151 research outputs found
The genetics and neuropathology of frontotemporal lobar degeneration
- Author
- A Goode
- A Hassan
- A Lipton
- A Nalbandian
- A Shatunov
- AA Luty
- AL Boxer
- AM Isaacs
- Anne Sieben
- AS Chen-Plotkin
- B Borroni
- B Borroni
- B Borroni
- C Cruchaga
- C Lomen-Hoerth
- C Troakes
- C Vance
- CC Weihl
- CC Weihl
- Christine Van Broeckhoven
- CL Ryan
- D Galimberti
- D Neary
- D Neary
- DG Munoz
- DG Munoz
- Diehl J JohnsonJK
- DM Ruddy
- DR Williams
- E Buratti
- E Buratti
- E Maria Di
- ED Roberson
- F Fecto
- F Yin
- G Skibinski
- GD Rabinovici
- GD Rabinovici
- GD Watts
- GG Kovacs
- GM Ringholz
- GS Pesiridis
- H Houlden
- H Laaksovirta
- H Seelaar
- H Seelaar
- H Stewart
- HR Morris
- I Ber Le
- I Ber Le
- I Ber Le
- I D’Souza
- I D’Souza
- I Ferrer
- I Gijselinck
- I Gijselinck
- I Gijselinck
- I Gijselinck
- I Mackenzie
- I Mackenzie
- IE Holm
- IE Holm
- IR Mackenzie
- IR Mackenzie
- IR Mackenzie
- IR Mackenzie
- IR Mackenzie
- J Brettschneider
- J Gass
- J Phukan
- J Simón-Sánchez
- J Simón-Sánchez
- J Sreedharan
- J Zee van der
- J Zee van der
- J Zee van der
- J Zee van der
- JD Rohrer
- JD Rohrer
- Jean-Jacques Martin
- JR Burrell
- JR Hodges
- JS Goldman
- JS Goldman
- JS Ju
- JS Ju
- JS Snowden
- JS Snowden
- K Josephs
- K Rascovsky
- K Sleegers
- K Sleegers
- K Sleegers
- L Benajiba
- LE Cox
- LK Kwong
- M Baker
- M Baker
- M Carecchio
- M Carecchio
- M Cruts
- M Cruts
- M Cruts
- M Cruts
- M DeJesus-Hernandez
- M Hutton
- M Letter De
- M Morita
- M Neumann
- M Neumann
- M Neumann
- M Neumann
- MA Es van
- Marc Cruts
- ME Murray
- MG Spillantini
- MG Spillantini
- MJ Kovach
- ML Gorno-Tempini
- MS Forman
- N Brouwers
- N Brouwers
- N Finch
- N Ticozzi
- NJ Cairns
- NJ Cairns
- NL Foster
- O Mukherjee
- P Damme Van
- P Poorkaj
- Patrick Cras
- Patrick Santens
- Paul Boon
- PC Sapp
- Peter-Paul De Deyn
- PN Valdmanis
- R Ghidoni
- R Pamphlett
- R Rademakers
- R Rademakers
- R Rademakers
- R Rademakers
- R Schröder
- R Vass
- RM Dai
- RR Davies
- S Al-Sarraj
- S Gydesen
- S Kumar-Singh
- S Love
- S Nunnemann
- S Roeber
- S Rollinson
- S Rollinson
- Sebastiaan Engelborghs
- SM Laws
- SM Rosso
- SS Shankaran
- T Arai
- T Langenhove Van
- T Lashley
- Tim Van Langenhove
- TJ Kwiatkowski Jr
- TL Edwards
- VE Kimonis
- VM Deerlin Van
- YJ Fu
- Z Ahmed
- Z Ahmed
- Z He
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Frontotemporal lobar degeneration (FTLD) is a heterogeneous group of disorders characterized by disturbances of behavior and personality and different types of language impairment with or without concomitant features of motor neuron disease or parkinsonism. FTLD is characterized by atrophy of the frontal and anterior temporal brain lobes. Detailed neuropathological studies have elicited proteinopathies defined by inclusions of hyperphosphorylated microtubule-associated protein tau, TAR DNA-binding protein TDP-43, fused-in-sarcoma or yet unidentified proteins in affected brain regions. Rather than the type of proteinopathy, the site of neurodegeneration correlates relatively well with the clinical presentation of FTLD. Molecular genetic studies identified five disease genes, of which the gene encoding the tau protein (MAPT), the growth factor precursor gene granulin (GRN), and C9orf72 with unknown function are most frequently mutated. Rare mutations were also identified in the genes encoding valosin-containing protein (VCP) and charged multivesicular body protein 2B (CHMP2B). These genes are good markers to distinguish underlying neuropathological phenotypes. Due to the complex landscape of FTLD diseases, combined characterization of clinical, imaging, biological and genetic biomarkers is essential to establish a detailed diagnosis. Although major progress has been made in FTLD research in recent years, further studies are needed to completely map out and correlate the clinical, pathological and genetic entities, and to understand the underlying disease mechanisms. In this review, we summarize the current state of the rapidly progressing field of genetic, neuropathological and clinical research of this intriguing condition
