43 research outputs found
Pesticide induced physiological and behavioural changes in an estuarine teleost Therapon jarbua (Forsk)
- Publication venue
- Publication date
- 01/01/1978
- Field of study
Static bioassays were conducted with pesticides like PP'-DDT, Dimethoate (Rogor) and Carbaryl (Sevin) to determine the median lethal concentrations (LC sub(50)) on an estuarine teleost Therapon jarbua (Forsk). The respiration rates of fishes exposed to pesticides, as well as those of controls were determined. Respiration abnormalities
were noticed in treated fishes. The metabolic rates are generally higher in treated fishes than in the controls. The behaviour of fishes exposed to LC sub(25) (96h) concentrations of pesticides is discussed. Estuarine fishes appear to be more sensitive and susceptible to pesticides than fresh water fishes. The pesticides affect the locomotory and swimming behaviour of fishes. Loss in weight of fishes exposed to LC sub(50) (96 h) concentration of pesticides was also estimated. The present report gives a comprehensive account of the toxic nature of these pesticides to fishes
Particlization in hybrid models
- Author
- B. Schenke
- B.R. Schlei
- C. Alt
- C. Alt
- C. Anderlik
- C. Anderlik
- C. Nonaka
- C. Shen
- C.M. Hung
- D. Adamova
- D. Molnar
- D. Ouerdane
- D.H. Rischke
- D.H. Rischke
- D.L. Book
- F. Cooper
- G. Wyvill
- H. Holopainen
- H. Petersen
- H. Petersen
- H. Petersen
- H. Petersen
- H. Petersen
- H. Song
- H. Song
- H. Sorge
- Hannah Petersen
- J. Adams
- J. Adams
- J. Sollfrank
- J. Steinheimer
- J.C. Roberts
- J.H. Lee
- J.P. Boris
- J.P. Boris
- K. Tamosiunas
- K. Werner
- K.A. Bugaev
- K.A. Bugaev
- L. Pang
- M. Bleicher
- M. Isse
- M.J. Düurst
- P. Huovinen
- P.F. Kolb
- P.F. Kolb
- P.F. Kolb
- Pasi Huovinen
- R. Venugopalan
- S. Arsene
- S. Bernard
- S.A. Bass
- S.A. Bass
- S.S. Adler
- S.V. Afanasiev
- T. Hirano
- V.K. Magas
- W.E. Lorensen
- Y. Cheng
- Y. Nara
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 20/09/2012
- Field of study
In hybrid models, which combine hydrodynamical and transport approaches to
describe different stages of heavy-ion collisions, conversion of fluid to
individual particles, particlization, is a non-trivial technical problem. We
describe in detail how to find the particlization hypersurface in a 3+1
dimensional model, and how to sample the particle distributions evaluated using
the Cooper-Frye procedure to create an ensemble of particles as an initial
state for the transport stage. We also discuss the role and magnitude of the
negative contributions in the Cooper-Frye procedure.Comment: 18 pages, 28 figures, EPJA: Topical issue on "Relativistic Hydro- and
Thermodynamics"; version accepted for publication, typos and error in Eq.(1)
corrected, the purpose of sampling and change from UrQMD to fluid clarified,
added discussion why attempts to cancel negative contributions of Cooper-Frye
are not applicable her
Space-time evolution and HBT analysis of relativistic heavy ion collisions in a chiral SU(3) x SU(3) model
- Author
- A. Chodos
- A. Chodos
- A. Dumitru
- A. Dumitru
- A. Dumitru
- A. Makhlin
- A. Makhlin
- A. Muronga
- B.D. Serot
- B.R. Schlei
- B.R. Schlei
- C. Adler
- C. Anderlik
- C. Greiner
- C. Greiner
- C. Greiner
- C. Spieles
- D. Ardouin
- D. Zschiesche
- D. Zschiesche
- D.H. Rischke
- D.H. Rischke
- D.H. Rischke
- E. Laermann
- E. Shuryak
