329 research outputs found
Gender influences end-of-life decisions
- Publication venue
- BioMed Central
- Publication date
- Field of study
The Architectural Design Rules of Solar Systems based on the New Perspective
- Author
- A Johnson
- AN Halliday
- Bijay Kumar Sharma
- BK Sharma
- C Broeg
- C Hellier
- CL Cook
- D Apes
- DD Sasselov
- DD Sasselov
- DP Rubicam
- F Marzari
- G Israelian
- GA Krasinsky
- GA Krasinsky
- GE Williams
- GH Darwin
- GH Darwin
- H Tanaka
- JE Chambers
- JJ Dukla
- JJ Lissauer
- JP Zahn
- KJ Epstein
- M Reidemeister
- ME Zolansky
- N Murray
- NC Santos
- P Goldreich
- RP Nelson
- S Ida
- S Leschiutta
- SN Cuzzi
- T Jong de
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 03/11/2009
- Field of study
On the basis of the Lunar Laser Ranging Data released by NASA on the Silver
Jubilee Celebration of Man Landing on Moon on 21st July 1969-1994, theoretical
formulation of Earth-Moon tidal interaction was carried out and Planetary
Satellite Dynamics was established. It was found that this mathematical
analysis could as well be applied to Star and Planets system and since every
star could potentially contain an extra-solar system, hence we have a large
ensemble of exoplanets to test our new perspective on the birth and evolution
of solar systems. Till date 403 exoplanets have been discovered in 390
extra-solar systems. I have taken 12 single planet systems, 4 Brown Dwarf -
Star systems and 2 Brown Dwarf pairs. Following architectural design rules are
corroborated through this study of exoplanets. All planets are born at inner
Clarke Orbit what we refer to as inner geo-synchronous orbit in case of
Earth-Moon System. By any perturbative force such as cosmic particles or
radiation pressure, the planet gets tipped long of aG1 or short of aG1. Here
aG1 is inner Clarke Orbit. The exoplanet can either be launched on death spiral
as CLOSE HOT JUPITERS or can be launched on an expanding spiral path as the
planets in our Solar System are. It was also found that if the exo-planet are
significant fraction of the host star then those exo-planets rapidly migrate
from aG1 to aG2 and have very short Time Constant of Evolution as Brown Dwarfs
have. This vindicates our basic premise that planets are always born at inner
Clarke Orbit. This study vindicates the design rules which had been postulated
at 35th COSPAR Scientific Assembly in 2004 at Paris, France, under the title
,New Perspective on the Birth & Evolution of Solar Systems.Comment: This paper has been reported to Earth,Moon and Planets Journal as
MOON-S-09-0007
A pre-Caloris synchronous rotation for Mercury
- Author
- ACM Correia
- ACM Correia
- Alexandre C. M. Correia
- C Fassett
- C Fassett
- CC Counselman III
- DT Blewett
- E Kokubo
- E Pierazzo
- G Colombo
- G Colombo
- GH Pettengill
- HJ Melosh
- J Laskar
- Jacques Laskar
- JJ Lissauer
- JJ Lissauer
- JK Harmon
- JL Margot
- L Dones
- M Le Feuvre
- M Le Feuvre
- MA Wieczorek
- MA Wieczorek
- Mark A. Wieczorek
- Mathieu Le Feuvre
- MD Campbell-Brown
- ME Davies
- Nicolas Rambaux
- P Goldreich
- PD Spudis
- RR Herrick
- SC Solomon
- SJ Peale
- W Bottke
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 11/12/2011
- Field of study
The planet Mercury is locked in a spin-orbit resonance where it rotates three
times about its spin axis for every two orbits about the Sun. The current
explanation for this unique state assumes that the initial rotation of this
planet was prograde and rapid, and that tidal torques decelerated the planetary
spin to this resonance. When core-mantle boundary friction is accounted for,
capture into the 3/2 resonance occurs with a 26% probability, but the most
probable outcome is capture into one of the higher-order resonances. Here we
show that if the initial rotation of Mercury were retrograde, this planet would
be captured into synchronous rotation with a 68% probability. Strong spatial
