138 research outputs found
Lithospheric architecture and mantle metasomatism linked to iron oxide Cu-Au ore formation: multidisciplinary evidence from the Olympic Dam region, South Australia
- Publication venue
- 'American Geophysical Union (AGU)'
- Publication date
- 01/01/2018
- Field of study
The role of lithospheric architecture and the mantle in the genesis of iron oxide copper‐gold (IOCG) deposits is controversial. Using the example of the Precambrian Gawler Craton (South Australia), which hosts the giant Olympic Dam IOCG deposit, we integrate geophysical data (seismic tomography and magnetotellurics) with geological and geochemical data to develop a new interpretation of the lithospheric setting of these deposits. Spatially, IOCG deposits are located above the margin of a mantle lithospheric zone with anomalously high electrical conductivities (resistivity 1.80). The high conductivity cannot be explained by water‐bearing olivine‐rich rock alone. Relatively fertile and metasomatized peridotitic mantle with additional high‐Vp/Vs phases, for example, clinohumite, hydrous garnet, and/or phlogopite, could explain the anomalous velocity and conductivity. The top of this high‐Vp/Vsh zone marks a midlithospheric discontinuity at ~100–130 km depth that is interpreted to reflect locally orthopyroxene‐rich mantle. A sub‐Moho zone with high Vp/Vsh at ~40–80 km depth correlates spatially with primitive Nd isotope signatures and arc‐related ~1,620–1,610 Ma magmatism and is interpreted as the eclogitic root of a magmatic arc. Mafic volcanics contemporaneous with ~1,590 Ma IOCG mineralization have geochemistry suggesting derivation from subduction‐modified lithospheric mantle. We suggest that Olympic Dam formed inboard of a continental margin in a postsubduction setting, related to foundering of previously refertilized and metasomatized lithospheric mantle. Deposits formed during the switch from compression to extension, following delamination‐related uplift and exhumation.R.G. Skirrow, S.E. van der Wielen, D.C. Champion, K. Czarnota, and S. Thie
Spatial variations in lead isotopes, Tasman Element, eastern Australia
- Author
- Publication venue
- 'Geoscience Australia'
- Publication date
- 01/01/2017
- Field of study
Lead isotope data from ore deposits and mineral occurrences in the Tasman Element of eastern Australia have been used to construct isotopic maps of this region. These maps exhibit systematic patterns in parameters derived from isotope ratios. The parameters include μ (238U/204Pb), as calculated using the Cumming and Richards (1975) lead evolution model, and the difference between true age of mineralisation and the Cumming and Richards lead isotope model age of mineralisation (Δt).
Variations in μ coincide with boundaries at the orogen, subprovince and zone scales. The boundary between the Lachlan and New England orogens is accompanied by a decrease in μ, and within the Lachlan Orogen, the Central Subprovince is characterised by μ that is significantly higher than in the adjacent Eastern and Western subprovinces. Within the Eastern Subprovince, the Cu-Au-rich Macquarie Arc is characterised by significantly lower μ relative to adjacent rocks.
The Macquarie Arc is also characterised by very high Δt (generally above 200 Myr). Other regions characterised by very high Δt include western Tasmania, the southeastern New England Orogen, and the Hodgkinson Province in northern Queensland. These anomalies are within a broad pattern of decreasing Δt from east to west, with Paleozoic deposits within or adjacent to Proterozoic crust characterised by Δt values of 50 Myr or below.
