48 research outputs found
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
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- Ahmadov F
- Ahmed WS
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- Aielli G
- Aizenberg I
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- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi F
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- Ali S
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- Allport PP
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- Alviggi MG
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- Amelung C
- Amidei D
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- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
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- Anders JK
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- Angelidakis S
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- Anisenkov AV
- Annovi A
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- Anthony MT
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- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Appelt C
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- Arcangeletti C
- Arce ATH
- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Assahsah J
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- Zhemchugov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Accuracy versus precision in boosted top tagging with the ATLAS detector
- Author
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- Aakvaag E
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- Abdelhameed S
- Abeling K
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- Fenton MJ
- Ferencz L
- Ferguson RAM
- Fernandez AA
- Fernoux MJV
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
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- Ferrer JAV
- Ferrere D
- Ferretti C
- Fiacco D
- Fiedler F
- Fiedler P
- Filho LEB
- Filipčič A
- Filmer EK
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fisher WC
- Fitschen T
- Fitzhugh PM
- Fleck I
- Fleischmann P
- Flick T
- Flores CAA
- Flores M
- Follega FM
- Fomin N
- Foo JH
- Formica A
- Forti AC
- Fortin E
- Fortman AW
- Foti MG
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- Fox H
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- Gabrielli A
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- Gaid S
- Galantzan S
- Gallas EJ
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- García C
- Gardner GL
- Gardner RW
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- Garg D
- Garg RB
- Gargan JM
- Garner CA
- Garrido SF
- Garvey CM
- Garzon GOY
- Gassmann VK
- Gaudio G
- Gautam V
- Gauzzi P
- Gavranovic J
- Gavrilenko IL
- Gavrilyuk A
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- Gekow A
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- Genest MH
- Gentry AD
- George S
- George WF
- Geralis T
- Gessinger-Befurt P
- Geyik ME
- Ghani M
- Ghazali YE
- Ghorbanian K
- Ghosal A
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- Ghosh A
- Giacobbe B
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- Giannini A
- Gibson SM
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- Gilbert AK
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- Gillberg D
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- Ginabat L
- Gingrich DM
- Giordani MP
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- Giugni D
- Giuli F
- Gkialas I
- Gladilin LK
- Glasman C
- Gledhill GR
- Glemža G
- Glisic M
- Gnesi I
- Go Y
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- Gocke B
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- Gokturk B
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- Gololo MGD
- Golubkov D
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- Gonzalez SV
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- Gonçalo R
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- Gorini B
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- Goshaw AT
- Gostkin MI
- Goswami S
- Gottardo CA
- Gotz SA
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- Goussiou AG
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- Gramstad E
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- Grant CM
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- Gravili FG
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- Gregor IM
- Greif KT
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- Gross E
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- Grundy JC
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- Guardia AB
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- Guida A
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- Guindon S
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- Gurdasani SS
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- Hangal DA
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- Harris YT
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- Hasegawa Y
- Haslbeck F
- Hassan S
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- Hawkings RJ
- Hayashi Y
- Hayden D
- Hayes C
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- Hays CP
- Hays JM
- Hayward HS
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- Heatley NB
- Hedberg V
- Heggelund AL
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- Hertenberger R
- Hervas L
- Hesping ME
- Hessey NP
- Hidaoui M
- Hidic N
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- Horii Y
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- Hrynevich A
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- Hsu S-C
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- Huang X
- Huang Y
- Huang Y
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- Iakovidis G
- Ibanez AP
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- Iglesias JAS
- Iguchi R
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- Iizawa T
- Ikegami Y
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- Irwin RK
- Ishino M
- Islam W
- Issever C
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- Izzo V
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- Jiménez YH
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- Ju X
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- Kalaitzidou I
- Kalderon CW
- Kang NJ
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- Kareem MJ
- Karentzos E
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- Karpova ZM
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- Karyukhin AN
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- Keeler R
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- Klimentov A
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- Koch SF
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- Kolay O
- Koletsou I
- Komarek T
- Kong AXY
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- Kontaxakis P
- Konya B
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- Kostyukhin VV
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- Kotwal A
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- Kourlitis E
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- Kurdysh O
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- Kyriacou NG
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- Lahbabi FZ
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- Latonova V
- Latour BMD
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- Le Pottier LT
- Le B
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- Liberti B
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- Luengo SIF
- Luise I
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- Ogrodnik A
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- Okumura Y
- Oleksiyuk I
- Oliveira MVS
- Oliver JL
- Onofre A
- Onyisi PUE
- Oreglia MJ
- Orellana GE
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- Ospanov R
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- Ovsiannikova T
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- Pizzi DA
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- Poblete PAU
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- Pollock ZB
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- Popa S
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- Poreba A
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- Zhemchugov A
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- Zimine NI
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- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- IOP Publishing
- Publication date
- 01/08/2024
- Field of study
Abstract
The identification of top quark decays where the top quark has a large momentum transverse to the beam axis, known as top tagging, is a crucial component in many measurements of Standard Model processes and searches for beyond the Standard Model physics at the Large Hadron Collider.
