627 research outputs found
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
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- Alagoz E
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- Albayrak EA
- Albergo S
- Albrow M
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- Alexander J
- Aliev T
- Almeida N
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- Alverson G
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- Anastassov A
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- Wissing C
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- Wood J
- Wood JS
- Worm SD
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- 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
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
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- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
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- 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
- Barbone L
- Bardak C
- Barfuss AF
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- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
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- Xiao H
- Xie S
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- Yang M
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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
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- 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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
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- Ahmad M
- Ahmad WH
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- Ahuja S
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- Akin IV
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- Albayrak EA
- Albergo S
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- Anagnostou G
- Anastassov A
- Anderson J
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- Andrea J
- Andreev V
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- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunes JR
- Antunovic Z
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- Apollinari G
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- Baarmand MM
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- Bauerdick LAT
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- Bedoya CF
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
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- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
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- Akgun B
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- Civinini C
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- CMS Collaboration
- Coarasa Perez JA
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- Cooper SI
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- Cutajar M
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
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- Zatserklyaniy A
- Zeinali M
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- Zeyrek M
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
- Abbrescia M
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- Cuevas J
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- Custodio A
- Cutajar M
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- Czellar S
- D'Agnolo RT
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- Da Costa EM
- Dabrowski A
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- 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
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Ziebarth EB
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Surat UE
- Svintradze I
- Svyatkovskiy A
- Swanson J
- Swartz M
- Symonds P
- Szillasi Z
- Szleper M
- Sznajder A
- Tadel M
- Takahashi M
- Tali B
- Tambe N
- Tan P
- Tao J
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
- Taylor L
- Tcholakov V
- Temple J
- Tenchini R
- Teng H
- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
- Theofilatos K
- Thom J
- Thomas L
- Thomas S
- Thompson J
- Thomsen J
- Thyssen F
- Tiko A
- Timciuc V
- Tinti G
- Tiras E
- Titov M
- Tkaczyk S
- Tlisov D
