173 research outputs found
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alexander J
- Aliev T
- Allfrey P
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Asaadi J
- Asghar MI
- Askew A
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avery P
- Avetisyan A
- Awad A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ballin J
- Ban Y
- Bandurin D
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauer J
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Bedoya CF
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Bell AJ
- Bell KW
- Bell P
- Bellan P
- Bellan R
- Bellinger JN
- Belotelov I
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Bender W
- Benedetti D
- Benelli G
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Bergholz M
- Beri SB
- Bernardini J
- Bernet C
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- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Besson A
- Betchart B
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bian JG
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boeriu O
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- Bolla G
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- Bolton T
- Bonacorsi D
- Bonato A
- Bondar N
- Bondu O
- Bontenackels M
- Boos E
- Borcherding F
- Borgia MA
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
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- Bostock F
- Botta C
- Boucerneur M
- Boudoul G
- Boulahouache C
- Boumediene D
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- Branca A
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- Breedon R
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- Buchmuller O
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- Butz E
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- Camanzi B
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- Campderros JD
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- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
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- Cavallari F
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- Cavanaugh R
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- Ceballos GG
- Cebra D
- Cepeda M
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- Cerci S
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- Cerminara G
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- Chabert EC
- Chadwick M
- Chakaberia I
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
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- Chen Y
- Chen Z
- Cheng TL
- Chertok M
- Chetluru V
- Cheung HWK
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Choi M
- Choi S
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- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cifuentes JAB
- Cihangir S
- Cimmino A
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Cole P
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
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- Cooper SI
- Cortabitarte RV
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
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- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
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- Cumalat JP
- Cuplov V
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- Cushman P
- Cussans D
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Darmenov N
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- David A
- Davids M
- Davies G
- De Araujo FTD
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Palma M
- De Roeck A
- De Souza SF
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Debreczeni G
- Deisher A
- Deiters K
- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demarteau M
- Demin P
- Demina R
- Demir D
- Demir Z
- Demortier L
- Denegri D
- Deniz M
- Depasse P
- Dero V
- Devroede O
- Dhingra N
- Di Giovanni GP
- Di Guida S
- Di Marco E
- Di Matteo L
- Diamond B
- Dias FA
- Dias MAF
- Diemoz M
- Dierlamm A
- Dimitrov A
- Dimitrov L
- Dinardo ME
- Dirkes G
- Dissertori G
- Dittmar M
- Djordjevic M
- Do Amaral SMS
- Dobrzynski L
- Dobur D
- Doesburg R
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- Draeger J
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- Dragoiu C
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- Dremin I
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- Dudko L
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- Duggan D
- Dumanoglu I
- Duric S
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- Dyulendarova M
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- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
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- Edelmaier CJ
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- Elliott-Peisert A
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- Elmer P
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- Erdmann W
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- Eskew C
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- Eugster J
- Eusebi R
- Evangelou I
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- Fabbri F
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- Fabbro B
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- Fabozzi F
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- Fahim A
- Falkiewicz A
- Fanfani A
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- Fantasia C
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- Farrell C
- Fasanella D
- Fassi F
- Faure JL
- Favaro C
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- Fay J
- Fehling D
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- Felcini M
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- Ferapontov A
- Ferencek D
- Ferguson T
- Fernandez M
- Ferrando A
- Ferri F
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- Field RD
- Fields LJ
- Finger M
- Finger M
- Fiore L
- Fiori F
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- Fisk I
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- Flix J
- Florez C
- Flossdorf A
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- Flucke G
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- Frangenheim J
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- Garfinkel AF
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- Gaultney V
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- Gavrilov V
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- Gaz A
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- Gentit FX
- Georgiou G
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- Gerbaudo D
- Gerber CE
- Gershtein Y
- Gerwig H
- Geurts FJM
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- Giammanco A
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- Giubilato P
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- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zakaria M
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- Zanetti M
- Zang J
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- Zarubin A
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- Zeuner WD
- Zeyrek M
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- Ziebarth EB
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- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
- Anghel IM
- Anguelov T
- Anh T. Vu
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- Antillon E
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- Bakirci MN
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- Xaplanteris L.