variations of the impact cratering rate would have existed at this time, and
these are shown to be consistent with the distribution of pre-Calorian impact
basins observed by Mariner 10 and MESSENGER. Escape from this highly stable
resonance is made possible by the momentum imparted by large basin-forming
impact events, and capture into the 3/2 resonance occurs subsequently under
favourable conditions.Comment: Nature Geosci., 201
Planet formation in Binaries
- Author
- A Eggenberger
- A Johansen
- A Nelson
- A Pierens
- A Zsom
- AL Kraus
- AP Boss
- AP Boss
- AP Hatzes
- C Hayashi
- CA Giuppone
- D Malmberg
- D Raghavan
- E Kokubo
- EV Quintana
- EV Quintana
- F Marzari
- F Marzari
- F Marzari
- F Marzari
- F Masset
- F Selsis
- G DuchĂȘne
- G Picogna
- G Rabl
- GJ Savonije
- H Jang-Condell
- J Blum
- J-W Xie
- J-W Xie
- J-W Xie
- J-W Xie
- JA Orosz
- JA Orosz
- JB Pollack
- JF Kasting
- JJ Lissauer
- JM Guedes
- JN Cuzzi
- L Doyle
- L Kaltenegger
- L Mayer
- LF RodrĂguez
- M Barbieri
- M Fragner
- ME Schwamb
- MJ Holman
- MJ Payne
- N Georgakarakos
- N Haghighipour
- N Haghighipour
- N Haghighipour
- O Hubickyj
- P Thebault
- P Thebault
- P Thebault
- P Thebault
- P Thebault
- R Dvorak
- R Dvorak
- R Dvorak
- R Dvorak
- R NeuhÀuser
- R Pierrehumbert
- R Rafikov
- RJ Harris
- RK Kopparapu
- RK Kopparapu
- S Desidera
- S Eggl
- S-B Qian
- S-J Paardekooper
- S-J Paardekooper
- T Roell
- TA Heppenheimer
- VB Kostov
- VB Kostov
- VB Kostov
- W Kley
- WF Welsh
- X Dumusque
- Y Abe
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 25/04/2016
- Field of study
Spurred by the discovery of numerous exoplanets in multiple systems, binaries
have become in recent years one of the main topics in planet formation
research. Numerous studies have investigated to what extent the presence of a
stellar companion can affect the planet formation process. Such studies have
implications that can reach beyond the sole context of binaries, as they allow
to test certain aspects of the planet formation scenario by submitting them to
extreme environments. We review here the current understanding on this complex
problem. We show in particular how each of the different stages of the
planet-formation process is affected differently by binary perturbations. We
focus especially on the intermediate stage of kilometre-sized planetesimal
accretion, which has proven to be the most sensitive to binarity and for which
the presence of some exoplanets observed in tight binaries is difficult to
explain by in-situ formation following the "standard" planet-formation
scenario. Some tentative solutions to this apparent paradox are presented. The
last part of our review presents a thorough description of the problem of
planet habitability, for which the binary environment creates a complex
situation because of the presence of two irradation sources of varying
distance.Comment: Review chapter to appear in "Planetary Exploration and Science:
Recent Advances and Applications", eds. S. Jin, N. Haghighipour, W.-H. Ip,
Springer (v2, numerous typos corrected
Planet Populations as a Function of Stellar Properties
- Author
- A Cumming
- A Izidoro
- A Mortier
- A Mortier
- A Silburt
- A Wolfgang
- A. Mortier
- AC Boley
- AN Youdin
- AP Boss
- AP Boss
- AW Howard
- AW Mann
- B Courcol
- B Rojas-Ayala
- Benjamin T. Montet
- BMS Hansen
- BMS Hansen
- C Beaugé
- C Cossou
- C Dressing
- C Dressing
- C Laws
- C Mordasini
- C Mordasini
- C Obermeier
- C Terquem
- Christian Clanton
- CJ Burke
- Courtney D. Dressing
- D Charbonneau
- D Foreman-Mackey
- D Huber
- D Huber
- DA Fischer
- Daniel C. Fabrycky
- DNC Lin
- Dun Wang
- E Chiang
- E Gaidos
- E Gaidos
- E Gaidos
- E Jehin
- E Jofré
- E Kokubo
- E Kokubo
- E Kokubo
- EA Petigura
- EA Petigura
- EJ Lee
- EW Thommes
- F Fressin
- F Meru
- FJ Ciesla
- G Gonzalez
- G Gonzalez
- G Gonzalez
- G Kennedy
- G Laughlin
- G Laughlin
