179 research outputs found
Particle Physics Probes Of Extra Spacetime Dimensions
- Publication venue
- 'Annual Reviews'
- Publication date
- 01/01/2002
- Field of study
The possibility that spacetime is extended beyond the familiar 3+1-dimensions
has intrigued physicists for a century. Indeed, the consequences of a
dimensionally richer spacetime would be profound. Recently, new theories with
higher dimensional spacetimes have been developed to resolve the hierarchy
problem in particle physics. These scenarios make distinct predictions which
allow for experiment to probe the existence of extra dimensions in new ways. We
review the conceptual framework of these scenarios, their implications in
collider and short-range gravity experiments, their astrophysical and
cosmological effects, as well as the constraints placed on these models from
present data.Comment: Submitted to Annual Review of Nuclear and Particle Science, 29 page
Tests of the Gravitational Inverse-Square Law
- Author
- Publication venue
- 'Annual Reviews'
- Publication date
- 22/07/2003
- Field of study
We review recent experimental tests of the gravitational inverse-square law
and the wide variety of theoretical considerations that suggest the law may
break down in experimentally accessible regions.Comment: 81 pages, 10 figures, submitted by permission of the Annual Review of
Nuclear and Particle Science. Final version of this material is scheduled to
appear in the Annual Review of Nuclear and Particle Science Vol. 53, to be
published in December 2003 by Annual Reviews, http://AnnualReviews.or
Constraints on Non-Newtonian Gravity from Recent Casimir Force Measurements
- Author
- A Kehagias
- A Roy
- BR Heckel
- BW Harris
- CD Hoyle
- CW Stubbs
- CW Stubbs
- DE Krause
- E Fischbach
- E Fischbach
- E Fischbach
- EG Floratos
- F Chen
- F. Chen
- FD Stacey
- Feinberg G.and Sucher, J
- G Bressi
- G Carugno
- G MĂŒller
- G.L. Smith
- GL Klimchitskaya
- GL Klimchitskaya
- GT Gillies
- J Chiaverini
- J Kim
- JC Long
- JC Long
- JH Gundlach
- JK Hoskins
- KA Milton
- L Randall
- L Randall
- M Bordag
- M. Bordag
- M. Bordag
- M. Bordag
- N Arkani-Hamed
- O Klein
- PW Milonni
- R.S. Decca
- S Dimopoulos
- SC Holding
- SK Lamoreaux
- SK Lamoreaux
- T Ederth
- T Kaluza
- U Mohideen
- V Sabbata
- V.M. Mostepanenko
- VA Kuzâmin
- VB Braginskii
- VM Mostepanenko
- VM Mostepanenko
- VM Mostepanenko
- VM Mostepanenko
- VM Mostepanenko
- VM Mostepanenko
- VM Mostepanenko
- VP Mitrofanov
- Y Su
- YT Chen
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 14/11/2003
- Field of study
Corrections to Newton's gravitational law inspired by extra dimensional
physics and by the exchange of light and massless elementary particles between
the atoms of two macrobodies are considered. These corrections can be described
by the potentials of Yukawa-type and by the power-type potentials with
different powers. The strongest up to date constraints on the corrections to
Newton's gravitational law are reviewed following from the E\"{o}tvos- and
Cavendish-type experiments and from the measurements of the Casimir and van der
Waals force. We show that the recent measurements of the Casimir force gave the
possibility to strengthen the previously known constraints on the constants of
hypothetical interactions up to several thousand times in a wide interaction
range. Further strengthening is expected in near future that makes Casimir
force measurements a prospective test for the predictions of fundamental
physical theories.Comment: 20 pages, crckbked.cls is used, to be published in: Proceedings of
the 18th Course of the School on Cosmology and Gravitation: The Gravitational
Constant. Generalized Gravitational Theories and Experiments (30 April- 10
May 2003, Erice). Ed. by G. T. Gillies, V. N. Melnikov and V. de Sabbata,
20pp. (Kluwer, in print, 2003
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
- King P
- 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
- Miyakawa O
- Miyoki S
- 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
- Overmier H
- Owen BJ
- Pan Y
- Papa MA
- Parameshwaraiah V
- Parameswaran A
- Parameswariah C
- Pedraza M
- Penn S
- 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.
