1,095 research outputs found
Automated segmentation of colorectal tumor in 3D MRI Using 3D multiscale densely connected convolutional neural network
- Author
- Publication venue
- 'Hindawi Limited'
- Publication date
- 01/01/2019
- Field of study
Get PDFThe main goal of this work is to automatically segment colorectal tumors in 3D T2-weighted (T2w) MRI with reasonable accuracy. For such a purpose, a novel deep learning-based algorithm suited for volumetric colorectal tumor segmentation is proposed. The proposed CNN architecture, based on densely connected neural network, contains multiscale dense interconnectivity between layers of fine and coarse scales, thus leveraging multiscale contextual information in the network to get better flow of information throughout the network. Additionally, the 3D level-set algorithm was incorporated as a postprocessing task to refine contours of the network predicted segmentation. The method was assessed on T2-weighted 3D MRI of 43 patients diagnosed with locally advanced colorectal tumor (cT3/T4). Cross validation was performed in 100 rounds by partitioning the dataset into 30 volumes for training and 13 for testing. Three performance metrics were computed to assess the similarity between predicted segmentation and the ground truth (i.e., manual segmentation by an expert radiologist/oncologist), including Dice similarity coefficient (DSC), recall rate (RR), and average surface distance (ASD). The above performance metrics were computed in terms of mean and standard deviation (mean ± standard deviation). The DSC, RR, and ASD were 0.8406 ± 0.0191, 0.8513 ± 0.0201, and 2.6407 ± 2.7975 before postprocessing, and these performance metrics became 0.8585 ± 0.0184, 0.8719 ± 0.0195, and 2.5401 ± 2.402 after postprocessing, respectively. We compared our proposed method to other existing volumetric medical image segmentation baseline methods (particularly 3D U-net and DenseVoxNet) in our segmentation tasks. The experimental results reveal that the proposed method has achieved better performance in colorectal tumor segmentation in volumetric MRI than the other baseline techniques
The economic impact of biosimilars in Italy : a scenario analysis
- Author
- Publication venue
- 'SAGE Publications'
- Publication date
- 01/01/2019
- Field of study
Get PDFBackground: the first generation of biotechnology drugs is reaching, or has already reached, the patent expiry and a large number of biosimilars is entering the Italian pharmaceutical market. The objective of the analysis was to evaluate the economic impacts of biosimilars on the national health expenditure in Italy between 2014 and 2020. Methods: Based on the information deriving from consumption per standard unit and equivalent patients, it was estimated monthly expenditure for some of the biological drugs currently available in Italy that have had or will have a patent expiry within the analysis period (infliximab, etanercept, adalimumab, insulin glargine, trastuzumab, rituximab, bevacizumab and insulin aspart). Pharmaceutical expenditure was calculated on hospital sales prices net of transparent discounts required by law and visible from the AIFA database. Three alternative scenarios have been developed based on the perceptions of a board of clinical experts, pharmacologists and pharmacoeconomists involved in the study. The experts involved analyzed the estimates of treated patients between 2014 and 2017 and reports their hypothetical biosimilar penetration during the period 2018-2020. The results were represented as the difference between the estimated expenditure in the absence of biosimilars and the estimated expenditure in the presence of biosimilars with the real or hypothetical biosimilar penetration. Results: considering the standard units dispensed for each year, the economic model estimate an annual expenditure in 2014 equal to € 1.47 billion for the molecules considered in the analysis. These estimates rise to € 1.54, € 1.50 billion and € 1.51 billion during 2015, 2016 and 2017 in the scenario without biosimilar introduction. Biosimilar introduction generates cost savings between € 3.8 million in 2015 and € 32.9 million in 2017 if compared with the scenario without. Assuming an increasing biosimilar penetration between 2018 and 2020, scenario analysis estimates a cumulative cost reduction equal to € 597 million. Conclusions: Overall, biosimilar penetration generates important cost reduction that could be re-invested in the National Health Sistem
Measurements of branching fraction ratios and CP-asymmetries in suppressed B^- -> D(-> K^+ pi^-)K^- and B^- -> D(-> K^+ pi^-)pi^- decays
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- Yu I.
- Yu S. S.
- Yun J. C.
- Zanetti A.
- Zeinali M.
- Zeise M.
- Zeng Y.
- Ziebarth E. B.
- Zito G.
- Zucchelli S..g Y.