- To W
- Toback D
- Tomalin IR
- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topaksu AK
- Torassa E
- Toropin A
- Torre P
- Tosi M
- Tosi S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Tropiano A
- Troshin S
- Tsamalaidze Z
- 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
- Ulrich R
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzunian A
- Vaandering EW
- 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
- Vartak A
- Vasquez Sierra R
- Vaughan J
- Vavilov S
- Vazquez Acosta M
- Vazquez Valencia F
- Veelken C
- Veeraraghavan V
- Velasco M
- Velicanu D
- Velkovska J
- Venditti R
- Venturi A
- Verdier P
- Verdini PG
- Veres GI
- Vergili LN
- Vergili M
- Verwilligen P
- Verzetti M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal Marono M
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
- Viret S
- Virto AL
- Vischia P
- Vishnevskiy D
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- 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 X
- Wang J
- Wang J
- Wang M
- Wang S
- Wang X
- Wang Z
- Wardle N
- Wasserbaech S
- Wayand S
- Wayne M
- Weber H
- Weber HA
- Weber M
- Weber M
- Wehrli L
- Weiler T
- Weinberg M
- Wendland L
- Weng Y
- Wenger EA
- Werner JS
- West C
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickramage N
- Widl E
- Wilken R
- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winer BL
- 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
- 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
- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Ethnobotanical remarks on Central and Southern Italy
- Author
- A Bianchi
- A Bruni
- A De Bellis
- A De Nino
- A Frigino
- A Pieroni
- A Pieroni
- A Pieroni
- AD Atzei
- AM Scherrer
- AZ Mercadante
- B Bellomaria
- BT Alvarez Arias
- C Chiovenda-Bensi
- C Pigorini Beri
- C Pigorini Beri
- CP Dutta
- DL De Vincentiis
- E De Simoni
- EL Camm
- EM Cappelletti
- EM Cappelletti
- F Conti
- F Lentini
- F Lentini
- F Lentini
- F Lentini
- F Tammaro
- F Tammaro
- F Zampiva
- FP Amico
- G Aliotta
- G Caneva
- G Corsi
- G Corsi
- G Finamore
- G Finamore
- G Picchi
- G Pitrè
- G Salerno
- G Salerno
- GM Nardelli
- J Friedman
- J Valnet
- J Valnet
- J Valnet
- JCT Uphof
- JL Guil-Guerrero
- L Bernardo
- L Fenaroli
- L Mariotti
- L Viegi
- LC Lahon
- Leporatti Maria Lucia
- M Bàthori
- MA Bonet
- ML Leporatti
- ML Leporatti
- ML Leporatti
- ML Leporatti
- ML Leporatti
- N Passalacqua
- N Passalacqua
- P Gastaldo
- P Lieutaghi
- P Lieutaghi
- PA Mattioli
- Paolo Maria Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- PM Guarrera
- R Barone
- RG Binder
- RR Paris
- S Ferri
- S La Sorsa
- S Maccioni
- SM El-Zalabani
- T Seppilli
- V Ostermann
- VL Shelyuto
- VL Shelyuto
- Z Pongràcz
- Z Zanetti
- Publication venue
- BioMed Central
- Publication date
- 01/01/2007
- Field of study
<p>Abstract</p> <p>Background</p> <p>The present paper is a brief survey on the ethnobotanical works published by the Authors since 1981, concerning the research carried out in some southern and central Italian regions. Before Roman domination these territories were first inhabited by local people, while the southern areas were colonized by the Greeks. These different cultural contributions left certain traces, both in the toponyms and in the vernacular names of the plants and, more generally, in the culture as a whole.</p> <p>Methods</p> <p>Field data were collected through open interviews, mainly of farmers, shepherds and elderly people, born or living in these areas for a long time. Voucher specimens of collected plants are preserved in the respective herbaria of the Authors and in the herbarium of "Roma Tre" University. Important contributions have been made by several students native to the areas under consideration. A comparative analysis with local specific ethnobotanical literature was carried out.