10 research outputs found
Technological change and employment: is Europe ready for the challenge?
- Author
- A Coad
- A Marshall
- A Mitra
- A Pakes
- AB Atkinson
- BH Hall
- C Edquist
- C Freeman
- C Freeman
- CB Frey
- CW Bischoff
- D Ciriaci
- D Guarascio
- E Appelbaum
- E Brynjolfsson
- E Brynjolfsson
- E Meschi
- EJ Hobsbawm
- EJ Hobsbawm
- F Aiello
- F Bogliacino
- F Bogliacino
- F Bogliacino
- F Bogliacino
- F Bogliacino
- F Crespi
- G Dosi
- G Dosi
- G Grimalda
- GSC Bruno
- GSC Bruno
- H Feldmann
- J Clark
- J Clark
- J Reenen van
- JC Musgrave
- JE Mendoza Cota
- JF Kiviet
- JR Hicks
- JR Hicks
- JS Mill
- K Marx
- K Marx
- K Wicksell
- L Gagliardi
- L Pasinetti
- M Arellano
- M Pianta
- M Pianta
- M Piva
- M Piva
- M Vivarelli
- M Vivarelli
- M Vivarelli
- M Vivarelli
- MI Nadiri
- MJG Bun
- N Greenan
- P Petit
- P Stoneman
- PJN Sinclair
- R Blundell
- R Boyer
- R Evangelista
- R Evangelista
- R Harrison
- R Layard
- R Simonetti
- S Lachenmaier
- T Antonucci
- TR Malthus
- UNIDO
- V Mastrostefano
- YS Katsoulacos
- YS Katsoulacos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for subsolar-mass black hole binaries in the second part of Advanced LIGO’s and Advanced Virgo’s third observing run
- 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 FEP
- Aritomi N
- Arnaud N
- Arogeti M
- Aronson SM
- Arun KG
- 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
- Brau JE
- Breschi M
- Briant T
- Briggs JH
- Brillet A
- Brinkmann M
- Brockill P
- 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 JC
- 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 D
- Chatterjee D
- 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 S
- Dattilo V
- Dave I
- Davier M
- Davies GSC
- 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
- de Souza Melo SA
- 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 JC
- 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
- Essick RC
- Estellés H
- Estevez D
- Etzel T
- Evans M
- Evans TM
- Evstafyeva T
- Ewing BE
- Fabrizi F
- Faedi F
- Fafone V
- Fair H
- Fairhurst S
- Fan PC
- Farah AM
- Farr B
- Farr WM
- Favaro G
- Favata M
- Fays M
- Fazio M
- Feicht J
- Fejer MM
- Fenyvesi E
- Ferguson DL
- Fernandez-Galiana A
- Ferrante I
- Ferreira TA
- Fidecaro F
- Figura P
- Fiori A
- Fiori I
- Fishbach M
- Fisher RP
- Fittipaldi R
- Fiumara V
- Flaminio R
- Floden E
- Fong HK
- Font JA
- Fornal B
- Forsyth PWF
- Franke A
- Frasca S
- Frasconi F
- Freed JP
- Frei Z
- Freise A
- Freitas O
- Frey R
- Fritschel P
- Frolov VV
- Fronzé GG
- Fujii Y
- Fujikawa Y
- Fujimoto Y
- Fulda P
- Fyffe M
- Gabbard HA
- Gabella WE
- Gadre BU
- Gair JR
- Gais J
- Galaudage S
- Gamba R
- Ganapathy D
- Ganguly A
- Gao D
- Gao D-F
- Gaonkar SG
- Garaventa B
- Garcia-Bellido J
- García-Nú nez C
- García-Quirós C
- Gardner KA
- Gargiulo J
- Garufi F
- Gasbarra C
- Gateley B
- Gayathri V
- Ge G-G
- Gemme G
- Gennai A
- George J
- Gerberding O
- Gergely L
- Ghonge S
- Ghosh A
- Ghosh A
- Ghosh S
- Ghosh S
- Ghosh T
- Giacoppo L
- Giaime JA
- Giardina KD
- Gibson DR
- Gier C
- Giri P
- Gissi F
- Gkaitatzis S
- Glanzer J
- Gleckl AE
- Godoy FG
- Godwin P
- Goetz E
- Goetz R
- Golomb J
- Goncharov B
- González G
- Gosselin M
- Gouaty R
- Gould DW
- Goyal S
- Grace B
- Grado A
- Graham V
- Granata M
- Granata V
- Gras S
- Grassia P
- Gray C
- Gray R
- Greco G
- Green AC
- Green R
- Gretarsson AM
- Gretarsson EM
- Griffith D
- Griffiths WL
- Griggs HL
- Grignani G
- Grimaldi A
- Grimm SJ
- Grote H
- Grunewald S
- Gruson AS
- Guerra D
- Guidi GM
- Guimaraes AR
- Gulati HK
- Gulminelli F
- Gunny AM
- Guo H-K
- Guo Y
- Gupta A
- Gupta A
- Gupta I
- Gupta P
- Gupta SK
- Gurs J
- Gustafson R
- Gutierrez N
- Guzman F
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- Hadiputrawan IPW
- Haegel L
- Haino S
- Halim O
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- Hannuksela O
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- Hanson J
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- Harry IW
- Hartwig D
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- Hayakawa H
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- Hayes FJ
- Healy J
- Heidmann A
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- Jadhav SP
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- Passuello D
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- Wysocki DM
- Xiao L
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- Yamashita K
- Yamazaki R
- Yang FW
- Yang KZ
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- Yang Y
- Yang Y-C
