141 research outputs found
Clusters of galaxies : observational properties of the diffuse radio emission
- Author
- A Bonafede
- A Bonafede
- A Bonafede
- A Bonafede
- A Finoguenov
- A Neronov
- A Pedlar
- AC Fabian
- AC Fabian
- AD Reid
- AG Pacholczyk
- AM Taylor
- AS Cohen
- B Ballarati
- B Dennison
- BJ Burn
- BM Gaensler
- BR McNamara
- BR McNamara
- BS Mason
- C Ferrari
- C Ferrari
- C Ferrari
- C Pfrommer
- C Vogt
- C Vogt
- CL Carilli
- CL Sarazin
- CL Sarazin
- D Dallacasa
- D Eckert
- D Guidetti
- D Guidetti
- D Guidetti
- D Ryu
- D Ryu
- DA Buote
- DE Harris
- DR Wik
- DR Wik
- E Middelberg
- E Orrù
- EL Blanton
- F Govoni
- F Govoni
- F Govoni
- F Govoni
- F Govoni
- F Govoni
- F Govoni
- F Govoni
- F Govoni
- F Govoni
- F Miniati
- F Miniati
- F Miniati
- F Tavecchio
- F Vazza
- F Vazza
- Federica Govoni
- G Brunetti
- G Brunetti
- G Brunetti
- G Brunetti
- G Brunetti
- G Brunetti
- G Brunetti
- G Brunetti
- G Brunetti
- G Gavazzi
- G Giovannini
- G Giovannini
- G Giovannini
- G Giovannini
- G Giovannini
- G Giovannini
- G Giovannini
- G Giovannini
- G Giovannini
- G Giovannini
- G Macario
- G Macario
- Gabriele Giovannini
- GB Taylor
- GB Taylor
- GB Taylor
- GK Miley
- H Böhringer
- H Böhringer
- H Liang
- H Xu
- H Xu
- HJA Röttgering
- HR Russel
- I Valtchanov
- J Bagchi
- J Bagchi
- J Bagchi
- J Bagchi
- J ZuHone
- JA Eilek
- JC Kempner
- JC Kempner
- JC Kempner
- JD Barrow
- JE Felten
- JE Noordam
- JJ Condon
- JM Lawler
- JO Burns
- JP Vallée
- JR Peterson
- JR Peterson
- K Dolag
- K Dolag
- K Dolag
- K Dolag
- K Dolag
- K Röttiger
- K Röttiger
- K-T Kim
- K-T Kim
- K-T Kim
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Feretti
- L Rudnick
- L Rudnick
- L Solovyeva
- Luigina Feretti
- M Ackermann
- M Bacchi
- M Brüggen
- M Brüggen
- M Girardi
- M Gitti
- M Gitti
- M Gitti
- M Gitti
- M Hoeft
- M Johnston-Hollitt
- M Johnston-Hollitt
- M Krause
- M Markevitch
- M Murgia
- M Murgia
- M Murgia
- M Murgia
- M Murgia
- M Rossetti
- M Thierbach
- MA Brentjens
- MA Brentjens
- MAG Willson
- Matteo Murgia
- MI Large
- MW Kunz
- MY Mao
- O Reimer
- OB Slee
- P Blasi
- P Blasi
- P Blasi
- P Kuchar
- P Mazzotta
- P Schuecker
- P-H Kuo
- PC Tribble
- PC Tribble
- PP Kronberg
- PP Kronberg
- R Barrena
- R Cassano
- R Cassano
- R Cassano
- R Cassano
- R Cassano
- R Cassano
- R Cassano
- R Durrer
- R Fusco-Femiano
- R Fusco-Femiano
- R Fusco-Femiano
- R Fusco-Femiano
- R Fusco-Femiano
- R Kale
- R Schlickeiser
- R Subrahmanyan
- RA Laing
- RA Laing
- RA Perley
- RB Rengelink
- RF Pizzo
- RF Pizzo
- RF Pizzo
- RJ Hanisch
- RJ Weeren van
- RJ Weeren van
- RJ Weeren van
- RJ Weeren van
- RJ Weeren van
- RJ Weeren van
- RJ Weeren van
- RJ Weeren van
- S Brown
- S Brown
- S Colafrancesco
- S Gabici
- S Giacintucci
- S Giacintucci
- S Giacintucci
- S Giacintucci
- S Giacintucci
- S Giacintucci
- S Giacintucci
- S Grandi De
- SE Nuza
- SS Komissarov
- ST Garrington
- ST Garrington
- SW Randall
- T Bogdanovic
- T Venturi
- T Venturi
- T Venturi
- T Venturi
- T Venturi
- TA Enßlin
- TA Enßlin
- TA Enßlin
- TA Enßlin
- TA Enßlin
- TE Clarke
- TE Clarke
- TE Jeltema
- TH Reiprich
- U Keshet
- U Keshet
- U Keshet
- V Petrosian
- V Vacca
- V Vacca
- VA Dogiel
- W Boschin
- W Boschin
- W Boschin
- W Tucker
- WG Mathews
- WJ Jaffe
- WJ Jaffe
- Y Fujita
- Y Fujita
- Y Rephaeli
- Y Xu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Clusters of galaxies, as the largest virialized systems in the Universe, are
ideal laboratories to study the formation and evolution of cosmic
structures...(abridged)... Most of the detailed knowledge of galaxy clusters
has been obtained in recent years from the study of ICM through X-ray
Astronomy. At the same time, radio observations have proved that the ICM is
mixed with non-thermal components, i.e. highly relativistic particles and
large-scale magnetic fields, detected through their synchrotron emission. The
knowledge of the properties of these non-thermal ICM components has increased
significantly, owing to sensitive radio images and to the development of
theoretical models. Diffuse synchrotron radio emission in the central and
peripheral cluster regions has been found in many clusters. Moreover
large-scale magnetic fields appear to be present in all galaxy clusters, as
derived from Rotation Measure (RM) studies. Non-thermal components are linked
to the cluster X-ray properties, and to the cluster evolutionary stage, and are
crucial for a comprehensive physical description of the intracluster medium.