</p> <p>Results</p> <p>The paper reports several examples concerning human and veterinary popular medicine and in addition some anti-parasitic, nutraceutic, dye and miscellaneous uses are also described. Moreover vernacular names and toponyms are cited. Eight regions of central and southern Italy (particularly Latium, Abruzzo, Marche and Basilicata) were investigated and the data obtained are presented in 32 papers. Most of the species of ethnobotanical interest have been listed in Latium (368 species), Marche (274) and Abruzzo (203). The paper also highlights particularly interesting aspects or uses not previously described in the specific ethnobotanical literature.</p> <p>Conclusion</p> <p>Phyto-therapy in central and southern Italy is nowadays practised by a few elderly people who resort to medicinal plants only for mild complaints (on the contrary food uses are still commonly practised). Nowadays therapeutic uses, unlike in the past, are less closely or not at all linked to ritual aspects. Several plants deserve to be taken into consideration not only from the anthropological or cultural point of view, but also for further phyto-chemical investigation. Our studies, as well as those of other authors, try to provide an original picture of the local ethno-biodiversity.</p
Combined Tevatron upper limit on gg->H->W+W- and constraints on the Higgs boson mass in fourth-generation fermion models
- Author
- Aaltonen T
- Abazov VM
- Abbott B
- Abolins M
- Acharya BS
- Adams M
- Adams T
- Adelman J
- Aguilo E
- Alexeev GD
- Alkhazov G
- Almenar CC
- Alton A
- Alverson G
- Alves GA
- Amerio S
- Amidei D
- Anastassov A
- Ancu LS
- Annovi A
- Antos J
- Aoki M
- Apollinari G
- Appel J
- Apresyan A
- Arisawa T
- Arnoud Y
- Arov M
- Artikov A
- Asaadi J
- Ashmanskas W
- Askew A
- Asman B
- Atramentov O
- Attal A
- Aurisano A
- Avila C
- Azfar F
- BackusMayes J
- Badaud F
- Badgett W
- Bagby L
- Baldin B
- Bandurin DV
- Banerjee S
- Barbaro Galtieri A
- Barberis E
- Barfuss AF
- Baringer P
- Barnes VE
- Barnett BA
- Barreto J
- Barria P
- Bartlett JF
- Bartos P
- Bassler U
- Bauer G
- Beale S
- Bean A
- Beauchemin PH
- Bedeschi F
- Beecher D
- Begalli M
- Begel M
- Behari S
- Belanger Champagne C
- Bellantoni L
- Bellettini G
- Bellinger J
- Benitez JA
- Benjamin D
- Beretvas A
- Beri SB
- Bernardi G
- Bernhard R
- Bertram I
- Besancon M
- Beuselinck R
- Bezzubov VA
- Bhat PC
- Bhatnagar V
- Bhatti A
- Binkley M
- Bisello D
- Bizjak I
- Blair RE
- Blazey G
- Blessing S
- Blocker C
- Bloom K
- Blumenfeld B
- Bocci A
- Bodek A
- Boehnlein A
- Boisvert V
- Boline D
- Bolton TA
- Boos EE
- Borissov G
- Bortoletto D
- Bose T
- Boudreau J
- Boveia A
- Brandt A
- Brau B
- Bridgeman A
- Brigliadori L
- Brock R
- Bromberg C
- Brooijmans G
- Bross A
- Brown D
- Brubaker E
- Bu XB
- Buchholz D
- Budagov J
- Budd HS
- Budd S
- Buehler M
- Buescher V
- Bunichev V
- Burdin S
- Burkett K
- Burnett TH
- Busetto G
- Bussey P
- Buszello CP
- Buzatu A
- Byrum KL
- Cabrera S
- Calancha C
- Calfayan P
- Calpas B
- Calvet S
- Camacho Perez E
- Camarda S
- Camillocci E. Solfaroli
- Cammin J
- Campanelli M
- Campbell M
- Canelli F
- Canepa A
- Carls B
- Carlsmith D
- Carosi R
- Carrasco Lizarraga MA
- Carrera E
- Carrillo S
- Carron S
- Casal B
- Casarsa M
- Casey BCK
- Castilla Valdez H
- Castro A
- Catastini P
- Cauz D
- Cavaliere V
- Cavalli Sforza M
- Cerri A
- Cerrito L
- Chakrabarti S
- Chakraborty D
- Chan KM
- Chandra A
- Chang SH
- Chen G
- Chen YC
- Chertok M
- Chevalier Thery S
- Chiarelli G
- Chlachidze G
- Chlebana F
- Cho DK
- Cho K
- Cho SW
- Choi S
- Chokheli D
- Chou JP
- Choudhary B
- Christoudias T
- Chung K
- Chung WH
- Chung YS
- Chwalek T
- Cihangir S
- Ciobanu CI
- Ciocci MA
- Claes D
- Clark A
- Clark D
- Clutter J
- Compostella G
- Convery ME
- Conway J
- Cooke M
- Cooper WE
- Corbo M
- Corcoran M
- Cordelli M
- Couderc F
- Cousinou MC
- Cox CA
- Cox DJ
- Crescioli F
- Croc A
- Cuevas J
- Culbertson R
- Cully JC
- Cutts D
- Cwiok M
- d'Ascenzo N
- d'Errico M
- D'Onofrio M
- da Costa JG
- Dagenhart D
- Das A
- Datta M
- Davies G
- Davies T
- de Barbaro P
- De Cecco S
- de Jong SJ
- De K
- De la Cruz Burelo E
- De Lorenzo G
- Deisher A
- Deliot F
- DELL'ORSO MAURO
- Deluca C
- Demarteau M
- Demina R
- Demortier L
- Deng J
- Deninno M
- Denisov D
- Denisov SP
- Desai S
- DeVaughan K
- Di Canto A
- Di Ruzza B
- Diehl HT
- Diesburg M
- Dittmann JR
- Dominguez A
- DONATI SIMONE
- Dong P
- Dorigo T
- Dorland T
- Dube S
- Dubey A
- Dudko LV
- Duggan D
- Duperrin A