GWTC-2.1: Deep extended catalog of compact binary coalescences observed by LIGO and Virgo during the first half of the third observing run
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- Adhikari RX
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- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
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- Allocca A
- Altin PA
- Amato A
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- Chatterjee C
- Chatterjee Debarati
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- Chen HY
- Chen J
- Chen X
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- Cheng H
- Cheong CK
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- Chiadini F
- Chiarini G
- Chierici R
- Chincarini A
- Chiofalo ML
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- Cho G
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- Cullen TJ
- Cumming A
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- Danila B
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- 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, all-frequency directional search for persistent gravitational waves from Advanced LIGO’s and Advanced Virgo’s first three observing runs
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- Yamamoto Kazuhiro
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- Yang Z
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- Yeeles DW
- Yelikar AB
- Ying M
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- Yokozawa T
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- Yu Hang
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- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeidler S
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- Zevin M
- Zhan M
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- Zhu XJ
- Zhu Z-H
- 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
First measurement of the |t|-dependence of coherent J/ψ photonuclear production
- Author
- Acharya S
- Acosta FT
- Adam J
- Adamova D
- Adler A
- Adolfsson J
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahn SU
- Aiola S
- Akindinov A
- Al-Turany M
- Alam SN
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- Ali Y
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
- Andrews HA
- Andronic A
- Angeletti M
- Anguelov V
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi MD
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie O Villalobos
- Bala R
- Balbastre G Conesa
- Baldisseri A
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- Baral RC
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- Barnby LS
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- Zinovjev G
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2021
- Field of study
The first measurement of the cross section for coherent J/ψ photoproduction as a function of |t|, the square of the momentum transferred between the incoming and outgoing target nucleus, is presented. The data were measured with the ALICE detector in ultra-peripheral Pb–Pb collisions at a centre-of-mass energy per nucleon pair sNN=5.02TeV with the J/ψ produced in the central rapidity region |y|<0.8, which corresponds to the small Bjorken-x range (0.3−1.4)×10−3.