- Zucchelli S.P.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Get PDFWe report the first reconstruction in hadron collisions of the suppressed
decays B^- -> D(-> K^+ pi^-)K^- and B^- -> D(-> K^+ pi^-)pi^-, sensitive to the
CKM phase gamma, using data from 7 fb^-1 of integrated luminosity collected by
the CDF II detector at the Tevatron collider. We reconstruct a signal for the
B^- -> D(-> K^+ pi^-)K^- suppressed mode with a significance of 3.2 standard
deviations, and measure the ratios of the suppressed to favored branching
fractions R(K) = [22.0 \pm 8.6(stat)\pm 2.6(syst)]\times 10^-3, R^+(K) =
[42.6\pm 13.7(stat)\pm 2.8(syst)]\times 10^-3, R^-(K)= [3.8\pm 10.3(stat)\pm
2.7(syst]\times 10^-3, as well as the direct CP-violating asymmetry A(K) =
-0.82\pm 0.44(stat)\pm 0.09(syst) of this mode. Corresponding quantities for
B^- -> D(-> K^+ pi^-)pi^- decay are also reported.Comment: 8 pages, 1 figure, accepted by Phys.Rev.D Rapid Communications for
Publicatio
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- 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
Get PDFThe 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
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- Xiao H
- Xie S
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- Yang M
- Yang Y
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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
- 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
Get PDFThe 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
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
Get PDFWe 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
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Won S
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- 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
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Get PDFThe 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
Search for the standard model Higgs boson in the H to ZZ to 2l 2nu channel in pp collisions at sqrt(s) = 7 TeV
- Author
- A Bredenstein
- A Bredenstein
- A Djouadi
- A Djouadi
- A Martin
- A. A. Ocampo Rios
- A. Adair
- A. Adiguzel
- A. Anastassov
- A. Apresyan
- A. Aranyi
- A. Askew
- A. Attikis
- A. Avetisyan
- A. B. Meyer
- A. Baden
- A. Barker
- A. Bean
- A. Belyaev
- A. Belyaev
- A. Benaglia
- A. Beretvas
- A. Bethani
- A. Bhatti
- A. Biselli
- A. Bocci
- A. Bodek
- A. Bonato
- A. Bornheim
- A. Branca
- A. Brinkerhoff
- A. Burgmeier
- A. C. Benvenuti
- A. C. Mignerey
- A. Cabrera
- A. Cakir
- A. Calderon
- A. Campbell
- A. Castro
- A. Chatterjee
- A. Cimmino
- A. Colaleo
- A. Custódio
- A. David
- A. De Benedetti
- A. De Cosa
- A. De Roeck
- A. Deisher
- A. Delgado Peris
- A. Dermenev
- A. Dierlamm
- A. Dimitrov
- A. Dominguez
- A. Drozdetskiy
- A. Elliott-Peisert
- A. Ellithi Kamel
- A. Ershov
- A. Everett
- A. F. Barfuss
- A. F. Osorio Oliveros
- A. Fahim
- A. Falkiewicz
- A. Fanfani
- A. Ferapontov
- A. Ferrando
- A. Flossdorf
- A. Gaddi
- A. Garcia-Bellido
- A. Gaz
- A. Geiser
- A. Ghezzi
- A. Giammanco
- A. Giassi
- A. Gilbert
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- A. Godshalk
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- PW Higgs
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- S. P. Singh
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- S. V. Gleyzer
- S. V. Rusakov
- S. Vanini
- S. Vavilov
- S. Viret
- S. W. Lee
- S. W. Li
- S. Wakefield
- S. Walsh
- S. Wang
- S. Wasserbaech
