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Abe, F.; Albrow, M.; Amendolia, S. R.; Amidei, D.; Antos̆, J.; Anway-Wiese, C.; Apollinari, G.; Areti, H.; Ataç, M.; Auchincloss, P.; Azfar, F.; Azzi, P.; Bacchetta, N.; Badgett, W.; Bailey, M. W.; Bao, J.; Barbaro, P. de; Barbaro-Galtieri, A.; Barnes, V. E.; Barnett, B. A.; Bartalini, P.; Bauer, G.; Baumann, Thomas; Bedeschi, F.; Behrends, S.; Belforte, S.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Benlloch, J.; Bensinger, J. R.; Benton, D.; Beretvas, A.; Berge, J. P.; Bertolucci, S.; Bhatti, A.; Biery, K.; Binkley, M.; Bird, F.; Bisello, D.; Blair, R. E.; Blocker, C.; Bodek, A.; Bokhari, W.; Bolognesi, V.; Bortoletto, D.; Boswell, C.; Boulos, T.; Brandenburg, G.; Bromberg, C.; Buckley-Geer, E.; Budd, H. S.; Burkett, K.; Busetto, G.; Byon-Wagner, A.; Byrum, K. L.; Cammerata, J.; Campagnari, C.; Campbell, M.; Caner, A.; Carithers, W.; Carlsmith, D.; Castro, A.; Cen, Y.; Cervelli, F.; Chao, H. Y.; Chapman, J.; Cheng, M. T.; Chiarelli, G.; Chikamatsu, T.; Chiou, C. N.; Cihangir, S.; Clark, A.; Cobal, M.; Contreras, M.; Conway, J.; Cooper, J.; Cordelli, M.; Couyoumtzelis, C.; Crane, D.; Cunningham, J. D.; Daniels, T.; DeJongh, F.; Delchamps, S.; Dell’Agnello, S.; Dell’Orso, M.; Demortier, L.; Denby, B.; Deninno, M.; Derwent, P. F.; Devlin, T.; Dickson, M.; Dittmann, J.; Donati, S.; Drucker, R. B.; Dunn, A.; Einsweiler, K.; Elias, J. E.; Ely, R.; Engels, E.; Eno, S. C.; Errede, D.; Errede, S.; Fan, Q.; Farhat, B.; Fiori, I.; Flaugher, B.; Foster, G. W.; Franklin, M.; Frautschi, M.; Freeman, J.; Friedman, J.; Frisch, H.; Fry, A.; Fuess, T. A.; Fukui, Y.; Funaki, S.; Gagliardi, G.; Galeotti, S.; Gallinaro, M.; Garfinkel, A. F.; Geer, S.; Gerdes, D. W.; Giannetti, P.; Giokaris, N.; Giromini, P.; Gladney, L.; Glenzinski, D.; Gold, M.; Gonzalez, J. Suarez; Gordon, A.; Goshaw, A. T.; Goulianos, K.; Grassmann, H.; Grewal, A.; Grieco, G.; Groer, L.; Grosso-Pilcher, C.; Haber, C.; Hahn, S. R.; Hamilton, R.; Handler, R.; Hans, R. M.; Hara, K.; Harral, B.; Harris, R. M.; Hauger, S. A.; Hauser, J.; Hawk, C.; Heinrich, J.; Cronin-Hennessy, D.; Hollebeek, R.; Holloway, L.; Hölscher, A.; Hong, S. J.; Houk, G.; Hu, P.; Huffman, B. T.; Hughes, R.; Hurst, P.; Huston, J.; Huth, J.; Hylen, J.; Incagli, M.; Incandela, J.; Iso, H.; Jensen, H.; Jessop, C.; Joshi, U.; Kadel, R. W.; Kajfasz, E.; Kamon, T.; Kaneko, T.; Kardelis, D. A.; Kasha, H.; Kato, Y.; Keeble, L.; Kennedy, R. D.; Kephart, R.; Kesten, P.; Kestenbaum, D.; Keup, R. M.; Keutelian, H.; Keyvan, F.; Kim, D. H.; Kim, H. S.; Kim, S. B.; Kim, S. H.; Kim, Y. K.; Kirsch, L.; Koehn, P.; Kondo, K.; Königsberg, J.; Köpp, S.; Kordas, K.; Koska, W.; Kovacs, E.; Kowald, W.; Krasberg, M.; Kroll, J.; Kruse, M.; Kuhlmann, S. E.; Kuns, E.; Laasanen, A. T.; Labanca, N.; Lammel, S.; Lamoureux, J. I.; LeCompte, T.; Leone, S.; Lewis, J. D.; Limon, P.; Lindgren, M.; Liss, T. M.; Lockyer, N. S.; Loomis, C.; Long, O. R.; Loreti, M.; Low, E. H.; Lu, J.; Lucchesi, D.; Luchini, C. B.; Lukens, P.; Maas, P.; Maeshima, K.; Maghakian, A.; Maksimović, P.; Mangano, M.; Mansour, J.; Mariotti, M.; Marriner, J. P.; Martin, A.; Matthews, J.; Mattingly, R.; McIntyre, P.; Mélèse, P.; Menzione, A.; Meschi, E.; Michail, G.; Mikamo, S.; Miller, Michael L.; Miller, R.; Mimashi, T.; Miscetti, S.; Mishina, M.; Mitsushio, H.; Miyashita, S.; Morita, Y.; Moulding, S.; Muêller, J.; Mukherjee, A.; Müller, Th.; Musgrave, P. W.; Nakae, L. F.; Nakano, I.; Nelson, Charles A.; Neuberger, D.; Newman-Holmes, C.; Nodulman, L.; Ogawa, S.; Oh, S. H.; Ohl, K. E.; Oishi, R.; Okusawa, T.; Pagliarone, C.; Paoletti, R.; Papadimitriou, V.; Park, S.; Patrick, J.; Pauletta, G.; Paulini, M.; Pescara, L.; Peters, Michael; Phillips, T. J.; Piacentino, G.; Pillai, M.; Plunkett, R.; Pondrom, L.; Produit, N.; Proudfoot, J.; Ptohos, F.; Punzi, G.; Ragan, K.; Rimondi, F.; Ristori, L.; Roach-Bellino, M.; Robertson, W. J.; Rodrigo, T.; Romano, J.; Rosenson, L.; Sakumoto, W. K.; Saltzberg, D.; Sansoni, A.; Scarpine, V.; Schindler, Andrea; Schlabach, P.; Schmidt, E. E.; Schmidt, M. P.; Schneider, O.; Sciacca, G.; Scribano, A.; Segler, S.; Seidel, S. C.; Seiya, Y.; Sganos, G.; Sgolacchia, A.; Shapiro, M.; Shaw, N. M.; Shen, Qing; Shepard, P. F.; Shimojima, M.; Shochet, M.; Siegrist, J.; Sill, A.; Sinervo, P.; Singh, P.; Skarha, J.; Sliwa, K.; Smith, D.; Snider, F. D.; Song, L.; Song, T.; Spalding, J.; Spiegel, L.; Sphicas, P.; Spies, A.; Stančo, L.; Steele, J.; Stefanini, A.; Strahl, K.; Strait, J.; Stuart, D.; Sullivan, G. W.; Sumorok, K.; Swartz, R. L.; Takahashi, T.; Takikawa, K.; Tartarelli, G. F.; Taylor, W.; Teng, P. K.; Teramoto, Y.; Tether, S.; Theriot, D.; Thomas, J. P.; Thomas, T. L.; Thun, R. P.; Timko, M.; Tipton, P.; Titov, A.; Tkaczyk, S.; Tollefson, K.; Tollestrup, A.; Tonnison, J.; Trocóniz, Jorge F de; Tseng, J.; Turcotte, M.; Turini, N.; Uemura, N.; Ukegawa, F.; Unal, G.; Brink, S. van den; Vejcik, S.; Vidal, R.; Vondráček, M.; Wagner, R. G.; Wagner, R. L.; Wainer, N.; Walker, R.; Wang, C. H.; Wang, G.; Wang, J.; Wang, M. J.; Wang, Q. F.; Warburton, A.; Watts, G.; Watts, T.; Webb, R.; Wendt, C.; Wenzel, H.; Wester, W. C.; Westhusing, T.; Wicklund, A. B.; Wicklund, E.; Wilkinson, R.; Williams, H. H.; Wilson, P.; Winer, B. L.; Wolinski, J.; Wu, D. Y.; Wu, X.; Wyss, J.; Yagil, A.; Yao, W-M.; Yasuoka, K.; Ye, Y.; Yeh, G. P.; Yeh, P.; Yin, M.; Yoh, J.; Yoshida, T.; Yovanovitch, D.; Yu, I.; Yun, J. C.; Zanetti, A.; Zetti, F.; Zhang, L.; Zhang, S.; Zhang, W.; Zucchelli, S.