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
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- 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
- Asner D
- 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
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck GA
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall 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
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek 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
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini 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-Jelisavcic I
- Bracinik J
- Braem A
- Branchini 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
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brown H
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- BScher V
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- 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
- Caballero J
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghi M
- Cameron D
- Camilocci ES
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepaa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciba K
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Cranshaw J
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuc C-M
- Curatolo M
- Curtis CJ
- Curull XE
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- Da Costa JBG
- Da Costa JGPF
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Daly CH
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Dawson JW
- Daya-Ishmukhametova RK
- de Asmundis R
- De Castro S
- De Cecco S
- De Graat J
- De Groot N
- De Jong P
- De la Hoz SG
- De la Taille C
- De la Torre H
- De Lima JGR
- De Lotto B
- De Mora L
- De Nooij L
- De Pedis D
- De Regie JBDV
- De Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Dean S
- Debbe R
- Dedovich DV
- Degenhardt J
- Dehchar M
- Del Papa C
- Del Peso J
- Del Prete T
- Deliyergiyev M
- Dell'Acqua A
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- Smizanska M
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- Takahashi Y
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- Torchiani I
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- Tyrvainen H
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- Uhrmacher M
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- Vorobel V
- Vorobiev AP
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- Vos M
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- Vossebeld JH
- Vranjes N
- Vrba V
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- Vukotic I
- Wagner P
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- Wosiek BK
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- Xie Y
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- Yagci KD
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- Yamaguchi H
- Yamamoto A
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- Yamamoto S
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- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
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- Youssef S
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- Yu J
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- Yurkewicz A
- Zaets VG
- Zaidan R
- 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
- Zhang J
- Zhang Q
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- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhuravlov V
- Zieminska D
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- 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
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Zhemchugov A
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- Zieminska D
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- Zitoun R
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- 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
Top Quark Mass Measurement in the lepton plus jets Channel Using a Matrix Element Method and in situ Jet Energy Calibration
- Author
- Aaltonen T
- Almenar CC
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Badgett W
- Barbaro Galtieri A
- Barnes VE
- Barnett BA
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- Bauce M
- Bauer G
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
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- Bisello D
- Bizjak I
- Bland KR
- Blumenfeld B
- Bocci A
- Bodek A
- Bortoletto D
- Boudreau J
- Boveia A
- Brau B
- Brigliadori L
- Brisuda A
- Bromberg C
- Brucken E
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- Budagov J
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- Zucchelli SD
- Zucchelli SSuzuki T
- Publication venue
- 'Purdue University (bepress)'
- Publication date
- 01/01/2010
- Field of study
A precision measurement of the top quark mass m(t) is obtained using a sample of t (t) over bar events from p (p) over bar collisions at the Fermilab Tevatron with the CDF II detector. Selected events require an electron or muon, large missing transverse energy, and exactly four high-energy jets, at least one of which is tagged as coming from a b quark. A likelihood is calculated using a matrix element method with quasi-Monte Carlo integration taking into account finite detector resolution and jet mass effects. The event likelihood is a function of mt and a parameter Delta(JES) used to calibrate the jet energy scale in situ. Using a total of 1087 events in 5.6 fb(-1) of integrated luminosity, a value of m(t) 173.0 +/- 1.2 GeV/c(2) is measured
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
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- Yilmaz M
