57 research outputs found
The node of Ranvier in CNS pathology
- Author
- A Battefeld
- A Desmazieres
- A Duflocq
- A Hayashi
- A Lorincz
- A Nans
- A Nazeri
- AA Jarjour
- AD Goodman
- AE Baum
- AH Seidl
- AM Pillai
- AR Blight
- B Popko
- B Zonta
- BD Trapp
- BG Xiao
- C Bi
- C Chen
- C Cifuentes-Diaz
- C Elliott
- C Gu
- C Hildebrand
- C Hildebrand
- C Kopp-Scheinpflug
- C Moll
- C O’Dushlaine
- CF Babbs
- D Grozeva
- David Attwell
- DL Browne
- DL Sherman
- E Ozkaynak
- E Peles
- E Peles
- E Stogmann
- E Wallstrom
- ED Buttermore
- EG Sozmen
- EK Mathey
- ET Landaas
- F Ullen
- G Wolswijk
- G Xie
- GP Garcia-Fresco
- GR Anderson
- H Kuba
- H Ouyang
- H Vacher
- H Wang
- HC Mefford
- HM Brew
- I Coman
- I Horresh
- I Vabnick
- I. Lorena Arancibia-Carcamo
- J Barry
- J Devaux
- J Devaux
- J Elia
- J Ritter
- J Rosenbluth
- J Rosenbluth
- J Sun
- J Wang
- JB Sun
- JC Rios
- JC Rios
- JD Hinman
- JD Kocsis
- JD Kocsis
- JI Friedman
- JJ Devaux
- JJ Harris
- JJ Lawrence
- JL Dupree
- JL Salzer
- JM Belloso
- JM Jensen
- JP Adelman
- JT Judy
- JX Gittelman
- K Honke
- K Sinha
- K Susuki
- K Susuki
- K Susuki
- K Xu
- KA Kleopa
- KA Nave
- KA Nave
- KC Hayes
- KH Ahn
- KH Maier-Hein
- KJ Smith
- KL Davis
- L Athanasiu
- L Horton
- M Labasque
- M Marella
- M Reindl
- M Savvaki
- M Traka
- MA Bhat
- MD Evans
- ME Boyle
- MJ Craner
- MJ Craner
- MK Demos
- MM Reimer
- MN Rasband
- MN Rasband
- MN Rasband
- MN Rasband
- MN Rasband
- MS Grubb
- N Denisenko-Nehrbass
- N Eijkelkamp
- N Schaeren-Wiemers
- O Maier
- OW Howell
- OW Howell
- P Charles
- P Jia
- P Roussos
- R Liguori
- R Nashmi
- R Schniepp
- R Shi
- RD Fields
- RE Foster
- RR Hansebout
- S Comu
- S Einheber
- S Einheber
- S Lee
- S Maljevic
- S Poliak
- S Tait
- Schizophrenia Psychiatric Genome-Wide Association Study C
- SG Waxman
- SI Judge
- SK Tighe
- SL Smart
- SM Zuberi
- SU Peters
- SY Chiu
- T Berger
- T Ishibashi
- T Koch
- T Tagoe
- TG Schulze
- W Sun
- Y Aoki
- Y Bakiri
- Y Fu
- Y Fu
- Y Ogawa
- Y Ogawa
- Y Ogawa
- Y Zhang
- Z Iqbal
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: GW170817 and GRB 170817A
- Author
- Abbott BP
- Abbott R
- Abbott TD
- Acernese F
- Ackley K
- Adams C
- Adams T
- Addesso P
- Adhikari RX
- Adya VB
- Affeldt C
- Afrough M
- Agarwal B
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Allen B
- Allen G
- Allocca A
- Aloy MA
- Altin PA
- Alvarez MD
- Amato A
- Ananyeva A
- Anderson SB
- Anderson WG
- Angelova SV
- Antier S
- Appert S
- Arai K
- Araya MC
- Areeda JS
- Arnaud N
- Arun KG
- Ascenzi S
- Ashton G
- Ast M
- Aston SM
- Astone P
- Atallah DV
- Aufmuth P
- Aulbert C
- AultONeal K
- Austin C
- Avila-Alvarez A
- Babak S
- Bacon P
- Bader MKM
- Bae S
- Baker PT
- Baldaccini F
- Ballardin G
- Ballmer SW
- Banagiri S
- Barayoga JC
- Barclay SE
- Barish BC
- Barker D
- Barkett K
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Bartos I
- Bassiri R
- Basti A
- Batch JC
- Bawaj M
- Bayley JC
- Bazzan M
- Bazzano A
- Becsy B
- Beer C
- Bejger M
- Belahcene I
- Bell AS
- Berger BK
- Bergmann G
- Bero JJ
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Bhagwat S
- Bhandare R
- Bilenko IA
- Billingsley G
- Billman CR
- Birch J
- Birney R
- Birnholtz O
- Biscans S
- Biscoveanu S
- Bisht A
- Bissaldi E
- Bitossi M
- Biwer C
- Bizouard MA
- Blackburn JK
- Blackburn L
- Blackman J
- Blair CD
- Blair DG
- Blair RM
- Bloemen S
- Bock O
- Bode N
- Boer M
- Bogaert G
- Bohe A
- Bondu F
- Bonilla E
- Bonnand R
- Boom BA
- Bork R
- Boschi V
- Bose S
- Bossie K
- Bouffanais Y
- Bozzi A
- Bozzo E
- Bradaschia C
- Brady PR
- Branchesi M
- Brandt S
- Brau JE
- Briant T
- Briggs MS
- Brillet A
- Brinkmann M
- Brisson V
- Brockill P
- Broida JE
- Brooks AF
- Brown DA
- Brown DD
- Brunett S
- Buchanan CC
- Buikema A
- Bulik T
- Bulten HJ
- Buonanno A
- Burns E
- Buskulic D
- Bustillo JC
- Buy C
- Byer RL
- Cabero M
- Cadonati L
- Cagnoli G
- Cahillane C
- Callister TA
- Calloni E
- Camp JB
- Canepa M
- Canizares P
- Cannon KC
- Cao H
- Cao J
- Capano CD
- Capocasa E
- Carbognani F
- Caride S
- Carney MF
- Casentini C
- Castro JMG
- Caudill S
- Cavaglia M
- Cavalier F
- Cavalieri R
- Cella G
- Cepeda CB
- Cerda-Duran P
- Cerretani G
- Cesarini E
- Chamberlin SJ
- Chan M
- Chao S
- Charlton P
- Chase E
- Chassande-Mottin E
- Chatterjee D
- Chatziioannou K
- Cheeseboro BD
- Chen HY
- Chen X
- Chen Y
- Chenevez J
- Cheng H-P
- Chia H
- Chincarini A
- Chiummo A
- Chmiel T
- Cho HS
- Cho M
- Chow JH
- Christensen N
- Chu Q
- Chua AJK
- Chua S
- Chung AKW
- Chung S
- Ciani G
- Ciolfi R
- Cirelli CE
- Cirone A
- Clara F
- Clark JA
- Clearwater P
- Cleva F
- Cleveland WH
- Cocchieri C
- Coccia E
- Cohadon P-F
- Cohen D
- Colla A
- Collaboration LIGOS
- Collaboration V
- Collette CG
- Cominsky LR
- Connaughton V
- Conti L
- Cooper SJ
- Corban P
- Corbitt TR
- Cordero-Carrion I
- Corley KR
- Cornish N
- Corsi A
- Cortese S
- Costa CA
- Costa CFDS
- Coughlin MW
- Coughlin SB
- Coulon J-P
- Countryman ST
- Courvoisier TJ-L
- Couvares P
- Covas PB
- Cowan EE
- Coward DM
- Cowart MJ
- Coyne DC
- Coyne R
- Creighton JDE
- Creighton TD
- Cripe J
- Crowder SG
- Cullen TJ
- Cumming A
- Cunningham L
- Cuoco E
- D'Antonio S
- Dal Canton T
- Dalya G
- Danilishin SL