They play an important role in the cluster formation and evolution. We review
here the observational properties of diffuse non-thermal sources detected in
galaxy clusters: halos, relics and mini-halos. We discuss their classification
and properties. We report published results up to date and obtain and discuss
statistical properties. We present the properties of large-scale magnetic
fields in clusters and in even larger structures: filaments connecting galaxy
clusters. We summarize the current models of the origin of these cluster
components, and outline the improvements that are expected in this area from
future developments thanks to the new generation of radio telescopes.Comment: Accepted for the publication in The Astronomy and Astrophysics
Review. 58 pages, 26 figure
Localization and broadband follow-up of the gravitational-wave transient GW150914
- Author
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla FB
- Abe F
- Abernathy MR
- Acernese F
- Ackermann M
- Ackley K
- Adame JA
- Adams C
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajello M
- Ajith P
- Albert A
- Allam S
- Allen B
- Allen WH
- Allison J
- Allocca A
- Altin PA
- Amati L
- Anderson B
- Anderson JP
- Anderson SB
- Anderson WG
- Annis J
- Antonelli LA
- Aptekar RL
- Arai K
- Araya MC
- Arceneaux CC
- Areeda JS
- Armstrong R
- Arnaud N
- Arun KG
- Ascenzi S
- Ashton G
- Ast M
- Aston SM
- Astone P
- Atwood WB
- Aufmuth P
- Aulbert C
- Axelsson M
- Babak S
- Bacon P
- Bader MKM
- Bai J
- Baiardi LC
- Baker PT
- Balanutsa P
- Baldaccini F
- Baldini L
- Ballardin G
- Ballmer SW
- Baltay C
- Banerji M
- Bannister K
- Barayoga JC
- Barbiellini G
- Barclay SE
- Barish BC
- Barker D
- Barlow T
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Barthelmy S
- Bartlett J
- Bartos I
- Bassiri R
- Basti A
- Bastieri D
- Batch JC
- Baune C
- Bavigadda V
- Bazzan M
- Bazzano A
- Behnke B
- Bejger M
- Bell AS
- Bell CJ
- Bell ME
- Bellazzini R
- Bellm E
- Benacquista M
- Benoit-Levy A
- Berger BK
- Berger E
- Bergman J
- Bergmann G
- Bernstein RA
- Beroiz M
- Berry CPL
- Bersanetti D
- Bersier DF
- Bertin E
- Bertolini A
- Betzwieser J
- Bhagwat S
- Bhalerao V
- Bhandare R
- Bhat PN
- Bilenko IA
- Billingsley G
- Birch J
- Birney R
- Biscans S
- Bisht A
- Bissaldi E
- Bissaldi E
- Bitossi M
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blackburn L
- Blair CD
- Blair DG
- Blair RM
- Blandford RD
- Bloemen S
- Bloom ED
- Bock O
- Bode MF
- Bodiya TP
- Boer M
- Bogaert G
- Bogan C
- Bohe A
- Bojtos P
- Bond C
- Bondu F
- Bonino R
- Bonnand R
- Boom BA
- Bork R
- Boschi V
- Bose S
- Bottacini E
- Botticella MT
- Bouffanais Y
- Bozzi A
- Bozzo E
- Bradaschia C
- Brady PR
- Braginsky VB
- Branchesi M
- Brandt S
- Brandt TJ
- Brandt TJ
- Brau JE
- Briant T
- Briggs MS
- Brillet A
- Brinkmann M
- Brisson V
- Brocato E
- Brockill P
- Broderick JW
- Brooks AF
- Brout D
- Brown DA
- Brown DD
- Brown NM
- Buchanan CC
- Buckley D
- Buckley-Geer E
- Budnev NM
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Burke DL
- Burns E
- Burrows DN
- Buskulic D
- Buson S
- Bustillo JC
- Buy C
- Byer RL
- Caballero-Garcia MD
- Cabral J
- Cadonati L
- Cagnoli G
- Cahillane C
- Caliandro GA
- Callister T
- Calloni E
- Cameron RA
- Camp JB
- Campana S
- Campbell H
- Cannon KC
- Cano Z
- Cao J
- Cao Y
- Capaccioli M
- Capano CD
- Capocasa E
- Capozzi D
- Cappellaro E
- Caragiulo M
- Caraveo PA
- Carbognani F
- Caride S
- Carretero J
- Casentini C
- Castander FJ
- Castellon A
- Castillo-Carrion S
- Castro JMG
- Castro-Tirado AJ
- Caudill S
- Cavaglia M
- Cavalier F
- Cavalieri R
- Cavazzuti E
- Cella G
- Cenko SB
- Cepeda CB
- Cerretani G
- Cesarini E
- Chakraborty R
- Chalermsongsak T
- Chamberlin SJ
- Chambers KC
- Chan M
- Chao S
- Charles E
- Charlton P
- Chassande-Mottin E
- Chatterjee S
- Chekhtman A
- Chen HY
- Chen T-W
- Chen Y
- Cheng C
- Chiang J
- Chiaro G
- Chincarini A
- Chippendale AP
- Chiummo A
- Cho HS
- Cho M
- Chornock R
- Chow JH
- Christensen N
- Chu Q
- Chua S
- Chung S
- Ciani G
- Ciprini S
- Clara F
- Claret A
- Clark JA
- Cleva F
- Cleveland W
- Cline T
- Coccia E
- Cohadon P-F
- Cohen-Tanugi J
- Colazo C
- Colla A
- Collabor DECGW-EM
- Collaboration ASKAP
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- Collaboration DES
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- Collette CG
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- Cominsky L
- Cominsky LR
- Connaughton V
- Conte A
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- Cook D
- Cook D
- Copperwheat CM
- Corbitt TR
- Cornish N
- Corsi A
- Cortese S
- Costa CA
- Costanza F
- Coughlin MW
- Coughlin SB
- Coulon J-P
- Countryman ST
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- Couvares P
- Covino S
- Cowan EE
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- Cowart MJ
- Cowperthwaite PS
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- Coyne DC
- Coyne R
- Craig K
- Creighton JDE
- Cripe J
- Croft S
- Crowder SG
- Cui C
- Cumming A
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- Cunningham L
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- Davier M
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- de Palma F
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- Degallaix J
