Publications by Cigdem Issever


Search for light resonances decaying to boosted quark pairs and produced in association with a photon or a jet in proton–proton collisions at √s=13 TeV with the ATLAS detector

Physics Letters B Elsevier 788 (2018) 316-335

M Aaboud, G Aad, B Abbott, G Artoni, M Backes, A Barr, C Issever

This Letter presents a search for new light resonances decaying to pairs of quarks and produced in association with a high-pT photon or jet. The dataset consists of proton–proton collisions with an integrated luminosity of 36.1 fb−1 at a centre-of-mass energy of √s=13 TeV recorded by the ATLAS detector at the Large Hadron Collider. Resonance candidates are identified as massive large-radius jets with substructure consistent with a particle decaying into a quark pair. The mass spectrum of the candidates is examined for local excesses above background. No evidence of a new resonance is observed in the data, which are used to exclude the production of a lepto-phobic axial-vector Z′ boson.


Search for pair production of Higgs bosons in the bb¯¯bb¯¯ final state using proton-proton collisions at s√=13 TeV with the ATLAS detector

Journal of High Energy Physics Springer Verlag 2019 (2019) 30

M Aaboud, G Aad, B Abbott, L Ambroz, G Artoni, M Backes, A Barr, L Beresford, D Bortoletto, JTP Burr, A Cooper-Sarkar, J Frost, E Gallas, M Nelson, R Nickerson, N Norjoharuddeen, M Petrov, MA Pickering, A Sharma, I Shipsey, C Tosciri, J Tseng, G Viehhauser, L Vigani, A Weidberg

A search for Higgs boson pair production in the bb¯¯bb¯¯ final state is carried out with up to 36.1 fb−1 of LHC proton-proton collision data collected at s√=13 TeV with the ATLAS detector in 2015 and 2016. Three benchmark signals are studied: a spin-2 graviton decaying into a Higgs boson pair, a scalar resonance decaying into a Higgs boson pair, and Standard Model non-resonant Higgs boson pair production. Two analyses are carried out, each implementing a particular technique for the event reconstruction that targets Higgs bosons reconstructed as pairs of jets or single boosted jets. The resonance mass range covered is 260–3000 GeV. The analyses are statistically combined and upper limits on the production cross section of Higgs boson pairs times branching ratio to bb¯¯bb¯¯ are set in each model. No significant excess is observed; the largest deviation of data over prediction is found at a mass of 280 GeV, corresponding to 2.3 standard deviations globally. The observed 95% confidence level upper limit on the non-resonant production is 13 times the Standard Model prediction. Open image in new window


Manual of BlackMax. A black-hole event generator with rotation, recoil, split branes, and brane tension. Version 2.02

Computer Physics Communications Elsevier 236 (2018) 285-301

DC Dai, C Issever, E Rizvi, G Starkman, D Stojkovic, J Tseng

<p>This is the users manual of the black-hole event generator BlackMax (Dai et al., 2008), which simulates the experimental signatures of microscopic and Planckian black-hole production and evolution at proton–proton, proton–antiproton and electron–positron colliders in the context of brane world models with low-scale quantum gravity. The generator is based on phenomenologically realistic models free of serious problems that plague low-scale gravity. It includes all of the black-hole gray-body factors known to date and incorporates the effects of black-hole rotation, splitting between the fermions, non-zero brane tension and black-hole recoil due to Hawking radiation (although not all simultaneously). The main code can be downloaded from Dai et al. (0000).</p> <p>Program summary</p> <p>Program title: BlackMax</p> <p>Program Files doi: http://dx.doi.org/10.17632/p9jg9dypcg.1</p> <p>Licensing provisions: GNU General Public License version 3</p> <p>Programming language: C (with Fortran subroutines)</p> <p>Nature of problem: In the class of models with low scale quantum gravity (known as the “TeV scale gravity models”) collisions of particles at the particle accelerators may lead to novel phenomena, in particular mini black hole production. In order to confirm or exclude this class of models, one needs to calculate the probability of the black hole production in collisions of particles, properties of the formed black holes (mass, spin, charge, momentum), and the signature of the black hole decay (Hawking radiation).</p> <p>Solution method: BlackMax calculates the probability of the black hole production by utilizing the so-called “geometric cross section” for black hole production. From the energy and quantum numbers of the colliding particles BlackMax calculates the mass, spin, charge, and momentum of the formed black holes. In the next step, BlackMax utilizes the greybody factors that characterize Hawking radiation and calculates the final output. The produced particles are then supposed to leave the signature in particle detectors.</p> <p>References: Phys. Rev. D 77, 076007 (2008)</p> <p>Theoretical background summary</p> <p>Models with TeV-scale quantum gravity offer very rich collider phenomenology. Most of them assume the existence of a three-plus-one-dimensional hypersurface, which is referred as “the brane,” where Standard-Model particles are confined, while only gravity and possibly other particles that carry no gauge quantum numbers, such as right handed neutrinos, can propagate in the full space, the so-called “bulk”. Under certain assumptions, this setup allows the fundamental quantum gravity energy scale, to be close to the electroweak scale. The observed weakness of gravity compared to other forces on the brane (i.e. in the laboratory) is a consequence of the large volume of the bulk which dilutes the strength of gravity. In the context of these models of TeV-scale quantum gravity, probably the most exciting new physics is the production of micro-black-holes in near-future accelerators like the Large Hadron Collider (LHC). According to the “hoop conjecture”, if the impact parameter of two colliding particles is less than two times the gravitational radius, rh, corresponding to their center of-mass energy (ECM), a black-hole with a mass of the order of ECM and horizon radius, rh, will form. Typically, this gravitational radius is approximately ECM /M*2. Thus, when particles collide at center-of-mass energies above M*, the probability of black-hole formation is high.</p> <p>Once a black-hole is formed, it is believed to decay via Hawking radiation. This Hawking radiation will consist of two parts: radiation of Standard-Model particles into the brane and radiation of gravitons and any other bulk modes into the bulk. The relative probability for the emission of each particle type is given by the gray-body factor for that mode. This gray-body factor depends on the properties of the particle (charge, spin, mass, momentum), of the black-hole (mass, spin, charge) and, in the context of TeV-scale quantum gravity, on environmental properties such as the number of extra dimensions, the location of the black-hole relative to the brane (or branes), etc. In order to properly describe the experimental signatures of black-hole production and decay one must therefore calculate the gray-body factors for all of the relevant degrees of freedom.</p> <p>Since a black hole can emit particles like quarks and gluons which cannot freely propagate long distance, one has to simulate the process of hadronization. The generator can be interfaced with hadronization generators Herwig and Pythia to obtain the final signature measurable in particle detectors.</p>


Search for Higgs boson pair production in the b¯bWW∗ decay mode at √s = 13 TeV with the ATLAS detector

Journal of High Energy Physics Springer Berlin Heidelberg 2019 (2019) 92

M Aaboud, G Aad, B Abbott, L Ambroz, G Artoni, M Backes, AJ Barr, L Beresford, D Bortoletto, J Burr, AM Cooper-Sarkar, JA Frost, EJ Gallas, F Giuli, C Gwenlan, C Hays, BT Huffman, C Issever, JKK Liu, L Marchese, K Nagai, ME Nelson, RB Nickerson, L Vigani, G Zemaityte

A search for Higgs boson pair production in the b ¯bWW∗ decay mode is performed in the b ¯b`νqq final state using 36.1 fb−1 of proton-proton collision data at a centreof-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider. No evidence of events beyond the background expectation is found. Upper limits on the non-resonant pp → HH production cross section of 10 pb and on the resonant production cross section as a function of the HH invariant mass are obtained. Resonant production limits are set for scalar and spin-2 graviton hypotheses in the mass range 500 to 3000 GeV.


Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in pp collisions at √s=13 TeV

Physical Review Letters American Physical Society 121 (2018) 081801

KJ Anderson, A Andreazza, V Andrei, S Angelidakis, I Angelozzi, A Angerami, AV Anisenkov, A Annovi, C Antel, MT Anthony, M Antonelli, DJA Antrim, ATH Arce, RE Ardell, FA Arduh, J-F Arguin, S Argyropoulos, O Arnaez, O Arslan, A Artamonov, G Artoni, S Artz, S Asai, N Asbah, EM Asimakopoulou

Searches for dijet resonances with sub-TeV masses using the ATLAS detector at the Large Hadron Collider can be statistically limited by the bandwidth available to inclusive single-jet triggers, whose data-collection rates at low transverse momentum are much lower than the rate from standard model multijet production. This Letter describes a new search for dijet resonances where this limitation is overcome by recording only the event information calculated by the jet trigger algorithms, thereby allowing much higher event rates with reduced storage needs. The search targets low-mass dijet resonances in the range 450–1800 GeV. The analyzed data set has an integrated luminosity of up to 29.3 fb−1 and was recorded at a center-of-mass energy of 13 TeV. No excesses are found; limits are set on Gaussian-shaped contributions to the dijet mass distribution from new particles and on a model of dark-matter particles with axial-vector couplings to quarks.


Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton-proton collisions at s=13  TeV with the ATLAS detector

European Physical Journal C: Particles and Fields Springer Verlag 78 (2018)

G Artoni, M Backes, A Barr, L Beresford, D Bortoletto, JTP Burr, J Frost, F Giuli, C Gwenlan, C Hays, T Huffman, C Issever, J Liu, L Marchese, R Nickerson, N Norjoharuddeen, M Petrov, MA Pickering, A Sharma, G Viehhauser, L Vigani, A Weidberg, G Zemaityte, M Zgubič

A search for new heavy particles that decay into top-quark pairs is performed using data collected from proton-proton collisions at a centre-of-mass energy of 13  TeV by the ATLAS detector at the Large Hadron Collider. The integrated luminosity of the data sample is 36.1 fb -1 . Events consistent with top-quark pair production are selected by requiring a single isolated charged lepton, missing transverse momentum and jet activity compatible with a hadronic top-quark decay. Jets identified as likely to contain b-hadrons are required to reduce the background from other Standard Model processes. The invariant mass spectrum of the candidate top-quark pairs is examined for local excesses above the background expectation. No significant deviations from the Standard Model predictions are found. Exclusion limits are set on the production cross-section times branching ratio for hypothetical Z' bosons, Kaluza-Kein gluons and Kaluza-Klein gravitons that decay into top-quark pairs.


Search for resonances in the mass distribution of jet pairs with one or two jets identified as b-jets in proton-proton collisions at root s=13 TeV with the ATLAS detector

