64 research outputs found
Cerebral pressure passivity in newborns with encephalopathy undergoing therapeutic hypothermia
- Publication venue
- Health Sciences Research Commons
- Publication date
- 01/01/2014
- Field of study
We extended our recent modification of the power spectral estimation approach to quantify spectral coherence. We tested both the standard and the modified approaches on simulated data, which showed that the modified approach was highly specific and sensitive to the coupling introduced in the simulation while the standard approach lacked these features. We also applied the modified and standard approaches to quantify the pressure passivity in 4 infants receiving therapeutic hypothermia. This was done by measuring the coupling between continuous cerebral hemoglobin differences and mean arterial blood pressure. Our results showed that the modified approach identified a lower pressure passivity index (PPI, percent time the coherence was above a predefined threshold) than the standard approach (P = 0.0027)
Coagulopathy in newborns with hypoxic ischemic encephalopathy (HIE) treated with therapeutic hypothermia: A retrospective case-control study
- Publication venue
- Health Sciences Research Commons
- Publication date
- 01/01/2014
- Field of study
Background
Newborns with hypoxic ischemic encephalopathy (HIE) are at risk for coagulopathy due to systemic oxygen deprivation. Additionally, therapeutic hypothermia (TH) slows enzymatic activity of the coagulation cascade, leading to constitutive prolongation of routinely assessed coagulation studies. The level of laboratory abnormality that predicts bleeding is unclear, leading to varying transfusion therapy practices. Methods
HIE infants treated with TH between 2008â2012 were included in this retrospective study. Initial, minimum (min) and maximum (max) values of International Normalized Ratio (INR), activated partial thromboplastin time (aPTT), fibrinogen (Fib) and platelet (PLT) count (measured twice daily during TH) were collected. Bleeding was defined as clinically significant if associated with 1) decreased hemoglobin (Hb) by 2 g/dL in 24 hours, 2) transfusion of blood products for hemostasis, or 3) involvement of a critical organ system. Laboratory data between the bleeding group (BG) and non-bleeding group (NBG) were compared. Variables that differed significantly between groups were evaluated with Receiver Operating Characteristic Curve (ROC) analyses to determine cut-points to predict bleeding. Results
Laboratory and bleeding data were collected from a total of 76 HIE infants with a mean (±SD) birthweight of 3.34â±â0.67 kg and gestational age of 38.6â±â1.9 wks. BG included 41 infants. Bleeding sites were intracranial (nâ=â13), gastrointestinal (nâ=â19), pulmonary (nâ=â18), hematuria (nâ=â11) or other (nâ=â1). There were no differences between BG and NBG in baseline characteristics (pâ\u3eâ0.05). Both groups demonstrated INR and aPTT values beyond the acceptable reference ranges utilized for full tem newborns. BG had higher initial and max INR, initial aPTT, and lower min PLT and min Fib compared to NBG. ROC analyses revealed that platelet count \u3c130 \u3eĂ 109/L, fib level2 discriminated BG from NBG. Conclusions
Laboratory evidence of coagulopathy is universal in HIE babies undergoing TH. Transfusion strategies to maintain PLT counts \u3e130 Ă 109/L, fib level \u3e1.5 g/L, and INRpopulation
Neonatal neurobehavioral abnormalities and MRI brain injury in encephalopathic newborns treated with hypothermia
- Author
- Publication venue
- Health Sciences Research Commons
- Publication date
- 01/09/2013
- Field of study
Background Neonatal Encephalopathy (NE) is a prominent cause of infant mortality and neurodevelopmental disability. Hypothermia is an effective neuroprotective therapy for newborns with encephalopathy. Post-hypothermia functionalâanatomical correlation between neonatal neurobehavioral abnormalities and brain injury findings on MRI in encephalopathic newborns has not been previously described. Aim To evaluate the relationship between neonatal neurobehavioral abnormalities and brain injury on magnetic resonance imaging (MRI) in encephalopathic newborns treated with therapeutic hypothermia. Study design Neonates with hypoxic ischemic encephalopathy (HIE) referred for therapeutic hypothermia were prospectively enrolled in this observational study. Neurobehavioral functioning was assessed with the NICU network neurobehavioral scale (NNNS) performed at target age 14 days. Brain injury was assessed by MRI at target age 7â10 days. NNNS scores were compared between infants with and without severe MRI injury. Subjects & outcome measures Sixty-eight term newborns (62% males) with moderate to severe encephalopathy underwent MRI at median 8 days (range 5â16) and NNNS at median 12 days of life (range 5â20). Fifteen (22%) had severe injury on MRI. Results Overall Total Motor Abnormality Score and individual summary scores for Non-optimal Reflexes and Asymmetry were higher, while Total NNNS Z-score across cognitive/behavioral domains was lower (reflecting poorer performance) in infants with severe MRI injury compared to those without (p \u3c 0.05). Conclusions Neonatal neurobehavioral abnormalities identified by the NNNS are associated with MRI brain injury in encephalopathic newborns post-hypothermia. The NNNS can provide an early functional assessment of structural brain injury in newborns, which may guide rehabilitative therapies in infants after perinatal brain injury
Study of the reaction e^{+}e^{-} -->J/psi\pi^{+}\pi^{-} via initial-state radiation at BaBar
- Author
- Adametz A
- Adye T
- Ahmed H
- Akar S
- Alam MS
- Albert J
- Andreassen R
- Angelini C
- Anulli F
- Arlen T.