- S. Wimpenny
- S. Won
- S. Xie
- S. Y. Jun
- Sandra S. Padula
- T Aaltonen
- T Junk
- T Kibble
- T. Adams
- T. Aliev
- T. Aziz
- T. Bergauer
- T. Boccali
- T. Bolton
- T. Bose
- T. Caebergs
- T. Camporesi
- T. Christiansen
- T. Chwalek
- T. Cornelis
- T. Dahms
- T. Danielson
- T. Dorigo
- T. du Pree
- T. Ferguson
- T. Frueboes
- T. Geralis
- T. Hebbeker
- T. Hermanns
- T. Hreus
- T. J. Kim
- T. J. Mertzimekis
- T. Kamon
- T. Khurshid
- T. Klimkovich
- T. Kolberg
- T. Kress
- T. Kuhr
- T. Kurca
- T. Kypreos
- T. Lampén
- T. Le Grand
- T. Libeiro
- T. Lindén
- T. Lomtadze
- T. Ma
- T. Maes
- T. Martins
- T. Medvedeva
- T. Miao
- T. Miceli
- T. Mäenpää
- T. Mäki
- T. Orimoto
- T. Pearson
- T. Peiffer
- T. Peltola
- T. R. Fernandez Perez Tomei
- T. Rodrigo
- T. Rohe
- T. Rommerskirchen
- T. Rovelli
- T. S. Anjos
- T. Sakuma
- T. Scarborough
- T. Schoerner-Sadenius
- T. Schum
- T. Schwarz
- T. Sinthuprasith
- T. Speer
- T. Tabarelli de Fatis
- T. Tuuva
- T. Virdee
- T. Weiler
- T. Whyntie
- T. Williams
- T. Y. Ling
- T. Yetkin
- Th. Müller
- U Aglietti
- U. Akgun
- U. Baur
- U. Behrens
- U. Berzano
- U. Dosselli
- U. E. Surat
- U. Gasparini
- U. Gebbert
- U. Goerlach
- U. Grundler
- U. Heintz
- U. Joshi
- U. Langenegger
- U. Nauenberg
- V Ravindran
- V. Adler
- V. Andreev
- V. Andreev
- V. Azzolini
- V. Bhatnagar
- V. Blobel
- V. Brigljevic
- V. Cherepanov
- V. Chetluru
- V. Chiochia
- V. Ciulli
- V. Cuplov
- V. D. Elvira
- V. Dero
- V. Dutta
- V. E. Barnes
- V. E. Bazterra
- V. Epshteyn
- V. Gaultney
- V. Gavrilov
- V. Genchev
- V. Golovtsov
- V. Grishin
- V. Hagopian
- V. Halyo
- V. Innocente
- V. J. Smith
- V. Kachanov
- V. Karimäki
- V. Karjavin
- V. Khachatryan
- V. Khotilovich
- V. Kim
- V. Konoplyanikov
- V. Kozhuharov
- V. Krutelyov
- V. Krychkine
- V. Kumar
- V. Lemaitre
- V. M. Ghete
- V. Maroussov
- V. Matveev
- V. Monaco
- V. Mossolov
- V. Murzin
- V. Oguri
- V. Oreshkin
- V. O’Dell
- V. Palichik
- V. Patras
- V. Pavlunin
- V. Perelygin
- V. Petrov
- V. Popov
- V. Rekovic
- V. Savrin
- V. Sharma
- V. Sharma
- V. Smirnov
- V. Sola
- V. Sordini
- V. Stolin
- V. Sulimov
- V. Tcholakov
- V. Timciuc
- V. Valuev
- V. Veeraraghavan
- V. Veszpremi
- V. Zhukov
- V. Zhukova
- W. A. Khan
- W. Adam
- W. Andrews
- W. Behrenhoff
- W. Bertl
- W. Bialas
- W. Busza
- W. Carvalho
- W. Clarida
- W. Cooper
- W. D. Teo
- W. D. Zeuner
- W. De Boer
- W. Dominik
- W. Erdmann
- W. Ferguson
- W. Flanagan
- W. Funk
- W. Gabella
- W. H. Smith
- W. Haj Ahmad
- W. Hopkins
- W. J. Spalding
- W. J. Womersley
- W. Johns
- W. Kiesenhofer
- W. Ko
- W. L. Aldá
- W. L. Prado Da Silva
- W. Lange
- W. Li
- W. Li
- W. Lin
- W. Lohmann
- W. Luo
- W. Lustermann
- W. Martin
- W. Reece
- W. Sakumoto
- W. Sun
- W. T. Ford
- W. To
- W. Van Doninck
- W. Waltenberger
- W. Wu
- W. Zou
- W.-S. Hou
- X. Janssen
- X. Meng
- X. Quan
- X. Shi
- X. T. Huang
- X. Wang
- Y. Assran
- Y. Bai
- Y. Ban
- Y. Chao
- Y. Chen
- Y. Cho
- Y. Choi
- Y. Eshaq
- Y. F. Liu
- Y. Fu
- Y. Gao
- Y. Gershtein
- Y. Gotra
- Y. Guo
- Y. H. Chang
- Y. H. Chang
- Y. Hsiung
- Y. Iiyama
- Y. Ivanov
- Y. J. Lei
- Y. J. Lu
- Y. K. Choi
- Y. Kim
- Y. Kubota
- Y. Kuessel
- Y. Lu
- Y. M. Tzeng
- Y. Ma
- Y. Mao
- Y. Maravin
- Y. Musienko
- Y. Onel
- Y. Pakhotin
- Y. Roh
- Y. S. Chung
- Y. Sirois
- Y. Tschudi
- Y. Tu
- Y. W. Chang
- Y. Weng
- Y. Yang
- Y. Yilmaz
- Y. Zheng
- Y.-J. Lee
- Yu. Andreev
- Z. Antunovic
- Z. C. Yang
- Z. Chen
- Z. Hatherell
- Z. Hu
- Z. J. Guo