The patterns in Δt are interpreted to reflect the presence of the two major tectonic components involved in the Paleozoic Tasman margin in Australia (cf., Münker, 2000): subducting proto-Pacific crust (Δt >150 Myr), and Proterozoic Australia crust (Δt < 50 Myr) on the over-riding plate. Proterozoic Australia crustal sources are interpreted to dominate the western parts of the Tasman Element and Proterozoic crust further to the west, whereas Pacific crustal sources are inferred to characterise western Tasmania and much of the eastern part of the Tasman Element. Contrasts in Δt between the Cambrian Mount Read Volcanics in western Tasmania and similar aged rocks in western Victoria and New South Wales make direct tectonic correlation between these rocks problematic
Pulsar Timing and its Application for Navigation and Gravitational Wave Detection
- Author
- A. Sesana
- A. Sesana
- A. Sesana
- A.W. Hotan
- C.M. Espinoza
- C.M. Will
- D.C. Backer
- D.J. Champion
- D.J. Reardon
- D.N. Matsakis
- F. Shankar
- F. Özel
- G. Desvignes
- G. Hobbs
- H.P. Robertson
- I.I. Shapiro
- J. Alsing
- J. Antoniadis
- J. Kormendy
- J.H. Taylor
- J.H. Taylor
- J.H. Taylor Jr.
- J.M. Weisberg
- J.P.W. Verbiest
- J.P.W. Verbiest
- J.R. Oppenheimer
- K. Yagi
- L. Lentati
- M. Kramer
- M. Yu
- M.A. Alpar
- M.A. McLaughlin
- M.D. Young
- M.G. Bernhardt
- M.G. Bernhardt
- P.B. Demorest
- P.C. Peters
- P.C.C. Freire
- P.C.C. Freire
- P.D. Lasky
- R. Blandford
- R. Haasteren van
- R. Smits
- R.H. Battin
- R.M. Shannon
- R.S. Foster
- R.W. Hellings
- S. Babak
- T. Damour
- T. Damour
- T. Damour
- T.M. Tauris
- V.M. Kaspi
- W. Becker
- W. Becker
- X.J. Zhu
- X.P. Deng
- X.P. Deng
- Z. Arzoumanian
- Z. Arzoumanian
- Z. Arzoumanian
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/05/2017
- Field of study
Pulsars are natural cosmic clocks. On long timescales they rival the
precision of terrestrial atomic clocks. Using a technique called pulsar timing,
the exact measurement of pulse arrival times allows a number of applications,
ranging from testing theories of gravity to detecting gravitational waves. Also
an external reference system suitable for autonomous space navigation can be
defined by pulsars, using them as natural navigation beacons, not unlike the
use of GPS satellites for navigation on Earth. By comparing pulse arrival times
measured on-board a spacecraft with predicted pulse arrivals at a reference
location (e.g. the solar system barycenter), the spacecraft position can be
determined autonomously and with high accuracy everywhere in the solar system
and beyond. We describe the unique properties of pulsars that suggest that such
a navigation system will certainly have its application in future astronautics.
We also describe the on-going experiments to use the clock-like nature of
pulsars to "construct" a galactic-sized gravitational wave detector for
low-frequency (f_GW ~1E-9 - 1E-7 Hz) gravitational waves. We present the
current status and provide an outlook for the future.Comment: 30 pages, 9 figures. To appear in Vol 63: High Performance Clocks,
Springer Space Science Review
Factors influencing terrestriality in primates of the Americas and Madagascar
- Author
- Adams D.B.
- Adams D.B.
- Allgas N.
- Allgas N.
- Amato K.R.
- Amato K.R.
- Andriamahaihavana M.
- Andriamahaihavana M.
- Aristizabal J.F.
- Aristizabal J.F.
- Baden A.L.
- Baden A.L.
- Balestri M.
- Balestri M.
- Barnett A.
- Barnett A.
- Bicca-Marques J.C.
- Bicca-Marques J.C.
- Bowler M.
- Bowler M.
- Boyle S.A.
- Boyle S.A.
- Brown M.
- Brown M.
- Caillaud D.
- Caillaud D.
- Calegaro-Marques C.
- Calegaro-Marques C.
- Campbell C.J.
- Campbell C.J.
- Campera M.
- Campera M.
- Campos F. A.
- Campos F. A.
- Cardoso T.S.
- Cardoso T.S.
- Carretero-Pinzón X.
- Carretero-Pinzón X.
- Champion J.
- Champion J.
- Chapman C.A.