PHYSICAL REVIEW D 98 (2018) ARTN 032016

M Aaboud, G Aad, B Abbott, O Abdinov, B Abeloos, DK Abhayasinghe, SH Abidi, OS AbouZeid, NL Abraham, H Abramowicz, H Abreu, Y Abulaiti, BS Acharya, S Adachi, L Adamczyk, J Adelman, M Adersberger, A Adiguzel, T Adye, AA Affolder, Y Afik, C Agheorghiesei, JA Aguilar-Saavedra, F Ahmadov, G Aielli, S Akatsuka, TPA Akesson, E Akilli, AV Akimov, GL Alberghi, J Albert, P Albicocco, MJA Verzini, S Alderweireldt, M Aleksa, IN Aleksandrov, C Alexa, T Alexopoulos, M Alhroob, B Ali, 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, BA Gonzalez, D Alvarez Piqueras, MG Alviggi, BT Amadio, YA Coutinho, L Ambroz, C Amelung, D Amidei, SPA Dos Santos, S Amoroso, CS Amrouche, C Anastopoulos, LS Ancu, N Andari, T Andeen, CF Anders, JK Anders, KJ Anderson, A Andreazza, V Andrei, CR Anelli, S Angelidakis, I Angelozzi, A Angerami, AV Anisenkov, A Annovi, C Antel, MT Anthony, M Antonelli, DJA Antrim, F Anulli, M Aoki, LA Bella, G Arabidze, Y Arai, JP Araque, V Araujo Ferraz, R Araujo Pereira, ATH Arce, RE Ardell, FA Arduh, J-F Arguin, S Argyropoulos, AJ Armbruster, LJ Armitage, A Armstrong, O Arnaez, H Arnold, M Arratia, O Arslan, A Artamonov, G Artoni, S Artz, S Asai, N Asbah, A Ashkenazi, EM Asimakopoulou, L Asquith, K Assamagan, R Astalos, RJ Atkin, M Atkinson, NB Atlay, K Augsten, G Avolio, R Avramidou, B Axen, MK Ayoub, G Azuelos, AE Baas, MJ Baca, H Bachacou, K Bachas, M Backes, P Bagnaia, M Bahmani, H Bahrasemani, AJ Bailey, JT Baines, M Bajic, C Bakalis, OK Baker, PJ Bakker, DB Gupta, EM Baldin, P Balek, F Balli, WK Balunas, J Balz, E Banas, A Bandyopadhyay, S Banerjee, AAE Bannoura, L Barak, WM Barbe, EL Barberio, D Barberis, M Barbero, T Barillari, M-S Barisits, J Barkeloo, T Barklow, N Barlow, R Barnea, SL Barnes, BM Barnett, RM Barnett, Z Barnovska-Blenessy, A Baroncelli, G Barone, AJ Barr, L Barranco Navarro, F Barreiro, J Barreiro Guimaraes da Costa, R Bartoldus, AE Barton, P Bartos, A Basalaev, A Bassalat, RL Bates, SJ Batista, S Batlamous, JR Batley, M Battaglia, M Bauce, F Bauer, KT Bauer, HS Bawa, JB Beacham, MD Beattie, T Beau, PH Beauchemin, P Bechtle, HC Beck, HP Beck, K Becker, M Becker, C Becot, A Beddall, AJ Beddall, VA Bednyakov, M Bedognetti, CP Bee, TA Beermann, M Begalli, M Begel, A Behera, JK Behr, AS Bell, G Bella, L Bellagamba, A Bellerive, M Bellomo, P Bellos, K Belotskiy, NL Belyaev, O Benary, D Benchekroun, M Bender, N Benekos, Y Benhammou, EB Noccioli, J Benitez, DP Benjamin, M Benoit, JR Bensinger, S Bentvelsen, L Beresford, M Beretta, D Berge, EB Kuutmann, N Berger, LJ Bergsten, J Beringer, S Berlendis, NR Bernard, G Bernardi, C Bernius, FU Bernlochner, T Berry, P Berta, C Bertella, G Bertoli, IA Bertram, GJ Besjes, OB Bylund, M Bessner, N Besson, A Bethani, S Bethke, A Betti, AJ Bevan, J Beyer, RMB Bianchi, O Biebel, D Biedermann, R Bielski, K Bierwagen, NV Biesuz, M Biglietti, TRV Billoud, M Bindi, A Bingul, C Bini, S Biondi, T Bisanz, JP Biswal, C Bittrich, DM Bjergaard, JE Black, KM Black, RE Blair, T Blazek, I Bloch, C Blocker, A Blue, U Blumenschein, D Blunier, GJ Bobbink, VS Bobrovnikov, SS Bocchetta, A Bocci, D Boerner, D Bogavac, AG Bogdanchikov, C Bohm, V Boisvert, P Bokan, T Bold, AS Boldyrev, AE Bolz, M Bomben, M Bona, JS Bonilla, M Boonekamp, A Borisov, G Borissov, J Bortfeldt, D Bortoletto, V Bortolotto, D Boscherini, M Bosman, JDB Sola, K Bouaouda, J Boudreau, EV Bouhova-Thacker, D Boumediene, C Bourdarios, SK Boutle, A Boveia, J Boyd, IR Boyko, AJ Bozson, J Bracinik, N Brahimi, A Brandt, G Brandt, O Brandt, F Braren, U Bratzler, B Brau, JE Brau, WDB Madden, K Brendlinger, AJ Brennan, L Brenner, R Brenner, S Bressler, B Brickwedde, DL Briglin, D Britton, D Britzger, I Brock, R Brock, G Brooijmans, T Brooks, WK Brooks, E Brost, JH Broughton, PAB de Renstrom, D Bruncko, A Bruni, G Bruni, LS Bruni, S Bruno, BH Brunt, M Bruschi, N Bruscino, P Bryant, L Bryngemark, T Buanes, Q Buat, P Buchholz, AG Buckley, IA Budagov, F Buehrer, MK Bugge, O Bulekov, D Bullock, TJ Burch, S Burdin, CD Burgard, AM Burger, B Burghgrave, K Burka, S Burke, I Burmeister, JTP Burr, D Buescher, V Buescher, E Buschmann, P Bussey, JM Butler, CM Buttar, JM Butterworth, P Butti, W Buttinger, A Buzatu, AR Buzykaev, G Cabras, SC Urban, D Caforio, H Cai, VMM Cairo, O Cakir, N Calace, P Calafiura, A Calandri, G Calderini, P Calfayan, G Callea, LP Caloba, SC Lopez, D Calvet, S Calvet, TP Calvet, M Calvetti, RC Toro, S Camarda, P Camarri, D Cameron, RC Armadans, C Camincher, S Campana, M Campanelli, A Camplani, A Campoverde, V Canale, MC Bret, J Cantero, T Cao, Y Cao, MDMC Garrido, I Caprini, M Caprini, M Capua, RM Carbone, R Cardarelli, FC Cardillo, I Carli, T Carli, G Carlino, BT Carlson, L Carminati, RMD Carney, S Caron, E Carquin, S Carra, GD Carrillo-Montoya, D Casadei, MP Casado, AF Casha, M Casolino, DW Casper, R Castelijn, FL Castillo, VC Gimenez, NF Castro, A Catinaccio, JR Catmore, A Cattai, J Caudron, V Cavaliere, E Cavallaro, D Cavalli, M Cavalli-Sforza, V Cavasinni, E Celebi, F Ceradini, LC Alberich, AS Cerqueira, A Cerri, L Cerrito, F Cerutti, A Cervelli, SA Cetin, A Chafaq, D Chakraborty, SK Chan, WS Chan, YL Chan, P Chang, JD Chapman, DG Charlton, CC Chau, CAC Barajas, S Che, A Chegwidden, S Chekanov, SV Chekulaev, GA Chelkov, MA Chelstowska, C Chen, CH Chen, H Chen, J Chen, J Chen, S Chen, SJ Chen, X Chen, Y Chen, Y-H Chen, HC Cheng, HJ Cheng, A Cheplakov, E Cheremushkina, RC El Moursli, E Cheu, K Cheung, L Chevalier, V Chiarella, G Chiarelli, G Chiodini, AS Chisholm, A Chitan, I Chiu, YH Chiu, MV Chizhov, K Choi, AR Chomont, S Chouridou, YS Chow, V Christodoulou, MC Chu, J Chudoba, AJ Chuinard, JJ Chwastowski, L Chytka, D Cinca, V Cindro, IA Cioara, A Ciocio, F Cirotto, ZH Citron, M Citterio, A Clark, MR Clark, PJ Clark, C Clement, Y Coadou, M Cobal, A Coccaro, J Cochran, AEC Coimbra, L Colasurdo, B Cole, AP Colijn, J Collot, PC Muino, E Coniavitis, SH Connell, IA Connelly, S Constantinescu, F Conventi, AM Cooper-Sarkar, F Cormier, KJR Cormier, M Corradi, EE Corrigan, F Corriveau, A Cortes-Gonzalez, MJ Costa, D Costanzo, G Cottin, G Cowan, BE Cox, J Crane, K Cranmer, SJ Crawley, RA Creager, G Cree, S Crepe-Renaudin, F Crescioli, M Cristinziani, V Croft, G Crosetti, A Cueto, TC Donszelmann, AR Cukierman, M Curatolo, J Cuth, S Czekierda, P Czodrowski, MJ Da Cunha Sargedas De Sousa, C Da Via, W Dabrowski, T Dado, S Dahbi, T Dai, F Dallaire, C Dallapiccola, M Dam, G D'amen, J Damp, JR Dandoy, MF Daneri, NP Dang, ND Dann, M Danninger, V Dao, G Darbo, S Darmora, O Dartsi, A Dattagupta, T Daubney, S D'Auria, W Davey, C David, T Davidek, DR Davis, E Dawe, I Dawson, K De, R De Asmundis, A De Benedetti, S De Castro, S De Cecco, N De Groot, P De Jong, H De la Torre, F De Lorenzi, A De Maria, D De Pedis, A De Salvo, U De Sanctis, A De Santo, KDV Corga, JBDV De Regie, C Debenedetti, DV Dedovich, N Dehghanian, M Del Gaudio, J Del Peso, D Delgove, F Deliot, CM Delitzsch, M Della Pietra, D Della Volpe, A Dell'Acqua, L Dell'Asta, M Delmastro, C