152 research outputs found
Tight coupling of leaf area index to canopy nitrogen and phosphorus across heterogeneous tallgrass prairie communities
- Author
- Anne E. Klodd
- AP Walker
- C Liu
- CA Quesada
- CJ Stevens
- CL Turner
- CL Turner
- DC Hartnett
- DG Milchunas
- DS Schimel
- EG Towne
- EG Towne
- EJ Raynor
- EK Koller
- ET Borer
- Gareth K. Phoenix
- GR Shaver
- HA Ajwa
- Hazel Waring
- J Murphy
- JB Nippert
- JB Nippert
- Jesse B. Nippert
- JJ Elser
- JM Blair
- KN Suding
- LC Johnson
- LE Street
- LE Street
- M Williams
- MD Abrams
- ML Avolio
- MT van Wijk
- NT Hobbs
- PB Reich
- PG Cech
- R Aerts
- R Bobbink
- RB McKane
- RH Anderson
- S Güsewell
- SA Damhoureyeh
- SD Fuhlendorf
- SE Allen
- SE Koerner
- SH Taylor
- SL Collins
- TR Seastedt
- TR Seastedt
- W Koerselman
- W Steffen
- Y Hautier
- Z Ratajczak
- Zak Ratajczak
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 25/08/2016
- Field of study
Nitrogen (N) and phosphorus (P) are limiting nutrients for many plant communities worldwide. Foliar N and P along with leaf area are among the most important controls on photosynthesis and hence productivity. However, foliar N and P are typically assessed as species level traits, whereas productivity is often measured at the community scale. Here, we compared the community-level traits of leaf area index (LAI) to total foliar nitrogen (TFN) and total foliar phosphorus (TFP) across nearly three orders of magnitude LAI in grazed and ungrazed tallgrass prairie in north-eastern Kansas, USA. LAI was strongly correlated with both TFN and TFP across communities, and also within plant functional types (grass, forb, woody, and sedge) and grazing treatments (bison or cattle, and ungrazed). Across almost the entire range of LAI values and contrasting communities, TFN:TFP ratios indicated co-limitation by N and P in almost all communities; this may further indicate a community scale trend of an optimal N and P allocation per unit leaf area for growth. Previously, results from the arctic showed similar tight relationships between LAI:TFN, suggesting N is supplied to canopies to maximize photosynthesis per unit leaf area. This tight coupling between LAI, N, and P in tallgrass prairie suggests a process of optimal allocation of N and P, wherein LAI remains similarly constrained by N and P despite differences in species composition, grazing, and canopy density
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
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- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
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- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Fitness Cost of Resistance to Bt Cotton Linked with Increased Gossypol Content in Pink Bollworm Larvae
- Author
- A Bravo
- Aaron J. Gassmann
- AF Janmaat
- AJ Gassmann
- AJ Gassmann
- B Raymond
- BE Tabashnik
- BE Tabashnik
- BE Tabashnik
- BE Tabashnik
- BE Tabashnik
- Bruce E. Tabashnik
- Christa Ellers-Kirk
- DM Higginson
- DS Falconer
- DW Crowder
- DW Onstad
- E Hill
- EG Midboe
- F Gould
- FL Ramsey
- G Sunilkumar
- Graham Head
- Guy Smagghe
- HM Graham
- JA Fabrick
- Jennifer L. Williams
- K Schlichting
- LJ Bird
- LJ Gahan
- LJ Gahan
- NP Storer
- P Bagla
- PL Adkinsson
- RD Stipanovic
- RG Orth
- RJ Hron
- Robert G. Orth
- S Downes
- S Morin
- S Morin
- TN Shaver
- WD Hutchison
- XJ Xu
- Y Carrière
- Y Carrière
- Y Carrière
- Y Carrière
- Y Carrière
- Y Carrière
- YB Mao
- Yves Carrière
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Fitness costs of resistance to Bacillus thuringiensis (Bt) crops occur in the absence of Bt toxins, when individuals with resistance alleles are less fit than individuals without resistance alleles. As costs of Bt resistance are common, refuges of non-Bt host plants can delay resistance not only by providing susceptible individuals to mate with resistant individuals, but also by selecting against resistance. Because costs typically vary across host plants, refuges with host plants that magnify costs or make them less recessive could enhance resistance management. Limited understanding of the physiological mechanisms causing fitness costs, however, hampers attempts to increase costs. In several major cotton pests including pink bollworm (Pectinophora gossypiella), resistance to Cry1Ac cotton is associated with mutations altering cadherin proteins that bind this toxin in susceptible larvae. Here we report that the concentration of gossypol, a cotton defensive chemical, was higher in pink bollworm larvae with cadherin resistance alleles than in larvae lacking such alleles. Adding gossypol to the larval diet decreased larval weight and survival, and increased the fitness cost affecting larval growth, but not survival. Across cadherin genotypes, the cost affecting larval growth increased as the gossypol concentration of larvae increased. These results suggest that increased accumulation of plant defensive chemicals may contribute to fitness costs associated with resistance to Bt toxins