- GAL Coleman
- GD Mulders
- GD Mulders
- GD Mulders
- GD Mulders
- GW Marcy
- GW Wetherill
- H Rein
- HE Schlichting
- I Pascucci
- IJM Crossfield
- IN Reid
- J Maldonado
- J Wang
- JA Johnson
- JA Johnson
- JA Johnson
- JB Pollack
- JE Chambers
- JJ Lissauer
- JL Christiansen
- JN Winn
- Jonathan J. Swift
- JP Williams
- K Fuhrmann
- K Kornet
- K Sadakane
- K.-M. Dittkrist
- KC Schlaufman
- KC Schlaufman
- KC Schlaufman
- Konstantin Batygin
- L Ghezzi
- L Pasquini
- LA Buchhave
- LA Buchhave
- LA Buchhave
- M Endl
- M Endl
- M Gillon
- M Ikoma
- M Mayor
- M Mayor
- M. Ansdell
- ME Everett
- MI Jones
- N. C. Santos
- NC Santos
- NC Santos
- NC Santos
- NC Santos
- P Goldreich
- P Pinilla
- PW Sullivan
- RC Terrien
- RI Dawson
- RL Gilliland
- Robert A. Wittenmyer
- RP Butler
- S Dong
- S Hekker
- S Ida
- S Ida
- S Ida
- S Mathur
- S Mohanty
- S Udry
- S Udry
- S. G. Sousa
- Sabine Reffert
- Scott A. Barenfeld
- Sean M. Andrews
- SG Sousa
- SN Raymond
- SN Raymond
- TD Morton
- TM Brown
- V. Zh. Adibekyan
- Vardan Adibekyan
- W Zhu
- WR Ward
- X Bonfils
- Y Hasegawa
- Y Hasegawa
- Y Takeda
- Y. Alibert
- Y. Alibert
- ZK Berta
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 30/04/2018
- Field of study
Exoplanets around different types of stars provide a window into the diverse
environments in which planets form. This chapter describes the observed
relations between exoplanet populations and stellar properties and how they
connect to planet formation in protoplanetary disks. Giant planets occur more
frequently around more metal-rich and more massive stars. These findings
support the core accretion theory of planet formation, in which the cores of
giant planets form more rapidly in more metal-rich and more massive
protoplanetary disks. Smaller planets, those with sizes roughly between Earth
and Neptune, exhibit different scaling relations with stellar properties. These
planets are found around stars with a wide range of metallicities and occur
more frequently around lower mass stars. This indicates that planet formation
takes place in a wide range of environments, yet it is not clear why planets
form more efficiently around low mass stars. Going forward, exoplanet surveys
targeting M dwarfs will characterize the exoplanet population around the lowest
mass stars. In combination with ongoing stellar characterization, this will
help us understand the formation of planets in a large range of environments.Comment: Accepted for Publication in the Handbook of Exoplanet
TESS Reveals a Short-period Sub-Neptune Sibling (HD 86226c) to a Known Long-period Giant Planet
- Author
- Anderson DR
- Barclay T
- Bouchy F
- Burt JA
- Butler RP
- Caldwell DA
- Collins KA
- Collins KI
- Crane JD
- Diaz MR
- Dorn C
- Eastman JD
- Feng F
- Flowers E
- Haldemann J
- Helled R
- Hellier C
- Jenkins JM
- Jenkins JS
- Jensen ELN
- Kane SR
- Latham DW
- Law N
- Lissauer JJ
- Luque R
- Mann AW
- Marmier M
- Mocnik T
- Nielsen LD
- Otegi JF
- Palle E
- Ricker GR
- Rose ME
- Seager S
- Segransan D
- Seidel JV
- Shectman SA
- Shporer A
- Teske J
- Torres G
- Udry S
- Vanderspek R
- Wang SX
- Winn JN
- Wolfgang A
- Wong I
- Ziegler C
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2020
- Field of study
The Transiting Exoplanet Survey Satellite mission was designed to find transiting planets around bright, nearby stars. Here, we present the detection and mass measurement of a small, short-period (â4 days) transiting planet around the bright (V = 7.9), solar-type star HD 86226 (TOI-652, TIC 22221375), previously known to host a long-period (~1600 days) giant planet. HD 86226c (TOI-652.01) has a radius of 2.16 ± 0.08 Râ and a mass of 7.25â1.12+1.19â Mâ, based on archival and new radial velocity data. We also update the parameters of the longer-period, not-known-to-transit planet, and find it to be less eccentric and less massive than previously reported. The density of the transiting planet is 3.97 g cmâ3, which is low enough to suggest that the planet has at least a small volatile envelope, but the mass fractions of rock, iron, and water are not well-constrained. Given the host star brightness, planet period, and location of the planet near both the "radius gap" and the "hot Neptune desert," HD 86226c is an interesting candidate for transmission spectroscopy to further refine its composition