- F.R. Brown
- G. Baym
- G. Bertsch
- G. Bertsch
- G. Goldhaber
- H. Stöcker
- H. Stöcker
- H. Stöcker
- H.A. Weldon
- J. Bolz
- J. Bolz
- J. Brachmann
- J. Letessier
- J. Theis
- J.D. Bjorken
- J.W. Harris
- K. Geiger
- K. Haglin
- K. Kajantie
- K. Kajantie
- K. Kajantie
- K. Kajantie
- K. Morita
- K.A. Bugaev
- M. Gyulassy
- M. Gyulassy
- M. Prakash
- M.A. Lisa
- M.A. Lisa
- N. Xu
- O. Scavenius
- O. Scavenius
- P. Braun-Munzinger
- P. Braun-Munzinger
- P. Papazoglou
- R. Venugopalan
- R.D. Pisarski
- R.M. Weiner
- S. Pratt
- S. Pratt
- S. Pratt
- S. Schramm
- S. Soff
- S. Soff
- S.A. Bass
- S.A. Bass
- S.E. Vance
- T. Csörgő
- T. Csörgő
- T. Schönfeld
- U. Wiedemann
- V.K. Magas
- W. Greiner
- Y. Hama
- Y. Hama
- Y. Iwasaki
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2002
- Field of study
The space-time dynamics and pion-HBT radii in central heavy ion-collisions at
CERN-SPS and BNL-RHIC are investigated within a hydrodynamic simulation. The
dependence of the dynamics and the HBT-parameters on the EoS is studied with
different parametrisations of a chiral SU(3) sigma-omega model. The
selfconsistent collective expansion includes the effects of effective hadron
masses, generated by the nonstrange and strange scalar condensates. Different
chiral EoS show different types of phase transitions and even a crossover. The
influence of the order of the phase transition and of the difference in the
latent heat on the space-time dynamics and pion-HBT radii is studied. A small
latent heat, i.e. a weak first-order chiral phase transition, or even a smooth
crossover leads to distinctly different HBT predictions than a strong first
order phase transition. A quantitative description of the data, both at SPS
energies as well as at RHIC energies, appears difficult to achieve within the
ideal hydrodynamical approach using the SU(3) chiral EoS. A strong first-order
quasi-adiabatic chiral phase transition seems to be disfavored by the pion-HBT
data from CERN-SPS and BNL-RHIC
Search for gravitational-wave transients associated with magnetar bursts in advanced LIGO and advanced Virgo data from the third observing run
- Author
- Abbott R
- Abe H
- Acernese F
- Ackley K
- Adhikari N
- Adhikari R.X
- Adkins V.K
- Adya V.B
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar O.D
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Alfaidi R.A
- Allocca A
- Altin P.A
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson S.B
- Anderson W.G
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Angelova S.V
- Ansoldi S
- Antelis J.M
- Antier S
- Apostolatos T
- Appavuravther E.Z
- Appert S
- Apple S.K
- Arai K
- Araya A
- Araya M.C
- Areeda J.S
- Arellano F.E. Peña
- Aritomi N
- Arnaud N
- Arogeti M
- Aronson S.M
- Arène M
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Assiduo M
- Aston S.M
- Astone P
- Aubin F
- Aultoneal K
- Austin C
- Babak S
- Badaracco F
- Bader M.K. M
- Badger C
- Bae S
- Bae Y
- Baer A.M
- Bagnasco S
- Bai Y
- Baird J
- Bajpai R
- Baka T
- Ball M
- Ballardin G
- Ballmer S.W
- Balsamo A
- Baltus G
- Banagiri S
- Banerjee B
- Bankar D
- Barayoga J.C
- Barbieri C
- Barish B.C
- Barker D
- Barneo P
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton M.A
- Bartos I
- Basak S
- Bassiri R
- Basti A
- Bawaj M
- Bayley J.C
- Bazzan M
- Becher B.R
- Bedakihale V.M
- Beirnaert F
- Bejger M
- Belahcene I
- Benedetto V