- Danzmann K
- Dasgupta A
- Dattilo V
- Dave I
- Davier M
- Davis D
- Daw EJ
- Day B
- De laurentis M
- De Pietri R
- De Rosa R
- De Rossi C
- de Varona O
- De S
- Debra D
- Degallaix J
- Del Pozzo W
- Deleglise S
- Demos N
- Denker T
- Dent T
- Dergachev V
- DeRosa RT
- DeSalvo R
- Devenson J
- Dhurandhar S
- Di Fiore L
- Di Giovanni M
- Di Girolamo T
- Di Lieto A
- Di Pace S
- Di Palma I
- Di Renzo F
- Diaz JC
- Diaz MC
- Diehl R
- Doctor Z
- Dolique V
- Domingo A
- Donovan F
- Dooley KL
- Doravari S
- Dorrington I
- Douglas R
- Downes TP
- Drago M
- Dreissigacker C
- Driggers JC
- Du Z
- Ducrot M
- Dupej P
- Dwyer SE
- Edo TB
- Edwards MC
- Effler A
- Eggenstein H-B
- Ehrens P
- Eichholz J
- Eikenberry SS
- Eisenstein RA
- Essick RC
- Estevez D
- Etienne ZB
- Etzel T
- Evans M
- Evans TM
- Factourovich M
- Fafone V
- Fair H
- Fairhurst S
- Fan X
- Farinon S
- Farr B
- Farr WM
- Fauchon-Jones EJ
- Favata M
- Fays M
- Fee C
- Fehrmann H
- Feicht J
- Fejer MM
- Fernandez-Galiana A
- Ferrante I
- Ferreira EC
- Ferrigno C
- Ferrini F
- Fidecaro F
- Finstad D
- Fiori I
- Fiorucci D
- Fishbach M
- Fisher RP
- Fitz-Axen M
- Flaminio R
- Fletcher M
- Fong H
- Font JA
- Forsyth PWF
- Forsyth SS
- Fournier J-D
- Frasca S
- Frasconi F
- Frei Z
- Freise A
- Frey R
- Frey V
- Fries EM
- Fritschel P
- Frolov VV
- Fulda P
- Fyffe M
- Gabbard H
- Gadre BU
- Gaebel SM
- Gair JR
- Gammaitoni L
- Ganija MR
- Gaonkar SG
- Garcia-Quiros C
- Garufi F
- Gateley B
- Gaudio S
- Gaur G
- Gayathri V
- Gehrels N
- Gemme G
- Genin E
- Gennai A
- George D
- George J
- Gergely L
- Germain V
- Ghonge S
- Ghosh A
- Ghosh A
- Ghosh S
- Giaime JA
- Giardina KD
- Giazotto A
- Gibby MH
- Giles MM
- Gill K
- Glover L
- Goetz E
- Goetz R
- Goldstein A
- Gomes S
- Goncharov B
- Gonzalez G
- Gopakumar A
- Gorodetsky ML
- Gossan SE
- Gosselin M
- Gouaty R
- Grado A
- Graef C
- Granata M
- Grant A
- Gras S
- Gray C
- Greco G
- Green AC
- Gretarsson EM
- Groot P
- Grote H
- Grunewald S
- Gruning P
- Guidi GM
- Guo X
- Gupta A
- Gupta MK
- Gushwa KE
- Gustafson EK
- Gustafson R
- Halim O
- Hall BR
- Hall ED
- Hamburg R
- Hamilton EZ
- Hammond G
- Haney M
- Hanke MM
- Hanks J
- Hanlon L
- Hanna C
- Hannam MD
- Hannuksela OA
- Hanson J
- Hardwick T
- Harms J
- Harry GM
- Harry IW
- Hart MJ
- Haster C-J
- Haughian K
- Healy J
- Heidmann A
- Heintze MC
- Heitmann H
- Hello P
- Hemming G
- Hendry M
- Heng IS
- Hennig J
- Heptonstall AW
- Hernandez IM
- Heurs M
- Hild S
- Hinderer T
- Hoak D
- Hofman D
- Holt K
- Holz DE
- Hopkins P
- Horst C
- Hough J
- Houston EA
- Howell EJ
- Hreibi A
- Hu YM
- Huerta EA
- Huet D
- Hughey B
- Hui CM
- Husa S
- Huttner SH
- Huynh-Dinh T
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- Inta R
- INTEGRAL
- Intini G
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- Isac J-M
- Isi M
- Iyer BR
- Izumi K
- Jacqmin T
- Jani K
- Jaranowski P
- Jawahar S
- Jimenez-Forteza F
- Johnson WW
- Johnson-McDaniel NK
- Jones DI
- Jones R
- Jonker RJG
- Jourdain E
- Jr CM
- Ju L
- Junker J
- Kalaghatgi CV
- Kalogera V
- Kamai B
- Kandhasamy S
- Kang G
- Kanner JB
- Kapadia SJ
- Karki S
- Karvinen KS
- Kasprzack M
- Kastaun W
- Katolik M
- Katsavounidis E
- Katzman W
- Kaufer S
- Kawabe K
- Kefelian F
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- Kennedy R
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- Khalili FY
- Khan I
- Khan S
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- Kim C
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- Kippen RM
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- Kissel JS
- Kleybolte L
- Klimenko S
- Knowles TD
- Kocevski D
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- Koley S
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- Kontos A
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- Korth WZ
- Kowalska I
- Kozak DB
- Kraemer C
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- Krishnan B
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- Kuulkers E
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- Wang WH
- Wang YF
- Ward RL
- Warner J
- Was M
- Watchi J
- Weaver B
- Wei L-W
- Weinert M
- Weinstein AJ
- Weiss R
- Wen L
- Wessel EK
- Wessels P
- Westerweck J
- Westphal T
- Wette K
- Whelan JT
- Whitcomb SE
- Whiting BF
- Whittle C
- Wilken D
- Williams D
- Williams RD
- Williamson AR
- Willis JL
- Willke B
- Wilson-Hodge CA
- Wimmer MH
- Winkler W
- Wipf CC
- Wittel H
- Woan G
- Woehler J
- Wofford J
- Wong KWK
- Worden J
- Wright JL
- Wu DS
- Wysocki DM
- Xiao S
- Yamamoto H
- Yancey CC
- Yang L
- Yap MJ
- Yazback M
- Yu H
- Yu H
- Yvert M
- Zadrozny A
- Zanolin M
- Zelenova T
- Zendri J-P
- Zertuche LM
- Zevin M
- Zhang L
- Zhang M
- Zhang T
- Zhang Y-H
- Zhao C
- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17, the gravitational-wave event GW170817 was observed by the Advanced LIGO and Virgo detectors, and the gamma-ray burst (GRB) GRB 170817A was observed independently by the Fermi Gamma-ray Burst Monitor, and the Anti-Coincidence Shield for the Spectrometer for the International Gamma-Ray Astrophysics Laboratory. The probability of the near-simultaneous temporal and spatial observation of GRB 170817A and GW170817 occurring by chance is 5.0×10−8. We therefore confirm binary neutron star mergers as a progenitor of short GRBs. The association of GW170817 and GRB 170817A provides new insight into fundamental physics and the origin of short GRBs. We use the observed time delay of (+1.74±0.05)s between GRB 170817A and GW170817 to: (i) constrain the difference between the speed of gravity and the speed of light to be between −3×10−15 and +7×10−16 times the speed of light, (ii) place new bounds on the violation of Lorentz invariance, (iii) present a new test of the equivalence principle by constraining the Shapiro delay between gravitational and electromagnetic radiation. We also use the time delay to constrain the size and bulk Lorentz factor of the region emitting the gamma-rays. GRB 170817A is the closest short GRB with a known distance, but is between 2 and 6 orders of magnitude less energetic than other bursts with measured redshift. A new generation of gamma-ray detectors, and subthreshold searches in existing detectors, will be essential to detect similar short bursts at greater distances. Finally, we predict a joint detection rate for the Fermi Gamma-ray Burst Monitor and the Advanced LIGO and Virgo detectors of 0.1-1.4 per year during the 2018-2019 observing run and 0.3-1.7 per year at design sensitivity
Multi-messenger observations of a binary neutron star merger
- Author
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- Aartsen MG
- Abbott BP
- Abbott R
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- Abeysekara AU
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- Yoshida S
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- Young DR
- Younk PW
- Yu Hang
- Yu Haocun
- Yu P-C
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- Zhang WC
- Zhang WZ
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Y-H
- Zhang YF
- Zhang YJ
- Zhang Z
- Zhang ZL
- Zhao C
- Zhao HS
- Zhao JL
- Zhao W
- Zhao XF
- Zheng SJ
- Zhou H
- Zhou J
- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- Zhu Y
- Zhu YX
- Zhu Z
- Ziegler A
- Zimmerman AB
- Zimmermann B
- Zimnukhov DS
- Ziolkowski M
- Zoll M
- Zong Z
- Zorn J
- Zornoza JD
- Zou CL
- Zuccarello F
- Zucker ME
- Zuniga J
- Zweizig J
- Zywucka N
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transient’s position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Willke B
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- Woan G
- Woehler J
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- Wu Ds
- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
- Yang L
- Yang Y
- Yang Z
- Yap Mj
- Yazback M
- Yeeles Dw
- Yu H
- Yu Hc
- Yuen Shr
- Zadrozny A
- Zadrozny Ak
- Zanolin M
- Zelenova T
- Zendri Jp
- Zevin M
- Zhang J
- Zhang L
- Zhang T
- Zhao C
- Zhao G
- Zhou M
- Zhou Z
- Zhu Xj
- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- College Park, MD : American Physical Society
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO's second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=3.47×10-25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering. © 2019 American Physical Society
Search for gravitational waves from Scorpius X-1 in the second Advanced LIGO observing run with an improved hidden Markov model
- Author
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- Wu Ds
- Wysocki Dm
- Xiao S
- Xu R
- Yamamoto H
- Yancey Cc
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- Zimmerman Ab
- Zucker Me
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
We present results from a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to track spin wandering. This search improves on previous HMM-based searches of LIGO data by using an improved frequency domain matched filter, the J-statistic, and by analyzing data from Advanced LIGO’s second observing run. In the frequency range searched, from 60 to 650 Hz, we find no evidence of gravitational radiation. At 194.6 Hz, the most sensitive search frequency, we report an upper limit on gravitational wave strain (at 95% confidence) of h95%0=3.47×10−25 when marginalizing over source inclination angle. This is the most sensitive search for Scorpius X-1, to date, that is specifically designed to be robust in the presence of spin wandering
GWTC-2.1: Deep extended catalog of compact binary coalescences observed by LIGO and Virgo during the first half of the third observing run
- Author
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- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 15/01/2024
- Field of study