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- Everett R
- Evrard AE
- Factourovich M
- Fafone V
- Fair H
- Fairhurst S
- Fan X
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- Fang Q
- Farinon S
- Farr B
- Farr WM
- Favata M
- Favuzzi C
- Fays M
- Fehrmann H
- Fejer MM
- Fender RP
- Feng L
- Fernandez CG
- Fernandez E
- Fernandez-Munoz R
- Ferrante I
- Ferrara EC
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- Fiori I
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- Fitzpatrick G
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- Getman F
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- Gill K
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- Giordano F
- Giroletti M
- Giuffrida G
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- Glanzman T
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- Gopakumar A
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- Gossan SE
- Gosselin M
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- Graff PB
- Granata M
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- GRAWITA
- Gray C
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- Hanks J
- Hanlon L
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- Hanson J
- Harding AK
- Hardwick T
- Haris K
- Harmanen J
- Harms J
- Harry GM
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- Hartman MT
- Harvey-Smith L
- Haster C-J
- Haughian K
- Hays E
- Heidmann A
- Heintze MC
- Heitmann H
- Hello P
- Hemming G
- Hendry M
- Heng IS
- Hennig J
- Heptonstall AW
- Herner K
- Heurs M
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- Hild S
- Hill AB
- Hiriart D
- Hjorth J
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- Hofman D
- Hollitt SE
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- Holz DE
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- Horesh A
- Hosken DJ
- Hotan A
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- Hu YM
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- Kumar P
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- Kuss M
- Kuulkers E
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- La Mura G
- Lackey BD
- Lahav O
- Laher R
- Lambas DG
- Landry M
- Lange J
- Lantz B
- Lares M
- Larsson S
- Lasky PD
- Latronico L
- Laugier R
- Laurent P
- Lazzarini A
- Lazzaro C
- Le Guillou L
- Leaci P
- Leavey S
- Lebigot EO
- Lee CH
- Lee HK
- Lee HM
- Lee K
- Lee WH
- Lenon A
- Leonardi M
- Leong JR
- Leroy N
- Letendre N
- Levan AJ
- Levin Y
- Levine BM
- Li J
- Li L
- Li TGF
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- Libson A
- Lima M
- Limatola L
- Lin H
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- Lisi M
- Littenberg TB
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- Longo F
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- Loriette V
- Lormand M
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- Machenschalk B
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- Magill J
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- Manske M
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- Mason K
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- Massinger TJ
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- 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
Multi-messenger observations of a binary neutron star merger
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- Salvadori I
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- Sampson LM
- Samtleben DFE
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- Schofield RMS
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- Schonbeck A
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- Schreiber E
- Schroder FG
- Schroder S
- Schroder SL
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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 transient’s 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
Observation and branching fraction measurement of the decay Ξb- → Λ0 bπ -
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- Ketel T
- Khanji B
- Kharisova A
- Kholodenko S
- Khreich G
- Kirn T
- Kirsebom VS
- Kitouni O
- Klaver S
- Kleijne N
- Klimaszewski K
- Kmiec MR
- Koliiev S
- Kolk L
- Kondybayeva A
- Konoplyannikov A
- Kopciewicz P
- Kopecna R
- Koppenburg P
- Korolev M
- Kostiuk I
- Kot O
- Kotriakhova S
- Kozachuk A
- Kravchenko P
- Kravchuk L
- Kreps M
- Kretzschmar S
- Krokovny P
- Krupa W
- Krzemien W
- Kubat J
- Kubis S
- Kucewicz W
- Kucharczyk M
- Kudryavtsev V
- Kulikova E
- Kupsc A
- Kutsenko BK
- Lacarrere D
- Lafferty G
- Lai A
- Lampis A
- Lancierini D
- Landesa Gomez C
- Lane JJ
- Lane R
- Langenbruch C
- Langer J
- Lantwin O
- Latham T
- Lazzari F
- Lazzeroni C
- Le Gac R
- Lee SH
- Lefevre R
- Leflat A
- Legotin S
- Lenisa P
- Leroy O
- Lesiak T
- Leverington B
- Li A
- Li H
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- Li P
- Li PR
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- Liang X
- Lin C
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- Lisovskyi V
- Litvinov R
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- Lobo Salvia A
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- Long T
- Longstaff I
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- Lopez Huertas A
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- Lovell GH