Machine learning techniques have improved the performance of top tagging algorithms, but the size of the systematic uncertainties for all proposed algorithms has not been systematically studied.
This paper presents the performance of several machine learning based top tagging algorithms on a dataset constructed from simulated proton-proton collision events measured with the ATLAS detector at √
s
= 13 TeV.
The systematic uncertainties associated with these algorithms are estimated through an approximate procedure that is not meant to be used in a physics analysis, but is appropriate for the level of precision required for this study.
The most performant algorithms are found to have the largest uncertainties, motivating the development of methods to reduce these uncertainties without compromising performance.
To enable such efforts in the wider scientific community, the datasets used in this paper are made publicly available.</jats:p
Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
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- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
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- Aizenberg I
- Akatsuka S
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- Alberghi GL
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- Aleksa M
- Aleksandrov IN
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- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
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- Cabras G
- Caforio D
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- Cakir IT
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- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
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- Cameron D
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- Canale V
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- Castillo FL
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- Catmore JR
- Cattai A
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- Celli F
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- Cheng CL
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- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
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- Chou Y
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- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
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- Ciubotaru DA
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- Corpe LD
- Corradi M
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- Cueto A
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- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
- Dabrowski W
- Dado T
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- Dawson I
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- de Jong P
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- De Maria A
- De Pedis D
- de Renstrom PAB
- De Sa RCL
- De Salvo A
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- De Vivie De Regie JB
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- Dodsworth D
- Doglioni C
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- Donato CD
- Donell DMM
- Dong B
- Donini J
- Donszelmann TC
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- Dova MT
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- Drechsler E
- Dreyer E
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- Dubreuil A
- Duchovni E
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- Dumitriu AE
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- Durglishvili A
- Dutta B
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- Dührssen M
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- D’Auria S
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- Eggleston MG
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- Farthouat P
- Fassi F
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- Fayard L
- Fedin OL
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- Fenyuk AB
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- Filipčič A
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fischer F
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- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flierl BM
- Flores L
- Flores M
- Follega FM
- Fomin N
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- Forland BC
- Formica A
- Forti AC
- Fortin E
- Foti MG
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- Freund WS
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- Furelos DV
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- Gallas EJ
- Gallop BJ
- Galvan IS
- Gama RG