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonelli S
- Antos J
- Anulli F
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- Apolle R
- Arabidze G
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- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- Arnaez O
- Arnault C
- Artamonov A
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- Arutinov D
- Asai S
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- Asman B
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- Atoian G
- Aubert B
- Auerbach B
- Auge E
- Augsten K
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- Avramidou R
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- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
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- Baker OK
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- Trzupek A
- Tsarouchas C
- Tseng JC-L
- Tsiakiris M
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsung J-W
- Tsuno S
- Tsybychev D
- Tua A
- Tuggle JM
- Turala M
- Turecek D
- Turlay E
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Typaldos D
- Tyrvainen H
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
- Unal G
- Underwood DG
- Undrus A
- Unel G
- Unno Y
- Urbaniec D
- Urkovsky E
- Urquijo P
- Urrejola P
- Usai G
- Uslenghi M
- Vacavant L
- Vacek V
- Vachon B
- Vahsen S
- Valderanis C
- Valenta J
- Valente P
- Valentinetti S
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
- van der Graaf H
- van der Kraaij E
- van der Poel E
- van der Ster D
- Van Eijk B
- van Eldik N
- van Gemmeren P
- van Kesteren Z
- van Vulpen I
- Vandelli W
- Vandoni G
- Vaniachine A
- Vankov P
- Vannucci F
- Vari R
- Varnes EW
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vegni G
- Veillet JJ
- Vellidis C
- Veloso F
- Veness R
- Veneziano S
- Ventura A
- Ventura D
- Ventura S
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vertogardov L
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
- Viegas FJTA
- Viehhauser GHA
- Viel S
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Viret S
- Virzi J
- Vitale A
- Vitells O
- Vivarelli I
- Vives Vaque F
- Vlachos S
- Vlasak M
- Vlasov N
- Vogel A
- Vokac P
- Volpi M
- Volpini G
- von der Schmitt H
- von Loeben J
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorobiev AP
- Vorwerk V
- Vos M
- Voss R
- Voss TT
- Vossebeld JH
- Vovenko AS
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wahlen H
- Wakabayashi J
- Walbersloh J
- Walch S
- Walder J
- Walker R
- Walkowiak W
- Wall R
- Waller P
- Wang C
- Wang H
- Wang J
- Wang JC
- Wang SM
- Warburton A
- Ward CP
- Warsinsky M
- Watkins PM
- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh AT
- Waugh BM
- Weber J
- Weber M
- Weber MS
- Weber P
- Weidberg AR
- Weingarten J
- Weiser C
- Wellenstein H
- Wells PS
- Wen M
- Wenaus T
- Wendler S
- Weng Z
- Wengler T
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Whalen K
- Wheeler-Ellis SJ
- Whitaker SP
- White A
- White MJ
- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicek F
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik LAM
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Willis W
- Willocq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wolter MW
- Wolters H
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wraight K
- Wright C
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wunstorf R
- Wynne BM
- Xaplanteris L
- Xella S
- Xie S
- Xie Y
- Xu C
- Xu D
- Xu G
- Yabsley B
- Yagci KD
- Yamada M
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang S
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao W-M
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zdrazil M
- Zeitnitz C
- Zeller M
- Zema PF
- Zemla A
- Zendler C
- Zenin AV
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- 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
Mutator dynamics in sexual and asexual experimental populations of yeast
- Author
- A Giraud
- AC Shaver
- AH Sturtevant
- AL Goldstein
- B Grimberg
- B Studamire
- C Zeyl
- CE Paquin
- CF Baer
- CF Gentile
- DA Thompson
- DM Ruderfer
- DM Wloch
- DW Hall
- E Alani
- EG Leigh
- EM Selva
- EM Selva
- EV Koonin
- F Baganz
- GT Marsischky
- HA Kuehne
- JA Hill
- JAGM de Visser
- JAGM de Visser
- JB André
