114 research outputs found
κ−(BEDT−TTF)2X organic crystals: superconducting versus antiferromagnetic instabilities in an anisotropic triangular lattice Hubbard model
- Author
- Publication venue
- 'Canadian Science Publishing'
- Publication date
- 23/10/2000
- Field of study
A Hubbard model at half-filling on an anisotropic triangular lattice has been
proposed as the minimal model to describe conducting layers of
κ−(BEDT−TTF)2X organic materials. The model interpolates between the
square lattice and decoupled chains. The κ−(BEDT−TTF)2X materials
present many similarities with cuprates, such as the presence of unconventional
metallic properties and the close proximity of superconducting and
antiferromagnetic phases. As in the cuprates, spin fluctuations are expected to
play a crucial role in the onset of superconductivity. We perform a
weak-coupling renormalization-group analysis to show that a superconducting
instability occurs. Frustration in the antiferromagnetic couplings, which
arises from the underlying geometrical arrangement of the lattice, breaks the
perfect nesting of the square lattice at half-filling. The spin-wave
instability is suppressed and a superconducting instability predominates. For
the isotropic triangular lattice, there are again signs of long-range magnetic
order, in agreement with studies at strong-coupling.Comment: 4 pages, 5 eps figs, to appear in Can. J. Phys. (proceedings of the
Highly Frustrated Magnetism (HFM-2000) conference, Waterloo, Canada, June
2000
GATA-2 and GATA-3 regulate trophoblast-specific gene expression in vivo.
- Author
- Publication venue
- Publication date
- 01/01/1997
- Field of study
We previously demonstrated that the zinc finger transcription factors GATA-2 and GATA-3 are expressed in trophoblast giant cells and that they regulate transcription from the mouse placental lactogen I gene promoter in a transfected trophoblast cell line. We present evidence here that both of these factors regulate transcription of the placental lactogen I gene, as well as the related proliferin gene, in trophoblast giant cells in vivo. Placentas lacking GATA-3 accumulate placental lactogen I and proliferi
Critical exponents and equation of state of the three-dimensional Heisenberg universality class
- Author
- A. Aharony
- A. Aharony
- A. Arrott
- A. Pelissetto
- A. Pelissetto
- A. Pelissetto
- A. Pelissetto
- A. Pelissetto
- A. Pelissetto
- A. Perumal
- A. Perumal
- A. Schwartz
- A.A. Caparica
- A.D. Bruce
- A.I. Sokolov
- A.J. Guttmann
- A.P. Gottlob
- Andrea Pelissetto
- B. Stroka
- B.D. Josephson
- C. Bagnuls
- C. Bervillier
- C. Bervillier
- C. Bervillier
- C. Bührer
- C. Holm
- C. Holm
- C. Holm
- C.A. Ramos
- C.S. Arnold
- C.S. Hong
- C.V. Mohan
- D.J. Wallace
- D.L. Hunter
- D.L. Hunter
- D.L. Hunter
- E. Brézin
- E. Brézin
- E. Brézin
- E. Brézin
- Ettore Vicari
- F. Jasch
- F.Y. Yang
- G.A. Baker Jr.
- G.A. Baker Jr.
- G.v. Gersdorff
- H. Kleinert
- H. Kleinert
- H. Kleinert
- H. Kleinert
- H.G. Ballesteros
- H.G. Ballesteros
- H.G. Ballesteros
- I.D. Lawrie
- I.M. Mryglod
- J. Adler
- J. Berges
- J. Mira
- J.C. Le Guillou
- J.C. Le Guillou
- J.H. Zhao
- J.H. Zhao
- J.J. Rehr
- J.M. Carmona
- J.S. Kouvel
- K. Binder
- K. Binder
- K. Ghosh
- K.E. Newman
- K.G. Chetyrkin
- L. Schäfer
- M. Barmatz
- M. Campostrini
- M. Campostrini
- M. Campostrini
- M. Campostrini
- M. Campostrini
- M. Caselle
- M. Hasenbusch
- M. Hasenbusch
- M. Hasenbusch
- M. Hasenbusch
- M. Hasenbusch
- M. Lüscher
- M. Marinelli
- M. Sambasiva Rao
- M. Sambasiva Rao
- M. Seeger
- M. Shaham
- M. Stroesser
- M.A. Kobeissi
- M.C. Martin
- M.E. Fisher
- M.E. Fisher
- M.E. Fisher
- M.E. Fisher
- M.R. Said
- Martin Hasenbusch
- Massimo Campostrini
- N. Tetradis
- O. Bohr
- O. Källbäck
- P. Butera
- P. Butera
- P. Butera
- P. Peczak
- P. Schofield
- P. Schofield
- P.D. Babu
- Paolo Rossi
- R. Abe
- R. Guida
- R. Guida
- R. Reisser
- R.H. Heffner
- S. Hikami
- S. Hikami
- S. Srinath
- S.-H. Tsai
- S.A. Larin
- S.E. Lofland
- S.E. Lofland
- S.F. Fischer
- S.G. Barsov
- S.N. Kaul
- S.N. Kaul
- S.N. Kaul
- T. Brückel
- T. Reisz
- V.I. Yukalov
- W. Bernreuther
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2002
- Field of study
We improve the theoretical estimates of the critical exponents for the
three-dimensional Heisenberg universality class. We find gamma=1.3960(9),
nu=0.7112(5), eta=0.0375(5), alpha=-0.1336(15), beta=0.3689(3), and
delta=4.783(3). We consider an improved lattice phi^4 Hamiltonian with
suppressed leading scaling corrections. Our results are obtained by combining
Monte Carlo simulations based on finite-size scaling methods and
high-temperature expansions. The critical exponents are computed from
high-temperature expansions specialized to the phi^4 improved model. By the
same technique we determine the coefficients of the small-magnetization
expansion of the equation of state. This expansion is extended analytically by
means of approximate parametric representations, obtaining the equation of
state in the whole critical region. We also determine a number of universal
amplitude ratios.Comment: 40 pages, final version. In publication in Phys. Rev.
