102 research outputs found
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Chemical transport modeling of potential atmospheric CO2 sinks
- Publication venue
- eScholarship, University of California
- Publication date
- 01/01/2003
- Field of study
The potential for carbon dioxide (CO2) sequestration via engineered chemical sinks is investigated using a three dimensional chemical transport model (CTM). Meteorological and chemical constraints for flat or vertical systems that would absorb CO2 from the atmosphere, as well as an example chemical system of calcium hydroxide (Ca(OH)2) proposed by Elliott et al. [Compensation of atmospheric CO2 buildup through engineered chemical sinkage, Geophys. Res. Lett. 28 (2001) 1235] are reviewed. The CTM examines land based deposition sinks, with 4° Ă 5° latitude/longitude resolution at various locations, and deposition velocities (v). A maximum uptake of âź20 Gton (1015 g) Cyr-1 is attainable with v ⼠5 cms-1 at a mid-latitude site. The atmospheric increase of CO2 (3 Gtonyr-1) can be balanced by an engineered sink with an area of no more than 75, 000 km2 at v of 1 cms-1. By building the sink upwards or splitting this area into narrow elements can reduce the active area by more than an order of magnitude as discussed in Dubey et al. Š 2002 Elsevier Science Ltd. All rights reserved
Search for Gravitational Waves from Primordial Black Hole Binary Coalescences in the Galactic Halo
- Author
- Abbott B
- Abbott R
- Adhikari R
- Ageev A
- Allen B
- Amin R
- Anderson SB
- Anderson WG
- Araya M
- Armandula H
- Ashley M
- Asiri F
- Aufmuth P
- Aulbert C
- Babak S
- Balasubramanian R
- Ballmer S
- Barish BC
- Barker C
- Barker D
- Barnes M
- Barr B.
- Barton MA
- Bayer K
- Beausoleil R
- Belczynski K
- Bennett R.
- Berukoff SJ
- Betzwieser J
- Bhawal B
- Bilenko IA
- Billingsley G
- Black E
- Blackburn K
- Blackburn L
- Bland B
- Bochner B
- Bogue L
- Bork R
- Bose S
- Brady PR
- Braginsky VB
- Brau JE
- Brown DA
- Bullington A
- Bunkowski A
- Buonanno A
- Burgess R
- Busby D
- Butler WE
- Byer RL
- Cadonati L
- Cagnoli G.
- Camp JB
- Cantley C.A.
- Cardenas L
- Carter K
- Casey M.M.
- Castiglione J
- Chandler A
- Chapsky J
- Charlton P
- Chatterji S
- Chelkowski S
- Chen Y
- Chickarmane V
- Chin D
- Christensen N
- Churches D
- Cokelaer T
- Colacino C
- Coldwell R
- Coles M
- Cook D
- Corbitt T
- Coyne D
- Creighton JDE
- Creighton TD
- Crooks D.R.M.
- Csatorday P
- Cusack BJ
- Cutler C
- DAmbrosio E
- Danzmann K
- Daw E
- DeBra D
- Delker T
- Dergachev V
- DeSalvo R
- Dhurandhar S
- Di Credico A
- Diaz M
- Ding H
- Drever RWP
- Dupuis R.J.
- Edlund JA
- Ehrens P
- Elliffe E.J.
- Etzel T
- Evans M
- Evans T
- Fairhurst S
- Fallnich C
- Farnham D
- Fejer MM
- Findley T
- Fine M
- Finn LS
- Franzen KY
- Freise A
- Frey R
- Fritschel P
- Frolov VV
- Fyffe M
- Ganezer KS
- Garofoli J
- Giaime JA
- Gillespie A
- Goda K
- Gonzalez G
- Gossler S
- Grandclement P
- Grant A.
- Gray C
- Gretarsson AM
- Grimmett D
- Grote H
- Grunewald S
- Guenther M
- Gustafson E
- Gustafson R
- Hamilton WO
- Hammond M
- Hanson J
- Hardham C
- Harms J
- Harry G
- Hartunian A
- Heefner J
- Hefetz Y
- Heinzel G
- Heng IS
- Hennessy M
- Hepler N
- Heptonstall A.
- Heurs M
- Hewitson M
- Hild S
- Hindman N
- Hoang P
- Hough J.
