15 research outputs found
Fuzzy Regression Approaches and Applications
- Author
- B. Hestmaty
- B. Kim
- C-B. Cheng
- C. Kao
- C. Kao
- C.-B. Cheng
- C.-B. Cheng
- D.H. Hong
- E.C. Ăzelkan
- F-M. Tseng
- F-M. Tseng
- F-M. Tseng
- F. Höppner
- H. Ishibuchi
- H. Tanaka
- H.T. Lee
- J.A. SĂĄnchez
- J.A. SĂĄnchez
- J.J. Buckley
- J.J. Buckley
- J.P. Dunyak
- K.K. Yen
- K.W. Ip
- L. Tran
- M-S. Yang
- M-S. Yang
- M. Hojati
- M.M. Nasrabadi
- M.M. Nasrabadi
- P-T. Chang
- P. Diamond
- P. DâUrso
- P. DâUrso
- P.M. Bell
- S.A. Soliman
- Y-H. O. Chang
- Y-H. O. Chang
- Y-S. Chen
- Y-S. Chen
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2006
- Field of study
Fuzzy regression analysis: Systematic review and bibliography
- Author
- Abdalla
- Abdalla
- Abdalla
- Agresti
- Akbari
- Akbari
- Akbari
- Alex
- Alex
- Alfonso
- Aliev
- Amiri
- An
- Apaydin
- Arabpour
- Arefi
- Arne Johannssen
- Arnold
- Arnold
- Arnold
- Arnold
- Arnold
- Arnold
- Arnold
- Arnold
- Arnold
- Atalay
- Azadeh
- Azadeh
- Azadeh
- Azadeh
- Azadeh
- Azadeh
- Azadeh
- Azadeh
- Azadeh
- Azadeh
- Bajestani
- Bajestani
- Bajestani
- Bajestani
- Bandemer
- Bardossy
- Bardossy
- Bardossy
- Bardossy
- Bargiela
- Berry-Stölzle
- Bisserier
- Bisserier
- Boreux
- Boreux
- Boukezzoula
- Buckley
- Buckley
- Buckley
- Buckley
- Castillo
- Celmins
- Celmins
- Celmins
- Celmins
- Cerny
- Cerny
- Cerny
- Chachi
- Chachi
- Chachi
- Chachi
- Chachi
- Chachi
- Chachi
- Chachi
- Chan
- Chan
- Chan
- Chan
- Chan
- Chan
- Chan
- Chan
- Chan
- Chan
- Chan
- Chan
- Chang
- Chang
- Chang
- Chang
- Chang
- Chang
- Chang
- Chang
- Chaudhuri
- Chen
- Chen
- Chen
- Chen
- Chen
- Chen
- Chen
- Chen
- Chen
- Chen
- Chen
- Chen
- Cheng
- Cheng
- Cheng
- Cheng
- Choi
- Choi
- Choi
- Choi
- Chou
- Chuang
- Chukhrova
- Chukhrova
- Chung
- Ciavolino
- Coppi
- Coppi
- Coppi
- Couso
- Darwish
- De Andres-Sanchez
- De Andres-Sanchez
- De Andres-Sanchez
- De Andres-Sanchez
- De Andres-Sanchez
- De Andres-Sanchez
- De Andres-Sanchez
- Diamond
- Diamond
- Diamond
- Diamond
- Diamond
- Diamond
- Diamond
- Dielman
- Domrachev
- Donoso
- Dubois
- Dubois
- Dubois
- Dunyak
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- DâUrso
- Farnoosh
- Farnoosh
- Fattahi
- Ferraro
- Ferraro
- Ferraro
- Ferraro
- Ferraro
- Ferraro
- Ferraro
- Fung
- Ge
- Ge
- Gharpuray
- Gholizadeh
- Ghoshray
- Gladysz
- Gladysz
- Gonzalez-Gonzalez
- Gonzalez-Rodriguez
- Guo
- Guo
- Hao
- Hao
- Hao
- Hao
- Hassanpour
- Hassanpour
- Hassanpour
- Hassanpour
- Hastie
- Hayashi
- He
- He
- He
- Hesamian
- Hesamian
- Hesamian
- Hesamian
- Heshmaty
- Hladik
- Hojati
- Hong
- Hong
- Hong
- Hong
- Hong
- Hong
- Hong
- Hong
- Hong
- Hong
- Hong
- Hong
- Hose
- Hosseinzadeh
- Hu
- Hu
- Huang
- Huang
- Huang
- Hung
- Hwang
- Höglund
- Icen
- Icen
- Icen
- Imoto
- Inuiguchi
- Inuiguchi
- Inuiguchi
- Ip
- Ip
- Ishibuchi
- Ishibuchi
- Ishibuchi
- Ishibuchi
- Ishibuchi
- Ivakhnenko
- Jajuga
- Jeng
- Jiang
- Jiang
- Jozsef
- Jung
- Kacprzyk
- Kahraman
- Kahraman
- Kandel
- Kao
- Kao
- Kao
- Karakasidis
- Karsak
- Karsak
- Kelkinnama
- Khan
- Khashei
- Kim
- Kim
- Kim
- Kim
- Kim
- Kim
- Kimura
- Kitchenham
- Klir
- Kocadagli
- Kocadagli
- Koissi
- KrÀtschmer
- KrÀtschmer
- KrÀtschmer
- KrÀtschmer
- Kula
- Kula
- Kula
- Kumar
- Kumar
- Kwong
- Kwong
- Kwong
- Kwong
- Körner
- Lai
- Lee
- Lee
- Lee
- Lee
- Lee
- Li
- Lin
- Lin
- Liu
- Liu
- Liu
- Liu
- Liu
- Lu
- Mashinchi
- McCauley-Bell
- McCauley-Bell
- Megri
- Ming
- Modarres
- Modarres
- Mogilenko
- Mohammadi
- Moskowitz
- Mosleh
- Mosleh
- Mosleh
- Mousavi
- Muzzioli
- Namdari
- Namdari
- Namdari
- Nasibov
- Nasrabadi
- Nasrabadi
- Nasrabadi
- Nasrabadi
- Nataliya Chukhrova
- Nazarko
- Niimura
- Nureize
- NĂ€ther
- NĂ€ther
- NĂ€ther
- NĂ€ther
- NĂ€ther
- NĂ€ther
- Otadi
- Pan
- Pan
- Papadopoulos
- Papadopoulos
- Parvathi
- Pehlivan
- Peters
- Petit-Renaud
- Petit-Renaud
- Poleshchuk
- Poleshchuk
- Pop
- Pourahmad
- Pourahmad
- Profillidis
- Puri
- Rabbani
- Rabiei
- Rafiei
- Ramedani
- Ramezani
- Ramli
- Ramli
- Ramli
- Redden
- Redden
- Roh
- Roldan
- Roldan Lopez de Hierro
- Roldan Lopez de Hierro
- Roychowdhury
- Sakawa
- Sakawa
- Sakawa
- Sakawa
- Salas
- Salmani
- Savic
- Savic
- Sekkeli
- Sener
- Sener
- Sener
- Shakouri
- Shakouri
- Shakouri
- Shakouri
- Shen
- Shimizu
- Sohn
- Sohn
- Soliman
- Song
- Stahl
- Su