The second Gravitational-Wave Transient Catalog, GWTC-2, reported on 39 compact binary coalescences observed by the Advanced LIGO and Advanced Virgo detectors between 1 April 2019 15 ∶ 00 UTC and 1 October 2019 15 ∶ 00 UTC. Here, we present GWTC-2.1, which reports on a deeper list of candidate events observed over the same period. We analyze the final version of the strain data over this period with improved calibration and better subtraction of excess noise, which has been publicly released. We employ three matched-filter search pipelines for candidate identification, and estimate the probability of astrophysical origin for each candidate event. While GWTC-2 used a false alarm rate threshold of 2 per year, we include in GWTC-2.1, 1201 candidates that pass a false alarm rate threshold of 2 per day. We calculate the source properties of a subset of 44 high-significance candidates that have a probability of astrophysical origin greater than 0.5. Of these candidates, 36 have been reported in GWTC-2. We also calculate updated source properties for all binary black hole events previously reported in GWTC-1. If the eight additional high-significance candidates presented here are astrophysical, the mass range of events that are unambiguously identified as binary black holes (both objects ≥ 3 M⊙ ) is increased compared to GWTC-2, with total masses from ∼ 14 M ⊙ for GW190924_021846 to ∼ 182 M⊙ for GW190426_190642. Source properties calculated using our default prior suggest that the primary components of two new candidate events (GW190403_051519 and GW190426_190642) fall in the mass gap predicted by pair-instability supernova theory. We also expand the population of binaries with significantly asymmetric mass ratios reported in GWTC-2 by an additional two events (the mass ratio is less than 0.65 and 0.44 at 90% probability for GW190403_051519 and GW190917_114630 respectively), and find that two of the eight new events have effective inspiral spins χeff > 0 (at 90% credibility), while no binary is consistent with χeff < 0 at the same significance. We provide updated estimates for rates of binary black hole and binary neutron star coalescence in the local Universe
All-sky search for continuous gravitational waves from isolated neutron stars in the early O3 LIGO data
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- Yamamoto Kazuhiro
- Yamamoto Kohei
- Yamamoto T
- Yamashita K
- Yamazaki R
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- Yang Yang
- Yang Yi
- Yang Z
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- Yeeles DW
- Yelikar AB
- Ying M
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- Zhu XJ
- Zhu Z-H
- Zucker ME
- Zweizig J
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 15/10/2021
- Field of study
We report on an all-sky search for continuous gravitational waves in the frequency band 20-2000 Hz and with a frequency time derivative in the range of [-1.0,+0.1]×10-8 Hz/s. Such a signal could be produced by a nearby, spinning and slightly nonaxisymmetric isolated neutron star in our Galaxy. This search uses the LIGO data from the first six months of Advanced LIGO's and Advanced Virgo's third observational run, O3. No periodic gravitational wave signals are observed, and 95% confidence-level (C.L.) frequentist upper limits are placed on their strengths. The lowest upper limits on worst-case (linearly polarized) strain amplitude h0 are ∼1.7×10-25 near 200 Hz. For a circularly polarized source (most favorable orientation), the lowest upper limits are ∼6.3×10-26. These strict frequentist upper limits refer to all sky locations and the entire range of frequency derivative values. For a population-averaged ensemble of sky locations and stellar orientations, the lowest 95% C.L. upper limits on the strain amplitude are ∼1.4×10-25. These upper limits improve upon our previously published all-sky results, with the greatest improvement (factor of ∼2) seen at higher frequencies, in part because quantum squeezing has dramatically improved the detector noise level relative to the second observational run, O2. These limits are the most constraining to date over most of the parameter space searched
All-sky, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
- Author
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- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 03/06/2022
- Field of study
We present the first results from an all-sky all-frequency (ASAF) search for
an anisotropic stochastic gravitational-wave background using the data from the
first three observing runs of the Advanced LIGO and Advanced Virgo detectors.
Upper limit maps on broadband anisotropies of a persistent stochastic
background were published for all observing runs of the LIGO-Virgo detectors.
However, a broadband analysis is likely to miss narrowband signals as the
signal-to-noise ratio of a narrowband signal can be significantly reduced when
combined with detector output from other frequencies. Data folding and the
computationally efficient analysis pipeline, {\tt PyStoch}, enable us to
perform the radiometer map-making at every frequency bin. We perform the search
at 3072 {\tt{HEALPix}} equal area pixels uniformly tiling the sky and in every
frequency bin of width 1/32~Hz in the range 20−1726~Hz, except for bins
that are likely to contain instrumental artefacts and hence are notched. We do
not find any statistically significant evidence for the existence of narrowband
gravitational-wave signals in the analyzed frequency bins. Therefore, we place
95% confidence upper limits on the gravitational-wave strain for each
pixel-frequency pair, the limits are in the range (0.030−9.6)×10−24. In addition, we outline a method to identify candidate
pixel-frequency pairs that could be followed up by a more sensitive (and
potentially computationally expensive) search, e.g., a matched-filtering-based
analysis, to look for fainter nearly monochromatic coherent signals. The ASAF