- Lu Y
- Lucarelli C
- Lucchesi D
- Luchuk S
- Lucio Martinez M
- Lukashenko V
- Luo Y
- Lupato A
- Luppi E
- Lynch K
- Lyu XR
- Ma R
- Maccolini S
- Machefert F
- Maciuc F
- Mackay I
- Madhan Mohan LR
- Madurai MM
- Maevskiy A
- Magdalinski D
- Maisuzenko D
- Majewski MW
- Malczewski JJ
- Malde S
- Malecki B
- Malentacca L
- Malinin A
- Maltsev T
- Manca G
- Mancinelli G
- Mancuso C
- Manera Escalero R
- Manuzzi D
- Manzari CA
- Marangotto D
- Marchand JF
- Marconi U
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- Marin Benito C
- Marks J
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- Martelli G
- Martellotti G
- Martinazzoli L
- Martinelli M
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- Martinez Vidal F
- Massafferri A
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- Mathad A
- Matiunin V
- Matteuzzi C
- Mattioli KR
- Mauri A
- Maurice E
- Mauricio J
- Mazurek M
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- Mcconnell L
- McGrath TH
- McHugh NT
- McNab A
- McNulty R
- Meadows B
- Meier G
- Melnychuk D
- Merk M
- Merli A
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- Miao D
- Miao H
- Mikhasenko M
- Milanes DA
- Minard MN
- Minotti A
- Minucci E
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- Mitzel DS
- Modak A
- Moedden A
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- Monteil S
- Morcillo Gomez A
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- Neustroev P
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- Nicolini J
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- Oblakowska-Mucha A
- Obraztsov V
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- Otalora Goicochea JM
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- Romanovskiy V
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- Ronchetti F
- Rotondo M
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- Ruiz Fernandez RA
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- Ryzhikov A
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- Sagidova N
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- Saitta B
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- Scarabotto A
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- Sciascia B
- Sciuccati A
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- Shapkin M
- Shchemerov I
- Shchutska L
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- Shekhtman L
- Shen Z
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- Spedicato E
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- Spiridenkov E
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- Westhenry BDC
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- Williams MRJ
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- Wislicki W
- Witek M
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- Wormser G
- Wotton SA
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- Wu J
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- Wyllie K
- Xian S
- Xiang Z
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- Yang D
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- Yeroshenko V
- Yeung H
- Yin H
- Yu CY
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- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zeng M
- Zhang C
- Zhang D
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- Zhang Y
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- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
- Zhou Y
- Zhovkovska V
- Zhu LZ
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- Zhukov V
- Zhuo J
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2023
- Field of study
Observation of Two New Excited Ξb0 States Decaying to Λb0 K-π+
- Author
- Aaij R
- Abdelmotteleb ASW
- Abrantes FG
- Ackernley T
- Adeva B
- Adinolfi M
- Afsharnia H
- Agapopoulou C
- Aidala CA
- Aiola S
- Ajaltouni Z
- Akar S
- Akiba KC
- Albero AA
- Albrecht J
- Alepuz CR
- Alessio F
- Alexander M
- Aliouche Z
- Alkhazov G
- Altarelli MP
- Amato S
- Amey JL
- Amhis Y
- An L
- Anderlini L
- Andreianov A
- Andreotti M
- Archilli F
- Artamonov A
- Artuso M
- Arzymatov K
- Aslanides E
- Atzeni M
- Audurier B
- Bachmann S
- Bachmayer M
- Back JJ
- Balagura V
- Baldini W
- Barajas CAC
- Barbetti M
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bashir S
- Bassi G
- Batsukh B
- Battig A
- Bay A
- Beck A
- Becker M
- Bedeschi F
- Bediaga I
- Beiter A
- Belavin V
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benito CM
- Berezhnoy A
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
- Beteta CA
- Betti F
- Bezshyiko I
- Bhasin S
- Bhom J
- Bian L
- Bieker MS
- Bifani S
- Billoir P
- Birch M
- Bishop FCR
- Bitadze A
- Bizzeti A
- Bjorn M
- Blago MP
- Blake T
- Blanc F
- Blusk S
- Bobulska D
- Boelhauve JA
- Boettcher T
- Boldyrev A
- Bondar A
- Bondar N
- Borghi S
- Borisyak M
- Borsato M
- Borsuk JT
- Bouchiba SA
- Bowcock TJV
- Boyer A
- Bozzi C
- Bradley MJ
- Braun S
- Brodski M
- Brodzicka J
- Brundu D
- Buonaura A
- Buonincontri L
- Burke AT
- Burr C
- Bursche A
- Butkevich A
- Butter JS
- Buytaert J
- Byczynski W
- Cadeddu S
- Cai H
- Calabrese R
- Calefice L
- Cali S
- Calladine R
- Calvi M
- Campana P
- Canudas NV
- Capelli S
- Capriotti L
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carli I