- Su
- Suk
- Sung
- Taheri
- Taheri
- Taheri
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tanaka
- Tavanai
- Theil
- Torabi
- Torkian
- Toyoura
- Tran
- Tranfield
- Tsaur
- Tsaur
- Tsaur
- Tseng
- Tseng
- Tsutsumi
- Tutmez
- Tutmez
- Vapnik
- Varga
- Wang
- Wang
- Wang
- Wang
- Wang
- Wang
- Wang
- Wang
- Watada
- Watada
- Watada
- Watada
- Watada
- Wei
- Wei
- Wen
- Wi
- Wieszczy
- Wu
- Wu
- Wu
- Wu
- Wu
- Wu
- WĂŒnsche
- Xizhao
- Xu
- Xu
- Xu
- Xue
- Yabuuchi
- Yabuuchi
- Yager
- Yang
- Yang
- Yang
- Yang
- Yang
- Yao
- Yazdanbakhsh
- Yeh
- Yen
- Yin
- Yoon
- Yoon
- Yoon
- Yoon
- Yu
- Yu
- Yu
- Yu
- Yu
- Zadeh
- Zadeh
- Zadeh
- Zadeh
- Zadeh
- Zeng
- Zhang
- Zhang
- Zhou
- Zimmermann
- Zolfaghari
- Zuo
- Zuo
- ĂgĂŒt
- Ăzelkan
- Ăzelkan
- Publication venue
- 'Elsevier BV'
- Publication date
- Field of study
Identification of microRNA signature in different pediatric brain tumors
- Author
- Bartel DP
- Birks DK
- Boman KK
- Braoudaki M
- Chen T
- Costa FF
- Dai J
- Diederichs S
- Dina Yehia
- DâUrso IP
- Faragalla H
- Ferretti E
- Filipazzi P
- Hala Taha
- Haque I
- Jonas S
- Laneve P
- Leichter AL
- Li KK-W
- Liang Y
- Louis DN
- Lund E
- Mariam G. Elzayat
- Marwa Tantawy
- Mestdagh P
- Paladini L
- Pezuk JA
- Sasayama T
- Sharma V
- Stoicea N
- Tihan T
- Van Wynsberghe PM
- Visani M
- Visani M
- Wang F
- Wang M
- Wang Y
- Xu H
- Zakrzewska M
- Zen K
- Zhang X
- Zhou L
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Recommended from our members
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGOâVirgo 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
- AndriÄ 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
- ArĂšne 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 CalderĂłn
- Buy C
- Byer RL
- BĂ©csy 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
- CavagliĂ M
- Cavalier F
- Cavalieri R
- Cella G
- CerdĂĄ-DurĂĄn 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
- CieĆlar 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-CarriĂłn 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
- CuryĆo M
- Dabadie P
- Dal Canton T
- DallâOsso 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
- DellâAquila 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
- DĂĄlya G
- DĂaz MC
- DâAngelo B
- DâAntonio S
- DâEmilio V
- DâOnofrio L
- DâUrso 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
- Ezquiaga JM
- 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
- GarcĂa-NĂșñez C
- GarcĂa-QuirĂłs 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 Abhirup
- Ghosh Archisman
- Ghosh Shaon
- Ghosh Shrobana
- Ghosh Tathagata
- 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
- GonzĂĄlez 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 Anchal
- Gupta Anuradha
- Gupta Ish
- Gupta P
- Gupta SK
- Gurs J
- Gustafson R
- Gutierrez N
- Guzman F
- Ha S
- Hadiputrawan IPW
- Haegel L
- Haino S
- Halim O
- Hall ED
- Hamilton EZ
- Hammond G
- Han W-B
- Haney M
- Hanks J
- Hanna C
- Hannam MD
- Hannuksela O
- Hansen H
- Hanson J
- Harada R
- Harder T
- Haris K
- Harms J
- Harry GM
- Harry IW
- Hartwig D
- Hasegawa K
- Haskell B
- Haster C-J
- Hathaway JS
- Hattori K
- Haughian K
- Hayakawa H
- Hayama K
- Hayes FJ
- 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
- Heng IS
- Hennes E
- Hennig J-S
- Hennig M
- Henshaw C
- Hernandez Vivanco F
- Hernandez AG
- Hernandez I Magaña
- Heurs M
- Hewitt AL
- Higginbotham S
- Hild S
- Hill P
- Himemoto Y
- Hines AS
- Hirata N
- Hirose C
- Ho T-C
- Hochheim S
- Hofman D
- Hohmann JN
- Holcomb DG
- Holland NA
- Hollows IJ
- Holmes ZJ
- Holt K
- Holz DE
- Hong Q
- Hough J
- Hourihane S
- Howell D
- Howell EJ
- Hoy CG
- Hoyland D
- Hreibi A
- Hsieh B-H
- Hsieh H-F
- Hsiung C
- Huang H-Y
- Huang P
- Huang Y
- Huang Y-C
- Huang Y-J
- Huddart AD
- Hughey B
- Hui DCY
- Hui V
- Husa S
- Huttner SH
- Huxford R
- Huynh-Dinh T
- Hyland J
- HĂŒbner MT
- Iandolo GA
- Ide S
- Idzkowski B
- Iess A
- Inayoshi K
- Inoue Y
- Iosif P
- Irwin J
- Isi M
- Ito K
- Itoh Y
- Iyer BR
- JaberianHamedan V
- Jacqmin T
- Jacquet P-E
- Jadhav SJ
- Jadhav SP
- Jain T
- James AL
- Jan AZ
- Jani K
- Janquart J
- Janssens K
- Janthalur NN
- Jaranowski P
- Jariwala D
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- Wysocki DM
- Xiao L
- Yadav N
- Yamada T
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- Yamamoto K