- JF Crow
- JH Gillespie
- JJ Bull
- JP Gogarten
- JP Gogarten
- K Ishii
- L Chao
- LJ Johnson
- M Kimura
- M Kimura
- M Lynch
- M Saparbaev
- Matthew R Gazzara
- MD Rose
- N Sugawara
- P Gerrish
- P Sliwa
- Paul D Sniegowski
- PD Sniegowski
- PD Sniegowski
- PJ Gerrish
- PJ Keller
- R Greenberg
- RA Fisher
- RAG Reenan
- RD Gietz
- RE Lenski
- SB Joseph
- SR Chambers
- T Johnson
- T Johnson
- TT Kibota
- W Tröbner
- Yevgeniy Raynes
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>In asexual populations, mutators may be expected to hitchhike with associated beneficial mutations. In sexual populations, recombination is predicted to erode such associations, inhibiting mutator hitchhiking. To investigate the effect of recombination on mutators experimentally, we compared the frequency dynamics of a mutator allele (<it>msh2</it>Δ) in sexual and asexual populations of <it>Saccharomyces cerevisiae</it>.</p> <p>Results</p> <p>Mutator strains increased in frequency at the expense of wild-type strains in all asexual diploid populations, with some approaching fixation in 150 generations of propagation. Over the same period of time, mutators declined toward loss in all corresponding sexual diploid populations as well as in haploid populations propagated asexually.</p> <p>Conclusions</p> <p>We report the first experimental investigation of mutator dynamics in sexual populations. We show that a strong mutator quickly declines in sexual populations while hitchhiking to high frequency in asexual diploid populations, as predicted by theory. We also show that the <it>msh2Δ </it>mutator has a high and immediate realized cost that is alone sufficient to explain its decline in sexual populations. We postulate that this cost is indirect; namely, that it is due to a very high rate of recessive lethal or strongly deleterious mutation. However, we cannot rule out the possibility that <it>msh2</it>Δ also has unknown directly deleterious effects on fitness, and that these effects may differ between haploid asexual and sexual populations. Despite these reservations, our results prompt us to speculate that the short-term cost of highly deleterious recessive mutations can be as important as recombination in preventing mutator hitchhiking in sexual populations.</p
Neural Network Development in Late Adolescents during Observation of Risk-Taking Action
- Author
- A Bechara
- A Bechara
- A Buchweitz
- A Gamma
- A Hurtado
- A Pfefferbaum
- A Simmons
- A Terracciano
- AD Craig
- AD Craig
- AE Poropat
- Akiko Hida
- AL Reiss
- Alessio Avenanti
- AN McCoy
- AR Braun
- AR Damasio
- BA Vogt
- BM Newman
- BM Newman
- BW Haas
- BW Roberts
- C Farrer
- C Kobayashi
- C Lamm
- CD Spielberger
- CI Wright
- CI Wright
- CJ Price
- CS Monk
- D Jolliffe
- D Keltner
- DH Zald
- DL Johnson
- DR Addis
- DR Corfield
- E Erikson
- E Erikson
- E Tanaka
- EA Mayer
- EG Marston
- ER Sowell
- ER Sowell
- G Bush
- G Matthews
- G Rizzolatti
- GL Shulman
- H Boecker
- HD Critchley
- HE den Ouden
- HJ Eysenk
- HJ Eysenk
- HJ Eysenk
- I Dumontheil
- J Chumbley
- J Downar
- J Eccles
- J Okuda
- J Talairach
- JD Cohen
- JE Schulenberg
- JG Vaidya
- JH Pfeifer
- JJ Arnett
- JJ Arnett
- JM Kilner
- JM Pearson
- JN Giedd
- JN Giedd
- JR Chumbley
- JS Feinstein
- Jun Umezawa
- JW Smoller
- K Beesdo
- K Fukuda
- K Okonogi
- K Omura
- Kazuo Mishima
- KE Watkins
- KJ Preacher
- KJ Preacher
- KK Watson
- KN Ochsner
- L Carr
- L Steinberg
- L Tanum
- LQ Uddin
- M Azmitia
- M Sollberger
- MB Stein
- ME Raichle
- MH De Moor
- Minori Enomoto
- Miyuki Tamura
- MJ Mason
- MK Johnson
- ML Phillips
- MP Paulus
- MP Paulus
- MS Hanby
- MS Harper
- N Davis
- N Gogtay
- NF Dronkers
- O Ludtke
- OJ Bienvenu
- OJ Bienvenu
- OP John
- P Damier
- P Damier
- P Jylha
- P Shaver
- PE Shrout
- PG Williams
- PT Costa
- PT Fox
- PW Burgess
- R Lieb
- R Lieb
- RC Oldfield
- RD Goodwin
- RJ Maddock
- RM Baron
- RR McCrae
- RW Blum
- S Berthoz
- S Brown
- S Burnett
- S Iwawaki
- S Tsujimoto
- SD Forman
- SE French
- SE Tabachnik
- SH Kim
- Shigekazu Higuchi
- SJ Blakemore
- SJ Blakemore
- SJT Branje
- SL Rauch
- T Butler
- T Canli
- T Mizuguchi
- T Paus
- TF Farrow
- TM Lee
- WW Zung
- Y Cheng
- Y Moriguchi
- Y Sakurai
- Yoshiya Moriguchi
- Publication venue
- Public Library of Science
- Publication date
- 29/06/2012
- Field of study