analysis is inherently independent of models describing any spectral or spatial
distribution of power. We demonstrate that the ASAF results can be
appropriately combined over frequencies and sky directions to successfully
recover the broadband directional and isotropic results
Lawson criterion for ignition exceeded in an inertial fusion experiment
- Author
- Abu-Shawareb H
- Acree R
- Adams J
- Adams P
- Addis B
- Aden R
- Adrian P
- Afeyan BB
- Aggleton M
- Aghaian L
- Aguirre A
- Aikens D
- Akre J
- Albert F
- Albrecht M
- Albright BJ
- Albritton J
- Alcala J
- Alday C
- Alessi DA
- Alexander N
- Alfonso J
- Alfonso N
- Alger E
- Ali SJ
- Ali ZA
- Alley WE
- Amala P
- Amendt PA
- Amick P
- Ammula S
- Amorin C
- Ampleford DJ
- Anderson RW
- Anklam T
- Antipa N
- Appelbe B
- Aracne-Ruddle C
- Araya E
- Arend M
- Arnold P
- Arnold T
- Asay J
- Atherton LJ
- Atkinson D
- Atkinson R
- Auerbach JM
- Austin B
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- Awwal AS
- Ayers J
- Ayers S
- Ayers T
- Azevedo S
- Bachmann B
- Back CA
- Bae J
- Bailey DS
- Bailey J
- Baisden T
- Baker KL
- Baldis H
- Barber D
- Barberis M
- Barker D
- Barnes A
- Barnes CW
- Barrios MA
- Barty C
- Bass I
- Batha SH
- Baxamusa SH
- Bazan G
- Beagle JK
- Beale R
- Beck BR
- Beck JB
- Bedzyk M
- Beeler RG
- Beeler RG
- Behrendt W
- Belk L
- Bell P
- Belyaev M
- Benage JF
- Benedetti LR
- Benedict LX
- Bennett G
- Berger R
- Bernat T
- Bernstein LA
- Berry B
- Bertolini L
- Berzak Hopkins L
- Besenbruch G
- Betcher J
- Bettenhausen R
- Betti R
- Bezzerides B
- Bhandarkar SD
- Bickel R
- Biener J
- Biesiada T
- Bigelow K
- Bigelow-Granillo J
- Bigman V
- Bionta RM
- Birge NW
- Bitter M
- Black AC
- Bleile R
- Bleuel DL
- Bliss E
- Bliss E
- Blue B
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- Boehm K
- Boley CD
- Bonanno R
- Bond EJ
- Bond T
- Bonino MJ
- Borden M
- Bourgade J-L
- Bousquet J
- Bowers J
- Bowers M
- Boyd R
- Bozek A
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- Bradley KS
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- Brantley PS
- Braun D
- Braun T
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- Briggs TM
- Britten J
- Brooks ED
- Browning D
- Bruhn MW
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- Bruns H
- Brunton G
- Bryant B
- Buczek T
- Bude J
- Buitano L
- Burkhart S
- Burmark J
- Burnham A
- Burr R
- Busby LE
- Butlin B
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- Cagadas B
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- Cahayag R
- Caldwell SE
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- Casavant D
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- Castor JI
- Castro C
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- Cavitt R
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- Cerjan C
- Chandler G
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- Choate C
- Chou J
- Chrien RE
- Chrisp M
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- Christensen M
- Christopherson AR
- Chung M
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- Clark A
- Clark DS
- Clark K
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- Claus L
- Cline B
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- Cobble JA
- Cochrane K
- Cohen B
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- Collins G
- Collins LA
- Collins TJB
- Conder A
- Conrad B
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- Cook AW
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- Cooper G
- Cope T
- Copeland SR
- Coppari F
- Cortez J
- Cox J
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- Crane J
- Craxton RS
- Cray M
- Crilly A
- Crippen JW
- Cross D
- Cuneo M
- Cuotts G
- Czajka CE
- Czechowicz D
- Daly T
- Danforth P
- Darbee R
- Darlington B
- Datte P
- Dauffy L
- Davalos G
- Davidovits S
- Davis J
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- Dawson S
- Day RD
- Day TH
- Dayton M
- Deck C
- Decker C
- Deeney C
- DeFriend KA
- Deis G
- Delamater ND
- Delettrez JA
- Demaret R
- Demos S
- Dempsey SM
- Desjardin R
- Desjardins T
- Desjarlais MP
- Dewald EL
- DeYoreo J
- Di Nicola J-MG
- Di Nicola P
- Diaz S
- Dimonte G
- Dittrich TR
- Divol L
- Dixit SN
- Dixon J
- Dodd ES
- Dolan D
- Donovan A
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- Dorrer C
- Dorsano N
- Douglas MR
- Dow D
- Downie J
- Downing E
- Dozieres M
- Draggoo V
- Drake D
- Drake RP
- Drake T
- Dreifuerst G
- DuBois DF
- DuBois PF
- Dunham G
- Dylla-Spears R
- Dymoke-Bradshaw AKL
- Dzenitis B
- Döppner T
- Ebbers C
- Eckart M
- Eddinger S
- Eder D
- Edgell D
- Edwards MJ
- Efthimion P
- Eggert JH
- Ehrlich B
- Ehrmann P
- Elhadj S
- Ellerbee C
- Elliott NS
- Ellison CL
- Elsner F
- Emerich M
- Engelhorn K
- England T
- English E
- Epperson P
- Epstein R
- Erbert G
- Erickson MA
- Erlandson A
- Erskine DJ
- Espinosa RJ
- Estabrook KG
- Estes C
- Evans S
- Fabyan A
- Fair J
- Fallejo R
- Farmer N
- Farmer WA
- Farrell M
- Fatherley VE
- Fedorov M
- Feigenbaum E
- Feit M
- Ferguson W
- Fernandez JC
- Fernandez-Panella A
- Fess S
- Field JE
- Filip CV
- Fincke JR
- Finn T
- Finnegan SM
- Finucane RG
- Fischer M
- Fisher A
- Fisher J
- Fishler B
- Fittinghoff D