- Hrynevych M
- Hua W
- Ito M
- Itoh Y
- Ivanov A
- Jennrich O.
- Johnson B
- Johnson WW
- Johnston WR
- Jones DI
- Jones L
- Jungwirth D
- Kalogera V
- Katsavounidis E
- Kawabe K
- Kawamura S
- Kells W
- Kern J
- Khan A
- Killbourn S.
- Killow C.J.
- Kim C
- King C
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- Klimenko S
- Koranda S
- Kotter K
- Kovalik J
- Kozak D
- Krishnan B
- Landry M
- Langdale J
- Lantz B
- Lawrence R
- Lazzarini A
- Lei M
- Leonor I
- Libbrecht K
- Libson A
- LIGO Sci Collaboration
- Lindquist P
- Liu S
- Logan J
- Lormand M
- Lubinski M
- Luck H
- Lyons TT
- Machenschalk B
- MacInnis M
- Mageswaran M
- Mailand K
- Majid W
- Malec M
- Mann F
- Marin A
- Marka S
- Maros E
- Mason J
- Mason K
- Matherny O
- Matone L
- Mavalvala N
- McCarthy R
- McClelland DE
- McHugh M
- McNabb JWC
- Mendell G
- Mercer RA
- Meshkov S
- Messaritaki E
- Messenger C
- Mitrofanov VP
- Mitselmakher G
- Mittleman R
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- Mohanty S
- Moreno G
- Mossavi K
- Mueller G
- Mukherjee S
- Murray P.
- Myers J
- Nagano S
- Nash T
- Nayak R
- Newton G.
- Nocera F
- Noel JS
- Nutzman P
- Olson T
- OReilly B
- Ottaway DJ
- Ottewill A
- Ouimette D
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- Owen BJ
- Pan Y
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- Parameshwaraiah V
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- Pedraza M
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- Pitkin M.
- Plissi M.
- Prix R
- Quetschke V
- Raab F
- Radkins H
- Rahkola R
- Rakhmanov M
- Rao SR
- Rawlins K
- Ray-Majumder S
- Re V
- Redding D
- Regehr MW
- Regimbau T
- Reid S.
- Reilly KT
- Reithmaier K
- Reitze DH
- Richman S
- Riesen R
- Riles K
- Rivera B
- Rizzi A
- Robertson D.I.
- Robertson N.A.
- Robison L
- Roddy S
- Rollins J
- Romano JD
- Romie J
- Rong H
- Rose D
- Rotthoff E
- Rowan S.
- Rudiger A
- Russell P
- Ryan K
- Salzman I
- Sandberg V
- Sanders GH
- Sannibale V
- Sathyaprakash B
- Saulson PR
- Savage R
- Sazonov A
- Schilling R
- Schlaufman K
- Schmidt V
- Schnabel R
- Schofield R
- Schutz BF
- Schwinberg P
- Scott SM
- Seader SE
- Searle AC
- Sears B
- Seel S
- Seifert F
- Sengupta AS
- Shapiro CA
- Shawhan P
- Shoemaker DH
- Shu QZ
- Sibley A
- Siemens X
- Sievers L
- Sigg D
- Sintes AM
- Smith JR
- Smith M
- Smith MR
- Sneddon P.H.
- Spero R
- Stapfer G
- Steussy D
- Strain K.A.
- Strom D
- Stuver A
- Summerscales T
- Sumner MC
- Sutton PJ
- Sylvestre J
- Takamori A
- Tanner DB
- Tariq H
- Taylor I
- Taylor R
- Thorne KA
- Thorne KS
- Tibbits M
- Tilav S
- Tinto M
- Tokmakov KV
- Torres C
- Torrie C
- Traylor G
- Tyler W
- Ugolini D
- Ungarelli C
- Vallisneri M
- van Putten M
- Vass S
- Vecchio A
- Veitch J.
- Vorvick C
- Vyachanin SP
- Wallace L
- Walther H
- Ward H.
- Ware B
- Watts K
- Webber D
- Weidner A
- Weiland U
- Weinstein A
- Weiss R
- Welling H
- Wen L
- Wen S
- Whelan JT
- Whitcomb SE
- Whiting BF
- Wiley S
- Wilkinson C
- Willems PA
- Williams PR
- Williams R
- Willke B
- Wilson A
- Winjum BJ
- Winkler W
- Wise S
- Wiseman AG
- Woan G.