- Yap MJ
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- Yeh S-W
- Yelikar AB
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu H
- Yu H
- Yuzurihara H
- Zadrożny A
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- 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
Search for gravitational waves from Scorpius X-1 with a hidden Markov model in O3 LIGO data
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi RA
- Allocca A
- Altin PA
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
- Andres N
- Andres-Carcasona M
- Andric T
- Angelova SV
- Ansoldi S
- Antelis JM
- Antier S
- Apostolatos T
- Appavuravther EZ
- Appert S
- Apple SK
- Arai K
- Araya A
- Araya MC
- Areeda JS
- Arellano FEP
- Arene M
- Aritomi N
- Arnaud N
- Arogeti M
- Aronson SM
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Assiduo M
- Aston SM
- Astone P
- Aubin F
- AultONeal K
- Austin C
- Babak S
- Badaracco F
- Bader MKM
- Badger C
- Bae S
- Bae Y
- Baer AM
- Bagnasco S
- Bai Y
- Baird J
- Bajpai R
- Baka T
- Ball M
- Ballardin G
- Ballmer SW
- Balsamo A
- Baltus G
- Banagiri S
- Banerjee B
- Bankar D
- Barayoga JC
- Barbieri C
- 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
- Becher BR
- Becsy B
- Bedakihale VM
- Beirnaert F
- Bejger M
- Belahcene I
- Benedetto V
- Beniwal D
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- Bennett TF
- Bentley JD
- BenYaala M
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- Berbel M
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- Berger BK
- Bernuzzi S
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- Betzwieser J
- Beveridge D
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- Bhardwaj U
- Bhatt R
- Bhattacharjee D
- Bhaumik S
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- Bilenko IA
- Billingsley G
- Bini S
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- Birnholtz O
- Biscans S
- Bischi M
- Biscoveanu S
- Bisht A
- Biswas B
- Bitossi M
- Bizouard M-A
- Blackburn JK
- Blair CD
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- Bouffanais Y
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- Clara F
- Clark JA
- Clearwater P
- Clesse S
- Cleva F
- Coccia E
- Codazzo E
- Cohadon P-F
- Cohen DE
- Collaboration KAGRA
- Collaboration LIGOS
- Collaboration V
- Colleoni M
- Collette CG
- Colombo A
- Colpi M
- Compton CM
- Conti L
- Cooper SJ
- Corban P
- Corbitt TR
- Cordero-Carrion I
- Corezzi S
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- Cornish NJ
- Corre D
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- Countryman ST
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- Cullen TJ
- Cumming A
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- Cuoco E
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- D'Antonio S
- D'Emilio V
- D'Onofrio L
- D'Urso D
- Dabadie P
- Dal Canton T
- Dall'Osso S
- Dalya G
- Dana A
- Danilishin S
- Danzmann K
- Darsow-Fromm C
- Dasgupta A
- Datrier LEH
- Datta S
- Datta S
- Dattilo V
- Dave I
- Davier M
- Davies GSC
- Davis D
- Davis MC
- Daw EJ
- De Laurentis M
- De Lillo F
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- De Matteis F
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- De Rosa R
- De Rossi C
- De Simone R
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- Del Favero V
- Del Pozzo W
- Deleglise S
- Dell'Aquila D
- DeMarchi LM
- Demos N
- Dent T
- Depasse A
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- 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
- Diaz JC
- Diaz MC
- Didio NA
- Dietrich T
- Ding B
- Divakarla AK
- Dmitriev A
- Doctor Z
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- Dooley KL
- Doravari S
- Drago M
- Driggers JC
- Drori Y
- Ducoin J-G
- Dupej P
- Dupletsa U
- Durante O
- Duverne P-A
- Dwyer SE
- 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
- Essick RC
- Estelles H
- Estevez D
- Etienne Z
- Etzel T
- Evans M
- Evans TM
- Evstafyeva T
- Ewing BE
- Fabrizi F
- Faedi F
- Fafone V
- Fair H
- Fairhurst S
- Fan PC
- Farah AM
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- Farr B
- Farr WM
- Fauchon-Jones EJ
- Favaro G
- Favata M
- Fays M
- Fazio M
- Feicht J
- Fejer MM
- Fenyvesi E
- Ferguson DL
- Fernandez-Galiana A
- Ferrante I
- Ferreira TA
- Fidecaro F
- Figura P
- Fiori A
- Fiori I
- Fishbach M
- Fisher RP
- Fittipaldi R
- Fiumara V
- Flaminio R
- Floden E
- Fong HK
- Font JA
- Fornal B
- Forsyth PWF
- Franke A
- Frasca S
- Frasconi F
- Freed JP
- Frei Z
- Freise A
- Freitas O
- Frey R
- Fritschel P
- Frolov VV
- Fronze GG