- Carniti P
- Cartelle PA
- Carus L
- Casasus MP
- Casse G
- Castro AP
- Castro JL
- Cattaneo M
- Cavallero G
- Cazon BRG
- Celani S
- Cerasoli J
- Cervenkov D
- Chadwick AJ
- Chapman MG
- Charles M
- Charpentier P
- Chatzikonstantinidis G
- Chefdeville M
- Chen C
- Chen S
- Chernov A
- Chobanova V
- Cholak S
- Chrzaszcz M
- Chubykin A
- Chulikov V
- Ciambrone P
- Cicala MF
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Cobbledick JL
- Coco V
- Coelho JAB
- Cogan J
- Cogneras E
- Cojocariu L
- Collins P
- Colombo T
- Congedo L
- Contu A
- Cooke N
- Coombs G
- Corredoira I
- Corti G
- Coutinho RS
- Couturier B
- Craik DC
- Crkovska J
- Currie R
- D'Ambrosio C
- D'Argent P
- Da Silva CL
- Dadabaev S
- Dai L
- Dall'Occo E
- Dalseno J
- Danilina A
- Davies JE
- Davis A
- De Almeida FLS
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Paula BS
- De Paula L
- De Serio M
- De Simone D
- De Simone P
- de Vries JA
- Dean CT
- Decamp D
- Dedu V
- Del Buono L
- Delaney B
- Dembinski HP
- Dendek A
- Denysenko V
- Derkach D
- Deschamps O
- Desse F
- Dettori F
- Dey B
- Di Cicco A
- Di Nezza P
- Diaz LC
- Diaz MV
- Didenko S
- Dijkstra H
- Dobishuk V
- Dong C
- Donohoe AM
- Dordei F
- dos Reis AC
- Douglas L
- Dovbnya A
- Downes AG
- Dudek MW
- Dufour L
- Duk V
- Durante P
- Durham JM
- Dutta D
- Dziurda A
- Dzyuba A
- Easo S
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Ek-In S
- Eklund L
- Ely S
- Ene A
- Epple E
- Escher S
- Eschle J
- Esen S
- Evans T
- Falabella A
- Fan J
- Fan Y
- Fang B
- Farry S
- Fazzini D
- Feo M
- Fernandez RAR
- Fernandez SG
- Fernez AD
- Ferrari F
- Ferrillo M
- Ferro-Luzzi M
- Figueras EV
- Filippov S
- Fini RA
- Fiorini M
- Firlej M
- Fischer KM
- Fitzgerald DS
- Fitzpatrick C
- Fiutowski T
- Fkiaras A
- Fleuret F
- Fontana M
- Fontanelli F
- Forty R
- Foulds-Holt D
- Francisco OD
- Frank M
- Franzoso E
- Frau G
- Frei C
- Friday DA
- Fu J
- Fuehring Q
- Gabriel E
- Galli D
- Gambetta S
- Gan Y
- Gandelman M
- Gandini P
- Gao Y
- Garau M
- Garcia LM
- Garcia OB
- Garrido L
- Gaspar C
- Geertsema RE
- Gerick D
- Gerken LL
- Gersabeck E
- Gersabeck M
- Gershon T
- Gerstel D
- Ghez P
- Giambastiani L
- Gibson V
- Giemza HK
- Gilman AL
- Giovannetti M
- Gioventu A
- Gironell PG
- Giubega L
- Giugliano C
- Gizdov K
- Gkougkousis EL
- Gligorov VV
- Gobel C
- Goicochea JMO
- Golobardes E
- Golubkov D
- Golutvin A
- Gomes A
- Gomez MC
- Gomez RV
- Goncerz M
- Gong G
- Gonzalo AB
- Gorbounov P
- Gorelov IV
- Gotti C
- Govorkova E
- Grabowski JP
- Grammatico T
- Gras CS
- Grauges E
- Graverini E
- Graziani G
- Grecu A
- Greeven LM
- Grieser NA
- Grillo L
- Gromov S
- Gu C
- Guarise M
- Guittiere M
- Gunther PA
- Gushchin E
- Guth A
- Guz Y
- Gys T
- Hadavizadeh T
- Haefeli G
- Haen C
- Haimberger J
- Halewood-leagas T
- Hamilton PM
- Hammerich JP
- Han Q
- Han X
- Hancock TH
- Hansmann-Menzemer S
- Harnew N
- Harrison T
- Hasse C
- Hatch M
- He J
- Hecker M
- Heijhoff K
- Heinicke K
- Hennequin AM
- Hennessy K
- Henry L
- Heuel J
- Hicheur A
- Hill D
- Hilton M
- Hollitt SE
- Hou R
- Hou Y
- Hu J
- Hu J
- Hu W
- Hu X
- Huang W
- Huang X
- Hulsbergen W
- Hunter RJ
- Hushchyn M
- Hutchcroft D
- Hynds D
- Ibis P
- Idzik M
- Ilin D
- Ilten P
- Inglessi A
- Ishteev A
- Ivshin K
- Jacobsson R
- Jage H
- Jakobsen S
- Jans E
- Jashal BK
- Jawahery A
- Jevtic V
- Jiang F
- John M
- Johnson D
- Jones CR
- Jones TP
- Jost B
- Jurik N
- Kadavath SHK
- Kandybei S
- Kang Y
- Karacson M
- Karpov M
- Keizer F
- Keller DM
- Kenzie M
- Ketel T
- Khanji B
- Kharisova A
- Kholodenko S
- Kirn T
- Kirsebom VS
- Kitouni O
- Klaver S
- Kleijne N
- Klimaszewski K
- Kmiec MR
- Koliiev S
- Kondybayeva A
- Konoplyannikov A
- Kopciewicz P
- Kopecna R
- Koppenburg P
- Korolev M
- Kostiuk I
- Kot O
- Kotriakhova S
- Kravchenko P
- Kravchuk L
- Krawczyk RD
- Kreps M
- Kress F
- Kretzschmar S
- Krokovny P
- Krupa W
- Krzemien W
- Kucewicz W
- Kucharczyk M
- Kudryavtsev V
- Kuindersma HS
- Kunde GJ
- Kvaratskheliya T
- Lacarrere D
- Lafferty G
- Lai A
- Lamas MR
- Lampis A
- Lancierini D
- Lane JJ
- Lane R
- Lanfranchi G
- Langenbruch C
- Langer J
- Lantwin O
- Latham T
- Lavra LS
- Lazzari F
- Le Gac R
- Lee SH
- Lefevre R
- Leflat A
- Legotin S
- Leite JB
- Lener MP
- Leroy O
- Lesiak T
- Leverington B
- Li H
- Li P
- Li S
- Li Y
- Li Y
- Li Z
- Liang X
- Lima VF
- Lin T
- Lindner R
- Lisovskyi V
- Litvinov R
- Liu G
- Liu H
- Liu Q
- Liu S
- Loi A
- Longstaff I
- Lopes JH
- Lopes LF
- Lopez JAR
- Lovell GH
- Lu Y
- Lucarelli C
- Lucchesi D
- Luchuk S
- Lukashenko V
- Luo Y
- Lupato A
- Luppi E
- Lupton O
- Lusiani A
- Lyu X
- Ma L
- Ma R
- Maccolini S
- Machado DT
- Machefert F
- Maciuc F
- Macko V
- Mackowiak P
- Maddrell-Mander S
- Madejczyk O
- Maev O
- Maevskiy A
- Magalhaes PC
- Maisuzenko D
- Majewski MW
- Malczewski JJ
- Malde S
- Malecki B
- Malinin A
- Maltsev T
- Malygina H
- Manca G
- Mancinelli G
- Manuzzi D
- Marangotto D
- Maratas J
- Marchand JF
- Marconi U
- Mariani S
- Marinangeli M
- Marks J
- Maronas LD
- Marshall AM
- Marshall PJ
- Martelli G
- Martellotti G
- Martin LMG
- Martinazzoli L
- Martinelli M
- Martinez ML
- Massafferri A
- Materok M
- Matev R
- Mathad A
- Mathe Z
- Matiunin V
- Matteuzzi C
- Mattioli KR
- Mauri A
- Maurice E
- Mauricio J
- Mazurek M