- Fitzsimmons P
- Flegel M
- Flippo KA
- Florio J
- Folta J
- Folta P
- Fooks J
- Foord M
- Foreman LR
- Forrest C
- Forsman A
- Fortner R
- Fournier K
- Fratanduono DE
- Frazier N
- Frazier T
- Frederick C
- Freeman MS
- Frenje J
- Frey D
- Frieders G
- Friedrich S
- Froula DH
- Fry J
- Fuller T
- Gaffney J
- Gales S
- Gambhir A
- Gao L
- Garbett WJ
- Garcia A
- Gates C
- Gatu Johnson M
- Gaut E
- Gauthier P
- Gavin Z
- Gaylord J
- Geissel M
- Georgeson J
- Geppert-Kleinrath H
- Geppert-Kleinrath V
- Gharibyan N
- Gibson C
- Gibson J
- Giraldez E
- Glebov V
- Glendinning SG
- Glenn S
- Glenzer SH
- Goade S
- Gobby PL
- Goldman SR
- Golick B
- Gomez M
- Goncharov V
- Goodin D
- Grabowski P
- Grafil E
- Graham P
- Grandy J
- Grasz E
- Graziani F
- Green T
- Greenman G
- Greenough JA
- Greenwood A
- Gregori G
- Griego JR
- Grim GP
- Grondalski J
- Gross S
- Guckian J
- Guler N
- Gunney B
- Guss G
- Génin F
- Haan S
- Hackbarth J
- Hackel L
- Hackel R
- Haefner C
- Hagmann C
- Hahn KD
- Hahn S
- Haid BJ
- Haines BM
- Hall BM
- Hall C
- Hall GN
- Hamamoto M
- Hamel S
- Hamilton CE
- Hammel BA
- Hammer JH
- Hampton G
- Hamza A
- Handler A
- Hansen S
- Hanson D
- Haque R
- Harding D
- Harding E
- Hares JD
- Harris DB
- Harte JA
- Hartouni EP
- Hatarik R
- Hatchett S
- Hauer AA
- Havre M
- Hawley R
- Hayes J
- Hayes J
- Hayes S
- Hayes-Sterbenz A
- Haynam CA
- Haynes DA
- Headley D
- Heal A
- Heebner JE
- Heerey S
- Heestand GM
- Heeter R
- Hein N
- Heinbockel C
- Hendricks C
- Henesian M
- Heninger J
- Henrikson J
- Henry EA
- Herbold EB
- Hermann MR
- Hermes G
- Hernandez JE
- Hernandez VJ
- Herrera OD
- Herrmann HW
- Herrmann MC
- Hewett D
- Hibbard R
- Hicks DG
- Hill D
- Hill K
- Hilsabeck T
- Hinkel DE
- Ho DD
- Ho VK
- Hoffer JK
- Hoffman NM
- Hohenberger M
- Hohensee M
- Hoke W
- Holdener D
- Holdener F
- Holder JP
- Holko B
- Holunga D
- Holzrichter JF
- Honig J
- Hoover D
- Hopkins D
- Hoppe M
- Hoppe ML
- Horner J
- Hornung R
- Horsfield CJ
- Horvath J
- Hotaling D
- House R
- Howell L
- Hsing WW
- Hu SX
- Huang H
- Huckins J
- Hui H
- Humbird KD
- Hund J
- Hunt J
- Hurricane OA
- Hutton M
- Huynh KH-K
- Iglesias C
- Igumenshchev IV
- Inandan L
- Indirect Drive ICF Collaboration
- Izumi N
- Jackson J
- Jackson M
- Jacobs SD
- James G
- Jancaitis K
- Jaquez J
- Jarboe J
- Jarrott LC
- Jasion D
- Jeet J
- Jenei AE
- Jensen J
- Jimenez J
- Jimenez R
- Jobe D
- Johal Z
- Johns HM
- Johnson D
- Johnson MA
- Johnson RJ
- Johnson S
- Johnson SA
- Johnson T
- Jones K
- Jones M
- Jones O
- Jorge R
- Jorgenson HJ
- Julian M
- Jun BI
- Jungquist R
- Kaae J
- Kabadi N
- Kaczala D
- Kalantar D
- Kangas K
- Karasiev VV
- Karasik M
- Karpenko V
- Kasarky A
- Kasper K
- Kauffman R
- Kaufman MI
- Keane C
- Keaty L
- Kegelmeyer L
- Keiter PA
- Kellett PA
- Kellogg J
- Kelly JH
- Kemic S
- Kemp AJ
- Kemp GE
- Kerbel GD
- Kerr SM
- Kershaw D
- Kessler TJ
- Key MH
- Khan SF
- Khater H
- Kiikka C
- Kilkenny J
- Kim Y
- Kim Y-J
- Kimko J
- Kimmel M
- Kindel JM
- King J
- Kirkwood RK
- Klaus L
- Klem D
- Kline JL
- Klingmann J
- Kluth G
- Knapp P
- Knauer J
- Knipping J
- Knudson M
- Kobs D
- Koch J
- Kohut T
- Kong C
- Koning JM
- Koning P
- Konior S
- Kornblum H
- Kot LB
- Kozioziemski B
- Kozlowski M
- Kozlowski PM
- Krammen J
- Krasheninnikova NS
- Kraus B
- Krauser W
- Kress JD
- Krieger E
- Kritcher AL
- Kroll JJ
- Kruer WL
- Kruse MKG
- Kucheyev S
- Kumbera M
- Kumpan S
- Kunimune J
- Kustowski B
- Kwan TJT
- Kyrala GA
- Laffite S
- Lafon M
- LaFortune K
- Lagin L
- Lahmann B
- Lairson B
- Land T
- Landen OL
- Lane M
- Laney D
- Langdon AB
- Langenbrunner J
- Langer SH
- Langro A
- Lanier NE
- Lanier TE
- Larson D
- Lasinski BF
- Lassle D
- LaTray D
- Lau G
- Lau N
- Laumann C
- Laurence A
- Laurence TA
- Lawson J
- Le Galloudec B
- Le Galloudec KK
- Le Pape S
- Le HP
- Leach RR
- Leal L
- Leatherland A
- LeChien K
- Lechleiter B
- Lee A
- Lee M
- Lee T
- Leeper RJ
- Lefebvre E
- Leidinger J-P
- LeMire B
- Lemke RW
- Lemos NC
- Lerche R
- Lerner S
- Letts S
- Levedahl K
- Lewis T
- Li CK
- Li H
- Li J
- Liao W
- Liao ZM
- Liebman J
- Liedahl D
- Lindford G
- Lindl JD
- Lindman EL
- Loey H
- London RA
- Long F
- Loomis EN
- Lopez FE
- Lopez H
- Losbanos E
- Loucks S
- Lowe-Webb R
- Ludwigsen AP
- Lundgren E
- Luo R
- Lusk J
- Lyons R
- Ma T
- Macallop Y
- MacDonald MJ
- MacGowan BJ
- Mack JM
- Mackinnon AJ
- MacLaren SA
- MacPhee AG
- Magelssen GR
- Magoon J
- Malone RM
- Malsbury T
- Managan R
- Mancini R
- Manes K
- Maney D
- Manha D
- Mannion OM
- Manuel AM
- Mapoles E
- Mara G
- Marcotte T
- Marin E
- Marinak MM
- Mariscal C
- Mariscal DA
- Mariscal EF
- Marley EV
- Marozas JA
- Marquez R
- Marshall CD
- Marshall FJ
- Marshall M
- Marshall S
- Marticorena J
- Martinez D
- Maslennikov I
- Mason D
- Mason RJ
- Masse L
- Massey W
- Masson-Laborde P-E
- Masters ND
- Mathisen D
- Mathison E
- Matone J
- Matthews MJ
- Mattoon C
- Mattsson TR
- Matzen K
- Mauche CW
- Mauldin M
- McAbee T
- McBurney M
- Mccarville T
- McCrory RL
- McEvoy AM
- McGuffey C
- Mcinnis M
- McKenty P
- McKinley MS
- McLeod JB
- McPherson A
- Mcquillan B
- Meamber M
- Meaney KD
- Meezan NB
- Mehlhorn TA
- Mehta NC
- Meissner R
- Menapace J
- Merrill FE
- Merritt BT