- Z. K. Liu
- Z. L. Trocsanyi
- Z. Szillasi
- Z. Wan
- Z. Wang
- Z. Zhang
- Zero J. Kim
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Get PDFA search for the standard model Higgs boson in the H to ZZ to 2l 2nu decay
channel, where l = e or mu, in pp collisions at a center-of-mass energy of 7
TeV is presented. The data were collected at the LHC, with the CMS detector,
and correspond to an integrated luminosity of 4.6 inverse femtobarns. No
significant excess is observed above the background expectation, and upper
limits are set on the Higgs boson production cross section. The presence of the
standard model Higgs boson with a mass in the 270-440 GeV range is excluded at
95% confidence level.Comment: Submitted to JHE
Combined search for the quarks of a sequential fourth generation
- Author
- A. A. Ocampo Rios
- A. Abdulsalam
- A. Adair
- A. Adiguzel
- A. Anastassov
- A. Apresyan
- A. Apyan
- A. Askew
- A. Attikis
- A. Avetisyan
- A. B. Meyer
- A. Baden
- A. Barker
- A. Bean
- A. Belyaev
- A. Belyaev
- A. Benaglia
- A. Beretvas
- A. Bethani
- A. Bhardwaj
- A. Bhatti
- A. Bocci
- A. Bodek
- A. Bonato
- A. Bornheim
- A. Branca
- A. Brinkerhoff
- A. Burgmeier
- A. C. Benvenuti
- A. C. Marini
- A. C. Mignerey
- A. Cakir
- A. Calamba
- A. Calderon
- A. Campbell
- A. Castro
- A. Chatterjee
- A. Cimmino
- A. Colaleo
- A. Custódio
- A. Dabrowski
- A. David
- A. De Benedetti
- A. De Cosa
- A. De Roeck
- A. Deisher
- A. Delgado Peris
- A. Dermenev
- A. Descroix
- A. Dierlamm
- A. Dimitrov
- A. Dominguez
- A. Drozdetskiy
- A. Elliott-Peisert
- A. Ellithi Kamel
- A. Everett
- A. F. Barfuss
- A. F. Osorio Oliveros
- A. Fahim
- A. Fanfani
- A. Ferapontov
- A. Ferrando
- A. G. Delannoy
- A. Garcia-Bellido
- A. Gaz
- A. Geiser
- A. Ghezzi
- A. Giammanco
- A. Giassi
- A. Gilbert
- A. Givernaud
- A. Godshalk
- A. Gozzelino
- A. Graziano
- A. Gribushin
- A. Gude
- A. Guneratne Bryer
- A. Gurrola
- A. Güth
- A. H. Ball
- A. Harel
- A. Heikkinen
- A. Heister
- A. Hervé
- A. Hinzmann
- A. Holzner
- A. Hunt
- A. Ivanov
- A. J. Bell
- A. Jafari
- A. Juodagalvis
- A. K. Mohanty
- A. K. Sanchez
- A. Kalinowski
- A. Kalogeropoulos
- A. Kamenev
- A. Karjalainen
- A. Kayis Topaksu
- A. Khan
- A. Kharchilava
- A. Khukhunaishvili
- A. Knutsson
- A. Kopecky
- A. Korablev
- A. Korpela
- A. Korytov
- A. Kraan
- A. Kropivnitskaya
- A. Kubik
- A. Kumar
- A. Kyriakis
- A. Lanaro
- A. Lanev
- A. Lath
- A. Ledovskoy
- A. Leonidov
- A. Lopez
- A. Lopez Virto
- A. Lucaroni
- A. Luthra
- A. Léonard
- A. M. Guler
- A. M. Rossi
- A. M. Sirunyan
- A. Malakhov
- A. Marinov
- A. Markina
- A. Markou
- A. Martelli
- A. Massironi
- A. Melo
- A. Messineo
- A. Mestvirishvili
- A. Meyer
- A. Moeller
- A. Mohammadi
- A. Mohapatra
- A. Montanari
- A. Morelos Pineda
- A. Mott
- A. Mussgiller
- A. Nappi
- A. Nayak
- A. Nikitenko
- A. Nowack
- A. Nürnberg
- A. O. M. Iorio
- A. Oehler
- A. Olbrechts
- A. Ostapchuk
- A. Ozpineci
- A. P. R. Gay
- A. P. Singh
- A. Panagiotou
- A. Papageorgiou
- A. Pashenkov
- A. Penzo
- A. Perieanu
- A. Perloff
- A. Perrotta
- A. Peterman
- A. Petrilli
- A. Petrukhin
- A. Pfeiffer
- A. Pin
- A. Polatoz
- A. Poll
- A. Pompili
- A. Popov
- A. Potenza
- A. Pozdnyakov
- A. Quintario Olmeda
- A. Racz
- A. Radi
- A. Raspereza
- A. Raval
- A. Rinkevicius
- A. Rizzi
- A. Romero
- A. Rose
- A. Rosowsky
- A. Ruiz-Jimeno
- A. Ryd
- A. S. Yoon
- A. Safonov
- A. Saha
- A. Sakharov
- A. Santocchia
- A. Santoro
- A. Savin
- A. Scheurer
- A. Schizzi