- McCann M
- Mcconnell L
- Mcgrath TH
- Mchugh NT
- McNab A
- McNulty R
- Mead JV
- Meadows B
- Meier G
- Meinert N
- Melnychuk D
- Meloni S
- Merk M
- Merli A
- Mikhasenko M
- Milanes DA
- Millard E
- Milovanovic M
- Minard MN
- Minotti A
- Minzoni L
- Mitchell SE
- Mitreska B
- Mitzel DS
- Modden A
- Mohammed RA
- Mohan LRM
- Moise RD
- Mombacher T
- Monroy IA
- Monteil S
- Morandin M
- Morello G
- Morello MJ
- Moreno PG
- Moron J
- Morris AB
- Morris AG
- Mountain R
- Mu H
- Muheim F
- Mulder M
- Muller D
- Muller K
- Murphy CH
- Murray D
- Muzzetto P
- Naik P
- Nakada T
- Nandakumar R
- Nanut T
- Nasteva I
- Needham M
- Neri I
- Neri N
- Neubert S
- Neufeld N
- Newcombe R
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- Wyllie K
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- Xiao D
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- Xu Z
- Yang D
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- Yang Y
- Yang Z
- Yang Z
- Yao Y
- Yeomans LE
- Yin H
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- Yuan X
- Yushchenko O
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
- Zhang D
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- Zhang S
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- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
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- Zhou Y
- Zhovkovska V
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- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Two narrow resonant states are observed in the Λb0K-π+ mass spectrum using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the LHCb experiment and corresponding to an integrated luminosity of 6 fb-1. The minimal quark content of the Λb0K-π+ system indicates that these are excited Ξb0 baryons. The masses of the Ξb(6327)0 and Ξb(6333)0 states are m[Ξb(6327)0]=6327.28-0.21+0.23±0.12±0.24 and m[Ξb(6333)0]=6332.69-0.18+0.17±0.03±0.22 MeV, respectively, with a mass splitting of Δm=5.41-0.27+0.26±0.12 MeV, where the uncertainties are statistical, systematic, and due to the Λb0 mass measurement. The measured natural widths of these states are consistent with zero, with upper limits of Γ[Ξb(6327)0]<2.20(2.56) and Γ[Ξb(6333)0]<1.60(1.92) MeV at a 90% (95%) credibility level. The significance of the two-peak hypothesis is larger than nine (five) Gaussian standard deviations compared to the no-peak (one-peak) hypothesis. The masses, widths, and resonant structure of the new states are in good agreement with the expectations for a doublet of 1D Ξb0 resonances
Precision measurement of CP violation in the penguin-mediated decay Bs0→ϕϕ
- Author
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- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2023
- Field of study
A flavor-tagged time-dependent angular analysis of the decay
Bs0→ϕϕ is performed using pp collision data collected
by the LHCb experiment at % at s=13 TeV, the center-of-mass energy of
13 TeV, corresponding to an integrated luminosity of 6 fb^{-1}. The
CP-violating phase and direct CP-violation parameter are measured
to be ϕssˉs=−0.042±0.075±0.009 rad and
∣λ∣=1.004±0.030±0.009, respectively, assuming the same values
for all polarization states of the ϕϕ system. In these results, the
first uncertainties are statistical and the second systematic. These parameters
are also determined separately for each polarization state, showing no evidence
for polarization dependence. The results are combined with previous LHCb
measurements using pp collisions at center-of-mass energies of 7 and 8 TeV,
yielding ϕssˉs=−0.074±0.069 rad and ∣lambda∣=1.009±0.030. This is the most precise study of time-dependent CP violation
in a penguin-dominated B meson decay. The results are consistent with
CP symmetry and with the Standard Model predictions.Comment: All figures and tables, along with any supplementary material and
additional information, are available at
https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2023-001.html (LHCb
public pages
Measurement of the Λb0→Λ(1520)μ+μ− differential branching fraction
- Author
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- Abdelmotteleb ASW
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- Abudinén F
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- Saborido Silva JJ
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- Sahoo N
- Saitta B
- Salomoni M
- Sanchez Gras C
- Sanderswood I
- Santacesaria R
- Santamarina Rios C
- Santimaria M
- Santoro L
- Santovetti E
- Saranin D
- Sarpis G
- Sarpis M
- Sarti A
- Satriano C
- Satta A
- Saur M
- Savrina D
- Sazak H
- Scantlebury Smead LG
- Scarabotto A
- Schael S
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- Schmelling M
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- Sellam S
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- Sergi A
- Serra N
- Sestini L
- Seuthe A
- Shang Y
- Shangase DM
- Shapkin M
- Shchemerov I
- Shchutska L
- Shears T
- Shekhtman L
- Shen Z
- Sheng S
- Shevchenko V
- Shi B
- Shields EB
- Shimizu Y
- Shmanin E
- Shorkin R
- Shupperd JD
- Siddi BG
- Silva Coutinho R
- Simi G
- Simone S
- Singla M
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- Skuza R
- Skwarnicki T
- Slater MW
- Smallwood JC
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- Soares Lavra L