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- Gargiulo S
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- Gavrilenko IL
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- Ghazali YE
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- Giordani MP
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- Girolamo AD
- Giugliarelli G
- Giugni D
- Giuli F
- Gkialas I
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- Gorišek A
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- Gostkin MI
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- Liberti B
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- Lipniacka A
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- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wollrath J
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- Wyatt TR
- Wynne BM
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- Xiotidis I
- Xu D
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- Yabsley B
- Yacoob S
- Yamaguchi N
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- Yamatani M
- Yamauchi H
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- Yao W-M
- Yap YC
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- Yeletskikh I
- Yexley MR
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LFG
- Zaid E
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
This paper presents the measurement of the electroweak production of two jets
in association with a Zγ pair with the Z boson decaying into two
neutrinos. It also presents the search for invisible or partially invisible
decays of a Higgs boson with a mass of 125 GeV produced through vector-boson
fusion with a photon in the final state. These results use data from LHC
proton-proton collisions at s = 13 TeV collected with the ATLAS
detector corresponding to an integrated luminosity of 139 fb−1. The event
signature, shared by all benchmark processes considered for measurements and
searches, is characterized by a significant amount of unbalanced transverse
momentum and a photon in the final state, in addition to a pair of forward
jets. For electroweak production of Zγ in association with two jets, the
background-only hypothesis is rejected with an observed (expected) significance
of 5.2 (5.1) standard deviations. The measured fiducial cross-section for this
process is 1.31±0.29 fb. Observed (expected) upper limit of 0.37 (0.34) at
95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to
invisible particles, assuming the Standard Model production cross-section. The
signature is also interpreted in the context of decays of a Higgs boson to a
photon and a dark photon. An observed (expected) 95% CL upper limit on the
branching ratio for this decay is set at 0.018 (0.017), assuming the 125 GeV
Standard Model Higgs boson production cross-section
Uptake and reduction of Se(IV) in two heterotrophic aerobic <em>Pseudomonads</em> strains isolated from boreal bog environment
- Author
- Brown TA Shrift A
- Bryant RD Laishley EJ
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2017
- Field of study
Disorders of the enteric nervous system — a holistic view
- Author
- 1000 Genomes Project Consortium
- A Abdoli
- A Akbar
- A Akbar
- A Bahrami
- A Cabal
- A Chalazonitis
- A Fasano
- A Gosain
- A Kozlowska
- A Lionett
- A Lionnet
- A Prasad
- A Schwiertz
- A Serra
- A Torroglosa
- A Tullio-Pelet
- A Ueki
- A Zauszkiewicz-Pawlak
- AD Farmer
- AJ Bergner
- AJ Burns
- AL Kirchgessner
- AM Goldstein
- AM Toure
- AR Trevizan
- AS Rolig
- B Aryal
- B Chandrasekharan
- B Liu
- B Luzon-Toro
- B Sovran
- BA Killinger
- BD Gulbransen
- BG Nezami
- BN Dugger
- BN Dugger
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- C Brandscheid
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- C Laranjeira
- C Mancuso
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- CH Knowles
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- DJ Lanska
- DM James
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- M Wunsch
- MA Odenwald
- MD Gershon
- MD Gershon
- MF Vaezi
- MJ Farthing
- MJ Workman
- ML Ferrari
- MM France
- MM Kaelberer
- MM Unger
- MP Murphy
- MP Sanchez
- MS Cirstea
- MT Liu
- MW Moore
- N Bodi
- N Jain
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- N Manabe
- N Nekrep
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- OB Tysnes
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- P Agostinho
- P Borghammer
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- PA Hughes
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- PP van der Veek
- PS Kabouridis
- R Bernier
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- X Cheng