Delporte, PA Delsart, DA DeMarco, S Demers, M Demichev, SP Denisov, D Denysiuk, L D'Eramo, D Derendarz, JE Derkaoui, F Derue, P Dervan, K Desch, C Deterre, K Dette, MR Devesa, PO Deviveiros, A Dewhurst, S Dhaliwal, FA Di Bello, A Di Ciaccio, L Di Ciaccio, WK Di Clemente, C Di Donato, A Di Girolamo, B Di Micco, R Di Nardo, KF Di Petrillo, A Di Simone, R Di Sipio, D Di Valentino, C Diaconu, M Diamond, FA Dias, TD Do Vale, MA Diaz, J Dickinson, EB Diehl, J Dietrich, SD Cornell, A Dimitrievska, J Dingfelder, F Dittus, F Djama, T Djobava, JI Djuvsland, MAB Do Vale, M Dobre, D Dodsworth, C Doglioni, J Dolejsi, Z Dolezal, M Donadelli, J Donini, A D'onofrio, M D'Onofrio, J Dopke, A Doria, MT Dova, AT Doyle, E Drechsler, E Dreyer, T Dreyer, M Dris, Y Du, J Duarte-Campderros, F Dubinin, M Dubovsky, A Dubreuil, E Duchovni, G Duckeck, A Ducourthial, OA Ducu, D Duda, A Dudarev, AC Dudder, EM Duffield, L Duflot, M Duhrssen, C Dulsen, M Dumancic, AE Dumitriu, AK Duncan, M Dunford, A Duperrin, HD Yildiz, M Duren, A Durglishvili, D Duschinger, B Dutta, D Duvnjak, M Dyndal, S Dysch, BS Dziedzic, C Eckardt, KM Ecker, RC Edgar, T Eifert, G Eigen, K Einsweiler, T Ekelof, M El Kacimi, R El Kosseifi, V Ellajosyula, M Ellert, F Ellinghaus, AA Elliot, N Ellis, J Elmsheuser, M Elsing, D Emeliyanov, Y Enari, JS Ennis, MB Epland, J Erdmann, A Ereditato, S Errede, M Escalier, C Escobar, B Esposito, OE Pastor, AI Etienvre, E Etzion, H Evans, A Ezhilov, M Ezzi, F Fabbri, L Fabbri, V Fabiani, G Facini, RM Faisca Rodrigues Pereira, RM Fakhrutdinov, S Falciano, PJ Falke, S Falke, J Faltova, Y Fang, M Fanti, A Farbin, A Farilla, EM Farina, T Farooque, S Farrell, SM Farrington, P Farthouat, F Fassi, P Fassnacht, D Fassouliotis, MF Giannelli, A Favareto, WJ Fawcett, L Fayard, OL Fedin, W Fedorko, M Feickert, S Feigl, L Feligioni, C Feng, EJ Feng, M Feng, MJ Fenton, AB Fenyuk, L Feremenga, J Ferrando, A Ferrari, P Ferrari, R Ferrari, DEF de Lima, A Ferrer, D Ferrere, C Ferretti, F Fiedler, A Filipcic, F Filthaut, KD Finelli, MCN Fiolhais, L Fiorini, C Fischer, WC Fisher, N Flaschel, I Fleck, P Fleischmann, RRM Fletcher, T Flick, BM Flierl, LM Flores, LRF Castillo, N Fomin, GT Forcolin, A Formica, FA Forster, AC Forti, AG Foster, D Fournier, H Fox, S Fracchia, P Francavilla, M Franchini, S Franchino, D Francis, L Franconi, M Franklin, M Frate, M Fraternali, D Freeborn, SM Fressard-Batraneanu, B Freund, WS Freund, D Froidevaux, JA Frost, C Fukunaga, T Fusayasu, J Fuster, O Gabizon, A Gabrielli, A Gabrielli, GP Gach, S Gadatsch, P Gadow, G Gagliardi, LG Gagnon, C Galea, B Galhardo, EJ Gallas, BJ Gallop, P Gallus, G Galster, RG Goni, KK Gan, S Ganguly, Y Gao, YS Gao, C Garcia, JE Garcia Navarro, JA Garcia Pascual, M Garcia-Sciveres, RW Gardner, N Garelli, V Garonne, K Gasnikova, A Gaudiello, G Gaudio, IL Gavrilenko, A Gavrilyuk, C Gay, G Gaycken, EN Gazis, CNP Gee, J Geisen, M Geisen, MP Geisler, K Gellerstedt, C Gemme, MH Genest, C Geng, S Gentile, C Gentsos, S George, D Gerbaudo, G Gessner, S Ghasemi, MG Bostanabad, M Ghneimat, B Giacobbe, S Giagu, N Giangiacomi, P Giannetti, SM Gibson, M Gignac, D Gillberg, G Gilles, DM Gingrich, MP Giordani, FM Giorgi, PF Giraud, P Giromini, G Giugliarelli, D Giugni, F Giuli, M Giulini, S Gkaitatzis, I Gkialas, EL Gkougkousis, P Gkountoumis, LK Gladilin, C Glasman, J Glatzer, PCF Glaysher, A Glazov, M Goblirsch-Kolb, J Godlewski, S Goldfarb, T Golling, D Golubkov, A Gomes, RG Gama, R Goncalo, G Gonella, L Gonella, A Gongadze, F Gonnella, JL Gonski, S Gonzalez de la Hoz, S Gonzalez-Sevilla, L Goossens, PA Gorbounov, HA Gordon, B Gorini, E Gorini, A Gorisek, AT Goshaw, C Gossling, MI Gostkin, CA Gottardo, CR Goudet, D Goujdami, AG Goussiou, N Govender, C Goy, E Gozani, I Grabowska-Bold, POJ Gradin, EC Graham, J Gramling, E Gramstad, S Grancagnolo, V Gratchev, PM Gravila, C Gray, HM Gray, ZD Greenwood, C Grefe, K Gregersen, IM Gregor, P Grenier, K Grevtsov, J Griffiths, AA Grillo, K Grimm, S Grinstein, P Gris, J-F Grivaz, S Groh, E Gross, J Grosse-Knetter, GC Grossi, ZJ Grout, C Grud, A Grummer, L Guan, W Guan, J Guenther, A Guerguichon, F Guescini, D Guest, R Gugel, B Gui, T Guillemin, S Guindon, U Gul, C Gumpert, J Guo, W Guo, Y Guo, Z Guo, R Gupta, S Gurbuz, G Gustavino, BJ Gutelman, P Gutierrez, C Gutschow, C Guyot, MP Guzik, C Gwenlan, CB Gwilliam, A Haas, C Haber, HK Hadavand, N Haddad, A Hadef, S Hagebock, M Hagihara, H Hakobyan, M Haleem, J Haley, G Halladjian, GD Hallewell, K Hamacher, P Hamal, K Hamano, A Hamilton, GN Hamity, K Han, L Han, S Han, K Hanagaki, M Hance, DM Handl, B Haney, R Hankache, P Hanke, E Hansen, JB Hansen, JD Hansen, MC Hansen, PH Hansen, K Hara, AS Hard, T Harenberg, S Harkusha, PF Harrison, NM Hartmann, Y Hasegawa, A Hasib, S Hassani, S Haug, R Hauser, L Hauswald, LB Havener, M Havranek, CM Hawkes, RJ Hawkings, D Hayden, C Hayes, CP Hays, JM Hays, HS Hayward, SJ Haywood, MP Heath, V Hedberg, L Heelan, S Heer, KK Heidegger, J Heilman, S Heim, T Heim, B Heinemann, JJ Heinrich, L Heinrich, C Heinz, J Hejbal, L Helary, A Held, S Hellesund, S Hellman, C Helsens, RCW Henderson, Y Heng, S Henkelmann, AMH Correia, GH Herbert, H Herde, V Herget, Y Hernandez Jimenez, H Herr, G Herten, R Hertenberger, L Hervas, TC Herwig, GG Hesketh, NP Hessey, JW Hetherly, S Higashino, E Higon-Rodriguez, K Hildebrand, E Hill, JC Hill, KK Hill, KH Hiller, SJ Hillier, M Hils, I Hinchliffe, M Hirose, D Hirschbuehl, B Hiti, O Hladik, DR Hlaluku, X Hoad, J Hobbs, N Hod, MC Hodgkinson, A Hoecker, MR Hoeferkamp, F Hoenig, D Hohn, D Hohov, TR Holmes, M Holzbock, M Homann, S Honda, T Honda, TM Hong, A Honle, BH Hooberman, WH Hopkins, Y Horii, P Horn, AJ Horton, LA Horyn, J-Y Hostachy, A Hostiuc, S Hou, A Hoummada, J Howarth, J Hoya, M Hrabovsky, J Hrdinka, I Hristova, J Hrivnac, A Hrynevich, T Hryn'ova, PJ Hsu, S-C Hsu, Q Hu, S Hu, Y Huang, Z Hubacek, F Hubaut, M Huebner, F Huegging, TB Huffman, EW Hughes, M 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Vankov, R Vari, EW Varnes, C Varni, T Varol, D Varouchas, A Vartapetian, KE Varvell, GA Vasquez, JG Vasquez, F Vazeille, DV Furelos, TV Schroeder, J Veatch, V Vecchio, LM Veloce, F Veloso, S Veneziano, A Ventura, M Venturi, N Venturi, V Vercesi, M Verducci, CMV Infante, W Verkerke, AT Vermeulen, JC Vermeulen, MC Vetterli, NV Maira, O Viazlo, I Vichou, T Vickey, OEV Boeriu, GHA Viehhauser, S Viel, L Vigani, M Villa, MV 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, MV Milosavljevic, V Vrba, M Vreeswijk, T Sfiligoj, R Vuillermet, I Vukotic, T Zenis, L Zivkovic, P Wagner, W Wagner, J Wagner-Kuhr, H Wahlberg, S Wahrmund, K Wakamiya, VM Walbrecht, J Walder, R Walker, W Walkowiak, V Wallangen, AM Wang, C Wang, F Wang, H Wang, H Wang, J Wang, J Wang, P Wang, Q Wang, R-J Wang, R Wang, R Wang, SM Wang, WT Wang, W Wang, WX Wang, Y 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Search for heavy resonances decaying to a photon and a hadronically decaying Z/W/H boson in pp collisions at root s=13 TeV with the ATLAS detector