- Sokoloff MD
- Soler FJP
- Solomin A
- Solovev A
- Solovyev I
- Song R
- Souza De Almeida FL
- Souza De Paula B
- Spaan B
- Spadaro Norella E
- Spedicato E
- Speer JG
- Spiridenkov E
- Spradlin P
- Sriskaran V
- Stagni F
- Stahl M
- Stahl S
- Stanislaus S
- Stein EN
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- Stevens H
- Strekalina D
- Su Y
- Suljik F
- Sun J
- Sun L
- Sun Y
- Swallow PN
- Swientek K
- Szabelski A
- Szumlak T
- Szymanski M
- T'Jampens S
- Tan Y
- Taneja S
- Tat MD
- Terentev A
- Teubert F
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- Tilquin H
- Tisserand V
- Tobin M
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- Tonani G
- Tong X
- Torres Machado D
- Tou DY
- Trippl C
- Tuci G
- Tuning N
- Ukleja A
- Unverzagt DJ
- Usachov A
- Ustyuzhanin A
- Uwer U
- Vagnoni V
- Valassi A
- Valenti G
- Valls Canudas N
- Van Dijk M
- Van Hecke H
- van Herwijnen E
- Van Hulse CB
- van Veghel M
- Vazquez Gomez R
- Vazquez Regueiro P
- Vecchi S
- Velthuis JJ
- Veltri M
- Venkateswaran A
- Veronesi M
- Vesterinen M
- Vieira D
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- Vilasis-Cardona X
- Vilella Figueras E
- Villa A
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- Vom Bruch D
- Vorobyev V
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- Vrahas C
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- Walsh J
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- Ward JA
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- Websdale D
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- Westhenry BDC
- White DJ
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- Wiederhold AR
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- Williams MRJ
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- Wotton SA
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- Wu J
- Wyllie K
- Xiang Z
- Xie Y
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- Xu L
- Xu L
- Xu M
- Xu Q
- Xu Z
- Xu Z
- Yang D
- Yang S
- Yang X
- Yang Y
- Yang Z
- Yang Z
- Yeomans LE
- Yeroshenko V
- Yeung H
- Yin H
- Yu J
- Yuan X
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zeng M
- Zhang C
- Zhang D
- Zhang J
- Zhang L
- Zhang S
- Zhang S
- Zhang Y
- Zhang Y
- Zhao Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
- Zhou Y
- Zhovkovska V
- Zhu X
- Zhu X
- Zhu Z
- Zhukov V
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- Publication date
- 01/01/2023
- Field of study
The branching fraction of the rare decay Λb0→Λ(1520)μ+μ− is measured for the first time, in the squared dimuon mass
intervals, q2, excluding the J/ψ and ψ(2S) regions. The data
sample analyzed was collected by the LHCb experiment at center-of-mass energies
of 7, 8, and 13 TeV, corresponding to a total integrated luminosity of $9\
\mathrm{fb}^{-1}.Theresultinthehighestq^{2}interval,q^{2} >15.0\
\mathrm{GeV}^2/c^4$, where theoretical predictions have the smallest model
dependence, agrees with the predictions.Comment: All figures and tables, along with any supplementary material and
additional information, are available at
https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-050.html (LHCb
public pages
Observation of Gravitational Waves from a Binary Black Hole Merger
- Author
- Abbott BP
- Abbott R
- Abbott TD
- Abernathy MR
- Acernese F
- Ackley K
- Adams C
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Allen B
- Allocca A
- Altin PA
- Anderson SB
- Anderson WG
- Arai K
- Arain MA
- Araya MC
- Arceneaux CC
- Areeda JS
- Arnaud N
- Arun KG
- Ascenzi S
- Ashton G
- Ast M
- Aston SM
- Astone P
- Aufmuth P
- Aulbert C
- Babak S
- Bacon P
- Bader MKM
- Baiardi LC
- Baker PT
- Baldaccini F
- Ballardin G
- Ballmer SW
- Barayoga JC
- Barclay SE
- Barish BC
- Barker D
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton MA
- Bartos I
- Bassiri R
- Basti A
- Batch JC
- Baune C
- Bavigadda V
- Bazzan M
- Behnke B
- Bejger M
- Belczynski C
- Bell AS
- Bell CJ
- Berger BK
- Bergman J
- Bergmann G
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Bhagwat S
- Bhandare R
- Bilenko IA
- Billingsley G
- Birch J
- Birney R
- Birnholtz O
- Biscans S
- Bisht A
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blair CD
- Blair DG
- Blair RM
- Bloemen S
- Bock O
- Bodiya TP
- Boer M
- Bogaert G
- Bogan C
- Bohe A
- Bojtos P
- Bond C
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- Buikema A
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- Cagnoli G
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- Callister T
- Calloni E
- Camp JB
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- Carbognani F
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- Caudill S
- Cavaglia M
- Cavalier F
- Cavalieri R
- Cella G
- Cepeda CB
- Cerretani G
- Cesarini E
- Chakraborty R
- Chalermsongsak T
- Chamberlin SJ
- Chan M
- Chao S
- Charlton P
- Chassande-Mottin E
- Chen HY
- Chen Y
- Cheng C
- Chincarini A
- Chiummo A
- Cho HS
- Cho M
- Chow JH
- Christensen N
- Chu Q
- Chua S
- Chung S
- Ciani G
- Clara F
- Clark JA
- Cleva F
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- Corsi A
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- Vallisneri M
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- van den Brand JFJ
