RFI flagging implications for short-duration transients
Astronomy and Computing Elsevier 23 (2018) 103-114
Authors:
Y Cendes, P Prasad, A Rowlinson, RAMJ Wijers, JD Swinbank, CJ Law, AJ van der Horst, D Carbone, JW Broderick, TD Staley, AJ Stewart, F Huizinga, G Molenaar, A Alexov, ME Bell, T Coenen, S Corbel, J Eislöffel, R Fender, J-M Grießmeier, P Jonker, M Kramer, M Kuniyoshi, M Pietka, B Stappers, M Wise, P ZarkaSearch for High-Mass Resonances Decaying to τν in pp Collisions at sqrt[s]=13 TeV with the ATLAS Detector.
Physical review letters 120:16 (2018) 161802
Authors:
M Aaboud, G Aad, B Abbott, O Abdinov, B Abeloos, SH Abidi, OS AbouZeid, NL Abraham, H Abramowicz, H Abreu, Y Abulaiti, BS Acharya, S Adachi, L Adamczyk, J Adelman, M Adersberger, T Adye, AA Affolder, Y Afik, C Agheorghiesei, JA Aguilar-Saavedra, SP Ahlen, F Ahmadov, G Aielli, S Akatsuka, TPA Åkesson, E Akilli, AV Akimov, GL Alberghi, J Albert, P Albicocco, MJ Alconada Verzini, S Alderweireldt, M Aleksa, IN Aleksandrov, C Alexa, G Alexander, T Alexopoulos, M Alhroob, B Ali, M Aliev, G Alimonti, J Alison, SP Alkire, C Allaire, BMM Allbrooke, BW Allen, PP Allport, A Aloisio, A Alonso, F Alonso, C Alpigiani, AA Alshehri, MI Alstaty, B Alvarez Gonzalez, D Álvarez Piqueras, MG Alviggi, BT Amadio, Y Amaral Coutinho, L Ambroz, C Amelung, D Amidei, SP Amor Dos Santos, S Amoroso, CS Amrouche, C Anastopoulos, LS Ancu, N Andari, T Andeen, CF Anders, JK Anders, KJ Anderson, A Andreazza, V Andrei, S Angelidakis, I Angelozzi, A Angerami, AV Anisenkov, A Annovi, C Antel, MT Anthony, M Antonelli, DJ 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Teuscher, SJ Thais, T Theveneaux-Pelzer, F Thiele, JP Thomas, PD Thompson, AS Thompson, LA Thomsen, E Thomson, Y Tian, RE Ticse Torres, VO Tikhomirov, Yu A Tikhonov, S Timoshenko, P Tipton, S Tisserant, K Todome, S Todorova-Nova, S Todt, J Tojo, S Tokár, K Tokushuku, E Tolley, M Tomoto, L Tompkins, K Toms, B Tong, P Tornambe, E Torrence, H Torres, E Torró Pastor, C Tosciri, J Toth, F Touchard, DR Tovey, CJ Treado, T Trefzger, F Tresoldi, A Tricoli, IM Trigger, S Trincaz-Duvoid, MF Tripiana, W Trischuk, B Trocmé, A Trofymov, C Troncon, M Trovatelli, F Trovato, L Truong, M Trzebinski, A Trzupek, F Tsai, KW Tsang, JC-L Tseng, PV Tsiareshka, N Tsirintanis, S Tsiskaridze, V Tsiskaridze, EG Tskhadadze, II Tsukerman, V Tsulaia, S Tsuno, D Tsybychev, Y Tu, A Tudorache, V Tudorache, TT Tulbure, AN Tuna, S Turchikhin, D Turgeman, I Turk Cakir, R Turra, PM Tuts, G Ucchielli, I Ueda, M Ughetto, F Ukegawa, G Unal, A Undrus, G Unel, FC Ungaro, Y Unno, K Uno, J Urban, P Urquijo, P Urrejola, G Usai, J Usui, L Vacavant, V Vacek, B Vachon, KOH Vadla, A Vaidya, C Valderanis, E Valdes Santurio, M Valente, S Valentinetti, A Valero, L Valéry, RA Vallance, A Vallier, JA Valls Ferrer, TR Van Daalen, W Van Den Wollenberg, H van der Graaf, P van Gemmeren, J Van Nieuwkoop, I van Vulpen, MC van Woerden, M Vanadia, W Vandelli, A Vaniachine, P Vankov, R Vari, EW Varnes, C Varni, T Varol, D Varouchas, A Vartapetian, KE Varvell, JG Vasquez, GA Vasquez, F Vazeille, D Vazquez Furelos, T Vazquez Schroeder, J Veatch, V Vecchio, LM Veloce, F Veloso, S Veneziano, A Ventura, M Venturi, N Venturi, V Vercesi, M Verducci, C Vergis, W Verkerke, AT Vermeulen, JC Vermeulen, MC Vetterli, N Viaux Maira, O Viazlo, I Vichou, T Vickey, OE Vickey Boeriu, GHA Viehhauser, S