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- Xie S
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- Zachariadou A
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- Zang SL
- Zarubin A
- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
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- Zhukov V
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- Ziebarth EB
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- Zinonos Z
- Zito G
- Zoeller MH
- Zotto P
- Zub S
- Zumerle G
- Zuranski A
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Constitutively elevated levels of SOCS1 suppress innate responses in DF-1 immortalised chicken fibroblast cells.
- Author
- A Tiwari
- A Yoshimura
- AC Reichard
- AJ Karpala
- AM Levy
- AM Turnley
- AY Wen
- B Schumacher
- B Sporri
- BA Croker
- CA Cotter
- CM Ahmed
- CM Ahmed
- CW Lee
- DJ Gough
- DL May
- E Buehler
- FA Mallette
- G Xu
- H Kallel
- H Kim
- H Kim
- H Mi
- H Qu
- H Yasukawa
- I Jordan
- I Jordan
- J Lee
- J Schaefer-Klein
- J Strebovsky
- J Zhang
- JD Mosca
- JJ Babon
- K Buttigieg
- K Nazerian
- K Otsuki
- K Rekha
- KJ Blight
- M Aricibasi
- M Hashimoto
- M Himly
- M Liniger
- M Narazaki
- MD Brown
- MW Pfaffl
- P King
- R Maas
- R Marais
- RD Hess
- S McComb
- S You
- S-m Gao
- SM Gao
- SM Laidlaw
- SW Brown
- T Hayashi
- X-X Hong
- Y Genzel
- Y Masuda
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 29/11/2017
- Field of study
The spontaneously immortalised DF-1 cell line is rapidly replacing its progenitor primary chicken embryo fibroblasts (CEFs) for studies on avian viruses such as avian influenza but no comprehensive study has as yet been reported comparing their innate immunity phenotypes. We conducted microarray analyses of DF-1 and CEFs, under both normal and stimulated conditions using chicken interferon-Îą (chIFN-Îą) and the attenuated infectious bursal disease virus vaccine strain PBG98. We found that DF-1 have an attenuated innate response compared to CEFs. Basal expression levels of Suppressor of Cytokine Signalling 1 (chSOCS1), a negative regulator of cytokine signalling in mammals, are 16-fold higher in DF-1 than in CEFs. The chSOCS1 âSOCS boxâ domain (which in mammals, interacts with an E3 ubiquitin ligase complex) is not essential for the inhibition of cytokine-induced JAK/STAT signalling activation in DF-1. Overexpression of SOCS1 in chIFN-Îą-stimulated DF-1 led to a relative decrease in expression of interferon-stimulated genes (ISGs; MX1 and IFIT5) and increased viral yield in response to PBG98 infection. Conversely, knockdown of SOCS1 enhanced induction of ISGs and reduced viral yield in chIFN-Îą-stimulated DF-1. Consequently, SOCS1 reduces induction of the IFN signalling pathway in chicken cells and can potentiate virus replication
Membrane Association of the PTEN Tumor Suppressor: Molecular Details of the Protein-Membrane Complex from SPR Binding Studies and Neutron Reflection
- Author
- A Di Cristofano
- A Di Cristofano
- A Goffin
- A Orrico
- AH Ross
- Alonzo H. Ross
- Arne Gericke
- BA Cornell
- BJ Kirby
- BL Stiles
- C Janetopoulos
- D Lingwood
- D Vaknin
- DJ McGillivray
- DJ McGillivray
- E Catmull
- F Heinrich
- Frank Heinrich
- G Valincius
- GE Herman
- H Nanda
- HP Wacklin
- IK Vockenroth
- J Wang
- JA Dura
- JE Curtis
- JO Lee
- K Narayan
- KL McBride
- L Boccone
- L Li
- L Simpson
- M Connolly
- M Groszer
- M Rahdar
- M Schalke
- MA Lemmon
- Marie-Claire Daou
- Markus J. Buehler
- Mathias LĂśsche
- MC Wiener
- MG Butler
- MT Stein
- NS Mutti
- P Mitra
- P Shekhar
- Prabhanshu Shekhar
- R Gupta
- RB Campbell
- RE Redfern
- RE Redfern
- S Das
- S Ogg
- S Shenoy
- S-P Ji
- Siddharth Shenoy
- T Maehama
- TP Russell
- U Golebiewska
- YH Huang
- Publication venue
- Public Library of Science
- Publication date
- 10/04/2012
- Field of study