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- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
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- 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
- 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
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla H
- Abe F
- Abeysekara AU
- Abramo LR
- Abramowski A
- Abreu P
- Acernese F
- Acero F
- Ackermann M
- Ackley K
- Ackley K
- Adams C
- Adams J
- Adams SM
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Afrough M
- Agarwal B
- Agathos M
- Agatsuma K
- Aggarwal N
- Aglietta M
- Agliozzo C
- Agudo I
- Aguiar OD
- Aguilar JA
- Aharonian F
- Ahlers M
- Ahrens M
- Aiello L
- Ain A
- Ajith P
- Akras S
- Al Samarai I
- Albert A
- Albert A
- Albuquerque IFM
- Albury JM
- Alcaniz JS
- Alexander KD
- Alfaro R
- Alighieri S Di Serego
- Allam S
- Allekotte I
- Allen B
- Allen G
- Allison J
- Allison JR
- Allocca A
- Almela A
- Altin PA
- Altmann D
- Alvarez C
- Alvarez JD
- Alvarez M Dovale
- Alvarez-Muiz J
- Amati L
- Amato A
- An T
- Ananyeva A
- Anastasi GA
- Anchordoqui L
- Andeen K
- Anderson JP
- Anderson SB
- Anderson T
- Anderson WG
- Andrada B
- Andre M
- Andreoni I
- Andreoni I
- Andringa S
- Angelova SV
- Anghinolfi M
- Angner EO
- Angus CR
- Annis J
- Ansseau I
- Antier S
- Anton G
- Antonelli LA
- Antonelli LA
- Anupama GC
- Aoki K
- Aoki W
- Appert S
- Aptekar RL
- Arai K
- Arakawa M
- Aramo C
- Araya MC
- Arcavi I
- Arceo R
- Ardid M
- Areeda JS
- Aresu G
- Argan A
- Argelles C
- Arnaud N
- Array LWA Long Wavelength
- Array MWA Murchison Widefield
- Arrieta M
- Arsene N
- Arteaga-Velzquez JC
- Artola R
- Arun KG
- Asakura Y
- Asaoka Y
- Ascenzi S
- Ashall C
- Ashley MCB
- Ashton G
- Asorey H
- Assis P
- Ast M
- Aston SM
- Astone P
- Atallah DV
- ATLAS
- Atwood WB
- Aubert J-J
- Aubert P
- Aublin J
- Auffenberg J
- Aufmuth P
- Aulbert C
- AultONeal K
- Austin C
- Avgitas T
- Avila G
- Avila-Alvarez A
- Awad A Kuotb
- Axani S
- Baar S
- Babak S
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- Bacon P
- Bader MKM
- Badescu AM
- Bae S
- Bagherpour H
- Bai X
- Bailes M
- Baker PT
- Balaceanu A
- Balanutsa PV
- Balasubramanian A
- Balbinot E
- Baldaccini F
- Baldini L
- Ballardin G
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- Barayoga JC
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- Barbato F
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- Barsuglia M
- Barta D
- Barthelmy SD
- Bartlett J
- Bartos I
- Barway S
- Barway S
- Barwick SW
- Basa S
- Bassiri R
- Basti A
- Bastieri D
- Batch JC
- Bauer FE
- Bauer FE
- Baum V
- Bawaj M
- Bay R
- Bayley JC
- Bazzan M
- Bazzano A
- Bchele M
- Beardmore AP
- Beardsley A
- Beatty JJ
- Becerril A
- Becherini Y
- Bechtol K
- Becker KH
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- Belhorma B
- Bell AS
- Bellazzini R
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- Benetti S
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- Benoit-Levy A
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- Bernardini MG
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- Berry CPL
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- Bertaina ME
- Bertin E
- Bertin V
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- Berton M
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- Bessell MS
- Besson DZ
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- Bonnefoy S
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- Booler T
- Boom BA
- Bordas P
- Bork R
- Bormuth R
- Borner M
- Borodai N
- Bos F
- Boschi V
- Bose D
- Bose S
- Boser S
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- Botner O
- Bottacini E
- Bottcher M
- Botti AM
- Botticella MT
- Bouffanais Y
- Bourbeau E
- Bourbeau J
- Bourret S
- Bouwhuis MC
- Bozzi A
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- Brandt S
- Brau JE
- Braun J
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- Camuccio R
- Cancio A
- Canepa M
- Canfora F
- Canizares P
- Cannella C
- Cannizzaro G
- Cannon KC
- Cano Z
- Cao H
- Cao J
- Cao XL
- Capaccioli M
- Capano CD
- Capasso M
- Capistrn T
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- Capone A
- Capozzi D
- Cappellaro E
- Caputo R
- Caramete L
- Caraveo P
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- Carbognani F
- Carboni G
- Cardenas B Vargas
- Cardillo M
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- Casella P
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- Cesarini E
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- Chamberlin SJ
- Chambers KC
- Chan M
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- Chatterjee D
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- Chatziioannou K
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- Chu Q
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- Chua S
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- Chung AKW
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- Clearwater P
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- Cooke J
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- Cordero-Carrion I
- Corley KR
- Cornish N
- Corongiu A
- Corral-Santana JM
- Corsi A
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- Costa E
- Costa-Duarte MV
- Costantin D
- Costantini H
- Cotti U
- Cotzomi J
- Coughlin M
- Coughlin MW
- Coughlin SB
- Coulon J-P
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- Countryman ST
- Courvoisier TJ-L
- Coutu S
- Couvares P
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- Covault CE
- Covino S
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- Coward DM
- Coward DM
- Cowart MJ