Search for Gravitational Waves Associated with Gamma-Ray Bursts Detected by Fermi and Swift during the LIGO-Virgo Run O3b
- 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.
- Appert S.
- Arai Koji
- Arai Koya
- Arai Y.
- Araki S.
- Araya A.
- Araya M.C.
- Areeda J.S.
- Arellano F. E. Peña
- Aritomi N.
- Arnaud N.
- Aronson S.M.
- Arun K.G.
- 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.
- 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.
- 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.
- Berry C.P.L.
- 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.
- Boldrini M.
- 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.
- 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.
- Bulik T.
- Bulten H.J.
- Buonanno A.
- Buscicchio R.
- Buskulic D.
- Bustillo J. Calderón
- Buy C.
- Byer R.L.
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- Cadonati L.
- Cagnoli G.
- Cahillane C.
- Callaghan J.D.
- Callister T.A.
- Calloni E.
- Cameron J.
- Camp J.B.
- Canepa M.
- Canevarolo S.
- Cannavacciuolo M.
- Cannon K.C.
- Canton T. Dal
- Cao H.
- Cao Z.
- Capocasa E.
- Capote E.
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- Carlin J.B.
- Carney M.F.
- Carpinelli M.
- Carrillo G.
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- Carver T.L.
- Casentini C.
- Castaldi G.
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- Cavaglià M.
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- Ceasar M.
- 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 Debarati
- Chatterjee Deep
- Chaturvedi M.
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- Cheung H.Y.
- Chia H.Y.
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- Chiarini G.
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- Chiofalo M.L.
- Chiummo A.
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- Choudhary R.K.
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- Christensen N.
- Chu H.
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- Chu Y.-K.
- Chua S.
- Chung K.W.
- Ciani G.
- Ciecielag P.
- Cieślar M.
- Cifaldi M.
- Ciobanu A.A.
- Ciolfi R.
- Cipriano F.
- Cirone A.
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- Clearwater P.
- Clesse S.
- Cleva F.
- Coccia E.
- Codazzo E.
- Cohadon P.-F.
- Cohen D.E.
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- Colleoni M.
- Collette C.G.
- Colombo A.
- Colpi M.
- Compton C.M.
- Constancio M.
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- Cordero-Carrión I.
- Corezzi S.
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- Corsi A.
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- Costa C.A.
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- Coulon J.-P.
- Countryman S.T.
- Cousins B.
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- Creighton J.D.E.
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- Cumming A.
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- D'Urso D.
- Dabadie P.
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- Dana A.
- Daneshgaranbajastani L.M.
- Danilishin S.
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- 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.
- Dean R.
- Debra D.
- Deenadayalan M.
- Degallaix J.
- Deléglise S.
- Demarchi L.M.
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- Dent T.
- Depasse A.
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- Dorrington I.
- Drago M.
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- Ducoin J.-G.
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- Durante O.
- Duverne P.-A.
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- E Melo I. Tosta
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- Fafone V.
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- Farr B.
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- Fauchon-Jones E.J.
- Favaro G.
- Favata M.
- Favero V. Del
- Fays M.
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- Feicht J.
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- Ferguson D.L.
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- Ferrante I.
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- Figura P.
- Fiore L. Di
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- Fiumara V.
- Flaminio R.
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- Forsyth P.W.F.
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- Frasconi F.
- Frederick C.
- Freed J.P.
- Frei Z.
- Freise A.
- Frey R.
- Fritschel P.
- Frolov V.V.
- Fronzo C. Di
- Fronzé G.G.
- Fujii Y.
- Fujikawa Y.
- Fukunaga M.
- Fukushima M.
- Fulda P.
- Fyffe M.
- Gabbard H.A.
- Gadre B.U.
- Gair J.R.
- Gais J.
- Galaudage S.
- Gamba R.
- Ganapathy D.
- Ganguly A.