The structure and function of the PTEN phosphatase is investigated by studying its membrane affinity and localization on in-plane fluid, thermally disordered synthetic membrane models. The membrane association of the protein depends strongly on membrane composition, where phosphatidylserine (PS) and phosphatidylinositol diphosphate (PI(4,5)P2) act pronouncedly synergistic in pulling the enzyme to the membrane surface. The equilibrium dissociation constants for the binding of wild type (wt) PTEN to PS and PI(4,5)P2 were determined to be Kdâź12 ÂľM and 0.4 ÂľM, respectively, and Kdâź50 nM if both lipids are present. Membrane affinities depend critically on membrane fluidity, which suggests multiple binding sites on the protein for PI(4,5)P2. The PTEN mutations C124S and H93R show binding affinities that deviate strongly from those measured for the wt protein. Both mutants bind PS more strongly than wt PTEN. While C124S PTEN has at least the same affinity to PI(4,5)P2 and an increased apparent affinity to PI(3,4,5)P3, due to its lack of catalytic activity, H93R PTEN shows a decreased affinity to PI(4,5)P2 and no synergy in its binding with PS and PI(4,5)P2. Neutron reflection measurements show that the PTEN phosphatase âscoots" along the membrane surface (penetration <5 Ă
) but binds the membrane tightly with its two major domains, the C2 and phosphatase domains, as suggested by the crystal structure. The regulatory C-terminal tail is most likely displaced from the membrane and organized on the far side of the protein, âź60 Ă
away from the bilayer surface, in a rather compact structure. The combination of binding studies and neutron reflection allows us to distinguish between PTEN mutant proteins and ultimately may identify the structural features required for membrane binding and activation of PTEN
Combined Tevatron upper limit on gg->H->W+W- and constraints on the Higgs boson mass in fourth-generation fermion models
- Author
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- Publication venue
- Publication date
- 01/01/2010
- Field of study
Report number: FERMILAB-PUB-10-125-EWe combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg->H->W+W- in p=pbar collisions at the Fermilab Tevatron Collider at sqrt{s}=1.96 TeV. With 4.8 fb-1 of integrated luminosity analyzed at CDF and 5.4 fb-1 at D0, the 95% Confidence Level upper limit on \sigma(gg->H) x B(H->W+W-) is 1.75 pb at m_H=120 GeV, 0.38 pb at m_H=165 GeV, and 0.83 pb at m_H=200 GeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% Confidence Level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process ggâHâW+W- in ppĚ
collisions at the Fermilab Tevatron Collider at âs=1.96ââTeV. With 4.8ââfb-1 of integrated luminosity analyzed at CDF and 5.4ââfb-1 at D0, the 95% confidence level upper limit on Ď(ggâH)ĂB(HâW+W-) is 1.75 pb at mH=120ââGeV, 0.38 pb at mH=165ââGeV, and 0.83 pb at mH=200ââGeV. Assuming the presence of a fourth sequential generation of fermions with large masses, we exclude at the 95% confidence level a standard-model-like Higgs boson with a mass between 131 and 204 GeV.Peer reviewe
CMS Data Processing Workflows during an Extended Cosmic Ray Run
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- Publication venue
- INSTITUTE OF PHYSICS PUBLISHING
- Publication date
- 01/01/2009
- Field of study
Peer reviewe
Aligning the CMS Muon Chambers with the Muon Alignment System during an Extended Cosmic Ray Run
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
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- Adam W
- Adams MR
- Adams T
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- Adler V
- Adolphi R
- Adzic P
- Afaq MA
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- Aguilar Benitez M
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- Altsybeev I
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- Andelin D
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- Publication venue
- Publication date
- 01/01/2009
- Field of study
Peer reviewe
Multi-messenger observations of a binary neutron star merger
- Author
- Aab A
- Aartsen MG
- Abbott BP
- Abbott R
- Abbott TD
- Abbott TMC
- Abdalla H
- Abe F
- Abeysekara AU
- Abramo LR
- Abramowski A
- Abreu P
- Acernese F
- Acero F
- Ackermann M
- Ackley K
- Ackley K
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- Agliozzo C
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- Aguilar JA
- Aharonian F
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- Aiello L
- Ain A
- Ajith P
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- Array LWA Long Wavelength
- Array MWA Murchison Widefield
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- Li XB
- Li XF
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- Parra A
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- Passuello D
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- Pearlstone BL
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- Pekeur NW
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- Piranomonte S