- A. Schmidt
- A. Sharma
- A. Sharma
- A. Singovsky
- A. Skuja
- A. Snigirev
- A. Sobol
- A. Solano
- A. Sparrow
- A. Spiezia
- A. Spiridonov
- A. Stahl
- A. Staiano
- A. Starodumov
- A. Svyatkovskiy
- A. Sznajder
- A. Sánchez-Hernández
- A. T. Laasanen
- A. T. Meneguzzo
- A. T. Serban
- A. Tapper
- A. Tatarinov
- A. Taurok
- A. Thea
- A. Tiko
- A. Toropin
- A. Tricomi
- A. Tropiano
- A. Tsirou
- A. Tumasyan
- A. Uzunian
- A. V. Gritsan
- A. Van Spilbeeck
- A. Vartak
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- W. J. Spalding
- W. J. Womersley
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- W. L. Aldá Júnior
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- Y. Assran
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- Y. Eshaq
- Y. F. Liu
- Y. Fu
- Y. Gao
- Y. Gershtein
- Y. Guo
- Y. H. Chang
- Y. H. Chang
- Y. Hsiung
- Y. Iiyama
- Y. Ivanov
- Y. J. Lei
- Y. J. Lu
- Y. K. Choi
- Y. Kim
- Y. Kubota
- Y. Kuessel
- Y. Lu
- Y. M. Tzeng
- Y. Ma
- Y. Mao
- Y. Maravin
- Y. Musienko
- Y. Onel
- Y. Pakhotin
- Y. Roh
- Y. S. Chung
- Y. Sirois
- Y. Tschudi
- Y. Tu
- Y. W. Chang
- Y. Weng
- Y. Yang
- Y. Yilmaz
- Y. Zheng
- Y.-J. Lee
- Yu. Andreev
- Z. Antunovic
- Z. C. Yang
- Z. Hatherell
- Z. Hu
- Z. J. Guo
- Z. K. Liu
- Z. L. Trocsanyi
- Z. Staykova
- Z. Szillasi
- Z. Tsamalaidze
- Z. Wang
- Z. Zhang
- Zero J. Kim
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Get PDFResults are presented from a search for a fourth generation of quarks
produced singly or in pairs in a data set corresponding to an integrated
luminosity of 5 inverse femtobarns recorded by the CMS experiment at the LHC in
2011. A novel strategy has been developed for a combined search for quarks of
the up and down type in decay channels with at least one isolated muon or
electron. Limits on the mass of the fourth-generation quarks and the relevant
Cabibbo-Kobayashi-Maskawa matrix elements are derived in the context of a
simple extension of the standard model with a sequential fourth generation of
fermions. The existence of mass-degenerate fourth-generation quarks with masses
below 685 GeV is excluded at 95% confidence level for minimal off-diagonal
mixing between the third- and the fourth-generation quarks. With a mass
difference of 25 GeV between the quark masses, the obtained limit on the masses
of the fourth-generation quarks shifts by about +/- 20 GeV. These results
significantly reduce the allowed parameter space for a fourth generation of
fermions.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- 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
- Alcaraz Maestre J
- Alda Junior WL
- Aldaya Martin M
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- 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
- Antonelli L
- Antunovic Z
- Apanasevich L
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- Vogel H
- Volkov A
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- Volodko A
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- Wickramage N
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- Winn D
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- Wissing C
- Wittich P
- Wittmer B
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- Wolf M
- Wolf R
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- Won S
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- 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
Get PDFA 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
- …