Emotional maturity and social awareness are important for adolescents, particularly college students beginning to face the challenges and risks of the adult world. However, there has been relatively little research into personality maturation and psychological development during late adolescence and the neural changes underlying this development. We investigated the correlation between psychological properties (neuroticism, extraversion, anxiety, and depression) and age among late adolescents (n = 25, from 18 years and 1 month to 22 years and 8 months). The results revealed that late adolescents became less neurotic, less anxious, less depressive and more extraverted as they aged. Participants then observed video clips depicting hand movements with and without a risk of harm (risk-taking or safe actions) during functional magnetic resonance imaging (fMRI). The results revealed that risk-taking actions elicited significantly stronger activation in the bilateral inferior parietal lobule, temporal visual regions (superior/middle temporal areas), and parieto-occipital visual areas (cuneus, middle occipital gyri, precuneus). We found positive correlations of age and extraversion with neural activation in the insula, middle temporal gyrus, lingual gyrus, and precuneus. We also found a negative correlation of age and anxiety with activation in the angular gyrus, precentral gyrus, and red nucleus/substantia nigra. Moreover, we found that insula activation mediated the relationship between age and extraversion. Overall, our results indicate that late adolescents become less anxious and more extraverted with age, a process involving functional neural changes in brain networks related to social cognition and emotional processing. The possible neural mechanisms of psychological and social maturation during late adolescence are discussed
Human and machine validation of 14 databases of dynamic facial expressions
- Author
- B Parkinson
- BJ Matuszewski
- D Bates
- D Dupré
- D Küster
- Dennis Küster
- E Goeleven
- E Krumhuber
- E Krumhuber
- E Siedlecka
- EG Krumhuber
- EG Krumhuber
- Eva G. Krumhuber
- G Sandbach
- H Aviezer
- H Yu
- HL Wagner
- iMotions
- J Piironen
- JA Russell
- K Greenaway
- L Zhang
- LF Barrett
- LF Barrett
- LF Barrett
- Lina Skora
- LK Kuhn
- M Beringer
- M Biehl
- M Kamachi
- M Maringer
- MG Calvo
- MG Calvo
- MG Frank
- MH Kayyal
- MT Motley
- N Yitzhak
- O Golan
- O Zinchenko
- P Ekman
- P Ekman
- P Shaver
- R Calvo
- RJ Morecraft
- S Namba
- S Stöckli
- S Van Erp
- Shushi Namba
- T Skiendziel
- TSH Wingenbach
- U Hess
- W Sato
- W Sato
- WE Rinn
- X Zhang
- Z Ambadar
- Z Zeng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 17/08/2020
- Field of study
With a shift in interest toward dynamic expressions, numerous corpora of dynamic facial stimuli have been developed over the past two decades. The present research aimed to test existing sets of dynamic facial expressions (published between 2000 and 2015) in a cross-corpus validation effort. For this, 14 dynamic databases were selected that featured facial expressions of the basic six emotions (anger, disgust, fear, happiness, sadness, surprise) in posed or spontaneous form. In Study 1, a subset of stimuli from each database (N = 162) were presented to human observers and machine analysis, yielding considerable variance in emotion recognition performance across the databases. Classification accuracy further varied with perceived intensity and naturalness of the displays, with posed expressions being judged more accurately and as intense, but less natural compared to spontaneous ones. Study 2 aimed for a full validation of the 14 databases by subjecting the entire stimulus set (N = 3812) to machine analysis. A FACS-based Action Unit (AU) analysis revealed that facial AU configurations were more prototypical in posed than spontaneous expressions. The prototypicality of an expression in turn predicted emotion classification accuracy, with higher performance observed for more prototypical facial behavior. Furthermore, technical features of each database (i.e., duration, face box size, head rotation, and motion) had a significant impact on recognition accuracy. Together, the findings suggest that existing databases vary in their ability to signal specific emotions, thereby facing a trade-off between realism and ecological validity on the one end, and expression uniformity and comparability on the other
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Alam MA
- Alam MS
- 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
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- 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
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncellia A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkovaa L
- Batley JR
- Battaglia A
- Battistin M
- Battistonia G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherlea R
- Bechtle R
- Beck HP
- Beckingham M
