1,087 research outputs found
The achievement of food and nutrition security in South Asia is deeply gendered
- Author
- A Cornwall
- AC Bellows
- AC Bellows
- B Agarwal
- B Harriss-White
- D Elson
- D Johnston
- E Cavatorta
- EC Lentz
- G Djurfeldt
- India State-level Disease Burden Initiative Collaborators.
- J Usta
- KW Springer
- LC Smith
- LK Ackerson
- LM Harris
- MM Chilton
- MM Chilton
- MS Swaminathan
- N Rao
- N Rao
- N Rao
- N Rao
- N Rao
- N Rao
- R Chattopadhyay
- RK Gope
- S Jones
- S Kadiyala
- V Prasad
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/04/2020
- Field of study
Women form an integral part of the agricultural sector, and in much of South Asia women make up a majority of the agricultural workforce, often compelled to work in order to meet their families’ basic needs. While their contributions are recognised as central to the food and nutrition security of households and communities, their work is not recognized or supported adequately by public policy and social institutions. Women continue to face inequality across key development indicators including health, education, and nutrition; discriminatory laws; and high levels of precarity in terms of income, employment conditions, safety and wellbeing. Social structures that promote gender inequality and inhibit the agency of women contribute to the South Asian enigma – the persistence of undernutrition despite economic growth – and must be addressed to achieve food and nutrition security
Влияние интенсивности механической активации на структуру гексагонального нитрида бора
- Author
- A Paolis
- A Petit
- A-CM Brasileiro
- AM Berry
- AM Birot
- B Sougoufara
- BC Mullin
- D Tepfer
- D Tepfer
- DL Rockwood
- E Davioud
- F Blondon
- FA Hassan
- FF White
- G Vancanneyt
- GW Bolton
- HG Diem
- J Koplow
- J Mackay
- J Sambrook
- JO Dawson
- JP Nitsch
- JW Hanover
- K Huss-Danell
- K Weising
- LF Benoit
- LW Moore
- M Bevan
- M Phelep
- M Tepfer
- M-F Michel
- MA Savka
- MD Chilton
- MLM Osta
- MM Abo
- National Research Council
- P Mazodier
- PL Schuerman
- RA Jefferson
- SL Rose
- T Christensen
- T Maniatis
- T Murashige
- YC Chang
- Publication venue
- Інститут надтвердих матеріалів ім. В.М. Бакуля НАН України
- Publication date
- 01/01/1994
- Field of study
Изучено влияние интенсивности механической активации на микроструктуру и свойства гексагонального нитрида бора (hBN).Вивчено вплив інтенсивності механічної активації на мікроструктуру і властивості гексагонального нітриду бору (hBN).The mechanical activation intensity effect on the microstructure and properties of hexagonal boron nitride (hBN) has been studied
Arsenic trioxide, a potent inhibitor of NF-κB, abrogates allergen-induced airway hyperresponsiveness and inflammation
- Author
- A Hoffmann
- A Hu
- A Kumar
- A Trautmann
- BN Kang
- BN Melgert
- C Boxall
- CK Wong
- DT Umetsu
- F Bureau
- F Chen
- G Yang
- H Hakonarson
- H Hakonarson
- J Das
- JN Kline
- JW Christman
- K EI Bakkouri
- K Nishikubo
- L Hart
- L Yang
- LF Zhou
- LF Zhou
- LF Zhou
- LF Zhou
- ME Poynter
- MM Grunstein
- N Miyahara
- PM Chilton
- PZ Zheng
- RJ Carmody
- RJ Ulevitch
- S Fujihara
- S Kierstein
- S Mathas
- WP Xie
- WW Busse
- X Shan
- XF Cui
- Y Chvatchko
- Y Yamamoto
- Z Zhu
- Publication venue
- BioMed Central
- Publication date
- 01/12/2006
- Field of study
BACKGROUND: Overactivation of nuclear factor κB (NF-κB) orchestrates airway eosinophilia, but does not dampen airway hyperresponsiveness in asthma. NF-κB repression by arsenic trioxide (As(2)O(3)) contributes to apoptosis of eosinophils (EOS) in airways. Here we provide evidence that As(2)O(3 )abrogates allergen (OVA)-induced airway eosinophilia by modulating the expression of IκBα, an NF-κB inhibitory protein, and decreases the airway hyperresponsiveness. METHODS: Using a murine model of asthma, the airway hyperresponsiveness was conducted by barometric whole-body plethysmography. Airway eosinophilia, OVA-specific IgE in serum, and chemokine eotaxin and RANTES (regulated upon activation, normal T cell expressed and secreted) in bronchoalveolar lavage fluid were measured by lung histology, Diff-Quick staining, and ELISA. Chemokine-induced EOS chemotactic activity was evaluated using EOS chemotaxis assay. Electrophoretic mobility shift assay and Western blot analysis were performed to assess pulmonary NF-κB