- Fujii Y
- Fujikawa Y
- Fujimoto Y
- Fulda P
- Fyffe M
- Gabbard HA
- Gadre BU
- Gair JR
- Gais J
- Galaudage S
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- Ganapathy D
- Ganguly A
- Gao D
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- Garaventa B
- Garcia-Quiros C
- Garufi F
- Gateley B
- Gayathri V
- Ge G-G
- Gemme G
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- Ghosh A
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- Giacomazzo B
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- Godwin P
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- Gouaty R
- Gould DW
- Goyal S
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- Grado A
- Graham V
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- Granata V
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- Griffiths WL
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- Grimm SJ
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- Guidi GM
- Guimaraes AR
- Guixe G
- Gulati HK
- Gunny AM
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- Guo Y
- Gupta A
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- Guzman F
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- Hadiputrawan IPW
- Haegel L
- Haino S
- Halim O
- Hall ED
- Hamilton EZ
- Hammond G
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- Haney M
- Hanks J
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- Hannam MD
- Hannuksela O
- Hansen H
- Hansen TJ
- Hanson J
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- Harry IW
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- Hathaway JS
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- Hayakawa H
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- Healy J
- Heidmann A
- Heidt A
- Heintze MC
- Heinze J
- Heinzel J
- Heitmann H
- Hellman F
- Hello P
- Helmling-Cornell AF
- Hemming G
- Hendry M
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- Hennes E
- Hennig J
- Hennig MH
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- Hernandez IM
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- Hewitt AL
- Higginbotham S
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- Hill P
- Himemoto Y
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- Hirose C
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- Hofman D
- Hohmann JN
- Holcomb DG
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- Hollows IJ
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- Holt K
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- Hong Q
- Hough J
- Hourihane S
- Howell EJ
- Hoy CG
- Hoyland D
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- Hsieh B-H
- Hsieh H-F
- Hsiung C
- Hsu Y
- Huang H-Y
- Huang P
- Huang Y
- Huang Y
- Huang Y-C
- Huang Y-J
- Hubner MT
- Huddart AD
- Hughey B
- Hui DCY
- Hui V
- Husa S
- Huttner SH
- Huxford R
- Huynh-Dinh T
- Ide S
- Idzkowski B
- Iess A
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- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2022
- Field of study
Results are presented for a semi-coherent search for continuous gravitational waves from the low-mass X-ray binary Scorpius X-1, using a hidden Markov model (HMM) to allow for spin wandering. This search improves on previous HMM-based searches of Laser Interferometer Gravitational-wave Observatory (LIGO) data by including the orbital period in the search template grid, and by analyzing data from the latest (third) observing run (O3). In the frequency range searched, from 60 to 500 Hz, we find no evidence of gravitational radiation. This is the most sensitive search for Scorpius X-1 using a HMM to date. For the most sensitive sub-band, starting at 256.06Hz, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=6.16×10−26, assuming the orbital inclination angle takes its electromagnetically restricted value ι=44∘. The upper limits on gravitational wave strain reported here are on average a factor of ∼3 lower than in the O2 HMM search. This is the first Scorpius X-1 HMM search with upper limits that reach below the indirect torque-balance limit for certain sub-bands, assuming ι=44∘
Searches for Gravitational Waves from Known Pulsars at Two Harmonics in the Second and Third LIGO-Virgo Observing Runs
- Author
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- Yamazaki R
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- Yang YC
- Yap MJ
- Yeeles DW
- Yeh SW
- Yelikar AB
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
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- Yu H
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- Zendri JP