The measured |t|-dependence is not described by computations based only on the Pb nuclear form factor, while the photonuclear cross section is better reproduced by models including shadowing according to the leading-twist approximation, or gluon-saturation effects from the impact-parameter dependent Balitsky–Kovchegov equation. These new results are therefore a valid tool to constrain the relevant model parameters and to investigate the transverse gluonic structure at very low Bjorken-x.publishedVersio
All-sky search for continuous gravitational waves from isolated neutron stars in the early O3 LIGO data
- Author
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- Yamamoto Kazuhiro
- Yamamoto Kohei
- Yamamoto T
- Yamashita K
- Yamazaki R
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- Yang Yang
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- Yeeles DW
- Yelikar AB
- Ying M
- Yokogawa K
- Yokoyama J
- Yokozawa T
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- Yu Hang
- Yu Haocun
- Yuzurihara H
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- Zevin M
- Zhan M
- Zhang H
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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
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aime' C
- Akchurin N
- Akgun B
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
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- Ahmad WH
- Ahuja S
- Akbiyik M
- Akchurin N
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- Albajar C
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- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Allen B
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- Alonso AG
- Alvarez JDR
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- Amsler C
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- Anderson D
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ¯
Resolving the strange behavior of extraterrestrial potassium in the upper atmosphere
- Author
- ACHARYA S
- ACOSTA FT
- ADAMOVA D
- ADOLFSSON J
- AGGARWAL MM
- AGNELLO M
- AGRAWAL N
- AHAMMED Z
- AHN SU
- AIOLA S
- AKINDINOV A
- AL-TURANY M
- ALAM SN
- ALBA JL
- ALBUQUERQUE DSD
- ALEKSANDROV D
- ALESSANDRO B
- ALI Y
- ALICI A
- ALKIN A
- ALME J
- ALT T
- ALTENKAMPER L
- ALTSYBEEV I
- ANAAM MN
- ANDREI C
- ANDREOU D
- ANDREWS HA
- ANDRONIC A
- ANGELETTI M
- ANGUELOV V
- ANSON C
- ANTICIC T
- ANTINORI F
- ANTONIOLI P
- ANWAR R
- APADULA N
- APHECETCHE L
- APPELSHAEUSER H
- ARCELLI S
- ARNALDI R
- ARNOLD OW
- ARSENE IC
- ARSLANDOK M
- AUDURIER B
- AUGUSTINUS A
- AVERBECK R
- AZMI MD
- BADALA A
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- BARNAFOLDI GG
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- BARTH K
- BARTSCH E
- BASTID N
- BASU S
- BATIGNE G
- BATYUNYA B
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- BEARDEN IG
- BECK H
- BEDDA C
- BEHERA NK
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- NAIK B
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- NAYAK K
- NAYAK R
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- SHARMA A
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- TANAKA N
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- TARIQ M
- TARZILA MG
- TAURO A
- TELESCA A