- Beniwal D
- Benjamin M.G
- Bennett T.F
- Bentley J.D
- Benyaala M
- Bera S
- Berbel M
- Bergamin F
- Berger B.K
- Bernuzzi S
- Bersanetti D
- Bertolini A
- Betzwieser J
- Beveridge D
- Bhandare R
- Bhandari A.V
- Bhardwaj U
- Bhatt R
- Bhattacharjee D
- Bhaumik S
- Bianchi A
- Bilenko I.A
- Billingsley G
- Bini S
- Birney R
- Birnholtz O
- Biscans S
- Bischi M
- Biscoveanu S
- Bisht A
- Biswas B
- Bitossi M
- Bizouard M.-A
- Blackburn J.K
- Blair C.D
- Blair D.G
- Blair R.M
- Bobba F
- Bode N
- Bogaert G
- Boldrini M
- Bolingbroke G.N
- Bonavena L.D
- Bondu F
- Bonilla E
- Bonnand R
- Booker P
- Boom B.A
- Bork R
- Boschi V
- Bose N
- Bose S
- Bossilkov V
- Boudart V
- Bouffanais Y
- Bozzi A
- Boër M
- Bradaschia C
- Brady P.R
- Bramley A
- Branch A
- Branchesi M
- Brau J.E
- Breschi M
- Briant T
- Briggs J.H
- Brillet A
- Brinkmann M
- Brockill P
- Brooks A.F
- Brooks J
- Brown D.D
- Brunett S
- Bruno G
- Bruntz R
- Bryant J
- Bucci F
- Bulik T
- Bulten H.J
- Buonanno A
- Burtnyk K
- Buscicchio R
- Buskulic D
- Buy C
- Byer R.L
- Bécsy B
- Cabourn Davies G.S
- Cabras G
- Cabrita R
- Cadonati L
- Caesar M
- Cagnoli G
- Cahillane C
- Calderón Bustillo J
- Callaghan J.D
- Callister T.A
- Calloni E
- Cameron J
- Camp J.B
- Canepa M
- Canevarolo S
- Cannavacciuolo M
- Cannon K.C
- Cao H
- Cao Z
- Capocasa E
- Capote E
- Carapella G
- Carbognani F
- Carlassara M
- Carlin J.B
- Carney M.F
- Carpinelli M
- Carrillo G
- Carullo G
- Carver T.L
- Casentini C
- Castaldi G
- Caudill S
- Cavaglià M
- Cavalier F
- Cavalieri R
- Cella G
- Cerdá-Durán P
- Cesarini E
- Chaibi W
- Champion E
- Chan C
- Chan C.-H
- Chan C.L
- Chan K
- Chan M
- Chandra K
- Chang I.P
- Chanial P
- Chao S
- Chapman-Bird C
- Charlton P
- Chase E.A
- Chassande-Mottin E
- Chatterjee C
- Chatterjee Debarati
- Chatterjee Deep
- Chaturvedi M
- Chaty S
- Chen C
- Chen D
- Chen H.Y
- Chen J
- Chen K
- Chen X
- Chen Y.-B
- Chen Y.-R
- Chen Z
- Cheng H
- Cheong C.K
- Cheung H.Y
- Chia H.Y
- Chiadini F
- Chiang C-Y
- Chiarini G
- Chierici R
- Chincarini A
- Chiofalo M.L
- Chiummo A
- Choudhary R.K
- Choudhary S
- Christensen N
- Chu Q
- Chu Y-K
- Chua S.S. Y
- Chung K.W
- Ciani G
- Ciecielag P
- Cieślar M
- Cifaldi M
- Ciobanu A.A
- Ciolfi R
- Cipriano F
- Clara F
- Clark J.A
- Clearwater P
- Clesse S
- Cleva F
- Coccia E
- Codazzo E
- Cohadon P.-F
- Cohen D.E
- Colleoni M
- Collette C.G
- Colombo A
- Colpi M
- Compton C.M
- Constancio M
- Conti L
- Cooper S.J
- Corban P
- Corbitt T.R
- Cordero-Carrión I
- Corezzi S
- Corley K.R
- Cornish N.J
- Corre D
- Corsi A
- Cortese S
- Costa C.A
- Cotesta R
- Cottingham R
- Coughlin M.W
- Coulon J.-P
- Countryman S.T
- Cousins B
- Couvares P
- Coward D.M
- Cowart M.J
- Coyne D.C
- Coyne R
- Creighton J.D. E
- Creighton T.D
- Criswell A.W
- Croquette M
- Crowder S.G
- Cudell J.R
- Cullen T.J
- Cumming A
- Cummings R
- Cunningham L
- Cuoco E
- Curyło M
- d'Angelo B
- d'Antonio S
- d'Emilio V
- d'Onofrio L
- d'Urso D
- Dabadie P
- Dal Canton T
- Dall'Osso S
- Dana A
- Danilishin S
- Danzmann K
- Darsow-Fromm C
- Dasgupta A
- Datrier L.E. H
- Datta Sayak
- Datta Sayantani
- Dattilo V
- Dave I
- Davier M
- Davis D
- Davis M.C
- Daw E.J
- de Laurentis M
- de Lillo F
- de Lillo N
- de Matteis F
- de Pietri R
- De Rosa R
- de Rossi C
- de Simone R
- Dean R
- Debra D
- Deenadayalan M
- Degallaix J
- del Favero V
- del Pozzo W
- Dell'Aquila D