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Recommended from our members
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGO–Virgo Network
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi RA
- Allocca A
- Alléné C
- Altin PA
- Amato A
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Ansoldi S
- Antelis JM
- Antier S
- Apostolatos T
- Appavuravther EZ
- Appert S
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- Areeda JS
- Arellano FE Peña
- Aritomi N
- Arnaud N
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- Bartlett J
- Barton MA
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- Bedakihale VM
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- Bell AS
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- Wysocki DM
- Xiao L
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- Yamada T
- Yamamoto H
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- Yamashita K
- Yamazaki R
- Yang FW
- Yang KZ
- Yang L
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- Yang Yang
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeidler S
- Zelenova T
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- Zevin M
- Zhan M
- Zhang H
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- Zhao Yue
- Zheng Y
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- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- The Astrophysical Journal
- Publication date
- 05/08/2024
- Field of study
Abstract
Gravitational lensing by massive objects along the line of sight to the source causes distortions to gravitational wave (GW) signals; such distortions may reveal information about fundamental physics, cosmology, and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO-Virgo network. We search for repeated signals from strong lensing by (1) performing targeted searches for subthreshold signals, (2) calculating the degree of overlap among the intrinsic parameters and sky location of pairs of signals, (3) comparing the similarities of the spectrograms among pairs of signals, and (4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by (1) frequency-independent phase shifts in strongly lensed images, and (2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the nondetection of GW lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects.</jats:p
Model-based Cross-correlation Search for Gravitational Waves from the Low-mass X-Ray Binary Scorpius X-1 in LIGO O3 Data
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Aguiar OD
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- Akutsu T
- Albanesi S
- Alfaidi RA
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- Alléné C
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- Amato A
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Ansoldi S
- Antelis JM
- Antier S
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- Areeda JS
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- Bagnasco S
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- Baird J
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- Bakel NV
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- Barker D
- Barneo P
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- Bedakihale VM
- Beirnaert F
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- Blackburn JK
- Blair CD
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- Yelikar AB
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- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2022
- Field of study
We present the results of a model-based search for continuous gravitational waves from the low-mass X-ray binary Scorpius X-1 using LIGO detector data from the third observing run of Advanced LIGO and Advanced Virgo. This is a semicoherent search that uses details of the signal model to coherently combine data separated by less than a specified coherence time, which can be adjusted to balance sensitivity with computing cost. The search covered a range of gravitational-wave frequencies from 25 to 1600 Hz, as well as ranges in orbital speed, frequency, and phase determined from observational constraints. No significant detection candidates were found, and upper limits were set as a function of frequency. The most stringent limits, between 100 and 200 Hz, correspond to an amplitude h0 of about 10−25 when marginalized isotropically over the unknown inclination angle of the neutron star's rotation axis, or less than 4 × 10−26 assuming the optimal orientation. The sensitivity of this search is now probing amplitudes predicted by models of torque balance equilibrium. For the usual conservative model assuming accretion at the surface of the neutron star, our isotropically marginalized upper limits are close to the predicted amplitude from about 70 to 100 Hz; the limits assuming that the neutron star spin is aligned with the most likely orbital angular momentum are below the conservative torque balance predictions from 40 to 200 Hz. Assuming a broader range of accretion models, our direct limits on gravitational-wave amplitude delve into the relevant parameter space over a wide range of frequencies, to 500 Hz or more