- Woods D
- Wooley R
- Worden J
- Wu W
- Yakushin I
- Yamamoto H
- Yoshida S
- Zaleski KD
- Zanolin M
- Zawischa I
- Zhang L
- Zhu R
- Zotov N
- Zucker M
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2005
- Field of study
We use data from the second science run of the LIGO gravitational-wave
detectors to search for the gravitational waves from primordial black hole
(PBH) binary coalescence with component masses in the range 0.2--1.0Mââ.
The analysis requires a signal to be found in the data from both LIGO
observatories, according to a set of coincidence criteria. No inspiral signals
were found. Assuming a spherical halo with core radius 5 kpc extending to 50
kpc containing non-spinning black holes with masses in the range 0.2--1.0Mââ, we place an observational upper limit on the rate of PBH coalescence
of 63 per year per Milky Way halo (MWH) with 90% confidence.Comment: 7 pages, 4 figures, to be submitted to Phys. Rev.
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Aldaya Martin M
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunovic Z
- Apanasevich L
- Appelt E
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Beernaert K
- Behr J
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhardwaj A
- Bhat PC
- Bhatnagar V
- Bhattacharya S
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- Bhatti A
- Bialkowska H
- Bian JG
- Bianchi G
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- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boeser C
- Boimska B
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
- Bontenackels M
- Boos E
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- Bourilkov D
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
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- CMS Collaboration
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- Ferapontov A
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- Ghete VM
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- Givernaud A
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- Gleyzer SV
- Glushkov I
- Gninenko S
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- Godinovic N
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- Yilmaz Y
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- Yun JC
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- de Cassagnac RG
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- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
A cross-sectional study of pedagogical strategies in nursing education: opportunities and constraints toward using effective pedagogy
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Multi-messenger observations of a binary neutron star merger
- Author
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- Array LWA Long Wavelength
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- Zhang T
- Zhang W
- Zhang WC
- Zhang WZ
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Y-H
- Zhang YF
- Zhang YJ
- Zhang Z
- Zhang ZL
- Zhao C
- Zhao HS
- Zhao JL
- Zhao W
- Zhao XF
- Zheng SJ
- Zhou H
- Zhou J
- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- Zhu Y
- Zhu YX
- Zhu Z
- Ziegler A
- Zimmerman AB
- Zimmermann B
- Zimnukhov DS
- Ziolkowski M
- Zoll M
- Zong Z
- Zorn J
- Zornoza JD
- Zou CL
- Zuccarello F
- Zucker ME
- Zuniga J
- Zweizig J
- Zywucka N
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transientâs position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
Prognostic model to predict postoperative acute kidney injury in patients undergoing major gastrointestinal surgery based on a national prospective observational cohort study.
- Author
- Aamir A
- Abbas J
- Abbas N
- Abbott TEF
- Abdalla M
- Abdikadir H
- Abuhussein N
- Acquaah F
- Adamson R
- Adeleye O
- Adeogun A
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- Ainsworth P
- Aishwarya G
- Ajibola-Taylor O
- Akhbari M
- Akhtar A
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- STARSurg Collaborative Writing Committee, Data analysis, Steering committee, Advisory group, Regional leads, Collaborators and validators
- STARSurg Collaborative Writing Committee, Data analysis, Steering committee, Advisory group, Regional leads, Collaborators and validators, Nepogodiev, D
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- Zubikarai G
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- Publication venue
- 'Wiley'
- Publication date
- 18/05/2018
- Field of study
Background: Acute illness, existing co-morbidities and surgical stress response can all contribute to postoperative acute kidney injury (AKI) in patients undergoing major gastrointestinal surgery. The aim of this study was prospectively to develop a pragmatic prognostic model to stratify patients according to risk of developing AKI after major gastrointestinal surgery. Methods: This prospective multicentre cohort study included consecutive adults undergoing elective or emergency gastrointestinal resection, liver resection or stoma reversal in 2-week blocks over a continuous 3-month period. The primary outcome was the rate of AKI within 7 days of surgery. Bootstrap stability was used to select clinically plausible risk factors into the model. Internal model validation was carried out by bootstrap validation. Results: A total of 4544 patients were included across 173 centres in the UK and Ireland. The overall rate of AKI was 14¡2 per cent (646 of 4544) and the 30-day mortality rate was 1¡8 per cent (84 of 4544). Stage 1 AKI was significantly associated with 30-day mortality (unadjusted odds ratio 7¡61, 95 per cent c.i. 4¡49 to 12¡90; P < 0¡001), with increasing odds of death with each AKI stage. Six variables were selected for inclusion in the prognostic model: age, sex, ASA grade, preoperative estimated glomerular filtration rate, planned open surgery and preoperative use of either an angiotensin-converting enzyme inhibitor or an angiotensin receptor blocker. Internal validation demonstrated good model discrimination (c-statistic 0¡65). Discussion: Following major gastrointestinal surgery, AKI occurred in one in seven patients. This preoperative prognostic model identified patients at high risk of postoperative AKI. Validation in an independent data set is required to ensure generalizability