- Chapman C.A.
- Chaves Ó.M.
- Chaves Ó.M.
- Chen-Kraus C.
- Chen-Kraus C.
- Colquhoun I.C.
- Colquhoun I.C.
- de Melo F.R.
- de Melo F.R.
- Dean B.
- Dean B.
- Donati G.
- Donati G.
- Dubrueil C.
- Dubrueil C.
- Ellis K.M.
- Ellis K.M.
- Eppley T.M.
- Eppley T.M.
- Erhart E.M.
- Erhart E.M.
- Evans K.J.E.
- Evans K.J.E.
- Fedigan L.M.
- Fedigan L.M.
- Felton A.M.
- Felton A.M.
- Ferreira R.G.
- Ferreira R.G.
- Fichtel C.
- Fichtel C.
- Fonseca M.L.
- Fonseca M.L.
- Fontes I.P.
- Fontes I.P.
- Fortes V.B.
- Fortes V.B.
- Fumian I.
- Fumian I.
- Ganzhorn J.U.
- Ganzhorn J.U.
- Gibson D.
- Gibson D.
- Gonçalves J.R.
- Gonçalves J.R.
- Guzzo G.B.
- Guzzo G.B.
- Hall K.
- Hall K.
- Hartwell K.S.
- Hartwell K.S.
- Heymann E.W.
- Heymann E.W.
- Hilário R.R.
- Hilário R.R.
- Hoeks S.
- Hoeks S.
- Holmes S.M.
- Holmes S.M.
- Irwin M.T.
- Irwin M.T.
- Johnson S.E.
- Johnson S.E.
- Kappeler P.M.
- Kappeler P.M.
- Kelley E.A.
- Kelley E.A.
- King T.
- King T.
- Knogge C.
- Knogge C.
- Koch F.
- Koch F.
- Kowalewski M.M.
- Kowalewski M.M.
- Lange L.R.
- Lange L.R.
- Lauterbur M.E.
- Lauterbur M.E.
- Lins P.
- Lins P.
- Louis E.E.
- Louis E.E.
- Lutz M.C
- Lutz M.C
- Martínez J.
- Martínez J.
- Melin A.D.
- Melin A.D.
- Mihaminekena T.H.
- Mihaminekena T.H.
- Mogilewsky M.S.
- Mogilewsky M.S.
- Moreira L.S.
- Moreira L.S.
- Moura L.A.
- Moura L.A.
- Muhle C.B.
- Muhle C.B.
- Nagy-Reis M.B.
- Nagy-Reis M.B.
- Norconk M.A.
- Norconk M.A.
- Notman H.
- Notman H.
- Ostner J.
- Ostner J.
- Owen M.A.
- Owen M.A.
- O’Mara M. T.
- O’Mara M. T.
- Patel E.R.
- Patel E.R.
- Pavelka M.S.M.
- Pavelka M.S.M.
- Pinacho-Guendulain B.
- Pinacho-Guendulain B.
- Porter L.M.
- Porter L.M.
- Pozo-Montuy G.
- Pozo-Montuy G.
- Raboy B.E.
- Raboy B.E.
- Rahalinarivo V.
- Rahalinarivo V.
- Raharinoro N.A.
- Raharinoro N.A.
- Rakotomalala Z.
- Rakotomalala Z.
- Ramos-Fernández G.
- Ramos-Fernández G.
- Rasamisoa D.C.
- Rasamisoa D.C.
- Ratsimbazafy J.
- Ratsimbazafy J.
- Ravaloharimanitra M.
- Ravaloharimanitra M.
- Razafindramanana J.
- Razafindramanana J.
- Razanaparany T.P.
- Razanaparany T.P.
- Righini N.
- Righini N.
- Robson N.M.
- Robson N.M.
- Sanamo J.
- Sanamo J.
- Santacruz N.
- Santacruz N.
- Santini L.
- Santini L.
- Sato H.
- Sato H.
- Sauther M.L.