PHYSICAL REVIEW D 98 (2018) ARTN 032015

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, F Ahmadov, G Aielli, S Akatsuka, TPA Akesson, 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, 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, BA Gonzalez, D Alvarez 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, DJA Antrim, F Anulli, M Aoki, LA Bella, G Arabidze, Y Arai, JP Araque, V Araujo Ferraz, R Araujo Pereira, ATH Arce, RE Ardell, FA Arduh, J-F Arguin, S Argyropoulos, AJ Armbruster, LJ Armitage, O Arnaez, H Arnold, M Arratia, O Arslan, A Artamonov, G Artoni, S Artz, S Asai, N Asbah, A Ashkenazi, EM Asimakopoulou, L Asquith, K Assamagan, R Astalos, RJ Atkin, M Atkinson, NB Atlay, K Augsten, G Avolio, R Avramidou, B Axen, MK Ayoub, G Azuelos, AE Baas, MJ Baca, H Bachacou, K Bachas, M Backes, P Bagnaia, M Bahmani, H Bahrasemani, AJ Bailey, JT Baines, M Bajic, OK Baker, PJ Bakker, DB Gupta, EM Baldin, P Balek, F Balli, WK Balunas, E Banas, A Bandyopadhyay, S Banerjee, AAE Bannoura, L Barak, WM Barbe, EL Barberio, D Barberis, M Barbero, T Barillari, M-S Barisits, J Barkeloo, T Barklow, N Barlow, R Barnea, SL Barnes, BM Barnett, RM Barnett, Z Barnovska-Blenessy, A Baroncelli, G Barone, AJ Barr, L Barranco Navarro, F Barreiro, JBG da Costa, R Bartoldus, AE Barton, P Bartos, A Basalaev, A Bassalat, RL Bates, SJ Batista, S Batlamous, JR Batley, M Battaglia, M Bauce, F Bauer, KT Bauer, HS Bawa, JB Beacham, MD Beattie, T Beau, PH Beauchemin, P Bechtle, HC Beck, HP Beck, K Becker, M Becker, C Becot, A Beddall, AJ Beddall, VA Bednyakov, M Bedognetti, CP Bee, TA Beermann, M Begalli, M Begel, A Behera, JK Behr, AS Bell, G Bella, L Bellagamba, A Bellerive, M Bellomo, K Belotskiy, NL Belyaev, O Benary, D Benchekroun, M Bender, N Benekos, Y Benhammou, EB Noccioli, J Benitez, DP Benjamin, M Benoit, JR Bensinger, S Bentvelsen, L Beresford, M Beretta, D Berge, EB Kuutmann, N Berger, LJ Bergsten, J Beringer, S Berlendis, NR Bernard, G Bernardi, C Bernius, FU Bernlochner, T Berry, P Berta, C Bertella, G Bertoli, IA Bertram, C Bertsche, GJ Besjes, OB Bylund, M Bessner, N Besson, A Bethani, S Bethke, A Betti, AJ Bevan, J Beyer, RMB Bianchi, O Biebel, D Biedermann, R Bielski, K Bierwagen, NV Biesuz, M Biglietti, TRV Billoud, M Bindi, A Bingul, C Bini, S Biondi, T Bisanz, C Bittrich, DM Bjergaard, JE Black, KM Black, RE Blair, T Blazek, I Bloch, C Blocker, A Blue, U Blumenschein, D Blunier, GJ Bobbink, VS Bobrovnikov, SS Bocchetta, A Bocci, C Bock, D Boerner, D Bogavac, AG Bogdanchikov, C Bohm, V Boisvert, P Bokan, T Bold, AS Boldyrev, AE Bolz, M Bomben, M Bona, JS Bonilla, M Boonekamp, A Borisov, G Borissov, J Bortfeldt, D Bortoletto, V Bortolotto, D Boscherini, M Bosman, JD Bossio Sola, J Boudreau, EV Bouhova-Thacker, D Boumediene, C Bourdarios, SK Boutle, A Boveia, J Boyd, IR Boyko, AJ Bozson, J Bracinik, N Brahimi, A Brandt, G Brandt, O Brandt, F Braren, U Bratzler, B Brau, JE Brau, WDB Madden, K Brendlinger, AJ Brennan, L Brenner, R Brenner, S Bressler, B Brickwedde, DL Briglin, TM Bristow, D Britton, D Britzger, I Brock, R Brock, G Brooijmans, T Brooks, WK Brooks, E Brost, JH Broughton, PAB de Renstrom, D Bruncko, A Bruni, G Bruni, LS Bruni, S Bruno, BH Brunt, M Bruschi, N Bruscino, P Bryant, L Bryngemark, T Buanes, Q Buat, P Buchholz, AG Buckley, IA Budagov, F Buehrer, MK Bugge, O Bulekov, D 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Cavalli-Sforza, V Cavasinni, E Celebi, F Ceradini, L Cerda Alberich, AS Cerqueira, A Cerri, L Cerrito, F Cerutti, A Cervelli, SA Cetin, A Chafaq, D Chakraborty, SK Chan, WS Chan, YL Chan, P Chang, JD Chapman, DG Charlton, CC Chau, CAC Barajas, S Che, A Chegwidden, S Chekanov, SV Chekulaev, GA Chelkov, MA Chelstowska, C Chen, CH Chen, H Chen, J Chen, S Chen, SJ Chen, X Chen, Y Chen, Y-H Chen, HC Cheng, HJ Cheng, A Cheplakov, E Cheremushkina, RC El Moursli, E Cheu, K Cheung, L Chevalier, V Chiarella, G Chiarelli, G Chiodini, AS Chisholm, A Chitan, I Chiu, YH Chiu, MV Chizhov, K Choi, AR Chomont, S Chouridou, YS Chow, V Christodoulou, MC Chu, J Chudoba, AJ Chuinard, JJ Chwastowski, L Chytka, D Cinca, V Cindro, IA Cioara, A Ciocio, F Cirotto, ZH Citron, M Citterio, A Clark, MR Clark, PJ Clark, RN Clarke, C Clement, Y Coadou, M Cobal, A Coccaro, J Cochran, AEC Coimbra, L Colasurdo, B Cole, AP Colijn, J Collot, P Conde Muino, E Coniavitis, SH Connell, IA Connelly, S Constantinescu, F 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Dumitriu, AK Duncan, M Dunford, A Duperrin, HD Yildiz, M Dueren, A Durglishvili, D Duschinger, B Dutta, D Duvnjak, M Dyndal, BS Dziedzic, C Eckardt, KM Ecker, RC Edgar, T Eifert, G Eigen, K Einsweiler, T Ekelof, M El Kacimi, R El Kosseifi, V Ellajosyula, M Ellert, F Ellinghaus, AA Elliot, N Ellis, J Elmsheuser, M Elsing, D Emeliyanov, Y Enari, JS Ennis, MB Epland, J Erdmann, A Ereditato, S Errede, M Escalier, C Escobar, B Esposito, O Estrada Pastor, AI Etienvre, E Etzion, H Evans, A Ezhilov, M Ezzi, F Fabbri, L Fabbri, V Fabiani, G Facini, RM Faisca Rodrigues Pereira, RM Fakhrutdinov, S Falciano, PJ Falke, S Falke, J Faltova, Y Fang, M Fanti, A Farbin, A Farilla, EM Farina, T Farooque, S Farrell, SM Farrington, P Farthouat, F Fassi, P Fassnacht, D Fassouliotis, MF Giannelli, A Favareto, WJ Fawcett, L Fayard, OL Fedin, W Fedorko, M Feickert, S Feigl, L Feligioni, C Feng, EJ Feng, M Feng, MJ Fenton, AB Fenyuk, L Feremenga, J Ferrando, A Ferrari, P Ferrari, R Ferrari, DEF de Lima, A 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Gemme, MH Genest, C Geng, S Gentile, C Gentsos, S George, D Gerbaudo, G Gessner, S Ghasemi, M Ghneimat, B Giacobbe, S Giagu, N Giangiacomi, P Giannetti, SM Gibson, M Gignac, D Gillberg, G Gilles, DM Gingrich, MP Giordani, FM Giorgi, PF Giraud, P Giromini, G Giugliarelli, D Giugni, F Giuli, M Giulini, S Gkaitatzis, I Gkialas, EL Gkougkousis, P Gkountoumis, LK Gladilin, C Glasman, J Glatzer, PCF Glaysher, A Glazov, M Goblirsch-Kolb, J Godlewski, S Goldfarb, T Golling, D Golubkov, A Gomes, R Goncalves Gama, R Goncalo, G Gonella, L Gonella, A Gongadze, F Gonnella, JL Gonski, S Gonzalez de la Hoz, S Gonzalez-Sevilla, L Goossens, PA Gorbounov, HA Gordon, B Gorini, E Gorini, A Gorisek, AT Goshaw, C Goessling, MI Gostkin, CA Gottardo, CR Goudet, D Goujdami, AG Goussiou, N Govender, C Goy, E Gozani, I Grabowska-Bold, POJ Gradin, EC Graham, J Gramling, E Gramstad, S Grancagnolo, V Gratchev, PM Gravila, C Gray, HM Gray, ZD Greenwood, C Grefe, K Gregersen, IM Gregor, P Grenier, K Grevtsov, J Griffiths, AA Grillo, K Grimm, S Grinstein, P Gris, J-F Grivaz, S Groh, E Gross, J Grosse-Knetter, GC Grossi, ZJ Grout, A Grummer, L Guan, W Guan, J Guenther, A Guerguichon, F Guescini, D Guest, O Gueta, R Gugel, B Gui, T Guillemin, S Guindon, U Gul, C Gumpert, J Guo, W Guo, Y Guo, Z Guo, R Gupta, S Gurbuz, G Gustavino, BJ Gutelman, P Gutierrez, NGG Ortiz, C Gutschow, C Guyot, MP Guzik, C Gwenlan, CB Gwilliam, A Haas, C Haber, HK Hadavand, N Haddad, A Hadef, S Hageboeck, M Hagihara, H Hakobyan, M Haleem, J Haley, G Halladjian, GD Hallewell, K Hamacher, P Hamal, K Hamano, A Hamilton, GN Hamity, K Han, L Han, S Han, K Hanagaki, M Hance, DM Handl, B Haney, R Hankache, P Hanke, E Hansen, JB Hansen, JD Hansen, MC Hansen, PH Hansen, K Hara, AS Hard, T Harenberg, S Harkusha, PF Harrison, NM Hartmann, Y Hasegawa, A Hasib, S Hassani, S Haug, R Hauser, L Hauswald, LB Havener, M Havranek, CM Hawkes, RJ Hawkings, D Hayden, C Hayes, CP Hays, JM Hays, HS Hayward, SJ Haywood, MP Heath, V Hedberg, L 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Waugh, AF Webb, S Webb, C Weber, MS Weber, SA Weber, SM 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, HJ Yang, HT Yang, S Yang, Y Yang, Z Yang, W-M Yao, YC Yap, Y Yasu, E Yatsenko, KHY Wong, J Ye, S Ye, I Yeletskikh, E Yigitbasi, E Yildirim, K Yorita, K Yoshihara, CJS Young, C Young, 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, D Zerwas, M Zgubic, DF Zhang, D Zhang, F Zhang, G Zhang, H Zhang, J Zhang, L Zhang, M Zhang, P Zhang, R Zhang, X Zhang, Y Zhang, Z Zhang, X Zhao, Y Zhao, Z Zhao, A Zhemchugov, B Zhou, C Zhou, L Zhou, MS Zhou, M Zhou, N Zhou, Y Zhou, CG Zhu, HL 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, G Zobernig, A Zoccoli, K Zoch, TG Zorbas, R Zou, M Zur Nedden, L Zwalinski, ATLAS Collaboration