- Arnaud N
- Asgeirsson DJ
- Aston D
- Atmacan H
- Aune T.
- Ayad R
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Bard DJ
- Barlow RJ
- Bartoldus R
- Batignani G
- Behera PK
- Behn E
- Beilicke M.
- Bellis M
- Ben-Haim E
- Benbow W.
- Benitez JF
- Bernard D
- Bernlochner FU
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhuyan B
- Bianchi F
- Biasini M
- Biassoni P
- Blinov VE
- Bloom PC
- Bomben M
- Bondioli M
- Bonneaud GR
- Bouvier A.
- Bozzi C
- Bradbury S. M.
- Brau J
- Briand H
- Brown DN
- Brown DN
- Buckley J. H.
- Bugaev V.
- Bunger C
- Burchat PR
- Buzykaev AR
- Byrum K.
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Cannon A.
- Cara M.
- Carpinelli M
- Cartaro C
- Casadio C.
- Casarosa G
- Cenci R
- Cervelli A
- Cesarini A.
- Chao DS
- Chauveau J
- Chavez CA
- Cheaib R
- Chen C
- Cheng CH
- Cheung C. C.
- Choi HHF
- Cibinetto G
- Ciupik L.
- Clark PJ
- Cochran J
- Coleman JP
- Connolly M. P.
- Contri R
- Convery MR
- Cowan G
- Cowan R
- Cremaldi L
- Cui W.
- Dallapiccola C
- Dasu S
- Dauncey PD
- Davier M
- Davies F.
- Davis CL
- de Almeida U. Barres
- de Monchenault GH
- De Nardo G
- de Sangro R
- Denig AG
- Derkach D
- Di Lodovico F
- Dickherber R.
- Doi A.
- Dorfan J
- Druzhinin VP
- Dubois-Felsmann GP
- Dujmic D
- Duke C.
- Dunwoodie W
- Ebert M
- Echenard B
- Edwards AJ
- Eigen G
- Eisner AM
- Emery S
- Ernst JA
- Errando M.
- Faccini R
- Falcone A.
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finley J. P.
- Finnegan G.
- Finocchiaro G
- Fioravanti E
- Flood KT
- Ford WT
- Forti F
- Fortson L.
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Furniss A.
- Gabareen AM
- Gabathuler E
- Gagliardi N
- Galante N.
- Gall D.
- Gamba D
- Gary JW
- Garzia I
- Gaspero M
- Gaz A
- Gershon TJ
- Gioi LL
- Giorgi MA
- Giovannini G.
- Giroletti M.
- Godambe S.
- Godang R
- Golubev VB
- Gorodeisky R
- Gradl W
- Graham MT
- Grauges E
- Grenier P
- Griessinger K
- Griffin S.
- Gritsan AV
- Grosdidier G
- Grube J.
- Grunberg O
- Guido E
- Guo ZJ
- Guttman N
- Gyuk G.
- Hada K.
- Hafner A
- Hamilton B
- Hamon O
- Hanna D.
- Hardee P.
- Harris D. E.
- Harrison PF
- Hartmann T
- Hast C
- Hearty C
- Hitlin DG
- Holder J.
- Hong TM
- Honscheid K
- Huan H.
- Huard Z
- Hui C. M.
- Hutchcroft DE
- Innes WR
- Izen JM
- Jackson G
- Jawahery A
- Jessop CP
- Junor W.
- Kaaret P.
- Karlsson N.
- Kass R
- Kelsey MH
- Kerth LT
- Kertzman M.
- Khan A
- Khassen Y.
- Kieda D.
- Kim P
- King GJ
- Kino M.
- Kirkby D
- Koch H
- Kocian ML
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kravchenko EA
- Krawczynski H.
- Krennrich F.
- Kroeger R
- Kroseberg J
- Lacker HM
- Lafferty GD
- Lanceri L
- Lang M. J.