activation and IκBα expression, respectively. RESULTS: As(2)O(3 )attenuated the allergen-induced serum IgE, chemokine expression of eotaxin and RANTES, and the EOS recruitment in bronchoalveolar lavage fluid, which is associated with an increased IκBα expression as well as a decreased NF-κB activation. Also, As(2)O(3 )suppressed the chemotaxis of EOS dose-dependently in vitro. Additionally, As(2)O(3 )significantly ameliorated the allergen-driven airway hyperresponsiveness, the cardinal feature underlying asthma. CONCLUSION: These findings demonstrate an essential role of NF-κB in airway eosinophilia, and illustrate a potential dissociation between airway inflammation and hyperresponsiveness. As(2)O(3 )likely exerts its broad anti-inflammatory effects by suppression of NF-κB activation through augmentation of IκBα expression in asthma
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Yang
- Yang
- Yang
- Yao
- Yeh
- Yi
- Yoh
- Yorita
- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
Measurement of the Forward-Backward Asymmetry in the B -> K(*) mu+ mu- Decay and First Observation of the Bs -> phi mu+ mu- Decay
- Author
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- Yilmaz Y
- Yoh J
- Yoo HD
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- Zanetti A
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- Zatserklyaniy A
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- Zhukova V
- Ziegler J
- Zielinski M
- Zucchelli SZucchelli Sira D
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We reconstruct the rare decays B+→K+μ+μ−, B0→K∗(892)0μ+μ−, and Bs0→ϕ(1020)μ+μ− in a data sample
corresponding to 4.4fb−1 collected in ppˉ collisions at
s=1.96TeV by the CDF II detector at the Fermilab Tevatron
Collider. Using 121±16 B+→K+μ+μ− and 101±12 B0→K∗0μ+μ− decays we report the branching ratios. In addition, we report
the measurement of the differential branching ratio and the muon
forward-backward asymmetry in the B+ and B0 decay modes, and the K∗0
longitudinal polarization in the B0 decay mode with respect to the squared
dimuon mass. These are consistent with the theoretical prediction from the
standard model, and most recent determinations from other experiments and of
comparable accuracy. We also report the first observation of the Bs0→ϕμ+μ−decayandmeasureitsbranchingratio{\mathcal{B}}(B^0_s \to
\phi\mu^+\mu^-) = [1.44 \pm 0.33 \pm 0.46] \times 10^{-6}using27 \pm 6signalevents.ThisiscurrentlythemostrareB^0_s$ decay observed.Comment: 7 pages, 2 figures, 3 tables. Submitted to Phys. Rev. Let
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Zachariadou A
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- Zelepoukine S
- Zeuner WD
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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
Measurements of the properties of Lambda_c(2595), Lambda_c(2625), Sigma_c(2455), and Sigma_c(2520) baryons
- Author
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- McIntyre P
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- Medvedeva T
- Mehta A
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- Zucchelli S Zucchelli Slli Sira D
- Zucchelli SZanetti A
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
We report measurements of the resonance properties of Lambda_c(2595)+ and
Lambda_c(2625)+ baryons in their decays to Lambda_c+ pi+ pi- as well as
Sigma_c(2455)++,0 and Sigma_c(2520)++,0 baryons in their decays to Lambda_c+
pi+/- final states. These measurements are performed using data corresponding
to 5.2/fb of integrated luminosity from ppbar collisions at sqrt(s) = 1.96 TeV,
collected with the CDF II detector at the Fermilab Tevatron. Exploiting the
largest available charmed baryon sample, we measure masses and decay widths
with uncertainties comparable to the world averages for Sigma_c states, and
significantly smaller uncertainties than the world averages for excited
Lambda_c+ states.Comment: added one reference and one table, changed order of figures, 17
pages, 15 figure
Search for a New Heavy Gauge Boson Wprime with Electron + missing ET Event Signature in ppbar collisions at sqrt(s)=1.96 TeV
- Author
- Aaltonen T
- Abdullin S
- Acosta D
- Acosta JG
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- Bauerdick LAT
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- McIntyre P
- McNulty R