A measurement of the calorimeter response to single hadrons and determination of the jet energy scale uncertainty using LHC Run-1 pp-collision data with the ATLAS detector.

European Physical Journal C: Particles and Fields Springer Verlag 77 (2017) 26-

M Aaboud, G Aad, B Abbott, G Artoni, A Barr, AK Becker, LA Beresford, D Bortoletto, JTP Burr, AM Cooper-Sarkar, M Crispin Ortuzar, WJ Fawcett, JA Frost, EJ Gallas, F Giuli, S Gupta, C Gwenlan, CP Hays, J Henderson, BT Huffman, C Issever, CW Kalderon, K Nagai, RB Nickerson, N Norjoharuddeen

A measurement of the calorimeter response to isolated charged hadrons in the ATLAS detector at the LHC is presented. This measurement is performed with 3.2 nb[Formula: see text] of proton-proton collision data at [Formula: see text] [Formula: see text] from 2010 and 0.1 nb[Formula: see text] of data at [Formula: see text] [Formula: see text] from 2012. A number of aspects of the calorimeter response to isolated hadrons are explored. After accounting for energy deposited by neutral particles, there is a 5% discrepancy in the modelling, using various sets of Geant4 hadronic physics models, of the calorimeter response to isolated charged hadrons in the central calorimeter region. The description of the response to anti-protons at low momenta is found to be improved with respect to previous analyses. The electromagnetic and hadronic calorimeters are also examined separately, and the detector simulation is found to describe the response in the hadronic calorimeter well. The jet energy scale uncertainty and correlations in scale between jets of different momenta and pseudorapidity are derived based on these studies. The uncertainty is 2-5% for jets with transverse momenta above 2 [Formula: see text], where this method provides the jet energy scale uncertainty for ATLAS.


Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector

European Physical Journal C Springer 77 (2017) 580-

M Aaboud, G Aad, B Abbott, G Artoni, M Backes, AJ Barr, AK Becker, L Beresford, D Bortoletto, J Burr, AM Cooper-Sarkar, WJ Fawcett, JA Frost, EJ Gallas, JKK Liu, L Marchese, K Nagai, RB Nickerson, N Norjoharuddeen, M Petrov, MA Pickering, NC Ryder, IPJ Shipsey, JC-L Tseng

The rejection of forward jets originating from additional proton–proton interactions (pile-up) is crucial for a variety of physics analyses at the LHC, including Standard Model measurements and searches for physics beyond the Standard Model. The identification of such jets is challenging due to the lack of track and vertex information in the pseudorapidity range | η| &gt; 2.5. This paper presents a novel strategy for forward pile-up jet tagging that exploits jet shapes and topological jet correlations in pile-up interactions. Measurements of the per-jet tagging efficiency are presented using a data set of 3.2 fb - 1 of proton–proton collisions at a centre-of-mass energy of 13 TeV collected with the ATLAS detector. The fraction of pile-up jets rejected in the range 2.5 &lt; | η| &lt; 4.5 is estimated in simulated events with an average of 22 interactions per bunch-crossing. It increases with jet transverse momentum and, for jets with transverse momentum between 20 and 50 GeV, it ranges between 49% and 67% with an efficiency of 85% for selecting hard-scatter jets. A case study is performed in Higgs boson production via the vector-boson fusion process, showing that these techniques mitigate the background growth due to additional proton–proton interactions, thus enhancing the reach for such signatures.