- Deléglise S
- Demarchi L.M
- 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
- Diaz J. Casanueva
- Didio N.A
- Dietrich T
- Ding B
- Divakarla A.K
- Dmitriev A
- Doctor Z
- Donahue L
- Donovan F
- Dooley K.L
- Doravari S
- Drago M
- Driggers J.C
- Drori Y
- Ducoin J.-G
- Dupej P
- Dupletsa U
- Durante O
- Duverne P.-A
- Dwyer S.E
- Dálya G
- Díaz M.C
- Eassa C
- Easter P.J
- Ebersold M
- Eckhardt T
- Eddolls G
- Edelman B
- Edo T.B
- Edy O
- Effler A
- Eguchi S
- Eichholz J
- Eikenberry S.S
- Eisenmann M
- Eisenstein R.A
- Ejlli A
- Engelby E
- Enomoto Y
- Errico L
- Essick R.C
- Estellés H
- Estevez D
- Etienne Z
- Etzel T
- Evans M
- Evans T.M
- Evstafyeva T
- Ewing B.E
- Fabrizi F
- Faedi F
- Fafone V
- Fair H
- Fairhurst S
- Fan P.C
- Farah A.M
- Farinon S
- Farr B
- Farr W.M
- Fauchon-Jones E.J
- Favaro G
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- Fays M
- Fazio M
- Feicht J
- Fejer M.M
- Fenyvesi E
- Ferguson D.L
- Fernandez-Galiana A
- Ferrante I
- Ferreira T.A
- Fidecaro F
- Figura P
- Fiori A
- Fiori I
- Fishbach M
- Fisher R.P
- Fittipaldi R
- Fiumara V
- Flaminio R
- Floden E
- Fong H.K
- Font J.A
- Fornal B
- Forsyth P.W. F
- Franke A
- Frasca S
- Frasconi F
- Freed J.P
- Frei Z
- Freise A
- Freitas O
- Frey R
- Fritschel P
- Frolov V.V
- Fronzé G.G
- Fujii Y
- Fujikawa Y
- Fujimoto Y
- Fulda P
- Fyffe M
- Gabbard H.A
- Gabella W.E
- Gadre B.U
- Gair J.R
- Gais J
- Galaudage S
- Gamba R
- Ganapathy D
- Ganguly A
- Gao D
- Gaonkar S.G
- Garaventa B
- García-Quirós C
- Garufi F
- Gateley B
- Gayathri V
- Ge G.-G
- Gemme G
- Gennai A
- George J
- Gerberding O
- Gergely L
- Gewecke P
- Ghonge S
- Ghosh Abhirup
- Ghosh Archisman
- Ghosh Shaon
- Ghosh Shrobana
- Ghosh Tathagata
- Giacomazzo B
- Giacoppo L
- Giaime J.A
- Giardina K.D
- Gibson D.R
- Gier C
- Giesler M
- Giri P
- Gissi F
- Gkaitatzis S
- Glanzer J
- Gleckl A.E
- Godwin P
- Goetz E
- Goetz R
- Gohlke N
- Golomb J
- Goncharov B
- González G
- Gosselin M
- Gouaty R
- Gould D.W
- Goyal S
- Grace B
- Grado A
- Graham V
- Granata M
- Granata V
- Grant A
- Gras S
- Grassia P
- Gray C
- Gray R
- Greco G
- Green A.C
- Green R
- Gretarsson A.M
- Gretarsson E.M
- Griffith D
- Griffiths W.L
- Griggs H.L
- Grignani G
- Grimaldi A
- Grimes E
- Grimm S.J
- Grote H
- Grunewald S
- Gruning P
- Gruson A.S
- Guerra D
- Guidi G.M
- Guimaraes A.R
- Guixé G
- Gulati H.K
- Gunny A.M
- Guo H.-K
- Guo Y
- Gupta Anchal
- Gupta Anuradha
- Gupta I.M
- Gupta P
- Gupta S.K
- Gustafson R
- Guzman F
- Ha S
- Hadiputrawan I.P. W
- Haegel L
- Haino S
- Halim O
- Hall E.D
- Hamilton E.Z
- Hammond G
- Han W.-B
- Haney M
- Hanks J
- Hanna C
- Hannam M.D
- Hannuksela O
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- Hansen T.J
- Hanson J
- Harder T
- Haris K
- Harms J
- Harry G.M
- Harry I.W
- Hartwig D
- Hasegawa K
- Haskell B
- Haster C.-J
- Hathaway J.S
- Hattori K
- Haughian K
- Hayakawa H
- Hayama K
- Hayes F.J
- Healy J
- Heidmann A
- Heidt A
- Heintze M.C
- Heinze J
- Heinzel J
- Heitmann H
- Hellman F
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- Helmling-Cornell A.F
- Hemming G
- Hendry M
- Heng I.S
- Hennes E
- Hennig J
- Hennig M.H
- Henshaw C
- Hernandez A.G
- Hernandez I. Magaña
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- Hewitt A.L
- Higginbotham S
- Hild S
- Hill P
- Himemoto Y
- Hines A.S
- Hirata N
- Hirose C