- Lange DJ
- Lankford AJ
- Latham TE
- Le Diberder F
- LeBohec S.
- Leddig T
- Lee CL
- Lee N. P.
- Lees JP
- Leith DWGS
- Leruste P
- Lewczuk MJ
- Lewis P
- Lindemann D
- Lindquist B
- Liu F
- Lo Vetere M
- Lockman WS
- Long O
- LoSecco JM
- Lou XC
- Lueck T
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Ly C.
- Lynch G
- Lynch HL
- MacFarlane DB
- Madrid J.
- Maier G.
- Malaescu B
- Mallik U
- Mandelkern M
- Manoni E
- Marchiori G
- Margoni M
- Martinelli M
- Martinez AJ
- Martinez-Vidal F
- Massaro F.
- Mattison TS
- Mazzoni MA
- McArthur S.
- McCann A.
- McConville W.
- McKenna JA
- Meadows BT
- Meyer WT
- Miyashita TS
- Monge MR
- Monorchio D
- Morandin M
- Moriarty P.
- Morii M
- Mukherjee R.
- Muller DR
- Mundell C. G.
- Munerato M
- Nagai H.
- Nauenberg U
- Neal H
- Negrini M
- Nelson S
- Neri N
- Nguyen X
- Nugent IM
- Nunez P. D.
- Oberhof B
- Ocariz J
- Olaiya EO
- Olsen J
- Ong R. A.
- Ongmongkolkul P
- Onorato G
- Onuchin AP
- Orr M.
- Otte A. N.
- Oyanguren A
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Paoloni E
- Park N.
- Park W
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pegna DL
- Peimer DR
- Perez A
- Perkins J. S.
- Perl M
- Perlman E. S.
- Peruzzi IM
- Piccolo M
- Pichel A.
- Piemontese L
- Piredda G
- Playfer S
- Pohl M.
- Poireau V
- Porter FC
- Posocco M
- Prasad V
- Prell S
- Prencipe E
- Prepost R
- Prokoph H.
- Puccio EMT
- Pulliam T
- Purohit MV
- Ragan K.
- Rakitin AY
- Rama M
- Randle-Conde A
- Ratcliff BN
- Raven G
- Reyes L. C.
- Reynolds P. T.
- Richman JD
- Ritchie JL
- Rizzo G
- Roache E.
- Roberts DA
- Robertson SH
- Robutti E
- Roney JM
- Roodman A
- Rose H. J.
- Rossi A
- Rotondo M
- Roudeau P
- Rubin AE
- Ruland AM
- Ruppel J.
- Sacco R
- Salnikov AA
- Santoro V
- Schindler RH
- Schroder H
- Schroeder T
- Schroedter M.
- Schubert KR
- Schumm BA
- Schune MH
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Sembroski G. H.
- Sentuerk G. D.
- Serednyakov SI
- Sevilla MF
- Sigamani M
- Sillanpaa A.
- Simard M
- Simi G
- Simonetto F
- Sinev NB
- Sitarek J.
- Sitt S
- Skovpen YI
- Smith AJS
- Smith JG
- Snyder A
- Sobczynska D.
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Sonnek P
- Spaan B
- Spanier F.
- Spanier SM
- Spiro S.
- Stamerra A.
- Steele I. A.
- Steinke B.
- Stocchi A
- Storz J.
- Stracka S
- Strah N.
- Stroili R
- Strom D
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sun L
- Suric T.
- Takalo L.
- Takami H.
- Taras P
- Tasneem N
- Tavecchio F.
- Telezhinsky I.
- Telnov AV
- Temnikov P.
- Terzic T.
- Tescaro D.
- Teshima M.
- Tesic G.
- Theiling M.
- Thibadeau S.
- Thom M.
- Tibolla O.
- Tico JG
- Tisserand V
- Todyshev KY
- Toki WH
- Torrence E
- Torres D. F.
- Touramanis C
- Treves A.
- Uwer U
- Va'vra J
- Vankov H.
- Varlotta A.
- Vasseur G
- Vassiliev V. V.
- Verderi M
- Vitale L
- Vitug GM
- Vivier M.
- Vogler P.
- Voss C
- Wagner AP
- Wagner R. M.
- Wagner SR
- Wakely S. P.
- Waldi R
- Walker R. C.
- Walsh JJ
- Wang WF
- Weekes T. C.
- Weitzel Q.
- West CA
- White RM
- Williams D. A.
- Wilson FF
- Wilson JR
- Wisniewski WJ
- Wittgen M
- Wood D. L.
- Wormser G
- Wray BC
- Wright DH
- Wright DM
- Wu SLL S. N.