Jet energy scale measurements and their systematic uncertainties in proton-proton collisions at root s=13 TeV with the ATLAS detector

PHYSICAL REVIEW D 96 (2017) ARTN 072002

M Aaboud, G Aad, B Abbott, J Abdallah, O Abdinov, B Abeloos, SH Abidi, OS AbouZeid, NL Abraham, H Abramowicz, H Abreu, R Abreu, Y Abulaiti, BS Acharya, S Adachi, L Adamczyk, J Adelman, M Adersberger, T Adye, AA Affolder, T Agatonovic-Jovin, C Agheorghiesei, JA Aguilar-Saavedra, SP Ahlen, F Ahmadov, G Aielli, S Akatsuka, H Akerstedt, TPA Akesson, AV Akimov, GL Alberghi, J Albert, P Albicocco, MJ Alconada Verzini, M Aleksa, IN Aleksandrov, C Alexa, G Alexander, T Alexopoulos, M Alhroob, B Ali, M Aliev, G Alimonti, J Alison, SP Alkire, BMM Allbrooke, BW Allen, PP Allport, A Aloisio, A Alonso, F Alonso, C Alpigiani, AA Alshehri, M Alstaty, BA Gonzalez, D Alvarez Piqueras, MG Alviggi, BT Amadio, Y Amaral Coutinho, C Amelung, D Amidei, SP Amor Dos Santos, A Amorim, S Amoroso, G Amundsen, 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, N Anjos, A Annovi, C Antel, M Antonelli, A 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Search for new phenomena in dijet events using 37 fb(-1) of pp collision data collected at root s=13 TeV with the ATLAS detector

PHYSICAL REVIEW D 96 (2017) ARTN 052004

M Aaboud, G Aad, B Abbott, J Abdallah, O Abdinov, B Abeloos, SH Abidi, OS AbouZeid, NL Abraham, H Abramowicz, H Abreu, R Abreu, Y Abulaiti, BS Acharya, S Adachi, L Adamczyk, J Adelman, M Adersberger, T Adye, AA Affolder, T Agatonovic-Jovin, C Agheorghiesei, JA Aguilar-Saavedra, SP Ahlen, F Ahmadov, G Aielli, S Akatsuka, H Akerstedt, TPA Akesson, AV Akimov, GL Alberghi, J Albert, P Albicocco, MJ Alconada Verzini, M Aleksa, IN Aleksandrov, C Alexa, G Alexander, T Alexopoulos, M Alhroob, B Ali, M Aliev, G Alimonti, J Alison, SP Alkire, BMM Allbrooke, BW Allen, PP Allport, A Aloisio, A Alonso, F Alonso, C Alpigiani, AA Alshehri, M Alstaty, BA Gonzalez, D Alvarez Piqueras, MG Alviggi, BT Amadio, YA Coutinho, C Amelung, D Amidei, SP Amor Dos Santos, A Amorim, S Amoroso, G Amundsen, 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, N Anjos, A Annovi, C Antel, M Antonelli, A Antonov, DJ 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Gregersen, IM Gregor, P Grenier, K Grevtsov, J Griffiths, AA Grillo, K Grimm, S Grinstein, P Gris, J-F Grivaz, S Groh, E Gross, J Grosse-Knetter, GC Grossi, ZJ Grout, A Grummer, L Guan, W Guan, J Guenther, F Guescini, D Guest, O Gueta, B Gui, E Guido, T Guillemin, S Guindon, U Gul, C Gumpert, J Guo, W Guo, Y Guo, R Gupta, S Gupta, G Gustavino, P Gutierrez, NGG Ortiz, C Gutschow, C Guyot, MP Guzik, C Gwenlan, CB Gwilliam, A Haas, C Haber, HK Hadavand, N Haddad, A Hadef, S Hageboeck, M Hagihara, H Hakobyan, M Haleem, J Haley, G Halladjian, GD Hallewell, K Hamacher, P Hamal, K Hamano, A Hamilton, GN Hamity, PG Hamnett, L Han, S Han, K Hanagaki, K Hanawa, M Hance, B Haney, R Hankache, P Hanke, JB Hansen, JD Hansen, MC Hansen, PH Hansen, K Hara, AS Hard, T Harenberg, F Hariri, S Harkusha, RD Harrington, PF Harrison, NM Hartmann, M Hasegawa, Y Hasegawa, A Hasib, S Hassani, S Haug, R Hauser, L Hauswald, LB Havener, M Havranek, CM Hawkes, RJ Hawkings, D Hayakawa, D Hayden, CP Hays, JM Hays, HS 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Topological cell clustering in the ATLAS calorimeters and its performance in LHC Run 1.

European Physical Journal. C, Particles and Fields Springer 77 (2017) 490-

G Aad, B Abbott, J Abdallah, AJ Barr, AK Becker, L Beresford, AM Cooper-Sarkar, JA Frost, EJ Gallas, C Gwenlan, CP Hays, BT Huffman, C Issever, K Nagai, RB Nickerson, MA Pickering, NC Ryder, JC-L Tseng, GHA Viehhauser, AR Weidberg

The reconstruction of the signal from hadrons and jets emerging from the proton–proton collisions at the Large Hadron Collider (LHC) and entering the ATLAS calorimeters is based on a three-dimensional topological clustering of individual calorimeter cell signals. The cluster formation follows cell signal-significance patterns generated by electromagnetic and hadronic showers. In this, the clustering algorithm implicitly performs a topological noise suppression by removing cells with insignificant signals which are not in close proximity to cells with significant signals. The resulting topological cell clusters have shape and location information, which is exploited to apply a local energy calibration and corrections depending on the nature of the cluster. Topological cell clustering is established as a wellperforming calorimeter signal definition for jet and missing transverse momentum reconstruction in ATLAS.


Performance of algorithms that reconstruct missing transverse momentum in √s = 8 TeV proton–proton collisions in the ATLAS detector

European Physical Journal C Spinger Verlag 77 (2017) 1-46

G Aad, B Abbott, J Abdallah, G Artoni, AJ Barr, K Becker, JK Behr, L Beresford, AM Cooper-Sarkar, M Crispin Ortuzar, A Dafinca, E Davis, JA Frost, EJ Gallas, S Gupta, C Gwenlan, D Hall, CP Hays, J Henderson, J Howard, TB Huffman, C Issever, NC Ryder, GHA Viehjauser, J Zhong

The reconstruction and calibration algorithms used to calculate missing transverse momentum ([Formula: see text] ) with the ATLAS detector exploit energy deposits in the calorimeter and tracks reconstructed in the inner detector as well as the muon spectrometer. Various strategies are used to suppress effects arising from additional proton-proton interactions, called pileup, concurrent with the hard-scatter processes. Tracking information is used to distinguish contributions from the pileup interactions using their vertex separation along the beam axis. The performance of the [Formula: see text] reconstruction algorithms, especially with respect to the amount of pileup, is evaluated using data collected in proton-proton collisions at a centre-of-mass energy of 8 [Formula: see text] during 2012, and results are shown for a data sample corresponding to an integrated luminosity of [Formula: see text]. The simulation and modelling of [Formula: see text]  in events containing a Z boson decaying to two charged leptons (electrons or muons) or a W boson decaying to a charged lepton and a neutrino are compared to data. The acceptance for different event topologies, with and without high transverse momentum neutrinos, is shown for a range of threshold criteria for [Formula: see text] , and estimates of the systematic uncertainties in the [Formula: see text]  measurements are presented.