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- Hofman D
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- Holcomb D.G
- Holland N.A
- Hollows I.J
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- Holz D.E
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- Hourihane S
- Howell E.J
- Hoy C.G
- Hoyland D
- Hreibi A
- Hsieh B-H
- Hsieh H-F
- Hsiung C
- Hsu Y
- Huang H-Y
- Huang P
- Huang Y-C
- Huang Y.-J
- Huang Yiting
- Huang Yiwen
- Huddart A.D
- Hughey B
- Hui D.C. Y
- Hui V
- Husa S
- Huttner S.H
- Huxford R
- Huynh-Dinh T
- Hübner M.T
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- Idzkowski B
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- Jacquet P.-E
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- James A.L
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- Jaranowski P
- Jariwala D
- Jaume R
- Jenkins A.C
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- Jeon C
- Jia W
- Jiang J
- Jin H.-B
- Johns G.R
- Johnston R
- Jones A.W
- Jones D.I
- Jones P
- Jones R
- Joshi P
- Ju L
- Jue A
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- Jung P
- Junker J
- Juste V
- Kaihotsu K
- Kajita T
- Kakizaki M
- Kalaghatgi C.V
- Kalogera V
- Kamai B
- Kamiizumi M
- Kanda N
- Kandhasamy S
- Kang G
- Kanner J.B
- Kao Y
- Kapadia S.J
- Kapasi D.P
- Karathanasis C
- Karki S
- Kashyap R
- Kasprzack M
- Kastaun W
- Kato T
- Katsanevas S
- Katsavounidis E
- Katzman W
- Kaur T
- Kawabe K
- Kawaguchi K
- Keitel D
- Key J.S
- Khadka S
- Khalili F.Y
- Khan S
- Khanam T
- Khazanov E.A
- Khetan N
- Khursheed M
- Kijbunchoo N
- Kim A
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- Kim J.C
- Kim K
- Kim W.S
- Kim Y.-M
- Kimball C
- Kimura N
- Kinley-Hanlon M
- Kirchhoff R
- Kissel J.S
- Klimenko S
- Klinger T
- Knee A.M
- Knowles T.D
- Knust N
- Knyazev E
- Kobayashi Y
- Koch P
- Koekoek G
- Kohri K
- Kokeyama K
- Koley S
- Kolitsidou P
- Kolstein M
- Komori K
- Kondrashov V
- Kong A.K. H
- Kontos A
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- Korobko M
- Kovalam M
- Koyama N
- Kozak D.B
- Kozakai C
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- Krishnendu N.V
- Królak A
- Kuehn G
- Kuei F
- Kuijer P
- Kulkarni S
- Kumar A
- Kumar Prayush
- Kumar Rahul
- Kumar Rakesh
- Kume J
- Kuns K
- Kuromiya Y
- Kuroyanagi S
- Kwak K
- Kéfélian F
- La Rosa I
- Lacaille G
- Lagabbe P
- Laghi D
- Lalande E
- Lalleman M
- Lam T.L
- Lamberts A
- Landry M
- Lane B.B
- Lang R.N
- Lange J
- Lantz B
- Lartaux-Vollard A
- Lasky P.D
- Laxen M
- Lazzarini A
- Lazzaro C
- Leaci P
- Leavey S
- Lebohec S
- Lecoeuche Y.K
- Lee E
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- Lee H.W
- Lee K
- Lee R
- Legred I.N
- Lehmann J
- Lemaître A
- Lenti M
- Leonardi M
- Leonova E
- Leroy N
- Letendre N
- Levesque C
- Levin Y
- Leviton J.N
- Leyde K
- Li A.K. Y
- Li B
- Li J
- Li K.L
- Li P
- Li T.G. F
- Li X
- Lin C-Y
- Lin E.T
- Lin F-K
- Lin F-L
- Lin H.L
- Lin L.C.-C
- Linde F
- Linker S.D
- Linley J.N
- Littenberg T.B
- Liu G.C
- Liu J
- Liu K
- Liu X
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- Zhu Z.-H
- Zucker M.E
- Zweizig J
- Publication venue
- American Astronomical Society
- Publication date
- 01/01/2024
- Field of study