- Dutt S
- Dyshkant A
- Eads M
- Ebina K
- Edmunds D
- Elagin A
- Ellison J
- Elvira VD
- Enari Y
- Eno S
- Erbacher R
- Errede D
- Errede S
- Ershaidat N
- Eusebi R
- Evans H
- Evdokimov A
- Evdokimov VN
- Facini G
- Fang HC
- Farrington S
- Fedorko WT
- Feild RG
- Feindt M
- Ferapontov AV
- Ferbel T
- Fernandez JP
- Fernandez PM
- Ferrazza C
- Fiedler F
- Field R
- Filthaut F
- Fisher W
- Fisk HE
- Flanagan G
- Forrest R
- Fortner M
- Fox H
- Frank MJ
- Franklin M
- Freeman JC
- Fuess S
- Furic I
- Gadfort T
- Gallinaro M
- Galyardt J
- Garberson F
- Garcia Bellido A
- Garcia JE
- Garfinkel AF
- Garosi P
- Garzon GJOY
- Gavrilov V
- Gay P
- Geist W
- Geng W
- Gerbaudo D
- Gerber CE
- Gerberich H
- Gerdes D
- Gershtein Y
- Gessler A
- Giagu S
- Giakoumopoulou V
- Giannetti P
- Gibson K
- Gillberg D
- Gimmell JL
- Ginsburg CM
- Ginther G
- Giokaris N
- Giordani M
- Giromini P
- Giunta M
- Giurgiu G
- Glagolev V
- Glenzinski D
- Gold M
- Goldschmidt N
- Golossanov A
- Golovanov G
- Gomez Ceballos G
- Gomez G
- Goncharov M
- Gonzalez BA
- Gonzalez O
- Gorelov I
- Goshaw AT
- Goulianos K
- Goussiou A
- Grannis PD
- Greder S
- Greenlee H
- Greenwood ZD
- Gregores EM
- Grenier G
- Gresele A
- Grinstein S
- Gris P
- Griso SP
- Grivaz JF
- Grohsjean A
- Grosso Pilcher C
- Group RC
- Grundler U
- Grunendahl S
- Grunewald MW
- Gunay Unalan Z
- Guo F
- Guo J
- Gutierrez G
- Gutierrez P
- Haas A
- Haber C
- Haefner P
- Hagopian S
- Hahn SR
- Haley J
- Halkiadakis E
- Hall I
- Han BY
- Han JY
- Han L
- Happacher F
- Hara K
- Harder K
- Hare D
- Hare M
- Harel A
- Harr RF
- Hartz M
- Hatakeyama K
- Hauptman JM
- Hays C
- Hays J
- Hebbeker T
- Heck M
- Hedin D
- Heinrich J
- Heinson AP
- Heintz U
- Hensel C
- Heredia De La Cruz I
- Herndon M
- Herner K
- Hesketh G
- Heuser J
- Hewamanage S
- Hidas D
- Hildreth MD
- Hill CS
- Hirosky R
- Hirschbuehl D
- Hoang T
- Hobbs JD
- Hocker A
- Hoeneisen B
- Hohlfeld M
- Hossain S
- Hou S
- Houben P
- Houlden M
- Hsu SC
- Hu Y
- Hubacek Z
- Hughes RE
- Hurwitz M
- Husemann U
- Huske N
- Hussein M
- Huston J
- Hynek V
- Iashvili I
- Illingworth R
- Incandela J
- Introzzi G
- Iori M
- Ito AS
- Ivanov A
- Jabeen S
- Jaffre M
- Jain S
- James E
- Jamin D
- Jang D
- Jayatilaka B
- Jeon EJ
- Jesik R
- Jha MK
- Jindariani S
- Johns K
- Johnson C
- Johnson M
- Johnson W
- Johnston D
- Jonckheere A
- Jones M
- Jonsson P
- Joo KK
- Jun SY
- Jung JE
- Junk TR
- Juste A
- Kaadze K
- Kajfasz E
- Kamon T
- Kar D
- Karchin PE
- Karmanov D
- Kasper PA
- Kato Y
- Katsanos I
- Kehoe R
- Kephart R
- Kermiche S
- Ketchum W
- Keung J
- Khalatyan N
- Khanov A
- Kharchilava A
- Kharzheev YN
- Khatidze D
- Khotilovich V
- Kilminster B
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- Kim JE
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- Kirby MH
- Kirsch L
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- Kohli JM
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- Kong DJ
- Konigsberg J
- Korytov A
- Kotwal AV
- Kozelov AV
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- Mal PK
- Malde S
- Malik S
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- Malyshev VL
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- Publication venue
- Publication date
- 01/01/2010
- Field of study
Report number: FERMILAB-PUB-10-125-EWe combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg->H->W+W- in p=pbar collisions at the Fermilab Tevatron Collider at sqrt{s}=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% Confidence Level upper limit on \sigma(gg->H) x B(H->W+W-) is 1.75 pb at m_H=120 GeV, 0.38 pb at m_H=165 GeV, and 0.83 pb at m_H=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% Confidence Level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg→H→W+W- in pp̅ collisions at the Fermilab Tevatron Collider at √s=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% confidence level upper limit on σ(gg→H)×B(H→W+W-) is 1.75 pb at mH=120 GeV, 0.38 pb at mH=165 GeV, and 0.83 pb at mH=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% confidence level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.Peer reviewe
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