Search for subsolar-mass black hole binaries in the second part of Advanced LIGO’s and Advanced Virgo’s third observing run
- Author
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- Macquet A
- Magazzù C
- Magee RM
- Maggiore R
- Magnozzi M
- Mahesh S
- Majorana E
- Makarem CN
- Maksimovic I
- Maliakal S
- Malik A
- Man N
- Mandic V
- Mangano V
- Mannix BR
- Mansell GL
- Mansingh G
- Manske M
- Mantovani M
- Mapelli M
- Marchesoni F
- Marion F
- Mark Z
- Markakis C
- Markosyan AS
- Markowitz A
- Maros E
- Marquina A
- Marsat S
- Martelli F
- Martin IW
- Martin RM
- Martinez M
- Martinez V
- Martinez VA
- Martinovic K
- Martynov DV
- Marx EJ
- Masalehdan H
- Mason K
- Masserot A
- Masso-Reid M
- Mastrogiovanni S
- Matas A
- Mateu-Lucena M
- Matiushechkina M
- Mavalvala N
- Ma’arif M
- McCann JJ
- McCarthy R
- McClelland DE
- McClincy PK
- McCormick S
- McCuller L
- McGhee GI
- McGinn J
- McGuire SC
- McIsaac C
- McIver J
- McLeod A
- McRae T
- McWilliams ST
- Meacher D
- Mehmet M
- Mehta AK
- Meijer Q
- Melatos A
- Melo ITE
- Mendell G
- Menendez-Vazquez A
- Menoni CS
- Mercer RA
- Mereni L
- Merfeld K
- Merilh EL
- Merritt JD
- Merzougui M
- Messenger C
- Messick C
- Meyers PM
- Meylahn F
- Mhaske A
- Miani A
- Miao H
- Michaloliakos I
- Michel C
- Michimura Y
- Middleton H
- Mihaylov DP
- Miller A
- Miller AL
- Miller B
- Millhouse M
- Mills JC
- Milotti E
- Minenkov Y
- Mio N
- Mir LM
- Miravet-Tenés M
- Mishkin A
- Mishra C
- Mishra T
- Mistry T
- Mitchell AL
- Mitra S
- Mitrofanov VP
- Mitselmakher G
- Mittleman R
- Miyakawa O
- Miyo K
- Miyoki S
- Mo G
- Modafferi LM
- Moguel E
- Mogushi K
- Mohapatra SRP
- Mohite SR
- Molina-Ruiz M
- Mondal C
- Mondin M
- Montani M
- Moore CJ
- Moragues J
- Morales ER
- Moraru D
- Morawski F
- More A
- More S
- Moreno C
- Moreno G
- Mori Y
- Morisaki S
- Morisue N
- Moriwaki Y
- Morras G
- Mours B
- Mow-Lowry CM
- Mozzon S
- Mu niz EA
- Muciaccia F
- Mukherjee D
- Mukherjee S
- Mukherjee S
- Mukherjee S
- Mukund N
- Mullavey A
- Munch J
- Murray PG
- Muusse S
- Márka S
- Márka Z
- Nadji SL
- Nagano K
- Nagar A
- Nagar T
- Nakamura K
- Nakano H
- Nakano M
- Nakayama Y
- Napolano V
- Nardecchia I
- Narola H
- Naticchioni L
- Nayak RK
- Neil BF
- Neilson J
- Nelson A
- Nelson TJN
- Nery M
- Neubauer P
- Neunzert A
- Ng KY
- Ng SWS
- Nguyen C
- Nguyen P
- Nguyen T
- Ni J
- Ni W-T
- Nichols SA
- Nieradka G
- Nishimoto T
- Nishizawa A
- Nissanke S
- Nitoglia E
- Niu W
- Nocera F
- Norman M
- North C
- Notte J
- Novak J
- Nozaki S
- Nurbek G
- Nuttall LK
- Obayashi Y
- Oberling J
- Oelker E
- Oertel M
- Ogaki W
- Oganesyan G
- Oh JJ
- Oh K
- Oh SH
- Ohashi M
- Ohashi T
- Ohkawa M
- Ohme F
- Ohta H
- Okutani Y
- Oliveri R
- Olivetto C
- Oohara K
- Oram R
- Ormiston RG
- Ormsby ND
- Orselli M
- Oshino S
- Ossokine S
- Osthelder C
- Otabe S
- Ottaway DJ
- Overmier H
- O’Brien BD
- O’Dell J
- O’Hanlon T
- O’Reilly B
- O’Shaughnessy R
- O’Shea E
- Pace AE
- Pagano G
- Pagano R
- Pagliaroli G
- Pai A
- Pai SA
- Pal S
- Palamos JR
- Palashov O
- Palomba C
- Pan K-C
- Panda PK
- Pang PTH
- Pannarale F
- Pant BC
- Panther FH
- Paoletti F
- Paoli A
- Paolone A
- Pappas G
- Parisi A
- Park J
- Parker W
- Pascucci D
- Pasqualetti A
- Passaquieti R
- Passuello D
- Patel M
- Patel NR
- Pathak M
- Patricelli B
- Patron AS
- Paul S
- Payne E
- Pedraza M
- Pedurand R
- Pegna R
- Pegoraro M
- Pele A
- Penano S
- Penn S
- Perego A
- Pereira A
- Pereira T
- Perez CJ
- Perkins CC
- Perreca A
- Perriès S
- Perry JW
- Pesios D
- Petermann J
- Pfeiffer HP
- Pham H
- Pham KA
- Phukon KS
- Phurailatpam H
- Piccinni OJ
- Pichot M
- Piendibene M
- Piergiovanni F
- Pierini L
- Pierra G
- Pierro V
- Pillant G
- Pillas M
- Pilo F
- Pina DM
- Pinard L
- Pineda-Bosque C
- Pinto IM
- Pinto M
- Piotrzkowski BJ
- Piotrzkowski K
- Pirello M
- Pitkin MD
- Placidi A
- Placidi E
- Planas ML
- Plastino W
- Poggiani R
- Polini E
- Pong DYT
- Ponrathnam S
- Porter EK
- Portilla ML
- Posnansky C
- Poulton R
- Powell J
- Pracchia M
- Pradier T
- Prajapati AK
- Prasai K
- Prasanna R
- Pratten G
- Principe M
- Prodi GA
- Prokhorov L
- Prosposito P
- Prudenzi L
- Puecher A
- Punturo M
- Puosi F
- Puppo P
- Périgois C
- Pürrer M
- Qi H
- Quartey N
- Quetschke V
- Quinonez PJ