Gravitational waves are expected to be produced from neutron star oscillations associated with magnetar giant f lares and short bursts. We present the results of a search for short-duration (milliseconds to seconds) and longduration (∼100 s) transient gravitational waves from 13 magnetar short bursts observed during Advanced LIGO, Advanced Virgo, and KAGRA’s third observation run. These 13 bursts come from two magnetars, SGR1935 +2154 and SwiftJ1818.0−1607. We also include three other electromagnetic burst events detected by FermiGBM which were identified as likely coming from one or more magnetars, but they have no association with a known magnetar. No magnetar giant flares were detected during the analysis period. We find no evidence of gravitational waves associated with any of these 16 bursts. We place upper limits on the rms of the integrated incident gravitational-wave strain that reach 3.6 × 10−²³ Hz at 100 Hz for the short-duration search and 1.1 ×10−²² Hz at 450 Hz for the long-duration search. For a ringdown signal at 1590 Hz targeted by the short-duration search the limit is set to 2.3 × 10−²² Hz. Using the estimated distance to each magnetar, we derive upper limits upper limits on the emitted gravitational-wave energy of 1.5 × 1044 erg (1.0 × 1044 erg) for SGR 1935+2154 and 9.4 × 10^43 erg (1.3 × 1044 erg) for Swift J1818.0−1607, for the short-duration (long-duration) search. Assuming isotropic emission of electromagnetic radiation of the burst fluences, we constrain the ratio of gravitational-wave energy to electromagnetic energy for bursts from SGR 1935+2154 with the available fluence information. The lowest of these ratios is 4.5 × 103
Open data from the third observing run of LIGO, Virgo, KAGRA, and GEO
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- Publication venue
- American Astronomical Society
- Publication date
- 01/01/2023
- Field of study
The global network of gravitational-wave observatories now includes five detectors, namely LIGO Hanford, LIGO Livingston, Virgo, KAGRA, and GEO 600. These detectors collected data during their third observing run, O3, composed of three phases: O3a starting in 2019 April and lasting six months, O3b starting in 2019 November and lasting five months, and O3GK starting in 2020 April and lasting two weeks. In this paper we describe these data and various other science products that can be freely accessed through the Gravitational Wave Open Science Center at https://gwosc.org. The main data set, consisting of the gravitational-wave strain time series that contains the astrophysical signals, is released together with supporting data useful for their analysis and documentation, tutorials, as well as analysis software packages
Constraints on the cosmic expansion history from GWTC–3
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- Publication venue
- 'American Astronomical Society'
- Publication date
- 07/06/2023
- Field of study
We use 47 gravitational wave sources from the Third LIGO–Virgo–Kamioka Gravitational Wave Detector Gravitational Wave Transient Catalog (GWTC–3) to estimate the Hubble parameter H(z), including its current value, the Hubble constant H0. 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⊙, followed by a drop-off. Assuming this mass scale does not evolve with the redshift results in a H(z) measurement, yielding H0=68−8+12km s−1Mpc−1 (68% credible interval) when combined with the H0 measurement from GW170817 and its electromagnetic counterpart. This represents an improvement of 17% with respect to the H0 estimate from GWTC–1. The second method associates each GW event with its probable host galaxy in the catalog GLADE+, statistically marginalizing over the redshifts of each event's potential hosts. Assuming a fixed BBH population, we estimate a value of H0=68−6+8km s−1Mpc−1 with the galaxy catalog method, an improvement of 42% with respect to our GWTC–1 result and 20% with respect to recent H0 studies using GWTC–2 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 H0) is the well-localized event GW190814
