93 research outputs found
Evidence for Adiabatic Magnetization of cold Dy_N Clusters
- Author
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2000
- Field of study
Magnetic properties of Dy_N clusters in a molecular beam generated with a
liquid helium cooled nozzle are investigated by Stern-Gerlach experiments. The
cluster magnetizations \mu_z are measured as a function of magnetic field (B =
0 - 1.6T) and cluster size (16 < N < 56). The most important observation is the
saturation of the magnetization \mu_z(B) at large field strengths. The
magnetization approaches saturation following the power law |\mu_z-\mu_0|
proportional to 1/\sqrt{B}, where \mu_0 denotes the magnetic moment. This gives
evidence for adiabatic magnetization.Comment: 4 pages, 3 figure
Anisotropy of ultra-thin ferromagnetic films and the spin reorientation transition
- Author
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 28/02/2002
- Field of study
The influence of uniaxial anisotropy and the dipole interaction on the
direction of the magnetization of ultra-thin ferromagnetic films in the
ground-state is studied. The ground-state energy can be expressed in terms of
anisotropy constants which are calculated in detail as function of the system
parameters and the film thickness. In particular non-collinear spin
arrangements are taken into account. Conditions for the appearance of a spin
reorientation transition are given and analytic results for the width of the
canted phase and its shift in applied magnetic fields associated with this
transition are derived.Comment: 6 pages, RevTeX
Spin Motion in Electron Transmission through Ultrathin Ferromagnetic Films Accessed by Photoelectron Spectroscopy
- Author
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 08/11/2002
- Field of study
Ab initio and model calculations demonstrate that the spin motion of
electrons transmitted through ferromagnetic films can be analyzed in detail by
means of angle- and spin-resolved core-level photoelectron spectroscopy. The
spin motion appears as precession of the photoelectron spin polarization around
and as relaxation towards the magnetization direction. In a systematic study
for ultrathin Fe films on Pd(001) we elucidate its dependence on the Fe film
thickness and on the Fe electronic structure. In addition to elastic and
inelastic scattering, the effect of band gaps on the spin motion is addressed
in particular.Comment: 4 pages, 5 figure
Schwinger boson theory of anisotropic ferromagnetic ultrathin films
- Author
- A. Abanov
- A. Auerbach
- A. Auerbach
- A. Berger
- A. Ecker
- A. Hucht
- A. Hucht
- A. Hucht
- A. Moschel
- A.V. Chubukov
- B. Schulz
- C. Herring
- C. Timm
- D. Li
- D.K. Morr
- D.P. Arovas
- D.P. Pappas
- Diep-the-Hung
- F.B. Anderson
- G. Garreau
- G. Lugert
- H.B. Callen
- H.B. Callen
- H.B.G. Casimir
- J. Schwinger
- J. Thomassen
- J.A.C. Bland
- K. Baberschke
- L.P. Shi
- M. Farle
- M. Farle
- M.E. Lines
- M.J. Manfra
- N. Read
- N. Read
- N.D. Mermin
- O. Iglesias
- O. Schulte
- O.A. Starykh
- P. Bruno
- P. Fröbrich
- P. Henelius
- P. Politi
- P.J. Jensen
- P.J. Jensen
- P.J. Jensen
- P.J. Jensen
- P.J. Jensen
- P.T. Saunders
- R. Allenspach
- R. Côté
- R. Tahir-Kheli
- R.P. Erickson
- R.P. Erickson
- S.B. Haley
- S.L. Sondhi
- S.M. Girvin
- S.T. Chui
- S.V. Maleev
- S.V. Tyablikov
- S.V. Tyablikov
- T. Holstein
- T.H. Moos
- U. Gradmann
- V.L. Pokrovsky
- W. Döring
- W. Haubenreisser
- X. Hu
- Y. Millev
- Y. Millev
- Y.T. Millev
- Y.T. Millev
- Z.Q. Qiu
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 14/09/2000
- Field of study
Ferromagnetic thin films with magnetic single-ion anisotropies are studied
within the framework of Schwinger bosonization of a quantum Heisenberg model.