- Quitzow-James R
- Quynh LN
- Raab FJ
- Raaijmakers G
- Radkins H
- Radulesco N
- Raffai P
- Rail SX
- Raja S
- Rajan C
- Ramirez KE
- Ramirez TD
- Ramos-Buades A
- Rana D
- Rana J
- Rangnekar PR
- Rapagnani P
- Ray A
- Raymond V
- Raza N
- Razzano M
- Read J
- Regimbau T
- Rei L
- Reid S
- Reid SW
- Reinhard M
- Reitze DH
- Relton P
- Renzini A
- Rettegno P
- Revenu B
- Reyes J
- Reza A
- Rezac M
- Rezaei AS
- Ricci F
- Richards D
- Richardson JW
- Richardson L
- Riles K
- Rinaldi S
- Robertson C
- Robertson NA
- Robie R
- Robinet F
- Rocchi A
- Rodriguez S
- Rolland L
- Rollins JG
- Romanelli M
- Romano R
- Romel CL
- Romero A
- Romero-Shaw IM
- Romie JH
- Ronchini S
- Roocke TJ
- Rosa IL
- Rosa L
- Rose CA
- Rosińska D
- Ross MP
- Rossello M
- Rowan S
- Rowlinson SJ
- Roy S
- Roy S
- Royzman A
- Rozza D
- Ruggi P
- Ruiz-Rocha K
- Ryan K
- Sachdev S
- Sadecki T
- Sadiq J
- Saffarieh P
- Saha S
- Saito Y
- Sakai K
- Sakellariadou M
- Sakon S
- Salafia OS
- Salces-Carcoba F
- Salconi L
- Saleem M
- Salemi F
- Sallé M
- Samajdar A
- San Martín ENT
- Sanchez EJ
- Sanchez JH
- Sanchez LE
- Sanchis-Gual N
- Sanders JR
- Sanuy A
- Saravanan TR
- Sarin N
- Sasli A
- Sassolas B
- Satari H
- Sathyaprakash BS
- Sauter O
- Savage RL
- Savant V
- Sawada T
- Sawant HL
- Sayah S
- Schaetzl D
- Scheel M
- Scheuer J
- Schiworski MG
- Schmidt P
- Schmidt S
- Schnabel R
- Schneewind M
- Schofield RMS
- Schulte BW
- Schutz BF
- Schwartz E
- Schönbeck A
- Scott J
- Scott SM
- Seglar-Arroyo M
- Sekiguchi Y
- Sellers D
- Sengupta AS
- Sentenac D
- Seo EG
- Sequino V
- Sergeev A
- Servignat G
- Shaffer YST
- Shahriar MS
- Shaikh MA
- Shams B
- Shandera S
- Shao L
- Sharma A
- Sharma P
- Shawhan P
- Shcheblanov NS
- Sheela A
- Sheridan E
- Shikano Y
- Shikauchi M
- Shimizu H
- Shimode K
- Shinkai H
- Shishido T
- Shoda A
- Shoemaker DH
- Shoemaker DM
- ShyamSundar S
- Sieniawska M
- Sigg D
- Silenzi L
- Siles JFN
- Singer LP
- Singh D
- Singh MK
- Singh N
- Singha A
- Sintes AM
- Sipala V
- Skliris V
- Slagmolen BJJ
- Slaven-Blair TJ
- Smetana J
- Smith JR
- Smith L
- Smith RJE
- Soldateschi J
- Somala SN
- Somiya K
- Song I
- Soni K
- Soni S
- Sordini V
- Sorrentino F
- Sorrentino N
- Soulard R
- Souradeep T
- Spagnuolo V
- Spencer AP
- Spera M
- Spinicelli P
- Srivastava AK
- Srivastava V
- Stachie C
- Stachurski F
- Steer DA
- Steinlechner J
- Steinlechner S
- Stergioulas N
- Stevenson S
- Stops DJ
- Strain KA
- Strang LC
- Stratta G
- Strong MD
- Strunk A
- Sturani R
- Stuver AL
- Subrahmanya SC
- Suchenek M
- Sudhagar S
- Sugimoto R
- Suh HG
- Sullivan AG
- Summerscales TZ
- Sun L
- Sunil S
- Sur A
- Suresh J
- Sutton PJ
- Suzuki T
- Suzuki T
- Suzuki T
- Swinkels BL
- Syx A
- Szczepańczyk MJ
- Szewczyk P
- Tacca M
- Tagoshi H
- Tait SC
- Takahashi H
- Takahashi R
- Takano S
- Takeda H
- Takeda M
- Talbot C
- Talbot CJ
- Tamanini N
- Tanaka K
- Tanaka T
- Tanaka T
- Tanasijczuk AJ
- Tanioka S
- Tanner DB
- Tao D
- Tao L
- Tapia RD
- Taranto C
- Taruya A
- Tasson JD
- Tenorio R
- Terhune JES
- Terkowski L
- Themann H
- Thirugnanasambandam MP
- Thomas M
- Thomas P
- Thomas S
- Thompson D
- Thompson EE
- Thompson JE
- Thondapu SR
- Thorne KA
- Thrane E
- Tiwari S
- Tiwari S
- Tiwari V
- Toivonen AM
- Tolley AE
- Tomaru T
- Tomura T
- Tonelli M
- Torres-Forné A
- Torrie CI
- Tournefier E
- Trapananti A
- Travasso F
- Traylor G
- Trenado J
- Trevor M
- Tringali MC
- Tripathee A
- Troiano L
- Trovato A
- Trozzo L
- Trudeau RJ
- Tsai D
- Tsang KW
- Tsang T
- Tsao J-S
- Tse M
- Tso R
- Tsuchida S
- Tsukada L
- Tsuna D
- Tsutsui T
- Turbang K
- Turconi M
- Turski C
- Tuyenbayev D
- Töyrä D
- Ubach H
- Ubhi AS
- Uchiyama T
- Udall RP
- Ueda A
- Uehara T
- Ueno K
- Ueshima G
- Unnikrishnan CS
- Urban AL
- Ushiba T
- Utina A
- Vahlbruch H
- Vaidya N
- Vajente G
- Vajpeyi A
- Valdes G
- Valentini M
- Vallero S
- Valsan V
- van Bakel N
- van Beuzekom M
- van Dael M
- Van de Walle A
- van den Brand JFJ
- Van Den Broeck C
- van Dongen J
- van Haevermaet H
- van Heijningen JV
- van Putten MHPM
- van Ranst Z
- van Remortel N
- Vander-Hyde DC
- Vanosky J
- Vardaro M
- Vargas AF
- Varma V
- Vasúth M
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venneberg J
- Venugopalan G
- Verdier P
- Verkindt D
- Verma P
- Verma Y
- Vermeulen SM
- Veske D
- Vetrano F
- Viceré A
- Vidyant S
- Viets AD
- Vijaykumar A
- Villa-Ortega V
- Vinet J-Y
- Virtuoso A
- Vitale S
- Vivanco FH
- Vocca H
- von Reis ERG
- von Wrangel JSA
- Vorvick C
- Vyatchanin SP
- Wade LE
- Wade M
- Wagner KJ
- Walet RC
- Walker M
- Wallace GS
- Wallace L
- Wang J
- Wang JZ
- Wang WH
- Ward RL
- Warner J
- Was M
- Washimi T
- Washington NY
- Watada K