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- Zhan M
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- Zhao G
- Zhao Y
- Zhao Y
- Zhou R
- Zhou Z
- Zhu XJ
- Zhu ZH
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2022
- 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 h (0) for the single-harmonic search along with limits on the pulsars' mass quadrupole moments Q (22) and ellipticities epsilon. 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 similar to 100 and similar to 20 more constraining than their spin-down limits, respectively. For the dual-harmonic searches, new limits are placed on the strain amplitudes C (21) and C (22). For 23 pulsars, we also present limits on the emission amplitude assuming dipole radiation as predicted by Brans-Dicke theory
Search for gravitational waves from Scorpius X-1 with a hidden Markov model in O3 LIGO data
- Author
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- Zimmerman AB
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- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2022
- Field of study
Results are presented for a semi-coherent search for continuous gravitational waves from the low-mass X-ray binary Scorpius X-1, using a hidden Markov model (HMM) to allow for spin wandering. This search improves on previous HMM-based searches of Laser Interferometer Gravitational-wave Observatory (LIGO) data by including the orbital period in the search template grid, and by analyzing data from the latest (third) observing run (O3). In the frequency range searched, from 60 to 500 Hz, we find no evidence of gravitational radiation. This is the most sensitive search for Scorpius X-1 using a HMM to date. For the most sensitive sub-band, starting at 256.06Hz, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=6.16×10−26, assuming the orbital inclination angle takes its electromagnetically restricted value ι=44∘. The upper limits on gravitational wave strain reported here are on average a factor of ∼3 lower than in the O2 HMM search. This is the first Scorpius X-1 HMM search with upper limits that reach below the indirect torque-balance limit for certain sub-bands, assuming ι=44∘
Search for continuous gravitational wave emission from the Milky Way center in O3 LIGO-Virgo data
- Author
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- Abe H
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- Yokozawa T
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- Zadrozny A
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- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
International audienceWe present a directed search for continuous gravitational wave (CW) signals emitted by spinningneutron stars located in the inner parsecs of the Galactic Center (GC). Compelling evidence for the presenceof a numerous population of neutron stars has been reported in the literature, turning this region into a veryinteresting place to look for CWs. In this search, data from the full O3 LIGO-Virgo run in the detectorfrequency band [10, 2000] Hz have been used. No significant detection was found and 95% confidencelevel upper limits on the signal strain amplitude were computed, over the full search band, with the deepestlimit of about 7.6×10−26 at ≃142 Hz. These results are significantly more constraining than those reportedin previous searches. We use these limits to put constraints on the fiducial neutron star ellipticity andr-mode amplitude. These limits can be also translated into constraints in the black hole mass–boson massplane for a hypothetical population of boson clouds around spinning black holes located in the GC
Searches for gravitational waves from known pulsars at two harmonics in the second and third LIGO-Virgo observing runs
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
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- Aggarwal N
- Aguiar OD
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- Ajith P
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- Albanesi S
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- Altin PA
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
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- Andrić T
- Andrés-Carcasona M
- Angelova SV
- Ansoldi S
- Antelis JM
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- Arellano FEP
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- Bagnasco S
- Bai Y
- Bailes M
- Baird J
- Bajpai R
- Baka T