- TELLEZ A
- TELLO A
- TERREVOLI C
- TEYSSIER B
- THAKUR D
- THAKUR S
- THOMAS D
- THORESEN F
- TIEULENT R
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- ULLALAND K
- UMAKA EN
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- UYSAL AK
- VALA M
- VALLE ZC
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- VARGAS A
- VARGYAS M
- VARMA R
- VASILEIOU M
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- VAUTHIER A
- VECHERNIN V
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- VOLPE G
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- VOSCEK D
- VRANIC D
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- VYVRE P
- WAGNER B
- WANG H
- WANG M
- WATANABE Y
- WEBER M
- WEBER SG
- WEGRZYNEK A
- WEISER DF
- WENZEL SC
- WESSELS JP
- WESTERHOFF U
- WHITEHEAD AM
- WIECHULA J
- WIKNE J
- WILK G
- WILKINSON J
- WILLEMS GA
- WILLIAMS MCS
- WILLSHER E
- WINDELBAND B
- WITT WE
- XU R
- YALCIN S
- YAMAKAWA K
- YANO S
- YIN Z
- YOKOYAMA H
- YOO IK
- YOON JH
- YURCHENKO V
- ZACCOLO V
- ZAMAN A
- ZAMPOLLI C
- ZANOLI HJC
- ZARDOSHTI N
- ZAROCHENTSEV A
- ZAVADA P
- ZAVIYALOV N
- ZBROSZCZYK H
- ZHALOV M
- ZHANG X
- ZHANG Y
- ZHANG Z
- ZHAO C
- ZHEREBCHEVSKII V
- ZHIGAREVA N
- ZHOU D
- ZHOU Y
- ZHOU Z
- ZHU H
- ZHU J
- ZHU Y
- ZICHICHI A
- ZIMMERMANN MB
- ZINOVJEV G
- ZMESKAL J
- ZOU S
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2014
- Field of study
It has been known since the 1960s that the layers of Na and K atoms, which occur between 80 and 105 km in the Earth's atmosphere as a result of meteoric ablation, exhibit completely different seasonal behavior. In the extratropics Na varies annually, with a pronounced wintertime maximum and summertime minimum. However, K varies semiannually with a small summertime maximum and minima at the equinoxes. This contrasting behavior has never been satisfactorily explained. Here we use a combination of electronic structure and chemical kinetic rate theory to determine two key differences in the chemistries of K and Na. First, the neutralization of K+ ions is only favored at low temperatures during summer. Second, cycling between K and its major neutral reservoir KHCO3 is essentially temperature independent. A whole atmosphere model incorporating this new chemistry, together with a meteor input function, now correctly predicts the seasonal behavior of the K layer
Search for gravitational waves associated with gamma-ray bursts detected by Fermi and Swift during the LIGO–Virgo run O3b
- Author
- Abbott R
- Abbott TD
- Acernese F
- Ackley K
- Adams C
- Adhikari N
- Adhikari RX
- Adya VB
- Affeldt C
- Agarwal D
- Agathos M
- Agatsuma K
- Aggarwal N
- Aguiar OD
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Albanesi S
- Allocca A
- Altin PA
- Amato A
- Anand C
- Anand S
- Ananyeva A
- Anderson SB
- Anderson WG
- Ando M
- Andrade T
- Andres N
- Andric T
- Angelova SV
- Ansoldi S
- Antelis JM
- Antier S
- Appert S
- Arai K
- Arai K
- Arai Y
- Araki S
- Araya A
- Araya MC
- Areeda JS
- Arellano FEP
- Arene M
- Aritomi N
- Arnaud N
- Aronson SM
- Arun KG
- Asada H
- Asali Y
- Ashton G
- Aso Y
- Assiduo M
- Aston SM
- Astone P
- Aubin F
- Austin C
- Babak S
- Badaracco F
- Bader MKM
- Badger C
- Bae S
- Bae Y
- Baer AM
- Bagnasco S
- Bai Y
- Baiotti L