Viel, L Vigani, M Villa, M Villaplana Perez, E Vilucchi, MG Vincter, VB Vinogradov, A Vishwakarma, C Vittori, I Vivarelli, S Vlachos, M Vogel, P Vokac, G Volpi, SE von Buddenbrock, E von Toerne, V Vorobel, K Vorobev, M Vos, JH Vossebeld, N Vranjes, M Vranjes Milosavljevic, V Vrba, M Vreeswijk, R Vuillermet, I Vukotic, P Wagner, W Wagner, J Wagner-Kuhr, H Wahlberg, S Wahrmund, K Wakamiya, J Walder, R Walker, W Walkowiak, V Wallangen, AM Wang, C Wang, F Wang, H Wang, H Wang, J Wang, J Wang, Q Wang, R-J Wang, R Wang, R Wang, SM Wang, T Wang, W Wang, W Wang, Y Wang, Z Wang, C Wanotayaroj, A Warburton, CP Ward, DR Wardrope, A Washbrook, PM Watkins, AT Watson, MF Watson, G Watts, S Watts, BM Waugh, AF Webb, S Webb, C Weber, MS Weber, SM Weber, SA Weber, JS Webster, AR Weidberg, B Weinert, J Weingarten, M Weirich, C Weiser, PS Wells, T Wenaus, T Wengler, S Wenig, N Wermes, MD Werner, P Werner, M Wessels, TD Weston, K Whalen, NL Whallon, AM Wharton, AS White, A White, MJ White, R White, D Whiteson, BW Whitmore, FJ Wickens, W Wiedenmann, M Wielers, C Wiglesworth, LAM Wiik-Fuchs, A Wildauer, F Wilk, HG Wilkens, HH Williams, S Williams, C Willis, S Willocq, JA Wilson, I Wingerter-Seez, E Winkels, F Winklmeier, OJ Winston, BT Winter, M Wittgen, M Wobisch, A Wolf, TMH Wolf, R Wolff, MW Wolter, H Wolters, VWS Wong, NL Woods, SD Worm, BK Wosiek, KW Wozniak, K Wraight, M Wu, SL Wu, X Wu, Y Wu, TR Wyatt, BM Wynne, S Xella, Z Xi, L Xia, D Xu, H Xu, L Xu, T Xu, W Xu, B Yabsley, S Yacoob, K Yajima, DP Yallup, D Yamaguchi, Y Yamaguchi, A Yamamoto, T Yamanaka, F Yamane, M Yamatani, T Yamazaki, Y Yamazaki, Z Yan, H Yang, H Yang, S Yang, Y Yang, Y Yang, Z Yang, W-M Yao, YC Yap, Y Yasu, E Yatsenko, KH Yau Wong, J Ye, S Ye, I Yeletskikh, E Yigitbasi, E Yildirim, K Yorita, K Yoshihara, C Young, CJS Young, J Yu, J Yu, X Yue, SPY Yuen, I Yusuff, B Zabinski, G Zacharis, R Zaidan, AM Zaitsev, N Zakharchuk, J Zalieckas, S Zambito, D Zanzi, C Zeitnitz, G Zemaityte, JC Zeng, Q Zeng, O Zenin, T Ženiš, D Zerwas, M Zgubič, D Zhang, D Zhang, F Zhang, G Zhang, H Zhang, J Zhang, L Zhang, L Zhang, M Zhang, P Zhang, R Zhang, R Zhang, X Zhang, Y Zhang, Z Zhang, X Zhao, Y Zhao, Z Zhao, A Zhemchugov, B Zhou, C Zhou, L Zhou, M Zhou, M Zhou, N Zhou, Y Zhou, CG Zhu, H Zhu, H Zhu, J Zhu, Y Zhu, X Zhuang, K Zhukov, V Zhulanov, A Zibell, D Zieminska, NI Zimine, S Zimmermann, Z Zinonos, M Zinser, M Ziolkowski, L Živković, G Zobernig, A Zoccoli, K Zoch, TG Zorbas, R Zou, M Zur Nedden, L Zwalinski, ATLAS CollaborationAbstract:
A search for high-mass resonances decaying to τν using proton-proton collisions at sqrt[s]=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb^{-1}. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W^{'} bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2-3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level.Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at √ s = 13 TeV with the ATLAS detector
Physical Review D American Physical Society 97:5 (2018) 052010
Authors:
M Aaboud, G Aad, B Abbott, Luca Ambroz, Giacomo Artoni, Moritz Backes, Alan Barr, Kathrin Becker, Lydia Beresford, Daniela Bortoletto, Jonathan TP Burr, Amanda M Cooper-Sarkar, James A Frost, Elizabeth J Gallas, Francesco Giuli, Claire Gwenlan, Christopher P Hays, B Todd Huffman, Cigdem Issever, Jesse KK Liu, Luigi Marchese, Koichi Nagai, Michael E Nelson, Richard B Nickerson, Nurfikri Norjoharuddeen, Mariyan Petrov, Ian PJ Shipsey, Jeffrey C-L Tseng, Georg HA Viehhauser, Luigi Vigani, Anthony R Weidberg, Gabija Zemaityte, Et al.Abstract:
A search for electroweak production of supersymmetric particles in scenarios with compressed mass spectra in final states with two low-momentum leptons and missing transverse momentum is presented. This search uses proton–proton collision data recorded by the ATLAS detector at the Large Hadron Collider in 2015–2016, corresponding to 36.1 fb−1 of integrated luminosity at √ s = 13 TeV. Events with same-flavor pairs of electrons or muons with opposite electric charge are selected. The data are found to be consistent with the Standard Model prediction. Results are interpreted using simplified models of R-parityconserving supersymmetry in which there is a small mass difference between the masses of the produced supersymmetric particles and the lightest neutralino. Exclusion limits at 95% confidence level are set on next-to-lightest neutralino masses of up to 130 GeV for Higgsino production and 170 GeV for wino production, and sleptons masses of up to 180 GeV for pair production of sleptons. In the compressed mass regime, the exclusion limits extend down to mass splittings of 3 GeV for Higgsino production, 2.5 GeV for wino production, and 1 GeV for slepton production. The results are also interpreted in the context of a radiatively-driven natural supersymmetry model with non-universal Higgs boson masses.Tracking of an electron beam through the solar corona with LOFAR
Astronomy and Astrophysics EDP Sciences 611 (2018) A57
Authors:
G Mann, F Breitling, C Vocks, H Aurass, M Steinmetz, KG Strassmeier, MM Bisi, RA Fallows, P Gallagher, A Kerdraon, A Mackinnon, J Magdalenic, H Rucker, J Anderson, A Asgekar, IM Avruch, ME Bell, MJ Bentum, G Bernardi, P Best, L Birzan, A Bonafede, JW Broderick, M Brueggen, HR Butcher, B Ciardi, A Corstanje, F de Gasperin, E de Geus, A Deller, S Duscha, J Eisloeffel, D Engels, H Falcke, Robert Fender, C Ferrari, W Frieswijk, MA Garrett, J Griessmeier, AW Gunst, M van Haarlem, TE Hassall, G Heald, JWT Hessels, M Hoeft, J Horandel, A Horneffer, E Juette, Aris Karastergiou, WFA KlijnAbstract:
The Sun's activity leads to bursts of radio emission, among other phenomena. An example is type-III radio bursts. They occur frequently and appear as short-lived structures rapidly drifting from high to low frequencies in dynamic radio spectra. They are usually interpreted as signatures of beams of energetic electrons propagating along coronal magnetic field lines. Here we present novel interferometric LOFAR (LOw Frequency ARray) observations of three solar type-III radio bursts and their reverse bursts with high spectral, spatial, and temporal resolution. They are consistent with a propagation of the radio sources along the coronal magnetic field lines with nonuniform speed. Hence, the type-III radio bursts cannot be generated by a monoenergetic electron beam, but by an ensemble of energetic electrons with a spread distribution in velocity and energy. Additionally, the density profile along the propagation path is derived in the corona. It agrees well with three-fold coronal density model by (1961, ApJ, 133, 983).On the nature of hydrogen-rich superluminous supernovae
Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 475:1 (2018) 1046-1072