Localization and broadband follow-up of the gravitational-wave transient GW150914
- Author
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- Zweizig J
- Publication venue
- Astrophysical Journal Letters
- Publication date
- 01/01/2016
- Field of study
A gravitational-wave (GW) transient was identified in data recorded by the Advanced Laser Interferometer Gravitational-wave Observatory (LIGO) detectors on 2015 September 14. The event, initially designated G184098 and later given the name GW150914, is described in detail elsewhere. By prior arrangement, preliminary estimates of the time, significance, and sky location of the event were shared with 63 teams of observers covering radio, optical, near-infrared, X-ray, and gamma-ray wavelengths with ground- and space-based facilities. In this Letter we describe the low-latency analysis of the GW data and present the sky localization of the first observed compact binary merger. We summarize the follow-up observations reported by 25 teams via private Gamma-ray Coordinates Network circulars, giving an overview of the participating facilities, the GW sky localization coverage, the timeline, and depth of the observations. As this event turned out to be a binary black hole merger, there is little expectation of a detectable electromagnetic (EM) signature. Nevertheless, this first broadband campaign to search for a counterpart of an Advanced LIGO source represents a milestone and highlights the broad capabilities of the transient astronomy community and the observing strategies that have been developed to pursue neutron star binary merger events. Detailed investigations of the EM data and results of the EM follow-up campaign are being disseminated in papers by the individual teams
Measurement of the rapidity and transverse momentum distributions of Z bosons in pp collisions at â(s)=7ââTeV
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- Yilmaz Y
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/10/2011
- Field of study
Measurements of the normalized rapidity (y) and transverse-momentum (qT) distributions of DrellâYan muon and electron pairs in the Z-boson mass region (60<Mââ<120ââGeV) are reported. The results are obtained using a data sample of proton-proton collisions at a center-of-mass energy of 7 TeV, collected by the CMS experiment at the Large Hadron Collider (LHC), corresponding to an integrated luminosity of 36ââpb-1. The distributions are measured over the ranges |y|<3.5 and qT<600ââGeV and compared with quantum chromodynamics (QCD) calculations using recent parton distribution functions to model the momenta of the quarks and gluons in the protons. Overall agreement is observed between the models and data for the rapidity distribution, while no single model describes the Z transverse-momentum distribution over the full range
Measurement of the differential cross section for isolated prompt photon production in pp collisions at 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta JG
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- Cirino G
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- Civinini C
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- Coarasa Perez JA
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- Codispoti G
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- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Dahmes B
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- Dallavalle GM
- Damgov J
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- Daubie E
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- Zabi A
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zhukov V
- Zhukova V
- Ziebarth EB
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- Zoeller MH
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- Ăzbek M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
A measurement of the differential cross section for the inclusive production of isolated prompt photons in proton-proton collisions at a center-of-mass energy of 7 TeV is presented. The data sample corresponds to an integrated luminosity of 36 pb(-1) recorded by the CMS detector at the LHC. The measurement covers the pseudorapidity range vertical bar eta vertical bar < 2.5 and the transverse energy range 25 < E-T < 400 GeV, corresponding to the kinematic region 0.007 < x(T) < 0.114. Photon candidates are identified with two complementary methods, one based on photon conversions in the silicon tracker and the other on isolated energy deposits in the electromagnetic calorimeter. The measured cross section is presented as a function of E-T in four pseudorapidity regions. The next-to-leading-order perturbative QCD calculations are consistent with the measured cross section
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