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck GA
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
- Branchini P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brown H
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- BScher V
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Caballero J
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghi M
- Cameron D
- Camilocci ES
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepaa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciba K
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Cranshaw J
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuc C-M
- Curatolo M
- Curtis CJ
- Curull XE
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- Da Costa JBG
- Da Costa JGPF
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Daly CH
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Dawson JW
- Daya-Ishmukhametova RK
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- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at sâ=8 TeV with the ATLAS detector
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- Zurzolo G
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fbâ1 of protonâproton collision data at âs = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via tËâtÏË01 or tËâ bÏ˱1 âbW(â)ÏË01 , where ÏË01 (Ï˱1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of tË â tÏË01 . For a branching fraction of 100%, top squark masses in the range 270â645 GeV are excluded for ÏË01 masses below 30 GeV. For a branching fraction of 50% to either tË â tÏË01 or tË â bÏ˱1 , and assuming the Ï˱1 mass to be twice the ÏË01 mass, top squark masses in the range 250â550 GeV are excluded for ÏË01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at âs=8TeV
- Author
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- Youssef S
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- Zaidan R
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- Zanello L
- Zanzi D
- Zeitnitz C
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- Zerwas D
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- Zhemchugov A
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fbâ1of data collected in protonâproton collisions at âs=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Born Too Soon: Accelerating actions for prevention and care of 15 million newborns born too soon
- Author
- A Conde-Agudelo
- A Prost
- AG Philip
- B Ekman
- BT Oshiro
- C Boschi-Pinto
- C Campbell
- CG Victora
- Christopher P Howson
- CP Howson
- DT Jamison
- E Baris
- Elizabeth Mary Mason
- Eve Lackritz
- F Althabe
- G Demirel
- G Msemo
- GF Smith
- H Blencowe
- H Blencowe
- HH Chang
- IK Friberg
- Ingrid K Friberg
- Institute of Medicine
- J Requejo
- JE Lawn
- JE Lawn
- JE Lawn
- JE Lawn
- JH Requejo
- Jim Larson
- José M Belizan
- Joy E Lawn
- JP Baker
- JS Gooding
- K Ban
- KJ Kerber
- L Liu
- Lori McDougall
- M Kinney
- March of Dimes PMNCH, Save the Children, WHO
- Mary V Kinney
- ME Wegman
- MG Gravett
- MK Mwaniki
- MS Kramer
- MV Kinney
- MV Kinney
- N Kultursay
- N Walker
- National Collaborating Centre for Women's and Children's Health
- NIH
- P Nygren
- PMNCH
- Preterm Birth Action Group
- R Bahl
- R Pattinson
- R Romero
- RL Goldenberg
- SS Goudar
- SV Dean
- T Lissauer
- U Samarasekera
- UNICEF
- United Nations Millennium Project
- United Nations Population Division
- WHO
- ZA Bhutta
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
- âŠ