- Becks KH
- Beddallc A
- Beddallc AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagambaa L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekrouna D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertina A
- Bertinelli F
- Bertoluccia F
- Besanaa MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Biancoa M
- Biebel O
- Bieniek SR
- Bierwagen K
- Biesiada J
- Bigliettia M
- Bilokon H
- Bindia M
- Binet S
- Bingulc A
- Binia C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazeka T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohma C
- Boisvert V
- Bold T
- Boldeaa V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovica I
- Borronia S
- Bos K
- Boscherinia D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcicb I
- Bracinik J
- Braem A
- Branchinia P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggia F
- Bromberg C
- Brooijmans G
- Brooksb WK
- Brown G
- Brown H
- Bruckman de Renstrom PA
- Bruncko D
- Bruneliere R
- Brunet S
- Brunia A
- Brunia G
- Bruschia M
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Budaa SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Byatt T
- Cabrera Urban S
- Caforioa D
- Cakir IT
- Cakira O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Calobaa LP
- Caloia R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghia M
- Cameron D
- Camillocci ES
- Campana S
- Campanelli M
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- Yamaguchi H
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- Yilmaz M
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- Zhang X
- Zhang Z
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- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Food security, climate change, and sustainable land management. A review
- Author
- A Hamid
- A Woodfine
- AA Agboola
- AA Agboola
- B Govaerts
- B Govaerts
- C Acharya
- C Dutilly-Diane
- C Thierfelder
- CC Mann
- CL Acharya
- D Garrity
- D Garrity
- D Tilman
- D Ussiri
- DR Huggins
- E Roose
- E Scopel
- E Scopel
- E Scopel
- EG Gregorich
- FAO
- FAO
- FR Leiva
- G Arnqvist
- G Branca
- G Branca
- G Schroth
- G Uhlen
- GE Osuji
- GE Shively
- Giacomo Branca
- I Vallis
- IAASTD
- J Ellis-Jones
- J Gurevitch
- J Henao
- J Rockström
- J Rockström
- J Rockström
- J Silvertown
- JE Kimmelshue
- JM Antle
- JN Pretty
- JN Pretty
- JN Pretty
- K Paustian
- K Vohland
- KE Giller
- KG Cassman
- KR Olson
- L Ringius
- L Soto-Pinto
- LCG Barros
- LE Drinkwater
- Leslie Lipper
- LV Verchot
- M Arshad
- M Kassie
- MA Saleen
- Maria Christina Jolejole
- N Hatibu
- N Scialabba
- Nancy McCarthy
- O Erenstein
- O Erenstein
- O Palm
- P Kaumbutho
- P Lavelle
- P Lavelle
- P Sanchez
- P Tschakert
- P Unger
- PK Sharma
- PZ Matata
- R Bhatt
- R Hine
- R Lal
- R Lal
- R Lal
- R Lal
- R Lal
- R Lal
- R Lal
- R Lal
- R Shetto
- R Thomas
- RA Nelson
- S Edwards
- S Franzel
- SN Ngigi
- TM Shaver
- UNFPA
- W Critchley
- WD Sakala
- World Bank
- Y Pan
- YX Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for the standard model Higgs boson in the diphoton decay channel with 4.9fb -1 of pp collision data at √s=7TeV with atlas
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- Abbott B
- Abdallah J
- Abdel Khalek S
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- Akiyama A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
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- Allbrooke BMM
- Allport PP
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- Chernyatin V
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- Cuhadar Donszelmann T
- Curatolo M
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- Czirr H
- Czodrowski P
- Czyczula Z
- Côté D
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- Zhemchugov A
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- Åkesson TPA
- Åsman B
- Publication venue
- Publication date
- 01/01/2012
- Field of study
A search for the standard model Higgs boson is performed in the diphoton decay channel. The data used correspond to an integrated luminosity of 4.9 fb-1 collected with the ATLAS detector at the Large Hadron Collider in proton-proton collisions at a center-of-mass energy of √s=7 TeV. In the diphoton mass range 110–150 GeV, the largest excess with respect to the background-only hypothesis is observed at 126.5 GeV, with a local significance of 2.8 standard deviations. Taking the look-elsewhere effect into account in the range 110–150 GeV, this significance becomes 1.5 standard deviations. The standard model Higgs boson is excluded at 95% confidence level in the mass ranges of 113–115 GeV and 134.5–136 GeV
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