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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
- ZadroĆŒny A
- Zanolin M
- Zeidler S
- Zelenova T
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- Zevin M
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- 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
Recommended from our members
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGOâVirgo Network
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhicary S
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
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- 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
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- Andrés-Carcasona M
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- 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
Search for subsolar-mass black hole binaries in the second part of Advanced LIGOâs and Advanced Virgoâs third observing run
- Author
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- Zweizig J
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 28/02/2023
- Field of study
Recommended from our members
Constraints on the Cosmic Expansion History from GWTCâ3
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari RX
- Adkins VK
- Adya VB
- Affeldt C
- Agarwal D
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- Aggarwal N
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- Anderson WG
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- Andres N
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- Angelova SV
- Ansoldi S
- Antelis JM
- Antier S
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- Appavuravther EZ
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- Arellano FE Peña
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- Billingsley G
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- Biscans S
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- Bisht A
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- Blair CD
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- Corezzi S
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- Couvares P
- Coward DM
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- Coyne DC
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- Creighton TD
- Criswell AW
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- Crowder SG
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- Datrier LEH
- Datta Sayak
- Datta Sayantani
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- de Souza Melo S Assis
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- DellâAquila D
- Deléglise S
- DeMarchi LM
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- Depasse A
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- Dhurandhar S
- Diaz J Casanueva
- Didio NA
- Dietrich T
- Ding B
- Divakarla AK
- Dmitriev A
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- e Melo I Tosta
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- Easter PJ
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- Eikenberry SS
- Eisenmann M
- Eisenstein RA
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- Engelby E
- Enomoto Y
- Errico L
- Essick RC
- Estellés H
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- Etienne Z
- Etzel T
- Evans M
- Evans TM
- Evstafyeva T
- Ewing BE
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- Faedi F
- Fafone V
- Fair H
- Fairhurst S
- Fan PC
- Farah AM
- Farinon S
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- Thirugnanasambandam MP
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- Wysocki DM
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- Yang Y-C
- Yang Yang
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- ZadroĆŒny A
- Zanolin M
- Zeidler S
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- Zevin M
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- Zhou R
- Zhou Z
- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- The Astrophysical Journal
- Publication date
- 07/06/2023
- Field of study
Abstract
We use 47 gravitational wave sources from the Third LIGOâVirgoâKamioka Gravitational Wave Detector Gravitational Wave Transient Catalog (GWTCâ3) to estimate the Hubble parameter H(z), including its current value, the Hubble constant H