- Medvedeva T
- Mehta A
- Mehtala P
- Meier M
- Mendez H
- Menzione A
- Merkel P
- Merlo JP
- Mermerkaya H
- Mesa D
- Mesropian C
- Mestvirishvili A
- Miao T
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- Mietlicki D
- Mignerey AC
- Miller DH
- Miner DC
- Mishra K
- Mitra A
- Mitselmakher G
- Miyake H
- Moed S
- Moeller A
- Moggi N
- Mondragon MN
- Moon CS
- Mooney M
- Moore R
- Morales J
- Morello MJ
- Morlock J
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- Mott A
- Mrenna S
- Mukherjee A
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- Muniz L
- Murat P
- Murray M
- Musienko Y
- Mussini M
- Nachtman J
- Nachtman J
- Nagai Y
- Naganoma J
- Nahn S
- Nakano I
- Napier A
- Nauenberg U
- Nett J
- Neu C
- Neubauer MS
- Neumeister N
- Newman HB
- Newman-Holmes C
- Newsom CR
- Nielsen J
- Nodulman L
- Noonan D
- Norbeck E
- Norniella O
- Nurse E
- O'Brien C
- O'Dell V
- Oakes L
- Odell N
- Ofierzynski RA
- Oh SH
- Oh YD
- Oksuzian I
- Okusawa T
- Oliveros S
- Olsen J
- Olson J
- Onel Y
- Orava R
- Orbak
- Ortolan L
- Ozok F
- Padley BP
- Pagliarone C
- Pakhotin Y
- Palencia E
- Papadimitriou V
- Paramonov AA
- Parashar N
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- Pauletta G
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- Paulini M
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- Paus C
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- Pellett DE
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- Perera L
- Petterson M
- Phillips TJ
- Piacentino G
- Pianori E
- Pilot J
- Piroue P
- Pitts K
- Plager C
- Pollack B
- Pondrom L
- Popescu S
- Pordes R
- Potamianos K
- Potamianos K
- Poukhov O
- Pozdnyakov A
- Prescott C
- Prokofyev O
- Prokoshin F
- Pronko A
- Prosper H
- Ptohos F
- Pueschel E
- Puigh D
- Punzi G
- Pursley J
- Radicci V
- Rahaman A
- Rahmat R
- Ralich R
- Ramakrishnan V
- Ranjan N
- Rappoccio S
- Redjimi R
- Redondo I
- Rekovic V
- Remington R
- Renton P
- Rescigno M
- Reucroft S
- Riley D
- Rimondi F
- Ristori L
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- Rodrigo T
- Rodriguez JL
- Rodriguez T
- Rogan C
- Rogers E
- Roland C
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- Rolli S
- Roser R
- Rossato K
- Rossi M
- Rubbo F
- Ruchti R
- Rudolph M
- Ruffini F
- Ruiz A
- Rumerio P
- Rusack R
- Russ J
- Russ J
- Rusu V
- Ryd A
- Saelim M
- Safonov A
- Saka H
- Sakumoto WK
- Sanders DA
- Sanders S
- Santanastasio F
- Santi L
- Saoulidou N
- Sartori L
- Sasseville M
- Sato K
- Saveliev V
- Savoy-Navarro A
- Schlabach P
- Schmidt A
- Schmidt EE
- Schmidt MP
- Schmitt M
- Schmitt M
- Schmitt M
- Schwarz T
- Scodellaro L
- Scribano A
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- Zucchelli Slli Sira D
- Zucchelli SYun JC
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2010
- Field of study
We present a search for a new heavy charged vector boson W′ decaying
to an electron-neutrino pair in ppˉ collisions at a center-of-mass
energy of 1.96\unit{TeV}. The data were collected with the CDF II detector
and correspond to an integrated luminosity of 5.3\unit{fb}^{-1}. No
significant excess above the standard model expectation is observed and we set
upper limits on σ⋅B(W′→eν). Assuming standard
model couplings to fermions and the neutrino from the W′ boson decay to
be light, we exclude a W′ boson with mass less than
1.12\unit{TeV/}c^2 at the 95\unit{%} confidence level.Comment: 7 pages, 2 figures Submitted to PR
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abbott B
- Abdallah J
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- Abdesselam A
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- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zinonos Z
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- Zitoun R
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- 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
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Abramowicz H
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- Acharya BS
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- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warrack N
- Washbrook A
- Watson AT
- Watson MF
- Watts G
- Waugh BM
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang Y
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
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