Two alternative bosonizations are discussed. We show that qualitatively correct
results are obtained even at the mean-field level of the theory, similar to
Schwinger boson results for other magnetic systems. In particular, the
Mermin-Wagner theorem is satisfied: a spontaneous magnetization at finite
temperatures is not found if the ground state of the anisotropic system
exhibits a continuous degeneracy. We calculate the magnetization and effective
anisotropies as functions of exchange interaction, magnetic anisotropies,
external magnetic field, and temperature for arbitrary values of the spin
quantum number. Magnetic reorientation transitions and effective anisotropies
are discussed. The results obtained by Schwinger boson mean-field theory are
compared with the many-body Green's function technique.Comment: 14 pages, including 7 EPS figures, minor changes, final version as
publishe
Adsorbate and thermally induced spin reorientation transition in low-temperature-grown Fe/Cu(001)
- Author
- A. Biedermann
- A. Biedermann
- A. Enders
- A. Kirilyuk
- A. Vaterlaus
- B. Heinrich
- B. Újfalussy
- D. Li
- D. Peterka
- D. Qian
- D. Spišak
- D.P. Pappas
- E. Mentz
- F. Jona
- G. Blyholder
- G. Haas
- H. Zillgen
- J. Bansmann
- J. Giergiel
- J. Giergiel
- J. Radnik
- J. Shen
- J. Thomassen
- K. Kern
- K. Man
- M. Salvietti
- M.A. Torija
- P. Bruno
- P. Ferro
- R. Allenspach
- R. Allenspach
- R. Moroni
- R. Vollmer
- R. Vollmer
- R. Vollmer
- S. Müller
- T. Gutjahr-Löser
- V. Morruzi
- W. Ling
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- Field of study
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
- 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
- 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
- Hansen H
- 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
- Hello P
- 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
- Heurs M
- Hewitt A.L
- Higginbotham S
- Hild S
- Hill P
- Himemoto Y
- Hines A.S
- Hirata N
- Hirose C
- Ho T-C
- Hochheim S
- Hofman D
- Hohmann J.N
- Holcomb D.G
- Holland N.A
- Hollows I.J
- Holmes Z.J
- Holt K
- Holz D.E
- Hong Q
- Hough J
- 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
- Ide S
- Idzkowski B
- Iess A
- Inayoshi K
- Inoue Y
- Iosif P
- Isi M
- Isleif K
- Ito K
- Itoh Y
- Iyer B.R
- Jaberianhamedan V
- Jacqmin T
- Jacquet P.-E
- Jadhav S.J
- Jadhav S.P
- Jain T
- James A.L
- Jan A.Z
- Jani K
- Janquart J
- Janssens K
- Janthalur N.N
- Jaranowski P
- Jariwala D
- Jaume R
- Jenkins A.C
- Jenner K
- 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
- Jung K
- 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
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- Kim J.C
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- 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
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- 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
- Koper N
- Korobko M
- Kovalam M
- Koyama N
- Kozak D.B
- Kozakai C
- Kringel V
- 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
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- Lantz B
- Lartaux-Vollard A
- Lasky P.D
- Laxen M
- Lazzarini A
- Lazzaro C
- Leaci P
- Leavey S
- Lebohec S
- Lecoeuche Y.K
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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
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- Li T.G. F
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- Lin C-Y
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- Lin L.C.-C
- Linde F
- Linker S.D
- Linley J.N
- Littenberg T.B
- Liu G.C
- Liu J
- Liu K
- Liu X
- Llamas F
- Lo R.K. L
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- London L.T
- Longo A
- Lopez D
- Lorenzini M
- Loriette V
- Lormand M
- Losurdo G
- Lott T.P
- Lough J.D
- Lousto C.O
- Lovelace G
- Lucaccioni J.F
- Lumaca D
- Lundgren A.P
- Luo L.-W
- Lynam J.E
- Lück H
- Ma'Arif M
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- 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
A joint Fermi-GBM and Swift-BAT analysis of gravitational-wave candidates from the third gravitational-wave observing run
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- 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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- 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
CANTED MAGNETIC MOMENTS AT THE Gd(0001) SURFACE
- Author
- Publication venue
- DigitalCommons@University of Nebraska - Lincoln
- Publication date
- 01/05/1993
- Field of study
With spin polarized electron spectroscopies, we have investigated ordered GD(0001) films deposited on W(110). The photoemission features of the gadolinium 5d surface state, the 4f levels, and the background exhibit considerable spin polarization along the same direction in the plane of the film, indicative of ferromagnetic coupling between the surface and the bulk. The 4f spin polarized photoemission data provides strong evidence that the surface 4f polarization differs from the bulk 4f polarization for Gd(0001). Our temperature dependent measurements with spin polarized secondary electron spectroscopy conclusively establishes that the surface of clean Gd(0001) possesses a perpendicular polarization component which persists to an enhanced surface Curie temperature. Small amounts of contamination at the surface result in the disappearance of the perpendicular component and, therefore, a more perfect ferromagnetic coupling between the surface and the bulk
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