257 research outputs found
Sample entropy analysis of EEG signals via artificial neural networks to model patients' consciousness level based on anesthesiologists experience.
- Publication venue
- 'Hindawi Limited'
- Publication date
- 01/01/2015
- Field of study
Electroencephalogram (EEG) signals, as it can express the human brain's activities and reflect awareness, have been widely used in many research and medical equipment to build a noninvasive monitoring index to the depth of anesthesia (DOA). Bispectral (BIS) index monitor is one of the famous and important indicators for anesthesiologists primarily using EEG signals when assessing the DOA. In this study, an attempt is made to build a new indicator using EEG signals to provide a more valuable reference to the DOA for clinical researchers. The EEG signals are collected from patients under anesthetic surgery which are filtered using multivariate empirical mode decomposition (MEMD) method and analyzed using sample entropy (SampEn) analysis. The calculated signals from SampEn are utilized to train an artificial neural network (ANN) model through using expert assessment of consciousness level (EACL) which is assessed by experienced anesthesiologists as the target to train, validate, and test the ANN. The results that are achieved using the proposed system are compared to BIS index. The proposed system results show that it is not only having similar characteristic to BIS index but also more close to experienced anesthesiologists which illustrates the consciousness level and reflects the DOA successfully.This research is supported by the Center forDynamical Biomarkers and Translational Medicine, National Central University, Taiwan, which is sponsored by Ministry of Science and Technology (Grant no. MOST103-2911-I-008-001). Also, it is supported by National Chung-Shan Institute of Science & Technology in Taiwan (Grant nos. CSIST-095-V301 and CSIST-095-V302)
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Observation of associated near-side and away-side long-range correlations in βsNN=5.02ββTeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
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- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
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- Chekulaev SV
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- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniΕ‘ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviΔ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ΞΟ) and pseudorapidity (ΞΞ·) are measured in βsNN=5.02ββTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ββΞΌb-1 of data as a function of transverse momentum (pT) and the transverse energy (Ξ£ETPb) summed over 3.1<Ξ·<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|ΞΞ·|<5) βnear-sideβ (ΞΟβΌ0) correlation that grows rapidly with increasing Ξ£ETPb. A long-range βaway-sideβ (ΞΟβΌΟ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small Ξ£ETPb, is found to match the near-side correlation in magnitude, shape (in ΞΞ· and ΞΟ) and Ξ£ETPb dependence. The resultant ΞΟ correlation is approximately symmetric about Ο/2, and is consistent with a dominant cosβ‘2ΞΟ modulation for all Ξ£ETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
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- Abramowicz H
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- Yilmaz M
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- Zeitnitz C
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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fbβ1 of sβ=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan Ξ² < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at sβ=7 TeV with the ATLAS detector
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Aben R
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- Yanush S
- Yao L
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- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
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- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yu J
- Yu J
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
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- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhu H
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Zβ² gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Ξ³ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbβ1 in the e + e β channel and 5.0 fbβ1 in the ΞΌ + ΞΌ βchannel. A Z β² boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Zβ² Models
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
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- Terashi K
- Terron J
- Testa M
- Teuscher RJ
- Therhaag J
- Theveneaux-Pelzer T
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tic T
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisscrant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tomoto M
- Tompkins L
- Toms K
- Tonoyan A
- Topfel C
- Topilin ND
- Toro RC
- Torrence E
- Torres H
- Toth J
- Touchard F
- Tovey FR
- Trefzger T
- Tremblet L
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Tripiana MF
- Triplett N
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- True P
- Trzebinski M
- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiakiris M
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsung J-W
- Tsuno S
- Tsybychev D
- Tua A
- Tudorache A
- Tudorache V
- Tuggle JM
- Turala M
- Turecek D
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ughetto N
- Ugland M
- Uhlenbrock M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Vacavant L
- Vacek V
- Vachon B
- Vahsen S
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallecorsa S
- Van Berg R
- Van der Deij PC
- van der Geer R
- van der Graaf H
- Van der Leeuw R
- van der Poel E
- van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- Van Nieuwkoop J
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vazquez JGP
- Vegni G
- Veillet JJ
- Veloso F
- Veness R
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Viehou I
- Viel S
- Villa M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Virzi J
- Vitells O
- Viti M
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wahlen H
- Wahrmund S
- Wakabayashi J
- Walch S
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Walsh B
- Wang C
- Wang H
- Wang H
- Wang J
- Wang J
- Wang R
- Wang SM
- Wang T
- Warburton A
- Ward CP
- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
- Watson AT
- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh AT
- Waugh BM
- Weber MS
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wenaus T
- Wendland D
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Wetter J
- Weydert C
- Whalen K
- White A
- White MJ
- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Williams S
- Willis W
- Willocq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yagci KD
- Yamada N
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or Ο lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, Ο, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan Ξ² in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Opposite polarities of ENSO drive distinct patterns of coral bleaching potentials in the southeast Indian Ocean.