0. Each gravitational wave (GW) signal provides the luminosity distance to the source, and we estimate the corresponding redshift using two methods: the redshifted masses and a galaxy catalog. Using the binary black hole (BBH) redshifted masses, we simultaneously infer the source mass distribution and H(z). The source mass distribution displays a peak around 34 M
â, followed by a drop-off. Assuming this mass scale does not evolve with the redshift results in a H(z) measurement, yielding
H
0
=
68
â
8
+
12
km
s
â
1
Mpc
â
1
(68% credible interval) when combined with the H
0 measurement from GW170817 and its electromagnetic counterpart. This represents an improvement of 17% with respect to the H
0 estimate from GWTCâ1. The second method associates each GW event with its probable host galaxy in the catalog GLADE+, statistically marginalizing over the redshifts of each eventâs potential hosts. Assuming a fixed BBH population, we estimate a value of
H
0
=
68
â
6
+
8
km
s
â
1
Mpc
â
1
with the galaxy catalog method, an improvement of 42% with respect to our GWTCâ1 result and 20% with respect to recent H
0 studies using GWTCâ2 events. However, we show that this result is strongly impacted by assumptions about the BBH source mass distribution; the only event which is not strongly impacted by such assumptions (and is thus informative about H
0) is the well-localized event GW190814.</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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- 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 Δ. 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 J0437â4715 and J0711â6830, 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 âŒ100 and âŒ20 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 10â25 when marginalized isotropically over the unknown inclination angle of the neutron star's rotation axis, or less than 4 Ă 10â26 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
Recommended from our members
A Joint Fermi-GBM and Swift-BAT Analysis of Gravitational-wave Candidates from the Third Gravitational-wave Observing Run
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- Shaikh MA
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- Shao L
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- Sheela A
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- Shoemaker DH
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- Slaven-Blair TJ
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- Soldateschi J
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- Song I
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- Strong MD
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- Subrahmanya S Chalathadka
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- Wysocki DM
- Xiao L
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- Yamamoto H
- Yamamoto K
- Yamamoto T
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- Yamazaki R
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- Yang Yang
- Yap MJ
- Yeeles DW
- Yeh S-W
- Yelikar AB
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- ZadroĆŒny A
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
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- Zhao Yue
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- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- The Astrophysical Journal
- Publication date
- 28/03/2024
- Field of study
Abstract
We present Fermi Gamma-ray Burst Monitor (Fermi-GBM) and Swift Burst Alert Telescope (Swift-BAT) searches for gamma-ray/X-ray counterparts to gravitational-wave (GW) candidate events identified during the third observing run of the Advanced LIGO and Advanced Virgo detectors. Using Fermi-GBM onboard triggers and subthreshold gamma-ray burst (GRB) candidates found in the Fermi-GBM ground analyses, the Targeted Search and the Untargeted Search, we investigate whether there are any coincident GRBs associated with the GWs. We also search the Swift-BAT rate data around the GW times to determine whether a GRB counterpart is present. No counterparts are found. Using both the Fermi-GBM Targeted Search and the Swift-BAT search, we calculate flux upper limits and present joint upper limits on the gamma-ray luminosity of each GW. Given these limits, we constrain theoretical models for the emission of gamma rays from binary black hole mergers.</jats:p