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- van der Schaaf L
- van Heijningen JV
- van Veggel AA
- Vander-Hyde DC
- Vardaro M
- Vass S
- Vasuth M
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- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venkateswara K
- Verkindt D
- Vetrano F
- Vicere A
- Vinciguerra S
- Vine DJ
- Vinet J-Y
- Vitale S
- Vo T
- Vocca H
- Vorvick C
- Voss D
- Vousden WD
- Vyatchanin SP
- Wade AR
- Wade LE
- Wade M
- Waldman SJ
- Walker M
- Wallace L
- Walsh S
- Wang G
- Wang H
- Wang M
- Wang X
- Wang Y
- Ward H
- Ward RL
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- Wei L-W
- Weinert M
- Weinstein AJ
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- Wette K
- Whelan JT
- Whitcomb SE
- White DJ
- Whiting BF
- Wiesner K
- Wilkinson C
- Willems PA
- Williams L
- Williams RD
- Williamson AR
- Willis JL
- Willke B
- Wimmer MH
- Winkelmann L
- Winkler W
- Wipf CC
- Wiseman AG
- Wittel H
- Woan G
- Worden J
- Wright JL
- Wu G
- Yablon J
- Yakushin I
- Yam W
- Yamamoto H
- Yancey CC
- Yap MJ
- Yu H
- Yvert M
- Zadrozny A
- Zangrando L
- Zanolin M
- Zendri J-P
- Zevin M
- Zhang F
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- Zhang Y
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- Zhou M
- Zhou Z
- Zhu XJ
- Zucker ME
- Zuraw SE
- Zweizig J
- Publication venue
- American Physical Society
- Publication date
- 01/01/2016
- Field of study
On September 14, 2015 at 09:50:45 UTC the two detectors of the Laser Interferometer Gravitational-Wave
Observatory simultaneously observed a transient gravitational-wave signal. The signal sweeps upwards in
frequency from 35 to 250 Hz with a peak gravitational-wave strain of 1.0 × 10−21. It matches the waveform
predicted by general relativity for the inspiral and merger of a pair of black holes and the ringdown of the
resulting single black hole. The signal was observed with a matched-filter signal-to-noise ratio of 24 and a
false alarm rate estimated to be less than 1 event per 203 000 years, equivalent to a significance greater
than 5.1σ. The source lies at a luminosity distance of 410þ160
−180 Mpc corresponding to a redshift z ¼ 0.09þ0.03 −0.04 .
In the source frame, the initial black hole masses are 36þ5
−4M⊙ and 29þ4
−4M⊙, and the final black hole mass is
62þ4
−4M⊙, with 3.0þ0.5 −0.5M⊙c2 radiated in gravitational waves. All uncertainties define 90% credible intervals.
These observations demonstrate the existence of binary stellar-mass black hole systems. This is the first direct
detection of gravitational waves and the first observation of a binary black hole merger
Recommended from our members
Prospects for Observing and Localizing Gravitational-Wave Transients with Advanced LIGO and Advanced Virgo.
- Author
- Abbott BP
- Abbott R
- Abbott TD
- Abernathy MR
- Acernese F
- Ackley K
- Adams C
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- Zweizig J
- Publication venue
- Living Rev Relativ
- Publication date
- 28/09/2021
- Field of study
We present a possible observing scenario for the Advanced LIGO and Advanced Virgo gravitational-wave detectors over the next decade, with the intention of providing information to the astronomy community to facilitate planning for multi-messenger astronomy with gravitational waves. We determine the expected sensitivity of the network to transient gravitational-wave signals, and study the capability of the network to determine the sky location of the source. We report our findings for gravitational-wave transients, with particular focus on gravitational-wave signals from the inspiral of binary neutron-star systems, which are considered the most promising for multi-messenger astronomy. The ability to localize the sources of the detected signals depends on the geographical distribution of the detectors and their relative sensitivity, and 90% credible regions can be as large as thousands of square degrees when only two sensitive detectors are operational. Determining the sky position of a significant fraction of detected signals to areas of 5 deg2 to 20 deg2 will require at least three detectors of sensitivity within a factor of ∼ 2 of each other and with a broad frequency bandwidth. Should the third LIGO detector be relocated to India as expected, a significant fraction of gravitational-wave signals will be localized to a few square degrees by gravitational-wave observations alone
Angular Analysis of the B+ -> K*(+)mu(+) mu(-) Decay
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- Ackernley T
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- Aidala CA
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- Zhukov V
- Zonneveld JB
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2021
- Field of study
We present an angular analysis of the
B
+
→
K
*
+
(
→
K
0
S
π
+
)
μ
+
μ
−
decay using
9
fb
−
1
of
p
p
collision data collected with the LHCb experiment. For the first time, the full set of
C
P
-averaged angular observables is measured in intervals of the dimuon invariant mass squared. Local deviations from standard model predictions are observed, similar to those in previous LHCb analyses of the isospin-partner
B
0
→
K
*
0
μ
+
μ
−
decay. The global tension is dependent on which effective couplings are considered and on the choice of theory nuisance parameters
- …