- Merritt EC
- Meyerhofer DD
- Mezyk S
- Mich RJ
- Michel PA
- Milam D
- Miller C
- Miller D
- Miller DS
- Miller E
- Miller EK
- Miller J
- Miller M
- Miller PE
- Miller T
- Miller W
- Miller-Kamm V
- Millot M
- Milovich JL
- Minner P
- Miquel J-L
- Mitchell S
- Molvig K
- Montesanti RC
- Montgomery DS
- Monticelli M
- Montoya A
- Moody JD
- Moore AS
- Moore E
- Moran M
- Moreno JC
- Moreno K
- Morgan BE
- Morrow T
- Morton JW
- Moses E
- Moy K
- Muir R
- Munro DH
- Munteanu FM
- Murillo MS
- Murphy TJ
- Murray JE
- Murray JR
- Nafziger J
- Nagayama T
- Nagel SR
- Nast R
- Negres RA
- Nelson A
- Nelson D
- Nelson J
- Nelson S
- Nemethy S
- Neumayer P
- Newman K
- Newton M
- Nguyen H
- Niemann C
- Nikroo A
- Nilson PM
- Nobile A
- Noorai V
- Nora R
- Norton M
- Nostrand M
- Note V
- Novell S
- Nowak PF
- Nunez A
- Nyholm RA
- O'Brien M
- Oceguera A
- Oertel JA
- Okui J
- Olejniczak B
- Oliveira J
- Olsen P
- Olson B
- Olson K
- Olson RE
- Opachich YP
- Orsi N
- Orth CD
- Owen M
- Padalino S
- Padilla E
- Paguio R
- Paguio S
- Paisner J
- Pajoom S
- Pak A
- Palaniyappan S
- Palma K
- Pannell T
- Papp F
- Paras D
- Parham T
- Park H-S
- Pasternak A
- Patankar S
- Patel MV
- Patel PK
- Patterson R
- Patterson S
- Paul B
- Paul M
- Pauli E
- Pearce OT
- Pearcy J
- Pedrotti B
- Peer A
- Pelz LJ
- Penetrante B
- Penner J
- Perez A
- Perkins LJ
- Pernice E
- Perry TS
- Person S
- Petersen D
- Petersen T
- Peterson DL
- Peterson EB
- Peterson JE
- Peterson JL
- Peterson K
- Peterson RR
- Petrasso RD
- Philippe F
- Phipps TJ
- Piceno E
- Pickworth L
- Ping Y
- Pino J
- Plummer R
- Pollack GD
- Pollaine SM
- Pollock BB
- Ponce D
- Ponce J
- Pontelandolfo J
- Porter JL
- Post J
- Poujade O
- Powell C
- Powell H
- Power G
- Pozulp M
- Prantil M
- Prasad M
- Pratuch S
- Price S
- Primdahl K
- Prisbrey S
- Procassini R
- Pruyne A
- Pudliner B
- Qiu SR
- Quan K
- Quinn M
- Quintenz J
- Radha PB
- Rainer F
- Ralph JE
- Raman KS
- Raman R
- Rambo P
- Rana S
- Randewich A
- Rardin D
- Ratledge M
- Ravelo N
- Ravizza F
- Rayce M
- Raymond A
- Raymond B
- Reed B
- Reed C
- Regan S
- Reichelt B
- Reis V
- Reisdorf S
- Rekow V
- Remington BA
- Rendon A
- Requieron W
- Rever M
- Reynolds H
- Reynolds J
- Rhodes J
- Rhodes M
- Rice B
- Rice NG
- Richardson MC
- Rieben R
- Rigatti A
- Riggs S
- Rinderknecht HG
- Ring K
- Riordan B
- Riquier R
- Rivers C
- Roberts D
- Roberts V
- Robertson G
- Robey HF
- Robles J
- Rocha P
- Rochau G
- Rodriguez J
- Rodriguez S
- Rosen M
- Rosenberg M
- Ross G
- Ross JS
- Ross P
- Rouse J
- Rovang D
- Rubenchik AM
- Rubery MS
- Ruiz CL
- Rushford M
- Russ B
- Rygg JR
- Ryujin BS
- Sacks RA
- Sacks RF
- Saito K
- Salmon T
- Salmonson JD
- Samuelson S
- Sanchez J
- Sanchez M
- Sangster C
- Saroyan A
- Sater J
- Satsangi A
- Sauers S
- Saunders R
- Sauppe JP
- Sawicki R
- Sayre D
- Scanlan M
- Schaffers K
- Schappert GT
- Schiaffino S
- Schlossberg DJ
- Schmidt DW
- Schmitt MJ
- Schneider DHG
- Schneider MB
- Schneider R
- Schoff M
- Schollmeier M
- Schrauth SE
- Schroeder CR
- Schölmerich M
- Scott HA
- Scott I
- Scott JM
- Scott RHH
- Scullard CR
- Sedillo T
- Seguin FH
- Seka W
- Senecal J
- Sepke SM
- Seppala L
- Sequoia K
- Severyn J
- Sevier JM
- Sewell N
- Seznec S
- Shah RC
- Shamlian J
- Shaughnessy D
- Shaw M
- Shaw R
- Shearer C
- Shelton R
- Shen N
- Sherlock MW
- Shestakov AI
- Shi EL
- Shin SJ
- Shingleton N
- Shmayda W
- Shor M
- Shoup M
- Shuldberg C
- Siegel L
- Silva FJ
- Simakov AN
- Sims BT
- Sinars D
- Singh P
- Sio H
- Skulina K
- Skupsky S
- Slutz S
- Sluyter M
- Smalyuk VA
- Smauley D
- Smeltser RM
- Smith C
- Smith I
- Smith J
- Smith L
- Smith R
- Sohn R
- Sommer S
- Sorce C
- Sorem M
- Soures JM
- Spaeth ML
- Spears BK
- Spears J
- Speas S
- Speck D
- Speck R
- Spinka T
- Springer PT
- Stadermann M
- Stahl B
- Stahoviak J
- Stanton LG
- Steele R
- Steele W
- Steinman D
- Stemke R
- Stephens R
- Sterbenz S
- Sterne P
- Stevens D
- Stevers J
- Still CB
- Stoeckl C
- Stoeffl W
- Stolken JS
- Stolz C
- Stone G
- Storm E
- Stoupin S
- Stout E
- Stowers I
- Strauser R
- Streckart H
- Streit J
- Strozzi DJ
- Suratwala T
- Sutcliffe G
- Suter LJ
- Sutton SB
- Svidzinski V
- Swadling G
- Sweet W
- Szoke A
- Tabak M
- Takagi M
- Tambazidis A
- Tang V
- Taranowski M
- Taylor LA
- Telford S
- Theobald W
- Thi M
- Thomas A
- Thomas CA
- Thomas I
- Thomas R
- Thompson IJ
- Thongstisubskul A
- Thorsness CB
- Tietbohl G
- Tipton RE
- Tobin M
- Tomlin N
- Tommasini R
- Toreja AJ
- Torres J
- Town RPJ
- Townsend S
- Trenholme J
- Trivelpiece A
- Trosseille C
- Truax H
- Trummer D
- Trummer S
- Truong T
- Tubbs D
- Tubman ER
- Tunnell T
- Turnbull D
- Turner RE
- Ulitsky M
- Upadhye R
- Vaher JL
- Van Wonterghem BM
- VanArsdall P
- VanBlarcom D
- Vandenboomgaerde M
- VanQuinlan R
- Varnum WS
- Velikovich AL
- Vella A
- Verdon CP
- Vermillion B
- Vernon S
- Vesey R
- Vickers J
- Vignes RM
- Visosky M
- Vocke J
- Volegov PL
- Von Rotz R
- Vonhof S
- Vu HX
- Vu M
- Wall D
- Wall J
- Wallace R
- Wallin B
- Walmer D
- Walsh CA
- Walters CF
- Waltz C
- Wan A
- Wang A
- Wang Y
- Wark JS
- Warner BE
- Watson J
- Watt RG
- Watts P
- Weaver J
- Weaver RP
- Weaver S
- Weber CR
- Weber P
- Weber SV
- Wegner P
- Weiss K
- Welday B