doi:10.1103/physrevlett.74.3538

Cited by 76 publications

(54 citation statements)

References 22 publications

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“…As shown in Figure 3, this improves on the recent DØ limit based on the dijet angular distribution [9]. Note that the region at cot θ ≈ 1 where our limit appears to provide a direct lower bound on M c has already been excluded by CDF's search for new particles decaying to dijets [16]. This is fortunate, because our limit actually becomes less reliable here: the condition M c > √ŝ , under which (2.4) is a reasonable approximation to coloron exchange, would no longer hold for the highest-energy data point.…”

Section: Discussionsupporting

confidence: 75%

Dijet mass spectrum limits on flavor-universal colorons

Bertram

Simmons

1998

Physics Letters B

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Using recent DØ data on the dijet mass spectrum, we present a limit on flavor-universal colorons. At 95% CL we find M c / cot θ > 837 GeV. We discuss the implications of this limit for models of quark compositeness, nonstandard gluon interactions, and dynamical electroweak symmetry breaking. In addition, we place a lower bound Λ A8 > 2.1 TeV on the scale of color-octet axial-vector contact interactions among quarks which could arise in models of

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Section: Discussionsupporting

confidence: 75%

Dijet mass spectrum limits on flavor-universal colorons

Bertram

Simmons

1998

Physics Letters B

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“…Several experiments have examined m jj distributions in search of new resonances [12][13][14][15][16][17]; recently, 1:13 fb À1 of p " p collision data at the Fermilab Tevatron collider have excluded the existence of excited quarks q Ã with mass 260 < m q Ã < 870 GeV [16]. This Letter reports the first search by the ATLAS experiment [18] at the LHC for such massive particles in pp collisions at a center-of-mass energy of ffiffi ffi s p ¼ 7 TeV, based on a data sample corresponding to an integrated luminosity of 315 nb À1 .…”

mentioning

confidence: 99%

Search for New Particles in Two-Jet Final States in 7 TeV Proton-Proton Collisions with the ATLAS Detector at the LHC

Aad¹,

Abbott²,

Abdallah³

et al. 2010

Phys. Rev. Lett.

Self Cite

118

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A search for new heavy particles manifested as resonances in two-jet final states is presented. The data were produced in 7 TeV proton-proton collisions by the LHC and correspond to an integrated luminosity of 315 nb⁻¹ collected by the ATLAS detector. No resonances were observed. Upper limits were set on the product of cross section and signal acceptance for excited-quark (q*) production as a function of q* mass. These exclude at the 95% C.L. the q* mass interval 0.30

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“…For FNAL δ = 25 Gev corresponds to ≈ 10 percent dijet mass determination for M dijet ≤ 225 Gev We have generated one million QCD events for each value of P T 0 and R to find 4-jet QCD background satisfying mass cuts (11,12) both for LHC and FNAL. As for FNAL typical accuracy in the determination of dijet invariant mass is 10 percent [1].…”

Section: Qcd Background Estimatesmentioning

confidence: 99%

“…In ref. [1] experimental bounds on new particles decaying to dijets have been obtained. However there are examples of new particles (scalar colour octets, squarks in model with R-parity violation etc.)…”

Section: Introductionmentioning

confidence: 99%

The Search for New Physics by the Measurement of the Four-Jet Cross-Section at LHC and Tevatron

Bityukov

Krasnikov

1997

Mod. Phys. Lett. A

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We investigate the possibility to look for new physics by the measurement of the 4-jet cross section at LHC and FNAL. In particular, we consider the model with scalar colour octet and the supersymmetric model with R-parity violation. In both models pair produced new particles decay into 2 jets thus leading to 4-jet events.Therefore, the measurement of the distributions of 4-jet differential cross section on on the invariant dijet masses allows to look for new physics. The main background comes from standard QCD 4-jet events. We find that at LHC it would be possible to discover scalar colour octet particles with a mass ≤ 900 Gev and for FNAL the corresponding bound is 175 Gev.

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Search for New Particles Decaying to Dijets inpp¯Collisions at√s=

Cited by 76 publications

References 22 publications

Dijet mass spectrum limits on flavor-universal colorons

Dijet mass spectrum limits on flavor-universal colorons

Search for New Particles in Two-Jet Final States in 7 TeV Proton-Proton Collisions with the ATLAS Detector at the LHC

The Search for New Physics by the Measurement of the Four-Jet Cross-Section at LHC and Tevatron

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