- Cowen DF
- Cowperthwaite P
- Coyle P
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- Creighton JDE
- Creighton TD
- Creusot A
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- Diogo F
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- Distefano C
- Djannati-Atao A
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- Dobie D
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- Doctor Z
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- Dolique V
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- Donovan F
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- Dornic D
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- Drouhin D
- Drout MR
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- Eggenstein H-B
- Egron E
- Ehrens P
- Ehrhardt T
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- Eichmann B
- Eifler TF
- Eikenberry SS
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- El Bojaddaini I
- El Khayati N
- El Moursli R Cherkaoui
- Elias-Rosa N
- Elipe G Torralba
- Eller P
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- Elmer E
- Elsasser D
- Emery G
- Emery SWK
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- Emrich D
- Engel K
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- Enzenhofer A
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- Escobar CO
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- Evangelista Y
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- Fan X
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- Feicht J
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- Fejer MM
- Feldbusch F
- Felde J
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- Fender RP
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- Fenu F
- Fermi GBM
- Fernandes MV
- Fernandez D
- Fernandez E
- Fernandez G Rodriguez
- Fernandez-Galiana A
- Feroci M
- Ferrante I
- Ferrari A
- Ferreira EC
- Ferrigno C
- Ferrini F
- Fiasson A
- Fick B
- Fidecaro F
- Figueira JM
- Filimonov K
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- Fioretti V
- Fiori I
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- Flaugher B
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- Forsyth PWF
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- Fosalba P
- Foster K
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- Fox OD
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- Fraija N
- Frail DA
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- Franzen T
- Frasca S
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- Fremling C
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- Fritschel P
- Frohmaier C
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- Frolov VV
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- Fryer CL
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- Fssling M
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- Fuchs T
- Fujii T
- Fujii YI
- Fujiyoshi T
- Fukazawa Y
- Fulda P
- Funk S
- Funk S
- Furusawa H
- Fuschino F
- Fusco LA
- Fusco P
- Fuster A
- Fyffe M
- Fynbo JPU
- Gabbard H
- Gabici S
- Gabovich AV
- Gadre BU
- Gaebel SM
- Gaensler BM
- Gaior R
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- Gaisser TK
- Gal-Yam A
- Galbany L
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- Gallagher J
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- Gao GH
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- Gargano F
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- Gate F
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- Gaudio S
- Gaudiomonte F
- Gaur G
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- Gayathri V
- Gaztanaga E
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- Gerhardt L
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- Getman F
- Gherghel-Lascu A
- Ghia PL
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- Ghisellini G
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- Ghosh Abhirup
- Ghosh Archisman
- Ghosh S
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- Giaime JA
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- Giannantonio T
- Gianotti F
- Giardina KD
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- Glsenkamp T
- Goedhart S
- Goetz E
- Goetz R
- Goldschmidt A
- Goldstein A
- Goldstein DA
- Golenetskii SV
- Golup G
- Gomboc A
- Gomes S
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- Goncalves DR
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- Goncharov B
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- Grp Las Cumbres Observatory
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- Gu YD
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- Guelbenzu A Nicuesa
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- Guiriec S
- Guo CC
- Guo X
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- Gurovich S
- Gusai V
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- 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
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Weiss R
- Wellmann F
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- Willke B
- Winkler W
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- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
- Yang L
- Yang Y
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- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- College Park, MD : American Physical Society
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO's second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=3.47Ă10-25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering. © 2019 American Physical Society
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