- Sauther M.L.
- Scarry C.J.
- Scarry C.J.
- Serio-Silva J.C.
- Serio-Silva J.C.
- Shanee S.
- Shanee S.
- Smith Aguilar S.E.
- Smith Aguilar S.E.
- Smith A.C.
- Smith A.C.
- Souza-Alves J.P.
- Souza-Alves J.P.
- Stavis V.K.
- Stavis V.K.
- Steffens K.J.E.
- Steffens K.J.E.
- Stone A.I.
- Stone A.I.
- Strier K.B.
- Strier K.B.
- Suarez S.A.
- Suarez S.A.
- Talebi M.
- Talebi M.
- Tecot S.R.
- Tecot S.R.
- Tujague M.P.
- Tujague M.P.
- Valenta K.
- Valenta K.
- Van Belle S.
- Van Belle S.
- Vasey N.
- Vasey N.
- Wallace R.B.
- Wallace R.B.
- Welch G.
- Welch G.
- Wright P. C.
- Wright P. C.
- Publication venue
- National Academy of Sciences, U. S.
- Publication date
- 01/01/2022
- Field of study
Among mammals, the order Primates is exceptional in having a high taxonomic richness in which the taxa are arboreal, semiterrestrial, or terrestrial. Although habitual terrestriality is pervasive among the apes and African and Asian monkeys (catarrhines), it is largely absent among monkeys of the Americas (platyrrhines), as well as galagos, lemurs, and lorises (strepsirrhines), which are mostly arboreal. Numerous ecological drivers and species-specific factors are suggested to set the conditions for an evolutionary shift from arboreality to terrestriality, and current environmental conditions may provide analogous scenarios to those transitional periods. Therefore, we investigated predominantly arboreal, diurnal primate genera from the Americas and Madagascar that lack fully terrestrial taxa, to determine whether ecological drivers (habitat canopy cover, predation risk, maximum temperature, precipitation, primate species richness, human population density, and distance to roads) or species-specific traits (body mass, group size, and degree of frugivory) associate with increased terrestriality. We collated 150,961 observation hours across 2,227 months from 47 species at 20 sites in Madagascar and 48 sites in the Americas. Multiple factors were associated with ground use in these otherwise arboreal species, including increased temperature, a decrease in canopy cover, a dietary shift away from frugivory, and larger group size. These factors mostly explain intraspecific differences in terrestriality. As humanity modifies habitats and causes climate change, our results suggest that species already inhabiting hot, sparsely canopied sites, and exhibiting more generalized diets, are more likely to shift toward greater ground use
Narrowband Searches for Continuous and Long-duration Transient Gravitational Waves from Known Pulsars in the LIGO-Virgo Third Observing Run
- Author
- Abbott R.
- Abbott T.D.
- Acernese F.
- Ackley K.
- Adams C.
- Adhikari N.
- Adhikari R.X.
- 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.
- 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.
- Angelova S.V.
- Ansoldi S.
- Antelis J.M.
- Antier S.
- Antonopoulou D.
- Appert S.
- Arai K.
- Arai K.
- Arai Y.
- Araki S.
- Araya A.
- Araya M.C.
- Areeda J.S.
- Arellano F.E.P.
- Aritomi N.
- Arnaud N.
- Aronson S.M.
- Arun K.G.
- Arzoumanian Z.
- Arène M.
- Asada H.
- Asali Y.
- Ashton G.
- Aso Y.
- Assiduo M.
- Aston S.M.
- Astone P.
- Aubin F.
- Austin C.
- Babak S.
- Badaracco F.
- Bader M.K.M.
- Badger C.
- Bae S.
- Bae Y.
- Baer A.M.
- Bagnasco S.
- Bai Y.
- Bailes M.
- Baiotti L.
- Baird J.
- Bajpai R.
- Ball M.
- Ballardin G.
- Ballmer S.W.
- Balsamo A.
- Baltus G.
- Banagiri S.
- 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.
- Bassiri R.