- Baird J
- Bajpai R
- Ball M
- Ballardin G
- Ballmer SW
- Balsamo A
- Baltus G
- Banagiri S
- Bankar D
- Barayoga JC
- Barbieri C
- Barish BC
- Barker D
- Barneo P
- Barone F
- Barr B
- Barsotti L
- Barsuglia M
- Barta D
- Bartlett J
- Barton MA
- Bartos I
- Bassiri R
- Basti A
- Bawaj M
- Bayley JC
- Baylor AC
- Bazzan M
- Becsy B
- Bedakihale VM
- Bejger M
- Belahcene I
- Benedetto V
- Beniwal D
- Bennett TF
- Bentley JD
- BenYaala M
- Bergamin F
- Berger BK
- Bernuzzi S
- Berry CPL
- Bersanetti D
- Bertolini A
- Betzwieser J
- Beveridge D
- Bhandare R
- Bhardwaj U
- Bhattacharjee D
- Bhaumik S
- Bilenko IA
- Billingsley G
- Bini S
- Birney R
- Birnholtz O
- Biscans S
- Bischi M
- Biscoveanu S
- Bisht A
- Biswas B
- Bitossi M
- Bizouard M-A
- Blackburn JK
- Blair CD
- Blair DG
- Blair RM
- Bobba F
- Bode N
- Boer M
- Bogaert G
- Boldrini M
- Bonavena LD
- Bondu F
- Bonilla E
- Bonnand R
- Booker P
- Boom BA
- Bork R
- Boschi V
- Bose N
- Bose S
- Bossilkov V
- Boudart V
- Bouffanais Y
- Bozzi A
- Bradaschia C
- Brady PR
- Bramley A
- Branch A
- Branchesi M
- Brau JE
- Breschi M
- Briant T
- Briggs JH
- Brillet A
- Brinkmann M
- Brockill P
- Brooks AF
- Brooks J
- Brown DD
- Brunett S
- Bruno G
- Bruntz R
- Bryant J
- Bulik T
- Bulten HJ
- Buonanno A
- Buscicchio R
- Buskulic D
- Bustillo JC
- Buy C
- Byer RL
- Cadonati L
- Cagnoli G
- Cahillane C
- Callaghan JD
- Callister TA
- Calloni E
- Cameron J
- Camp JB
- Canepa M
- Canevarolo S
- Cannavacciuolo M
- Cannon KC
- Canton TD
- Cao H
- Cao Z
- Capocasa E
- Capote E
- Carapella G
- Carbognani F
- Carlin JB
- Carney MF
- Carpinelli M
- Carrillo G
- Carullo G
- Carver TL
- Casentini C
- Castaldi G
- Caudill S
- Cavaglia M
- Cavalier F
- Cavalieri R
- Ceasar M
- Cella G
- Cerda-Duran P
- Cesarini E
- Chaibi W
- Chakravarti K
- Champion E
- Chan C
- Chan C-H
- Chan CL
- Chan K
- Chan M
- Chandra K
- Chanial P
- Chao S
- Charlton P
- Chase EA
- Chassande-Mottin E
- Chatterjee C
- Chatterjee D
- Chatterjee D
- Chaturvedi M
- Chaty S
- Chatziioannou K
- Chen C
- Chen HY
- Chen J
- Chen K
- Chen X
- Chen Y-B
- Chen Y-R
- Chen Z
- Cheng H
- Cheong CK
- Cheung HY
- Chia HY
- Chiadini F
- Chiang C-Y
- Chiarini G
- Chierici R
- Chincarini A
- Chiofalo ML
- Chiummo A
- Cho G
- Cho HS
- Choudhary RK
- Choudhary S
- Christensen N
- Chu H
- Chu Q
- Chu Y-K
- Chua S
- Chung KW
- Ciani G
- Ciecielag P
- Cieslar M
- Cifaldi M
- Ciobanu AA
- Ciolfi R
- Cipriano F
- Cirone A
- Clara F
- Clark EN
- Clark JA
- Clarke L
- Clearwater P
- Clesse S
- Cleva F
- Coccia E
- Codazzo E
- Cohadon P-F
- Cohen DE
- Cohen L
- Collaboration KAGRA
- Collaboration LIGOS
- Collaboration LIGOS
- Collaboration V
- Collaboration V
- Colleoni M
- Collette CG
- Colombo A
- Colpi M
- Compton CM
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- Cooper SJ
- Corban P
- Corbitt TR
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- Creighton TD
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- Croquette M
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- Fauchon-Jones EJ
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- Hayakawa H
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- Inayoshi K
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- Kamiizumi M
