5,547 research outputs found
First observations of separated atmospheric nu_mu and bar{nu-mu} events in the MINOS detector
- Author
- Adamson P
- Alexopoulos T
- Allison WWM
- Alner GJ
- Anderson K
- Andreopoulos C
- Andrews M
- Andrews R
- Arroyo C
- Avvakumov S
- Ayres DS
- Baller B
- Barish B
- Barker MA
- Barnes PD
- Barr G
- Barrett WL
- Beall E
- Becker BR
- Belias A
- Bergfeld T
- Bernstein RH
- Bhattacharya D
- Bishai M
- Blake A
- Bocean V
- Bock B
- Bock GJ
- Boehm J
- Boehnlein DJ
- Bogert D
- Border PM
- Bower C
- Boyd S
- Buckley-Geer E
- Byon-Wagner A
- Cabrera A
- Chapman JD
- Chase TR
- Chernichenko SK
- Childress S
- Choudhary BC
- Cobb JH
- Collaboration MMINOS
- Cossairt JD
- Courant H
- Crane DA
- Culling AJ
- Dawson JW
- De Santo A
- DeMuth DM
- Dierckxsens M
- Diwan MV
- Dorman M
- Drake G
- Ducar R
- Durkin T
- Erwin AR
- Escobar CO
- Evans J
- Fackler OD
- Feldman GJ
- Felt N
- Fields TH
- Ford R
- Frohne MV
- Gallagher HR
- Gebhard M
- Godley A
- Gogos J
- Goodman MC
- Gornushkin Y
- Gouffon P
- Grashorn E
- Grossman N
- Grudzinski JJ
- Grzelak K
- Guarino V
- Habig A
- Halsall R
- Hanson J
- Harris D
- Harris EF
- Harris PG
- Hartnell J
- Hartouni EP
- Hatcher R
- Heller K
- Hill N
- Ho Y
- Howcroft C
- Hylen J
- Ignatenko M
- Indurthy D
- Irwin GM
- James C
- Jenner L
- Jensen D
- Joffe-Minor T
- Kafka T
- Kang HJ
- Kasahara SMS
- Kilmer J
- Kim H
- Koizumi G
- Kopp S
- Kordosky M
- Koskinen DJ
- Kostin M
- Krakauer DA
- Kumaratunga S
- Ladran AS
- Lang K
- Laughton C
- Lebedev A
- Lee R
- Lee WY
- Libkind MA
- Litchfield PJ
- Litchfield RP
- Liu J
- Longley NP
- Lucas P
- Luebke W
- Madani S
- Maher E
- Makeev V
- Mann WA
- Marchionni A
- Marino AD
- Marshak ML
- Marshall JS
- McDonald J
- McGowan A
- Meier JR
- Merzon GI
- Messier MD
- Michael DG
- Milburn RH
- Miller JL
- Miller WH
- Mishra SR
- Miyagawa PS
- Moore C
- Morfin J
- Morse R
- Mualem L
- Mufson S
- Murgia S
- Murtagh MJ
- Musser J
- Naples D
- Nelson C
- Nelson JK
- Newman HB
- Nezrick F
- Nichol RJ
- Nicholls TC
- Ochoa-Ricoux JP
- Oliver J
- Oliver WP
- Onuchin VA
- Osiecki T
- Ospanov R
- Paley J
- Paolone V
- Para A
- Patzak T
- Pavlovich Z
- Pearce GF
- Pearson N
- Peck CW
- Perry C
- Peterson EA
- Petyt DA
- Ping H
- Piteira R
- Pla-Dalmau A
- Plunkett RK
- Price LE
- Proga M
- Pushka DR
- Rahman D
- Rameika RA
- Raufer TM
- Read AL
- Rebel B
- Reyna DE
- Rosenfeld C
- Rubin HA
- Ruddick K
- Ryabov VA
- Saakyan R
- Sanchez MC
- Saoulidou N
- Schneps J
- Schoessow PV
- Schreiner P
- Schwienhorst R
- Semenov VK
- Seun SM
- Shanahan P
- Shield PD
- Smart W
- Smirnitsky V
- Smith C
- Smith PN
- Sousa A
- Speakman B
- Stamoulis P
- Stefanik A
- Sullivan P
- Swan JM
- Symes PA
- Tagg N
- Talaga RL
- Tetteh-Lartey E
- Thomas J
- Thompson J
- Thomson MA
- Thron JL
- Trendler R
- Trevor J
- Trostin I
- Tsarev VA
- Tzanakos G
- Urheim J
- Vahle P
- Vakili M
- Vaziri K
- Velissaris C
- Verebryusov V
- Viren B
- Wai L
- Ward CP
- Ward DR
- Watabe M
- Webb RC
- Weber A
- Wehmann A
- West N
- White C
- White RF
- Wojcicki SG
- Wright DM
- Wu QK
- Yan WG
- Yang T
- Yumiceva FX
- Yun JC
- Zheng H
- Zois M
- Zwaska R
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2005
- Field of study
The complete 5.4 kton MINOS far detector has been taking data since the beginning of August 2003 at a depth of 2070 meters water-equivalent in the Soudan mine, Minnesota. This paper presents the first MINOS observations of nuÂľ and [overline nu ]Âľ charged-current atmospheric neutrino interactions based on an exposure of 418 days. The ratio of upward- to downward-going events in the data is compared to the Monte Carlo expectation in the absence of neutrino oscillations, giving Rup/downdata/Rup/downMC=0.62-0.14+0.19(stat.)Âą0.02(sys.). An extended maximum likelihood analysis of the observed L/E distributions excludes the null hypothesis of no neutrino oscillations at the 98% confidence level. Using the curvature of the observed muons in the 1.3 T MINOS magnetic field nuÂľ and [overline nu ]Âľ interactions are separated. The ratio of [overline nu ]Âľ to nuÂľ events in the data is compared to the Monte Carlo expectation assuming neutrinos and antineutrinos oscillate in the same manner, giving R[overline nu ][sub mu]/nu[sub mu]data/R[overline nu ][sub mu]/nu[sub mu]MC=0.96-0.27+0.38(stat.)Âą0.15(sys.), where the errors are the statistical and systematic uncertainties. Although the statistics are limited, this is the first direct observation of atmospheric neutrino interactions separately for nuÂľ and [overline nu ]Âľ
Search for Nucleon Decay with Final States l+ eta, nubar eta, and nubar pi+,0 Using Soudan 2
- Author
- Allison WWM
- Alner GJ
- Ayres DS
- Barrett WL
- Bode C
- Border PM
- Chung J
- Cobb JH
- Cotton R
- Courant H