- Basti A.
- Basu A.
- Bawaj M.
- Bayley J.C.
- Baylor A.C.
- Bazzan M.
- Bedakihale V.M.
- Bejger M.
- Belahcene I.
- Benedetto V.
- Beniwal D.
- Bennett T.F.
- Bentley J.D.
- Benyaala M.
- Bergamin F.
- Berger B.K.
- Bernuzzi S.
- Bersanetti D.
- Bertolini A.
- Betzwieser J.
- Beveridge D.
- Bhandare R.
- Bhardwaj U.
- Bhattacharjee D.
- Bhaumik S.
- 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.
- Boer M.
- Bogaert G.
- Bogdanov S.
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- Bonavena L.D.
- Bondu F.
- Bonilla E.
- Bonnand R.
- Booker P.
- Boom B.A.
- Bork R.
- Boschi V.
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- Bossilkov V.
- Boudart V.
- Bouffanais Y.
- Bozzi A.
- Bradaschia C.
- Brady P.R.
- Bramley A.
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- Brau J.E.
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- Briggs J.H.
- Brillet A.
- Brinkmann M.
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- Brunett S.
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- Cagnoli G.
- Cahillane C.
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- Callister T.A.
- Calloni E.
- Cameron J.
- Camp J.B.
- Canepa M.
- Canevarolo S.
- Cannavacciuolo M.
- Cannon K.C.
- Canton T.D.
- Cao H.
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- Capocasa E.
- Capote E.
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- Carlin J.B.
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- Castaldi G.
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- Cella G.
- Cerdá-Durán P.
- Cesarini E.
- Chaibi W.
- Chakravarti K.
- Champion E.
- Chan C.
- Chan C.-H.
- Chan C.L.
- Chan K.
- Chan M.
- Chandra K.
- Chanial P.
- Chao S.
- Charlton P.
- Chase E.A.
- Chassande-Mottin E.
- Chatterjee C.
- Chatterjee D.
- Chatterjee D.
- Chaturvedi M.
- Chaty S.
- Chen C.
- 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.
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- Chiarini G.
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- Chiofalo M.L.
- Chiummo A.
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- Cipriano F.
- Cirone A.
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- Corban P.
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- Cordero-Carrión I.
- Corezzi S.
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- Cortese S.
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- Cotesta R.
- Coughlin M.W.
- Coulon J.-P.
- Countryman S.T.
- Cousins B.
- Couvares P.
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- Creighton J.D.E.
- Creighton T.D.
- Criswell A.W.
- Croquette M.
- Crowder S.G.
- Crowter K.
- 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.
- Dall'Osso S.
- Dana A.
- Daneshgaranbajastani L.M.
- Danilishin S.
- Danzmann K.
- Darsow-Fromm C.
- Dasgupta A.
- Datrier L.E.H.
- Datta S.
- Dattilo V.
- Dave I.
- Davier M.
- Davies G.S.
- 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.
- Deléglise S.
- Demarchi L.M.
- Demos N.
- Dent T.
- Depasse A.
- Desalvo R.
- Dhurandhar S.
- Diaz J.C.
- Diaz-Ortiz M.
- Didio N.A.
- Dietrich T.
- Ding B.
- Divakarla A.K.
- Dmitriev A.
- Doctor Z.
- Donovan F.
- Dooley K.L.
- Doravari S.
- Dorrington I.
- Drago M.
- Driggers J.C.
- Drori Y.
- Ducoin J.-G.
- Dupej P.
- Durante O.
- Duverne P.-A.
- Dwyer S.E.
- Dálya G.
- Díaz M.C.
- E Melo, I.T.
- 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.
- Enoto T.
- Errico L.
- Espinoza C.M.
- Essick R.C.
- Estellés H.
- Estevez D.
- Etienne Z.
- Etzel T.
- Evans M.
- Evans T.M.
- Ewing B.E.
- Fafone V.
- Fair H.
- Fairhurst S.
- Farah A.M.
