so-called Brownian spider. Transition…

Probability · Mathematics 2015-07-02 Endre Csáki , Miklós Csörgő , Antonia Földes , Pál Révész

In magnetically accreting white dwarfs, the height above the white dwarf surface where the standing shock is formed is intimately related with the accretion rate and the white dwarf mass. However, it is difficult to measure. We obtained new…

High Energy Astrophysical Phenomena · Physics 2018-01-09 G. J. M. Luna , K. Mukai , M. Orio , P. Zemko

Air shower experiments have detected cosmic ray events of energies upto 300 EeV. Most likely these cosmic rays have originated from compact objects. Their exact sources are yet to be identified. It has been suggested before that gamma ray…

Cosmology and Nongalactic Astrophysics · Physics 2010-01-05 Nayantara Gupta

The mass of the top quark is measured in 36.3 fb$^{-1}$ of LHC proton-proton collision data collected with the CMS detector at $\sqrt{s}$ = 13 TeV. The measurement uses a sample of top quark pair candidate events containing one isolated…

High Energy Physics - Experiment · Physics 2023-11-30 CMS Collaboration

(abridged) When preplanetary bodies reach proportions of ~1 km or larger in size, their accretion rate is enhanced due to gravitational focusing (GF). We have developed a new numerical model to calculate the collisional evolution of the…

Earth and Planetary Astrophysics · Physics 2015-05-19 C. W. Ormel , C. P. Dullemond , M. Spaans

We present calculations for the evolution and surviving mass of highly-irradiated extrasolar giant planets (EGPs) at orbital semimajor axes ranging from 0.023 to 0.057 AU using a generalized scaled theory for mass loss, together with new…

Astrophysics · Physics 2007-05-23 W. B. Hubbard , M. F. Hattori , A. Burrows , I. Hubeny , D. Sudarsky

Resonances just above the proton threshold in 30S affect the 29P(p,gamma)30S reaction under astrophysical conditions. The (p,gamma)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances.…

Using data collected at the Pierre Auger Observatory during the past 3.7 years, we demonstrated a correlation between the arrival directions of cosmic rays with energy above ~ 6x10^{19} electron volts and the positions of active galactic…

Astrophysics · Physics 2012-08-27 The Pierre Auger Collaboration

We propose an alternative interpretation of the top events discovered at the Tevatron in 1995. Given that the charge of the $b$ quark jet cannot be measured for the whole sample with certainty, the signal can be due to a quark of charge…

High Energy Physics - Phenomenology · Physics 2008-11-26 Darwin Chang , We-Fu Chang , Ernest Ma

We show that the mass and width of an unstable particle are precisely defined by the pole in the complex energy plane, $\mu = m - (i/2)\Gamma$, by identifying the width, $\Gamma$, with the particle's decay rate and the mass, $m$, with the…

High Energy Physics - Phenomenology · Physics 2024-02-09 Scott Willenbrock