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- Piro AL
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- Pisanu T
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- Poolakkil S
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- Popolizio P
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- Prado RR
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- Principe G
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- Prodi GA
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- Prokoph H
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- Prrer M
- Przybylski GT
- Pulone L
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- Reposeur T
- Resconi E
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- Riviere C
- Rizi V
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- Robie R
- Robinet F
- Rocchi A
- Rochester LS
- Rodi J
- Rodriguez H
- Rojas D Avila
- Rojas-Bravo C
- Rojo J Rodriguez
- Rol E
- Rolland L
- Rollins JG
- Roma VJ
- Romano R
- Romel CL
- Romer AK
- Romero M Dominguez
- Romie JH
- Romoli C
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- Roques J-P
- Rosa-Gonzlez D
- Rosell A Carnero
- Rosenberg M
- Rosetti S
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- Ross MP
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- Rosswog S
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- Roth M
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- Rowlinson A
- Rowlinson A
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- Ruiz R Gracia
- Ruiz-Velasco E
- Rulten CB
- Rumyantsev VV
- Rusu F
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- Ryckbosch D
- Rykoff ES
- Rysewyk D
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- Sadecki T
- Sadeghian L
- Sadler EM
- Sadler EM
- Saffe C
- Saffi SJ
- Saftoiu A
- Sahakian V
- Sai N
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- Saito Y
- Sakamaki A
- Sakamoto T
- Sakellariadou M
- Sako M
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- Salafia OS
- Salamida F
- Salazar H
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- Saleem M
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- Salemi F
- Salina G
- Salmon L
- Salvadori I
- Salvaterra R
- Samajdar A
- Sammut L
- Sampedro L
- Sampson LM
- Samtleben DFE
- Sanchez B
- Sanchez DA
- Sanchez E
- Sanchez EJ
- Sanchez F
- Sanchez LE
- Sanchez-Losa A
- Sanchez-Lucas P
- Sanchez-Ramirez R
- Sanchis-Gual N
- Sand DJ
- Sandberg V
- Sanders JR
- Sandoval A
- Sandrock A
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- Sansom EK
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- Santangelo A
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- Santos EM
- Sapienza P
- Sarazin F
- Sarkar S
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- Sasaki M
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- Satalecka K
- Sathyaprakash BS
- Sato R
- Saulson PR
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- Sauter O
- Savage RL
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- Sawadsky A
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- Schlegel DJ
- Schlickeiser R
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- Schmidt BP
- Schmidt D
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- Schnabel R
- Schneider A
- Schneider M
- Schneiter M
- Schoenell W
- Schoenen S
- Schofield RMS
- Scholten O
- Schonbeck A
- Schoneberg S
- Schoorlemmer H
- Schovnek P
- Schreiber E
- Schroder FG
- Schroder S
- Schroder SL
- Schssler F
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- Schuette D
- Schulte BW
- Schultz ASB
- Schulz A
- Schulz A
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- Schumacher J
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- Schwalbe SG
- Schwanke U
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- Schweyer T
- Sciutto SJ
- Scolnic D
- Scott J
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- Secco LF
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- Segreto A
- Seidel E
- Seitenzahl IR
- Sekiguchi Y
- Sellers D
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- Sengupta AS
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- Sergeev A
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- Seunarine S
- Sevilla-Noarbe I
- Seyffert AS
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- Shah AA
- Shahriar MS
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- Shang Z
- Shannon RM