- Author
- A Hoell
- AF Pearce
- AF Pearce
- AG Marshall
- AG Marshall
- AJ Hobday
- AP Kerswell
- AR Halford
- BJ Henley
- C Jones
- CM Spillman
- CW Speed
- DP Dee
- E Kintisch
- FP Lima
- G Liu
- HH Hendon
- HY Kao
- J Salinger
- J Zinke
- J Zinke
- JA Moore
- JEN Veron
- JJ Luo
- JM Lough
- JM Slingo
- JP Gilmour
- JPA Hobbs
- JS Kug
- K Ashok
- M Depczynsk
- M Feng
- M Feng
- M Feng
- M Kanamitsu
- MC Wheeler
- MC Wheeler
- MJ McPhaden
- O Hoegh-Guldberg
- SK Behera
- T Doi
- T Kataoka
- T Tozuka
- T Wernberg
- TP Hughes
- W Han
- WJ Cai
- WJ Cai
- WJ Cai
- WQ Han
- Y Du
- Y Du
- Y Du
- Y Kajikawa
- ZT Richards
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Episodic anomalously warm sea surface temperature (SST) extremes, or marine heatwaves (MHWs), amplify ocean warming effects and may lead to severe impacts on marine ecosystems. MHW-induced coral bleaching events have been observed frequently in recent decades in the southeast Indian Ocean (SEIO), a region traditionally regarded to have resilience to global warming. In this study, we assess the contribution of El NiΓ±o-Southern Oscillation (ENSO) to MHWs across the mostly understudied reefs in the SEIO. We find that in extended summer months, the MHWs at tropical and subtropical reefs (divided at ~20Β°S) are driven by opposite ENSO polarities: MHWs are more likely to occur at the tropical reefs during eastern Pacific El NiΓ±o, driven by enhanced solar radiation and weaker Australian Monsoon, some likely alleviated by positive Indian Ocean Dipole events, and at the subtropical reefs during central Pacific La NiΓ±a, mainly caused by increased horizontal heat transport, and in some cases reinforced by local air-sea interactions. Madden-Julian Oscillations (MJO) also modulate the MHW occurrences. Projected future increases in ENSO and MJO intensity with greenhouse warming will enhance thermal stress across the SEIO. Implementing forecasting systems of MHWs can be used to anticipate future coral bleaching patterns and prepare management responses
The impact of temperature and Wolbachia infection on vector competence of potential dengue vectors Aedes aegypti and Aedes albopictus in the transmission of dengue virus serotype 1 in southern Taiwan
- Author
- AA Khasnis
- BW Alto
- C Christiansen-Jucht
- C Lin
- Cheng-Hui Tsai
- Cheo Lin
- Chien-Ling Su
- DJ Gubler
- DM McLean
- DM Watts
- EL Kaplan
- Hwa-Jen Teng
- JR Anderson
- JW Mains
- KH Tsai
- L Mousson
- LB Carrington
- LB Carrington
- LB Carrington
- M Chan
- MI Salazar
- OJ Brady
- P Barbazan
- P Lu
- PA Ross
- Pei-Yun Shu
- PY Shu
- S Bhatt
- SB Halstead
- SF Chang
- SL Dobson
- T Walker
- Tien-Huang Chen
- W HH
- W Zhou
- Y Ooi
- YH Ye
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
STAT3 can be activated through paracrine signaling in breast epithelial cells
- Author
- A Jemal
- A Kate Sasser
- AK Sasser
- B Gu
- Brett M Hall
- Brian Hutzen
- C Yao
- CE van Roozendaal
- CJ Watson
- CL Chen
- CP Lim
- CV Clevenger
- D Conze
- D Hanahan
- EB Haura
- FC Hsieh
- H Knupfer
- H Yu
- H Yu
- HH Yeh
- Huey-Jen Lin
- Jacqueline C Lieblein
- JC Chang
- JE Darnell Jr
- JF Bromberg
- Jiayuh Lin
- JN Ihle
- JN Ihle
- JP Evans
- L Ronnov-Jessen
- LA O'Sullivan
- M Berishaj
- M Rincon
- MA Blaskovich
- MS Bendre
- NA Bhowmick
- NA Bhowmick
- NG Copeland
- PB Sehgal
- PJ Real
- R Buettner
- R Garcia
- R Garcia
- R Kalluri
- Sarah Ball
- SY Sung
- T Bowman
- T Bowman
- TD Tlsty
- Tim HM Huang
- WY Chen
- Z Duan
- Z Wen
- Z Zhong
- Publication venue
- BioMed Central
- Publication date
- 01/01/2008
- Field of study
<p>Abstract</p> <p>Background</p> <p>Many cancers, including breast cancer, have been identified with increased levels of phosphorylated or the active form of Signal Transducers and Activators of Transcription 3 (STAT3) protein. However, whether the tumor microenvironment plays a role in this activation is still poorly understood.</p> <p>Methods</p> <p>Conditioned media, which contains soluble factors from MDA-MB-231 and MDA-MB-468 breast cancer cells and breast cancer associated fibroblasts, was added to MCF-10A breast epithelial and MDA-MB-453 breast cancer cells. The stimulation of phosphorylated STAT3 (p-STAT3) levels by conditioned media was assayed by Western blot in the presence or absence of neutralized IL-6 antibody, or a JAK/STAT3 inhibitor, JSI-124. The stimulation of cell proliferation in MCF-10A cells by conditioned media in the presence or absence of JSI-124 was subjected to MTT analysis. IL-6, IL-10, and VEGF levels were determined by ELISA analysis.