- Farinon S.
- Farr B.
- Farr W.M.
- Farrow N.W.
- Fauchon-Jones E.J.
- Favaro G.
- Favata M.
- 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.
- Fiore L.D.
- Fiori I.
- Fishbach M.
- Fisher R.P.
- Fittipaldi R.
- Fiumara V.
- Flaminio R.
- Floden E.
- Flynn C.M.L.
- Fong H.
- Fonseca E.
- Font J.A.
- Fornal B.
- Forsyth P.W.F.
- Franke A.
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- Zweizig J.
- Publication venue
- London : Institute of Physics Publ.
- Publication date
- 01/01/2022
- Field of study
Isolated neutron stars that are asymmetric with respect to their spin axis are possible sources of detectable continuous gravitational waves. This paper presents a fully coherent search for such signals from eighteen pulsars in data from LIGO and Virgo's third observing run (O3). For known pulsars, efficient and sensitive matched-filter searches can be carried out if one assumes the gravitational radiation is phase-locked to the electromagnetic emission. In the search presented here, we relax this assumption and allow both the frequency and the time derivative of the frequency of the gravitational waves to vary in a small range around those inferred from electromagnetic observations. We find no evidence for continuous gravitational waves, and set upper limits on the strain amplitude for each target. These limits are more constraining for seven of the targets than the spin-down limit defined by ascribing all rotational energy loss to gravitational radiation. In an additional search, we look in O3 data for long-duration (hours-months) transient gravitational waves in the aftermath of pulsar glitches for six targets with a total of nine glitches. We report two marginal outliers from this search, but find no clear evidence for such emission either. The resulting duration-dependent strain upper limits do not surpass indirect energy constraints for any of these targets. © 2022. The Author(s). Published by the American Astronomical Society
Search for Gravitational Waves Associated with Gamma-Ray Bursts Detected by Fermi and Swift during the LIGO-Virgo Run O3b
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- Yamamoto Kazuhiro
- Yamamoto Kohei
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- Ying M.
- Yokogawa K.
- Yokoyama J.
- Yokozawa T.
- Yoo J.
- Yoshioka T.
- Yu Hang
- Yu Haocun
- Yuzurihara H.
- Zadrzny A.
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- Zimmerman A.B.
- Zucker M.E.
- Zweizig J.
- Publication venue
- London : Institute of Physics Publ.
- Publication date
- 01/01/2022
- Field of study
We search for gravitational-wave signals associated with gamma-ray bursts (GRBs) detected by the Fermi and Swift satellites during the second half of the third observing run of Advanced LIGO and Advanced Virgo (2019 November 1 15:00 UTC-2020 March 27 17:00 UTC). We conduct two independent searches: A generic gravitational-wave transients search to analyze 86 GRBs and an analysis to target binary mergers with at least one neutron star as short GRB progenitors for 17 events. We find no significant evidence for gravitational-wave signals associated with any of these GRBs. A weighted binomial test of the combined results finds no evidence for subthreshold gravitational-wave signals associated with this GRB ensemble either. We use several source types and signal morphologies during the searches, resulting in lower bounds on the estimated distance to each GRB. Finally, we constrain the population of low-luminosity short GRBs using results from the first to the third observing runs of Advanced LIGO and Advanced Virgo. The resulting population is in accordance with the local binary neutron star merger rate. © 2022. The Author(s). Published by the American Astronomical Society
Search for gravitational-wave transients associated with magnetar bursts in advanced LIGO and advanced Virgo data from the third observing run
- Author
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- 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
A joint Fermi-GBM and Swift-BAT analysis of gravitational-wave candidates from the third gravitational-wave observing run
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- 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.
- Zhou R.
- Zhou Z.
- Zhu X.J.
- Zhu Z.-H.
- Zimmerman A.B.
- Zucker M.E.
- Zweizig J.
- 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
Constraints on the cosmic expansion history from GWTC–3
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- Zweizig J.
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/06/2023
- 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
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
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