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- Ohkawa M
- Ohme F
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- Pedraza M
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- Pereira T
- Perez CJ
- Perigois C
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- Pinto M
- Piotrzkowski K
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- Planas L
- Plastino W
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- Pong DYT
- Ponrathnam S
- Popolizio P
- Porter EK
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- Pracchia M
- Pradier T
- Prajapati AK
- Prasai K
- Prasanna R
- Pratten G
- Principe M
- Prodi GA
- Prokhorov L
- Prosposito P
- Prudenzi L
- Puecher A
- Puerer M
- Punturo M
- Puosi F
- Puppo P
- Qi H
- Quetschke V
- Quitzow-James R
- Quynh LN
- Raab FJ
- Raaijmakers G
- Radkins H
- Radulesco N
- Raffai P
- Rail SX
- Raja S
- Rajan C
- Ramirez KE
- Ramirez TD
- Ramos-Buades A
- Rana J
- Rapagnani P
- Rapol UD
- Ray A
- Raymond V
- Raza N
- Razzano M
- Read J
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- Regimbau T
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- Reid S
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- Reitze DH
- Relton P
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- Rezac M
- Ricci F
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- Richardson L
- Riemenschneider G
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- Robertson NA
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- Robinet F
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- Romano R
- Romel CL
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- Romero-Shaw IM
- Romie JH
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- Roy S
- Roy S
- Rozza D
- Ruggi P
- Ryan K
- Sachdev S
- Sadecki T
- Sadiq J
- Sago N
- Saito S
- Saito Y
- Sakai K
- Sakai Y
- Sakellariadou M
- Sakuno Y
- Salafia OS
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- Saleem M
- Salemi F
- Samajdar A
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- Sanchis-Gual N
- Sanders JR
- Sanuy A
- Saravanan TR
- Sarin N
- Sassolas B
- Satari H
- Sathyaprakash BS
- Sato S
- Sato T
- Sauter O
- Savage RL
- Sawada T
- Sawant D
- Sawant HL
- Sayah S
- Schaetzl D
- Scheel M
- Scheuer J
- Schiworski M
- Schmidt P
- Schmidt S
- Schnabel R
- Schneewind M
- Schoenbeck A
- Schofield RMS
- Schulte BW
- Schutz BF
- Schwartz E
- Scott J
- Scott SM
- Seglar-Arroyo M
- Sekiguchi T
- Sekiguchi Y
- Sellers D
- Sengupta AS
- Sentenac D
- Seo EG
- Sequino V
- Sergeev A
- Setyawati Y
- Shaffer T
- Shahriar MS
- Shams B
- Shao L
- Sharma A
- Sharma P
- Sharma-Chaudhary S
- Shawhan P
- Shcheblanov NS
- Shibagaki S
- Shikauchi M
- Shimizu R
- Shimoda T
- Shimode K
- Shinkai H
- Shishido T
- Shoda A
- Shoemaker DH
- Shoemaker DM
- ShyamSundar S
- Sieniawska M
- Sigg D
- Singer LP
- Singh D
- Singh N
- Singha A
- Sintes AM
- Sipala V
- Skliris V
- Slagmolen BJJ
- Slaven-Blair TJ
- Smetana J
- Smith JR
- Smith RJE
- Soldateschi J
- Somala SN
- Somiya K
- Son EJ
- Soni K
- Soni S
- Sordini V
- Sorrentino F
- Sorrentino N
- Sotani H
- Soulard R
- Souradeep T
- Sowell E
- Spagnuolo V
- Spencer AP
- Spera M
- Srinivasan R
- Srivastava AK
- Srivastava V
- Staats K
- Stachie C
- Steer DA