A joint Fermi-GBM and Swift-BAT analysis of gravitational-wave candidates from the third gravitational-wave observing run
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- Publication venue
- American Astronomical Society
- Publication date
- 01/04/2024
- Field of study
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
Microbiology of nutrient regeneration. Part III Experimental studies on marine nitrification
- Publication venue
- NISCAIR-CSIR, India
- Publication date
- 01/06/1977
- Field of study
10-14Nitrification process was investigated in the tropical Vellar Estuary, by in situ experiments. Variation in nitrifying capacity in both estuarine and sea water was measured. Biological potential of estuarine water in the nitrification was greater than that of neritic water. Oxidation of ammonia to nitrate occurred without accumulation of nitrite. Marine nitrifiers (both ammonium oxidizers and nitrite oxidizers) were active in the photic zone of the coastal waters. In situ experiments revealed that nitrate reduction and ammonia oxidation were significant processes in the estuarine and coastal waters. Ammonia production, nitrite formation and nitrite oxidation took place simultaneously. At lower temperatures, decomposition was not retarded as much as the mineralization and hence dissolved organic nitrogen accumulated. Seasonal variations were also found in some of the biological processes. Concentration and distribution of nitrite (a transitory product formed from ammonia and nitrate) were influenced both by physical and biological processes
Microbiology of nutrient regeneration. Part II Distribution of nitrifying bacteria in Vellar Estuary
- Publication venue
- NISCAIR-CSIR, India
- Publication date
- 01/06/1977
- Field of study
6-9Nitrifying capacity or the biological potential in nitrification of both sediments and overlying water were tested. Ammonia oxidizing bacteria and nitrite oxidizing bacteria were estimated both in water and sediments in 4 zones of Vellar Estuary, Tamil Nadu, India. Both marine and limnetic forms of bacteria were counted along with other environmental parameters. Generally, nitrification process was more in sediments than in the water column. Distribution of marine and limnetic forms of nitrifying bacteria was chiefly controlled by salinity. In the monsoon months, nitrifying bacteria of limnetic or terrestrial origin dominated the marine form. In other months, marine nitrifying bacteria were more in marine and tidal zones of the estuary with a decrease towards upstream. Salinity and substrate concentration (ammonia and nitrite) were found to be the chief controlling factors of these bacteria
Studies on the nutrition of marine flatfish. The effect of dietary protein content on certain cell components and enzymes in the liver of Pleuronectes platessa
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study