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- 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
Model-based Cross-correlation Search for Gravitational Waves from the Low-mass X-Ray Binary Scorpius X-1 in LIGO O3 Data
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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 Binaries in the First Half of Advanced LIGO’s and Advanced Virgo’s Third Observing Run
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- Wysocki DM
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- Yamazaki R
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- Yap MJ
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- Yeh S-W
- Yelikar AB
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
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- Yuzurihara H
- Zadrozny A
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- Zhou R
- Zhou Z
- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- Publication date
- 24/09/2021
- Field of study
International audienceWe report on a search for compact binary coalescences where at least one binary component has a mass between 0.2 M⊙ and 1.0 M⊙ in Advanced LIGO and Advanced Virgo data collected between 1 April 2019 1500 UTC and 1 October 2019 1500 UTC. We extend our previous analyses in two main ways: we include data from the Virgo detector and we allow for more unequal mass systems, with mass ratio q≥0.1. We do not report any gravitational-wave candidates. The most significant trigger has a false alarm rate of 0.14 yr-1. This implies an upper limit on the merger rate of subsolar binaries in the range [220−24200] Gpc-3 yr-1, depending on the chirp mass of the binary. We use this upper limit to derive astrophysical constraints on two phenomenological models that could produce subsolar-mass compact objects. One is an isotropic distribution of equal-mass primordial black holes. Using this model, we find that the fraction of dark matter in primordial black holes in the mass range 0.2 M⊙<mPBH<1.0 M⊙ is fPBH≡ΩPBH/ΩDM≲6%. This improves existing constraints on primordial black hole abundance by a factor of ∼3. The other is a dissipative dark matter model, in which fermionic dark matter can collapse and form black holes. The upper limit on the fraction of dark matter black holes depends on the minimum mass of the black holes that can be formed: the most constraining result is obtained at Mmin=1 M⊙, where fDBH≡ΩDBH/ΩDM≲0.003%. These are the first constraints placed on dissipative dark models by subsolar-mass analyses
All-sky, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
- Author
- Abbott R
- Abe H
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- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
We present the first results from an all-sky all-frequency (ASAF) search for an anisotropic stochastic gravitational-wave background using the data from the first three observing runs of the Advanced LIGO and Advanced Virgo detectors. Upper limit maps on broadband anisotropies of a persistent stochastic background were published for all observing runs of the LIGO-Virgo detectors. However, a broadband analysis is likely to miss narrowband signals as the signal-to-noise ratio of a narrowband signal can be significantly reduced when combined with detector output from other frequencies. Data folding and the computationally efficient analysis pipeline, PyStoch, enable us to perform the radiometer map-making at every frequency bin. We perform the search at 3072 HEALPix equal area pixels uniformly tiling the sky and in every frequency bin of width 1-32 Hz in the range 20-1726 Hz, except for bins that are likely to contain instrumental artefacts and hence are notched. We do not find any statistically significant evidence for the existence of narrowband gravitational-wave signals in the analyzed frequency bins. Therefore, we place 95\% confidence upper limits on the gravitational-wave strain for each pixel-frequency pair, the limits are in the range (0.030 - 9.6) \times10^{-24}. In addition, we outline a method to identify candidate pixel-frequency pairs that could be followed up by a more sensitive (and potentially computationally expensive) search, e.g., a matched-filtering-based analysis, to look for fainter nearly monochromatic coherent signals. The ASAF analysis is inherently independent of models describing any spectral or spatial distribution of power. We demonstrate that the ASAF results can be appropriately combined over frequencies and sky directions to successfully recover the broadband directional and isotropic results