</p> <p>Results</p> <p>Our results demonstrated that conditioned media from cell lines with constitutively active STAT3 are sufficient to induce p-STAT3 levels in various recipients that do not possess elevated p-STAT3 levels. This signaling occurs through the JAK/STAT3 pathway, leading to STAT3 phosphorylation as early as 30 minutes and is persistent for at least 24 hours. ELISA analysis confirmed a correlation between elevated levels of IL-6 production and p-STAT3. Neutralization of the IL-6 ligand or gp130 was sufficient to block increased levels of p-STAT3 (Y705) in treated cells. Furthermore, soluble factors within the MDA-MB-231 conditioned media were also sufficient to stimulate an increase in IL-6 production from MCF-10A cells.</p> <p>Conclusion</p> <p>These results demonstrate STAT3 phosphorylation in breast epithelial cells can be stimulated by paracrine signaling through soluble factors from both breast cancer cells and breast cancer associated fibroblasts with elevated STAT3 phosphorylation. The induction of STAT3 phosphorylation is through the IL-6/JAK pathway and appears to be associated with cell proliferation. Understanding how IL-6 and other soluble factors may lead to STAT3 activation via the tumor microenvironment will provide new therapeutic regimens for breast carcinomas and other cancers with elevated p-STAT3 levels.</p
Model-Based Deconvolution of Cell Cycle Time-Series Data Reveals Gene Expression Details at High Resolution
- Author
- A Campbell
- A Csikasz-Nagy
- A Kelly
- A Newton
- A Reisenauer
- AN Netravali
- B Brewer
- B Gorbatyuk
- B Grunenfelder
- BJ Smith
- C Jacobs
- CC Guet
- D Bates
- D Lockhart
- D Longo
- D Orlando
- D Siegal-Gaskins
- Dan Siegal-Gaskins
- DY Hung
- E Jen
- E Korobkova
- E Quardokus
- EB Purcell
- EG Biondi
- EM Judd
- EM Ozbudak
- G Banfalvi
- G Zweiger
- HH McAdams
- I Domian
- I Golding
- J Holtzendorff
- J Levsky
- JL Stove
- Joel S. Bader
- Joshua N. Ash
- K Shedden
- L Tenorio
- M Evinger
- M Rowicka
- M Sackett
- M Thanbichler
- M Valencia-Burton
- MB Elowitz
- MT Laub
- MT Laub
- N Brenner
- N Rosenfeld
- P Brazhnik
- P Craven
- P Lu
- P Ma
- P Qiu
- PJ Green
- PT McGrath
- S DiTalia
- S Li
- S Roy
- Sean Crosson
- T Chiaverotti
- T Hastie
- TJ Strovas
- U Jenal
- X Shen
- Z Bar-Joseph
- Z Bar-Joseph
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
In both prokaryotic and eukaryotic cells, gene expression is regulated across the cell cycle to ensure βjust-in-timeβ assembly of select cellular structures and molecular machines. However, present in all time-series gene expression measurements is variability that arises from both systematic error in the cell synchrony process and variance in the timing of cell division at the level of the single cell. Thus, gene or protein expression data collected from a population of synchronized cells is an inaccurate measure of what occurs in the average single-cell across a cell cycle. Here, we present a general computational method to extract βsingle-cellβ-like information from population-level time-series expression data. This method removes the effects of 1) variance in growth rate and 2) variance in the physiological and developmental state of the cell. Moreover, this method represents an advance in the deconvolution of molecular expression data in its flexibility, minimal assumptions, and the use of a cross-validation analysis to determine the appropriate level of regularization. Applying our deconvolution algorithm to cell cycle gene expression data from the dimorphic bacterium Caulobacter crescentus, we recovered critical features of cell cycle regulation in essential genes, including ctrA and ftsZ, that were obscured in population-based measurements. In doing so, we highlight the problem with using population data alone to decipher cellular regulatory mechanisms and demonstrate how our deconvolution algorithm can be applied to produce a more realistic picture of temporal regulation in a cell
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