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- Sharp RG
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- Shilon I
- Shimizu Y
- Shimomukai R
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- Shoemaker DH
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- Siemens X
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- Singer LP
- Singh A
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- Sintes AM
- Siskind EJ
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- Ziegler A
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- Zimnukhov DS
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- 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 transientâs 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 dijet resonances in 7 TeV pp collisions at CMS
- Author
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- Abbiendi G
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- Zoeller MH
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
This is the Pre-print version of the Article. The official published version of the paper can be accessed from the link below - Copyright @ 2010 APSA search for narrow resonances in the dijet mass spectrum is performed using data corresponding to an integrated luminosity of 2.9ââpb-1 collected by the CMS experiment at the Large Hadron Collider. Upper limits at the 95% confidence level are presented on the product of the resonance cross section, branching fraction into dijets, and acceptance, separately for decays into quark-quark, quark-gluon, or gluon-gluon pairs. The data exclude new particles predicted in the following models at the 95% confidence level: string resonances, with mass less than 2.50 TeV, excited quarks, with mass less than 1.58 TeV, and axigluons, colorons, and E6 diquarks, in specific mass intervals. This extends previously published limits on these models.This work is supported by FMSR (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); Academy of Sciences and NICPB (Estonia); Academy of Finland, ME, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTD (Serbia); MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAK and TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA)
Transverse-momentum and pseudorapidity distributions of charged hadrons in pp collisions at âs=7 TeV
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- Virto AL
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- Vitulo P
- Viviani C
- Vlasov E
- Vlimant JR
- Vodopiyanov I
- Vogel H
- Volkov A
- Volobouev I
- Volodko A
- Volpe R
- Volyanskyy D
- Vorobiev I
- Vorobyev A
- Voutilainen M
- Wagner SR
- Wagner-Kuhr J
- Wakefield S
- Wallny R
- Walsh S
- Waltenberger W
- Walzel G
- Wan Z
- Wang CC
- Wang D
- Wang J
- Wang J
- Wang M
- Wang X
- Wang Z
- Warchol J
- Ward S
- Wardrope D
- Wayne M
- Weber H
- Weber M
- Weber M
- Wehrli L
- Wei JT
- Weinberg M
- Weinberger M
- Wendland L
- Weng J
- Weng Y
- Wenger EA
- Werner JS
- Wetzel J
- Whitbeck A
- Whitmore J
- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
- Wilke L
- Wilken R
- Wilkinson R
- Williams G
- Williams JC
- Willmott C
- Wimpenny S
- Winn D
- Wissing C
- Witherell M
- Wittich P
- Wittmer B
- Woehri HK
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu JH
- Wu W
- Wulz CE
- Wyslouch B
- Xiao H
- Xie S
- Yagil A
- Yan M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyaniy A
- Zeidler C
- Zeinali M
- Zeise M
- Zennamo J
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zinonos Z
- Zito G
- Zoeller MH
- Zorbilmez C
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Charged-hadron transverse-momentum and pseudorapidity distributions in proton-proton collisions at âs=7ââTeV are measured with the inner tracking system of the CMS detector at the LHC. The charged-hadron yield is obtained by counting the number of reconstructed hits, hit pairs, and fully reconstructed charged-particle tracks. The combination of the three methods gives a charged-particle multiplicity per unit of pseudorapidity dNch/dΡ||Ρ|<0.5=5.78Âą0.01(stat)Âą0.23(syst) for non-single-diffractive events, higher than predicted by commonly used models. The relative increase in charged-particle multiplicity from âs=0.9 to 7 TeV is [66.1Âą1.0(stat)Âą4.2(syst)]%. The mean transverse momentum is measured to be 0.545Âą0.005(stat)Âą0.015(syst)ââGeV/c. The results are compared with similar measurements at lower energies
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