- Steinlechner J
- Steinlechner S
- Stops DJ
- Stover M
- Strain KA
- Strang LC
- Stratta G
- Strunk A
- Sturani R
- Stuver AL
- Subrahmanya SC
- Sudhagar S
- Sudhir V
- Sugimoto R
- Suh HG
- Summerscales TZ
- Sun H
- Sun L
- Sunil S
- Sur A
- Suresh J
- Sutton PJ
- Suzuki T
- Suzuki T
- Swinkels BL
- Szczepanczyk MJ
- Szewczyk P
- Tacca M
- Tagoshi H
- Tait SC
- Takahashi H
- Takahashi R
- Takamori A
- Takano S
- Takeda H
- Takeda M
- Talbot C
- Talbot CJ
- Tanaka H
- Tanaka K
- Tanaka K
- Tanaka T
- Tanaka T
- Tanasijczuk AJ
- Tanioka S
- Tanner DB
- Tao D
- Tao L
- Taranto C
- Tasson JD
- Telada S
- Tenorio R
- Terhune JE
- Terkowski L
- Thirugnanasambandam MP
- Thomas M
- Thomas P
- Thompson EE
- Thompson JE
- Thondapu SR
- Thorne KA
- Thrane E
- Tiwari S
- Tiwari S
- Tiwari V
- Toivonen AM
- Toland K
- Tolley AE
- Tomaru T
- Tomigami Y
- Tomura T
- Tonelli M
- Torres-Forne A
- Torrie CI
- Toyra D
- Trapananti A
- Travasso F
- Traylor G
- Trevor M
- Tringali MC
- Tripathee A
- Troiano L
- Trovato A
- Trozzo L
- Trudeau RJ
- Tsai D
- Tsai DS
- Tsang KW
- Tsang T
- Tsao J-S
- Tse M
- Tso R
- Tsubono K
- Tsuchida S
- Tsukada L
- Tsuna D
- Tsutsui T
- Tsuzuki T
- Turbang K
- Turconi M
- Tuyenbayev D
- Ubhi AS
- Uchikata N
- Uchiyama T
- Udall RP
- Ueda A
- Uehara T
- Ueno K
- Ueshima G
- Unnikrishnan CS
- Uraguchi F
- Urban AL
- Ushiba T
- Utina A
- Vahlbruch H
- Vajente G
- Vajpeyi A
- Valdes G
- Valentini M
- Valsan V
- van Bakel N
- van Beuzekom M
- van den Brand JFJ
- Van Den Broeck C
- van der Schaaf L
- van Heijningen JV
- van Putten MHPM
- van Remortel N
- Vander-Hyde DC
- Vanosky J
- Vardaro M
- Vargas AF
- Varma V
- Vasuth M
- Vecchio A
- Vedovato G
- Veitch J
- Veitch PJ
- Venneberg J
- Venugopalan G
- Verkindt D
- Verma P
- Verma Y
- Veske D
- Vetrano F
- Vicere A
- Vidyant S
- Viets AD
- Vijaykumar A
- Villa-Ortega V
- Vinet J-Y
- Virtuoso A
- Vitale S
- Vivanco FH
- Vo T
- Vocca H
- von Reis ERG
- von Wrangel JSA
- Vorvick C
- Vyatchanin SP
- Wade LE
- Wade M
- Wagner KJ
- Walet RC
- Walker M
- Wallace GS
- Wallace L
- Walsh S
- Wang J
- Wang JZ
- Wang WH
- Ward RL
- Warner J
- Was M
- Washimi T
- Washington NY
- Watchi J
- Weaver B
- Webster SA
- Weinert M
- Weinstein AJ
- Weiss R
- Weller CM
- Wellmann F
- Wen L
- Wessels P
- Wette K
- Whelan JT
- White DD
- Whiting BF
- Whittle C
- Wilken D
- Williams D
- Williams MJ
- Williamson AR
- Willis JL
- Willke B
- Wilson DJ
- Winkler W
- Wipf CC
- Wlodarczyk T
- Woan G
- Woehler J
- Wofford JK
- Wong ICF
- Wu C
- Wu DS
- Wu H
- Wu S
- Wysocki DM
- Xiao L
- Xu W-R
- Yamada T
- Yamamoto H
- Yamamoto K
- Yamamoto K
- Yamamoto T
- Yamashita K
- Yamazaki R
- Yang FW
- Yang L
- Yang Y
- Yang Y
- Yang Z
- Yap MJ
- Yeeles DW
- Yelikar AB
- Ying M
- Yokogawa K
- Yokoyama J
- Yokozawa T
- Yoo J
- Yoshioka T
- Yu H
- Yu H
- Yuzurihara H
- Zadrozny A
- Zanolin M
- Zeidler S
- Zelenova T
- Zendri J-P
- Zevin M
- Zhan M
- Zhang H
- Zhang J
- Zhang L
- Zhang T
- Zhang Y
- Zhao C
- Zhao G
- Zhao Y
- Zhao Y
- Zheng Y
- Zhou R
- Zhou Z
- Zhu XJ
- Zhu Z-H
- Zimmerman AB
- Zucker ME
- Zweizig J
- Publication venue
- 'American Astronomical Society'
- 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
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