- Watarai D
- Watchi J
- Wayt KE
- Weaver B
- Weaving CR
- Webster SA
- Weinert M
- Weinstein AJ
- Weiss R
- Weller CM
- Weller RA
- Wellmann F
- Wen L
- Wette K
- Weßels P
- Whelan JT
- White DD
- Whiting BF
- Whittle C
- Wilk OS
- Wilken D
- Williams CE
- Williams D
- Williams MJ
- Williamson AR
- Willis JL
- Willke B
- Wipf CC
- Woan G
- Woehler J
- Wofford JK
- Wojtowicz IA
- Wong D
- Wong ICF
- Wright M
- Wu C
- Wu DS
- Wu H
- Wysocki DM
- Xiao L
- Yadav N
- Yamada T
- Yamamoto H
- Yamamoto K
- Yamamoto T
- Yamashita K
- Yamazaki R
- Yang FW
- Yang KZ
- Yang L
- Yang Y
- Yang Y
- Yang Y-C
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu H
- Yu H
- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Y
- Zhao C
- Zhao G
- Zhao Y
- Zhao Y
- Zheng Y
- Zhou R
- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 28/02/2023
- Field of study
Recommended from our members
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGO–Virgo Network
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi RA
- Allocca A
- Alléné C
- Altin PA
- Amato A
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Ansoldi S
- Antelis JM
- Antier S
- Apostolatos T
- Appavuravther EZ
- Appert S
- Apple SK
- Arai K
- Araya A
- Araya MC
- Areeda JS
- Arellano FE Peña
- Aritomi N
- Arnaud N
- Arogeti M
- Aronson SM
- Arène M
- Asada H
- Ashton G
- Aso Y
- Assiduo M
- Aston SM
- Astone P
- Aubin F
- AultONeal K
- Babak S
- Badaracco F
- Badger C
- Bae S
- Bae Y
- Bagnasco S
- Bai Y
- Baier JG
- Baird J
- Bajpai R
- Baka T
- Ball M
- Ballardin G
- Ballmer SW
- Baltus G
- Banagiri S
- Banerjee B
- Bankar D
- Barayoga JC
- Barish BC
- Barker D
- Barneo P
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton MA
- Bartos I
- Basak S
- Bassiri R
- Basti A
- Bawaj M
- Bayley JC
- Bazzan M
- Bedakihale VM
- Beirnaert F
- Bejger M
- Belahcene I
- Bell AS
- Benedetto V
- Beniwal D
- Benoit W
- Bentley JD
- BenYaala M
- Bera S
- Berbel M
- Bergamin F
- Berger BK
- Bernuzzi S
- Beroiz M
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Beveridge D
- Bhandare R
- Bhandari AV
- Bhardwaj U
- Bhatt R
- Bhattacharjee D
- Bhaumik S
- Bianchi A
- Bilenko IA
- Bilicki M
- Billingsley G
- Bini S
- Birnholtz O
- Biscans S
- Bischi M
- Biscoveanu S
- Bisht A
- Biswas B
- Bitossi M
- Bizouard M-A
- Blackburn JK
- Blair CD
- Blair DG
- Blair RM
- Bobba F
- Bode N
- Bogaert G
- Boldrini M
- Bolingbroke GN
- Bonavena LD
- Bondarescu R
- Bondu F
- Bonilla E
- Bonnand R
- Booker P
- Bork R
- Boschi V
- Bose N
- Bose S
- Bossilkov V
- Boudart V
- Bouffanais Y
- Bozzi A
- Boër M
- Bradaschia C
- Brady PR
- Bramley A
- Branch A
- Branchesi M
- Brand JFJ van den
- Brau JE
- Breschi M
- Briant T
- Briggs JH
- Brillet A
- Brinkmann M
- Brockill P
- Broeck C Van Den
- Brooks AF
- Brooks J
- Brown DD
- Brunett S
- Bruno G
- Bruntz R
- Bryant J
- Bucci F
- Buchanan J
- Bulik T
- Bulten HJ
- Buonanno A
- Burtnyk K
- Buscicchio R
- Buskulic D
- Bustillo J Calderón
- Buy C
- Byer RL
- Bécsy B
- Cabras G
- Cabrita R
- Cadonati L
- Cagnoli G
- Cahillane C
- Callaghan JD
- Callister TA
- Calloni E
- Camp JB
- Canepa M
- Caneva G
- Cannavacciuolo M
- Cannon KC
- Cao H
- Cao Z
- Capistran LA
- Capocasa E
- Capote E
- Carapella G
- Carbognani F
- Carlassara M
- Carlin JB
- Carpinelli M
- Carrillo G
- Carter JJ
- Carullo G
- Casentini C
- Castaldi G
- Caudill S
- Cavaglià M
- Cavalier F
- Cavalieri R
- Cella G
- Cerdá-Durán P
- Cesarini E
- Chaibi W
- Chakalis W
- Champion E
- Chan C
- Chan C-H
- Chan CL
- Chan K
- Chan M
- Chandra K
- Chang IP
- Chang W
- Chanial P
- Chao S
- Chapman-Bird C
- Charlton P
- Chassande-Mottin E
- Chatterjee C
- Chatterjee Debarati
- Chatterjee Deep
- Chaturvedi M
- Chaty S
- Chatziioannou K
- Chen C
- Chen D
- Chen HY
- Chen J
- Chen K
- Chen X
- Chen Y
- Chen Y-B
- Chen Y-R
- Cheng H
- Chessa P
- Cheung HY
- Chia HY
- Chiadini F
- Chiang C-Y
- Chiarini G
- Chierici R
- Chincarini A
- Chiofalo ML
- Chiummo A
- Choudhary RK
- Choudhary S
- Christensen N
- Chu Q
- Chu Y-K
- Chua SSY
- Chung KW
- Ciani G
- Ciecielag P
- Cieślar M
- Cifaldi M
- Ciobanu AA
- Ciolfi R
- Clara F
- Clark JA
- Clarke TA
- Clearwater P
- Clesse S
- Cleva F
- Coccia E
- Codazzo E
- Cohadon P-F
- Cohen DE
- Colleoni M
- Collette CG
- Colombo A
- Colpi M
- Compton CM
- Conti L
- Cooper SJ
- Corban P
- Corbitt TR
- Cordero-Carrión I
- Corezzi S
- Cornish NJ
- Corsi A
- Cortese S
- Coschizza AC
- Cotesta R
- Cottingham R
- Coughlin MW
- Coulon J-P
- Countryman ST
- Cousins B
- Couvares P
- Coward DM
- Cowart MJ
- Coyne DC
- Coyne R
- Craig K
- Creighton JDE
- Creighton TD
- Criswell AW
- Croquette M
- Crowder SG
- Cudell JR
- Cullen TJ
- Cumming A