- Wulsin HW
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- Young CC
- Yushkov AN
- Zabalza V.
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- Zandanel F.
- Zanin R.
- Ziegler V
- Zitzer B.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We study the process e+eââJ/ÏÏ+Ïâ with
initial-state-radiation events produced at the PEP-II asymmetric-energy
collider. The data were recorded with the BaBar detector at center-of-mass
energies 10.58 and 10.54 GeV, and correspond to an integrated luminosity of 454
fbâ1. We investigate the J/ÏÏ+Ïâ mass
distribution in the region from 3.5 to 5.5 GeV/c2. Below 3.7
GeV/c2 the Ï(2S) signal dominates, and above 4
GeV/c2 there is a significant peak due to the Y(4260). A fit to
the data in the range 3.74 -- 5.50 GeV/c2 yields a mass value
4244±5 (stat) ±4 (syst)MeV/c2 and a width value 114â15+16â (stat)±7(syst)MeV for this state. We do not
confirm the report from the Belle collaboration of a broad structure at 4.01
GeV/c2. In addition, we investigate the Ï+Ïâ system
which results from Y(4260) decay
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
- 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
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- Annovi A
- Antonaki A
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- Antonov A
- Antos J
- Anulli F
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- Apolle R
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- Aracena I
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- Aranda CP
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- Arguin J-F
- Arik E
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- Armbruster AJ
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- Bagnaia P
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- Bai Y
- Bailey DC
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- Baker MD
- Baker OK
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- Castanheira MTD
- Castillo LRF
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- Cataneo F
- Catinaccio A
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- Cattai A
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- Chareyre E
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- Chelkov GA
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- Chernyatin V
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- Chromek-Burckhart D
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- Yoosootiniya R
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- Yurkewicz A
- Zaets VG
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- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
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- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- 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
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- 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 âs = 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 pTâ„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 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{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 the standard model Higgs boson in the diphoton decay channel with 4.9fb -1 of pp collision data at âs=7TeV with atlas
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- Ă kesson TPA
- Ă sman 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 4.9ââfb-1 collected with the ATLAS detector at the Large Hadron Collider in proton-proton collisions at a center-of-mass energy of âs=7ââTeV. In the diphoton mass range 110â150 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 110â150 GeV, this significance becomes 1.5 standard deviations. The standard model Higgs boson is excluded at 95% confidence level in the mass ranges of 113â115 GeV and 134.5â136 GeV
Search for the standard model Higgs boson in the diphoton decay channel with 4.9fb -1 of pp collision data at âs=7TeV with atlas
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aenia T
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- AivkoviÄ L
- Akdogan T
- 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
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
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- Alon R
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- Alvarez Gonzalez B
- Alviggi MG
- Amako K
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- 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 4.9ââfb-1 collected with the ATLAS detector at the Large Hadron Collider in proton-proton collisions at a center-of-mass energy of âs=7ââTeV. In the diphoton mass range 110â150 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 110â150 GeV, this significance becomes 1.5 standard deviations. The standard model Higgs boson is excluded at 95% confidence level in the mass ranges of 113â115 GeV and 134.5â136 GeV
MRI for neurodevelopmental prognostication in the high-risk term infant.
- Author
- Publication venue
- Health Sciences Research Commons
- Publication date
- 01/03/2015
- Field of study
A new approach to define acute kidney injury in term newborns with hypoxic ischemic encephalopathy.
- Publication venue
- Health Sciences Research Commons
- Publication date
- 01/07/2016
- Field of study
BACKGROUND: Current definitions of acute kidney injury (AKI) are not sufficiently sensitive to identify all newborns with AKI during the first week of life.
METHODS: To determine whether the rate of decline of serum creatinine (SCr) during the first week of life can be used to identify newborns with AKI, we reviewed the medical records of 106 term neonates at risk of AKI who were treated with hypothermia for hypoxic ischemic encephalopathy (HIE).
RESULTS: Of the newborns enrolled in the study, 69 % showed a normal rate of decline of SCr toââ„50 % and/or reached SCr levels ofââ€0.6 mg/dl before the 7th day of life, and therefore had an excellent clinical outcome (control group). Thirteen newborns with HIE (12 %) developed AKI according to an established neonatal definition (AKI-KIDGO group), and an additional 20 newborns (19 %) showed a rate of decline of SCr of
CONCLUSIONS: The rate of decline of SCr provides a sensitive approach to identify term newborns with AKI during the first week of life
Pneumothorax in the newborn: Clinical presentation, risk factors and outcomes
- Publication venue
- Health Sciences Research Commons
- Publication date
- 01/01/2013
- Field of study
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