- Gao D.
- Gaonkar S.G.
- Garaventa B.
- García-Núñez C.
- García-Quirós C.
- Garufi F.
- Gateley B.
- Gaudio S.
- 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
- Giacomazzo B.
- Giacoppo L.
- Giaime J.A.
- Giardina K.D.
- Gibson D.R.
- Gier C.
- Giesler M.
- Giorgio C. Di
- Giovanni F. Di
- Giovanni M. Di
- Giri P.
- Girolamo T. Di
- Gissi F.
- Glanzer J.
- Gleckl A.E.
- Godwin P.
- Goetz E.
- Goetz R.
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- Goncharov B.
- González G.
- Gopakumar A.
- Gosselin M.
- Gouaty R.
- Gould D.W.
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- Grado A.
- Granata M.
- Granata V.
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- Guo Y.
- Gupta Anchal
- Gupta Anuradha
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- Gustafson R.
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- Kalogera V.
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- Kang G.
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- Krishnendu N.V.
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- Yamamoto Kazuhiro
- Yamamoto Kohei
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- Yang Z.
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- Yelikar A.B.
- Ying M.
- Yokogawa K.
- Yokoyama J.
- Yokozawa T.
- Yoo J.
- Yoshioka T.
- Yu Hang
- Yu Haocun
- Yuzurihara H.
- Zadrzny A.
- Zanolin M.
- Zeidler S.
- Zelenova T.
- Zendri J.-P.
- Zevin M.
- Zhan M.
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- Zhao Yue
- Zheng Y.
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- Zhu Z.-H.
- 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
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.
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- 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-wave transients associated with magnetar bursts in advanced LIGO and advanced Virgo data from the third observing run
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- Washington N.Y
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- Weinstein A.J
- Weiss R
- Weller C.M
- Weller R.A
- Wellmann F
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- Wessels P
- Wette K
- Whelan J.T
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- Whittle C
- Wilken D
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- Williams M.J
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- Wysocki D.M
- Xiao L
- Yamada T
- Yamamoto H
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- Yang Yang
- Yap M.J
- Yeeles D.W
- Yeh S.-W
- Yelikar A.B
- Ying M
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu Hang
- Yu Haocun
- Yuzurihara H
- Zadrożny A
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- Zevin M
- Zhan M
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- Zhao Yue
- Zhou R
- Zhou Z
- Zhu X.J
- 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
A joint Fermi-GBM and Swift-BAT analysis of gravitational-wave candidates from the third gravitational-wave observing run
- Author
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- Abe H.
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- 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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- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2023
- 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
Effects of particulates, heavy metals and acid gas on the removals of NO and PAHs by V2O5-WO3 catalysts in waste incineration system
- Publication venue
- 'Elsevier BV'
- Publication date
- 11/06/2014
- Field of study
This study investigated the activities of prepared and commercial V2O5-WO3 catalysts for simultaneous removals of NO and polycyclic aromatic hydrocarbons (PAHs) and the influences of particulates, heavy metals, SO2, and HCl on the performances of catalysts. The experiments were carried out in a laboratory-scale waste incineration system equipped with a catalyst reactor. The DREs of PAHs by prepared and commercial V2O5-WO3 catalysts were 64% and 72%, respectively. Increasing the particulate concentrations in flue gas suppressed the DRE of PAHs, but increasing the carbon content on surface of catalysts promotes the NO conversions. The DRE of PAHs by the catalysts was significantly decreased by the increased concentrations of heavy metal Cd, but was promoted by high concentration of Pb. The influence level of SO2 was higher than HCl on the performances of V2O5-WO3 catalysts for PAHs removal, but was lower than HCl for NO removal. Prepared and commercial V2O5-WO3 catalysts have similar trends on the effects of particulates, heavy metals, SO2, and HCl. The results of ESCA analysis reveal that the presences of these pollutants on the surface of catalysts did not change the chemical state of V and W. (C) 2009 Elsevier B.V. All rights reserved
Influence of vacancy defect density on electrical properties of armchair single wall carbon nanotube
- Publication venue
- 'Elsevier BV'
- Publication date
- 06/06/2014
- Field of study
The relationship between the bandgap and the vacancy density is investigated from first principles. The range influence of a vacancy defect due to structural deformation is characterized and a microscopic explanation is proposed to relate the structural deformation to the bandgap variation. In order to investigate the effect of the defect density on carbon nanotube, 5 models of (5,5) armchair carbon nanotubes were built with the defect density as one vacancy per 79, 119, 159, 199 and 239 carbon atoms, respectively. The long range of influence of a MVD is characterized by structural deformation analysis and the strain caused by the MVD is the main reason to cause the strong fluctuation in bandgap of the defected armchair SWCNTs. However, no simple correlation between the MVD density and bandgap, are found. Our results can shed some light on the instability of the defected armchair SWCNTs in electronic properties synthesized via ion-irradiation for future potential applications. (C) 2007 Elsevier B.V. All rights reserved
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