- Cummings R
- Cuoco E
- Curyło M
- Dabadie P
- Dal Canton T
- Dall’Osso S
- Dana A
- Danilishin S
- Danzmann K
- Darsow-Fromm C
- Dasgupta A
- Datrier LEH
- Datta Sayak
- Datta Sayantani
- Dattilo V
- Dave I
- Davier M
- Davies GS Cabourn
- Davis D
- Davis MC
- Daw EJ
- Dax M
- De Laurentis M
- De Lillo F
- De Lillo N
- De Matteis F
- De Pietri R
- De Rosa R
- De Rossi C
- De Simone R
- DeBra D
- Deenadayalan M
- Degallaix J
- Del Favero V
- Del Pozzo W
- Dell’Aquila D
- Deléglise S
- Demos N
- Dent T
- Depasse A
- DeSalvo R
- Dhurandhar S
- Di Fiore L
- Di Fronzo C
- Di Giorgio C
- Di Giovanni F
- Di Giovanni M
- Di Girolamo T
- Di Lieto A
- Di Michele A
- Di Pace S
- Di Palma I
- Di Renzo F
- Diab R
- Diaz J Casanueva
- Didio NA
- Dietrich T
- Diksha D
- Divakarla AK
- Dmitriev A
- Doctor Z
- Doleva PP
- Donahue L
- Donovan F
- Dooley KL
- Dooney T
- Doravari S
- Dorosh O
- Drago M
- Driggers JC
- Drori Y
- Ducoin J-G
- Dunn L
- Dupletsa U
- Durante O
- Duverne P-A
- Dwyer SE
- Dálya G
- Díaz MC
- D’Angelo B
- D’Antonio S
- D’Emilio V
- D’Onofrio L
- D’Urso D
- Eassa C
- Easter PJ
- Ebersold M
- Eckhardt T
- Eddolls G
- Edelman B
- Edo TB
- Edy O
- Effler A
- Eguchi S
- Eichholz J
- Eikenberry SS
- Eisenmann M
- Eisenstein RA
- Ejlli A
- Engelby E
- Enomoto Y
- Errico L
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- Yu Hang
- Yu Haocun
- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang T
- Zhang Y
- Zhao C
- Zhao G
- Zhao Y
- Zhao Yue
- Zheng Y
- Zhou R
- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- The Astrophysical Journal
- Publication date
- 01/08/2024
- Field of study
Abstract
Gravitational lensing by massive objects along the line of sight to the source causes distortions to gravitational wave (GW) signals; such distortions may reveal information about fundamental physics, cosmology, and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO-Virgo network. We search for repeated signals from strong lensing by (1) performing targeted searches for subthreshold signals, (2) calculating the degree of overlap among the intrinsic parameters and sky location of pairs of signals, (3) comparing the similarities of the spectrograms among pairs of signals, and (4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by (1) frequency-independent phase shifts in strongly lensed images, and (2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the nondetection of GW lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects.</jats:p
Searches for gravitational waves from known pulsars at two harmonics in the second and third LIGO-Virgo observing runs
- Author
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- Wysocki DM
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- Yap MJ
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- Yeh S-W
- Yelikar AB
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- Yu H
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- Zadrożny A
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- Zevin M
- Zhan M
- Zhang H
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- Zhao G
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- Zhao Y
- Zhou R
- Zhou Z
- Zhu XJ
- Zhu Z-H
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 25/05/2022
- Field of study
We present a targeted search for continuous gravitational waves (GWs) from 236 pulsars using data from the third observing run of LIGO and Virgo (O3) combined with data from the second observing run (O2). Searches were for emission from the l = m = 2 mass quadrupole mode with a frequency at only twice the pulsar rotation frequency (single harmonic) and the l = 2, m = 1, 2 modes with a frequency of both once and twice the rotation frequency (dual harmonic). No evidence of GWs was found, so we present 95% credible upper limits on the strain amplitudes h0 for the single-harmonic search along with limits on the pulsars' mass quadrupole moments Q22 and ellipticities ε. Of the pulsars studied, 23 have strain amplitudes that are lower than the limits calculated from their electromagnetically measured spin-down rates. These pulsars include the millisecond pulsars J0437−4715 and J0711−6830, which have spin-down ratios of 0.87 and 0.57, respectively. For nine pulsars, their spin-down limits have been surpassed for the first time. For the Crab and Vela pulsars, our limits are factors of ∼100 and ∼20 more constraining than their spin-down limits, respectively. For the dual-harmonic searches, new limits are placed on the strain amplitudes C21 and C22. For 23 pulsars, we also present limits on the emission amplitude assuming dipole radiation as predicted by Brans-Dicke theory