- Demuth DM
- Fields TH
- Gallagher HR
- Goodman MC
- Gran R
- Joffe-Minor T
- Kafka T
- Kasahara SMS
- Leeson W
- Litchfield PJ
- Mann WA
- Marshak ML
- Milburn RH
- Miller WH
- Mualem L
- Napier A
- Oliver WP
- Pearce GF
- Peterson EA
- Petyt DA
- Price LE
- Ruddick K
- Sanchez M
- Schneps J
- Stassinakis A
- Thron JL
- Wakely SP
- Wall D
- West N
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2000
- Field of study
We have searched for nucleon decay into five two-body final states using a
4.4 kiloton-year fiducial exposure of the Soudan 2 iron tracking calorimeter.
For proton decay into the fully visible final states mu+ eta and e+ eta, we
observe zero and one event, respectively, that satisfy our search criteria for
nucleon decay. The lifetime lower limits (tau/B) thus implied are 89 x 10^30
years and 81 x 10^30 years at 90% confidence level. For neutron decay into
nubar eta, we obtain the lifetime lower limit 71 x 10^30 years. Limits are also
reported for neutron decay into nubar pi0, and for proton decay into nubar pi+.Comment: 24 pages, 9 figures, 3 table
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
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- Bauerdick LAT
- Baumgartel D
- Baur U
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- Bazterra VE
- Bean A
- Beauceron S
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- Xiao H
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
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- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
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- Zumerle G
- Zuranski A
- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Constraints on the Ď_(c1) versus Ď_(c2) polarizations in proton-proton collisions at âs = 8 TeV
- Author
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- Zorbilmez C.
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- Zuo X.
- Zuolo D.
- Ălvarez FernĂĄndez A.
- Ăzçelik Ă.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 24/04/2020
- Field of study
The polarizations of promptly produced Ď_(c1) and Ď_(c2) mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at âs=8ââTeV. The Ď_c states are reconstructed via their radiative decays Ď_c â J/ĎÎł, with the photons being measured through conversions to eâşeâť, which allows the two states to be well resolved. The polarizations are measured in the helicity frame, through the analysis of the Ď_(c2) to Ď_(c1) yield ratio as a function of the polar or azimuthal angle of the positive muon emitted in the J/Ď â ÎźâşÎźâť decay, in three bins of J/Ď transverse momentum. While no differences are seen between the two states in terms of azimuthal decay angle distributions, they are observed to have significantly different polar anisotropies. The measurement favors a scenario where at least one of the two states is strongly polarized along the helicity quantization axis, in agreement with nonrelativistic quantum chromodynamics predictions. This is the first measurement of significantly polarized quarkonia produced at high transverse momentum
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
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- Thom J
- Thomas L
- Thomas S
- Thompson J
- Thomsen J
- Thyssen F
- Tiko A
- Timciuc V
- Tinti G
- Tiras E
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tomalin IR
- Tomaszewska J
- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topaksu AK
- Torassa E
- Toropin A
- Torre P
- Tosi M
- Tosi S
- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Triantis FA
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tupputi S
- Turkewitz J
- Turner M
- Tuuva T
- Tuve C
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
- Valdata M
- Valls N
- Valuev V
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Remortel N
- Van Spilbeeck A
- Vander Velde C
- Vanelderen L
- Vanini S
- Vanlaer P
- Varela J
- Varelas N
- Vargas JER
- Vartak A
- Vasil'ev S
- Vaughan J
- Vavilov S
- Vazquez Valencia F
- Veelken C
- Veeraraghavan V
- Velasco M
- Velicanu D
- Velkovska J
- Ventura S
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili LN
- Vergili M
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vichoudis P
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Vischia P
- Vishnevskiy D
- Vitulo P
- Viviani C
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volpe R
- Vorobiev I
- Vorobyev A
- Vorobyev A
- Voutilainen M
- Vuosalo C
- Vutova M
- Wagner P
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh R
- Walsh S
- Waltenberger W
- Walzel G
- Wan Z
- Wang D
- Wang J
- Wang J
- Wang M
- Wang S
- Wang X
- Wang Z
- Wardle N
- Wardrope D
- Wasserbaech S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
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