- Welser-Sherrill L
- Wheeler GF
- Whistler W
- White RK
- Whitley HD
- Whitman P
- Wickett ME
- Widmann K
- Widmayer C
- Wiedwald J
- Wilcox R
- Wilcox S
- Wild C
- Wilde BH
- Wilde CH
- Wilhelmsen K
- Wilke MD
- Wilkens H
- Wilkins P
- Wilks SC
- Williams EA
- Williams GJ
- Williams W
- Williams WH
- Wilson B
- Wilson DC
- Wilson E
- Wilson R
- Winters S
- Wisoff J
- Wittman M
- Wolfe J
- Wong A
- Wong KW
- Wong L
- Wong N
- Wood R
- Woodhouse D
- Woodruff J
- Woods DT
- Woods S
- Woodworth BN
- Wooten E
- Wootton A
- Work K
- Workman JB
- Wright J
- Wu M
- Wuest C
- Wysocki FJ
- Xu H
- Yamaguchi M
- Yang B
- Yang ST
- Yatabe J
- Yeamans CB
- Yee BC
- Yi SA
- Yin L
- Young B
- Young CS
- Young CV
- Young P
- Youngblood K
- Zacharias R
- Zagaris G
- Zaitseva N
- Zaka F
- Ze F
- Zeiger B
- Zika M
- Zimmerman GB
- Zobrist T
- Zuegel JD
- Zylstra AB
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 06/07/2022
- Field of study
For more than half a century, researchers around the world have been engaged in attempts to achieve fusion ignition as a proof of principle of various fusion concepts. Following the Lawson criterion, an ignited plasma is one where the fusion heating power is high enough to overcome all the physical processes that cool the fusion plasma, creating a positive thermodynamic feedback loop with rapidly increasing temperature. In inertially confined fusion, ignition is a state where the fusion plasma can begin "burn propagation" into surrounding cold fuel, enabling the possibility of high energy gain. While "scientific breakeven" (i.e., unity target gain) has not yet been achieved (here target gain is 0.72, 1.37 MJ of fusion for 1.92 MJ of laser energy), this Letter reports the first controlled fusion experiment, using laser indirect drive, on the National Ignition Facility to produce capsule gain (here 5.8) and reach ignition by nine different formulations of the Lawson criterion
The node of Ranvier in CNS pathology.
- Author
- A Battefeld
- A Desmazieres
- A Duflocq
- A Hayashi
- A Lorincz
- A Nans
- A Nazeri
- AA Jarjour
- AD Goodman
- AE Baum
- AH Seidl
- AM Pillai
- AR Blight
- B Popko
- B Zonta
- BD Trapp
- BG Xiao
- C Bi
- C Chen
- C Cifuentes-Diaz
- C Elliott
- C Gu
- C Hildebrand
- C Hildebrand
- C Kopp-Scheinpflug
- C Moll
- C O’Dushlaine
- CF Babbs
- D Grozeva
- David Attwell
- DL Browne
- DL Sherman
- E Ozkaynak
- E Peles
- E Peles
- E Stogmann
- E Wallstrom
- ED Buttermore
- EG Sozmen
- EK Mathey
- ET Landaas
- F Ullen
- G Wolswijk
- G Xie
- GP Garcia-Fresco
- GR Anderson
- H Kuba
- H Ouyang
- H Vacher
- H Wang
- HC Mefford
- HM Brew
- I Coman
- I Horresh
- I Vabnick
- I. Lorena Arancibia-Carcamo
- J Barry
- J Devaux
- J Devaux
- J Elia
- J Ritter
- J Rosenbluth
- J Rosenbluth
- J Sun
- J Wang
- JB Sun
- JC Rios
- JC Rios
- JD Hinman
- JD Kocsis
- JD Kocsis
- JI Friedman
- JJ Devaux
- JJ Harris
- JJ Lawrence
- JL Dupree
- JL Salzer
- JM Belloso
- JM Jensen
- JP Adelman
- JT Judy
- JX Gittelman
- K Honke
- K Sinha
- K Susuki
- K Susuki
- K Susuki
- K Xu
- KA Kleopa
- KA Nave
- KA Nave
- KC Hayes
- KH Ahn
- KH Maier-Hein
- KJ Smith
- KL Davis
- L Athanasiu
- L Horton
- M Labasque
- M Marella
- M Reindl
- M Savvaki
- M Traka
- MA Bhat
- MD Evans
- ME Boyle
- MJ Craner
- MJ Craner
- MK Demos
- MM Reimer
- MN Rasband
- MN Rasband
- MN Rasband
- MN Rasband
- MN Rasband
- MS Grubb
- N Denisenko-Nehrbass
- N Eijkelkamp
- N Schaeren-Wiemers
- O Maier
- OW Howell
- OW Howell
- P Charles
- P Jia
- P Roussos
- R Liguori
- R Nashmi
- R Schniepp
- R Shi
- RD Fields
- RE Foster
- RR Hansebout
- S Comu
- S Einheber
- S Einheber
- S Lee
- S Maljevic
- S Poliak
- S Tait
- Schizophrenia Psychiatric Genome-Wide Association Study C
- SG Waxman
- SI Judge
- SK Tighe
- SL Smart
- SM Zuberi
- SU Peters
- SY Chiu
- T Berger
- T Ishibashi
- T Koch
- T Tagoe
- TG Schulze
- W Sun
- Y Aoki
- Y Bakiri
- Y Fu
- Y Fu
- Y Ogawa
- Y Ogawa
- Y Ogawa
- Y Zhang
- Z Iqbal
- Publication venue
- Publication date
- 01/01/2014
- Field of study
Healthy nodes of Ranvier are crucial for action potential propagation along myelinated axons, both in the central and in the peripheral nervous system. Surprisingly, the node of Ranvier has often been neglected when describing CNS disorders, with most pathologies classified simply as being due to neuronal defects in the grey matter or due to oligodendrocyte damage in the white matter. However, recent studies have highlighted changes that occur in pathological conditions at the node of Ranvier, and at the associated paranodal and juxtaparanodal regions where neurons and myelinating glial cells interact. Lengthening of the node of Ranvier, failure of the electrically resistive seal between the myelin and the axon at the paranode, and retraction of myelin to expose voltage-gated K(+) channels in the juxtaparanode, may contribute to altering the function of myelinated axons in a wide range of diseases, including stroke, spinal cord injury and multiple sclerosis. Here, we review the principles by which the node of Ranvier operates and its molecular structure, and thus explain how defects at the node and paranode contribute to neurological disorders
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