Boosting Higgs pair production in the bbbb final state with multivariate techniques

European Physical Journal C Springer Verlag 76 (2016)

J Rojo, JK Behr, D Bortoletto, JA Frost, NP Hartland, C Issever, J Rojo

The measurement of Higgs pair production will be a cornerstone of the LHC program in the coming years. Double Higgs production provides a crucial window upon the mechanism of electroweak symmetry breaking and has a unique sensitivity to the Higgs trilinear coupling. We study the feasibility of a measurement of Higgs pair production in the b ¯bb¯b final state at the LHC. Our analysis is based on a combination of traditional cut-based methods with state-of-the-art multivariate techniques. We account for all relevant backgrounds, including the contributions from light and charm jet mis-identification, which are ultimately comparable in size to the irreducible 4b QCD background. We demonstrate the robustness of our analysis strategy in a high pileup environment. For an integrated luminosity of L = 3 ab−1 , a signal significance of S/√ B ' 3 is obtained, indicating that the b ¯bb¯b final state alone could allow for the observation of double Higgs production at the High Luminosity LHC.


Identification of high transverse momentum top quarks in pp collisions at √s = 8 TeV with the ATLAS detector

Journal of High Energy Physics Springer 2016 (2016)

AJ Barr, AK Becker, LA Beresford, AM Cooper-Sarkar, JA Frost, EJ Gallas, C Gwenlan, CP Hays, BT Huffman, C Issever, CW Kalderon, K Nagai, RB Nickerson, MA Pickering, NC Ryder, JC-L Tseng, GHA Viehhauser, AR Weidberg

This paper presents studies of the performance of several jet-substructure techniques, which are used to identify hadronically decaying top quarks with high transverse momentum contained in large-radius jets. The efficiency of identifying top quarks is measured using a sample of top-quark pairs and the rate of wrongly identifying jets from other quarks or gluons as top quarks is measured using multijet events collected with the ATLAS experiment in 20.3 fb^−1 of 8 TeV proton-proton collisions at the Large Hadron Collider. Predictions from Monte Carlo simulations are found to provide an accurate description of the performance. The techniques are compared in terms of signal efficiency and background rejection using simulations, covering a larger range in jet transverse momenta than accessible in the dataset. Additionally, a novel technique is developed that is optimized to reconstruct top quarks in events with many jets.


A new method to distinguish hadronically decaying boosted Z bosons from W bosons using the ATLAS detector

European Physical Journal C Springer Verlag 76 (2016)

AJ Barr, K Becker, JK Behr, L Beresford, AM Cooper-Sarkar, MC Ortuzar, A Dafinca, E Davies, JA Frost, EJ Gallas, S Gupta, C Gwenlan, D Hall, CP Hays, J Henderson, J Howard, TB Huffman, C Issever, CW Kalderon, LA Kogan, A Lewis, K Nagai, RB Nickerson, MA Pickering

The distribution of particles inside hadronic jets produced in the decay of boosted W and Z bosons can be used to discriminate such jets from the continuum background. Given that a jet has been identified as likely resulting from the hadronic decay of a boosted W or Z boson, this paper presents a technique for further differentiating Z bosons from W bosons. The variables used are jet mass, jet charge, and a b-tagging discriminant. A likelihood tagger is constructed from these variables and tested in the simulation of W′→ WZ for bosons in the transverse momentum range 200 GeV &lt; pT&lt; 400 GeV in s= 8 TeV pp collisions with the ATLAS detector at the LHC. For Z-boson tagging efficiencies of ϵZ= 90 , 50, and 10 % , one can achieve W+-boson tagging rejection factors (1 / ϵW+ ) of 1.7, 8.3 and 1000, respectively. It is not possible to measure these efficiencies in the data due to the lack of a pure sample of high pT, hadronically decaying Z bosons. However, the modelling of the tagger inputs for boosted W bosons is studied in data using a tt¯ -enriched sample of events in 20.3 fb- 1 of data at s= 8 TeV. The inputs are well modelled within uncertainties, which builds confidence in the expected tagger performance.


Performance of pile-up mitigation techniques for jets in pp collisions at √s = 8 TeV using the ATLAS detector

European Physical Journal C: Particles and Fields Springer 76 (2016) 581

AJ Beddall, A Beddall, VA Bednyakov, CP Bee, LJ Beemster, TA Beermann, M Begel, JK Behr, C Belanger-Champagne, WH Bell, G Bella, L Bellagamba, A Bellerive, M Bellomo, K Belotskiy, O Beltramello, O Benary, D Benchekroun, M Bender, S Bentvelsen, M Beretta, D Berge, N Berger, FU Bernlochner, T Berry

The large rate of multiple simultaneous proton–proton interactions, or pile-up, generated by the Large Hadron Collider in Run 1 required the development of many new techniques to mitigate the adverse effects of these conditions. This paper describes the methods employed in the ATLAS experiment to correct for the impact of pile-up on jet energy and jet shapes, and for the presence of spurious additional jets, with a primary focus on the large 20.3 fb−1 data sample collected at a centre-of-mass energy of s√=8 TeV . The energy correction techniques that incorporate sophisticated estimates of the average pile-up energy density and tracking information are presented. Jet-to-vertex association techniques are discussed and projections of performance for the future are considered. Lastly, the extension of these techniques to mitigate the effect of pile-up on jet shapes using subtraction and grooming procedures is presented.


Search for pair production of Higgs bosons in the bb¯bb¯ final state using proton-proton collisions at sqrt(s)=13  TeV with the ATLAS detector

Physical Review D American Physical Society 94 (2016) 1-29

C Issever, AJ Barr, K Becker, L Beresford, D Bortoletto, AM Cooper-Sarkar, M Crispin Ortuzar, WJ Fawcett, JA Frost, EJ Gallas, F Guili, S Gupta, C Gwenlan, CP Hays, J Henderson, TB Huffman, RB Nickerson, N Norjaharuddeen, M Petrov, MA Pickering, JC-L Tseng, GHA Viehhauser, L Vigani, AR Weidberg, J Zhong

A search for Higgs-boson pair production in the bb¯bb¯ final state is carried out with 3.2  fb−1 of proton-proton collision data collected at s√=13  TeV with the ATLAS detector. The data are consistent with the estimated background and are used to set upper limits on the production cross section of Higgs-boson pairs times branching ratio to bb¯bb¯ for both nonresonant and resonant production. In the case of resonant production of Kaluza-Klein gravitons within the Randall-Sundrum model, upper limits in the 24 to 91 fb range are obtained for masses between 600 and 3000 GeV, at the 95% confidence level. The production cross section times branching ratio for nonresonant Higgs-boson pairs is also constrained to be less than 1.22 pb, at the 95% confidence level.


Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at √s=13 TeV

Physics Letters B Elsevier 760 (2016) 520-537

M Aaboud, G Aad, B Abbott, G Artoni, A Barr, AK Becker, LA Beresford, D Bortoletto, JTP Burr, AM Cooper-Sarkar, M Crispin Ortuzar, WJ Fawcett, JA Frost, EJ Gallas, F Giuli, S Gupta, C Gwenlan, CP Hays, J Henderson, BT Huffman, C Issever, CW Kalderon, K Nagai, RB Nickerson

A search for physics beyond the Standard Model, in final states with at least one high transverse momentum charged lepton (electron or muon) and two additional high transverse momentum leptons or jets, is performed using 3.2 fb−1 of proton–proton collision data recorded by the ATLAS detector at the Large Hadron Collider in 2015 at √s=13 TeV source. The upper end of the distribution of the scalar sum of the transverse momenta of leptons and jets is sensitive to the production of high-mass objects. No excess of events beyond Standard Model predictions is observed. Exclusion limits are set for models of microscopic black holes with two to six extra dimensions.

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