457 research outputs found
Insect herbivory dampens Subarctic birch forest C sink response to warming
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 28/10/2022
- Field of study
Climate warming is anticipated to make high latitude ecosystems stronger C sinks through increasing plant production. This effect might, however, be dampened by insect herbivores whose damage to plants at their background, non-outbreak densities may more than double under climate warming. Here, using an open-air warming experiment among Subarctic birch forest field layer vegetation, supplemented with birch plantlets, we show that a 2.3 degrees C air and 1.2 degrees C soil temperature increase can advance the growing season by 1-4 days, enhance soil N availability, leaf chlorophyll concentrations and plant growth up to 400%, 160% and 50% respectively, and lead up to 122% greater ecosystem CO2 uptake potential. However, comparable positive effects are also found when insect herbivory is reduced, and the effect of warming on C sink potential is intensified under reduced herbivory. Our results confirm the expected warming-induced increase in high latitude plant growth and CO2 uptake, but also reveal that herbivorous insects may significantly dampen the strengthening of the CO2 sink under climate warming. Warming is expected to increase C sink capacity in high-latitude ecosystems, but plant-herbivore interactions could moderate or offset this effect. Here, Silfver and colleagues test individual and interactive effects of warming and insect herbivory in a field experiment in Subarctic forest, showing that even low intensity insect herbivory strongly reduces C sink potential
Planck intermediate results. XLI. A map of lensing-induced B-modes
- Author
- Ade Par
- Aghanim N
- Ashdown M
- Aumont J
- Ay Aj
- B
- Baccigalupi C
- Barreiro Rb
- Bartolo N
- Basak S
- Battaner E
- Benabed K
- Benoit-Levy A
- Bernard J-
- Bersanelli M
- Bielewicz P
- Bock Jj
- Bonaldi A
- Bonavera L
- Bond Jr
- Borrill J
- Bouchet Fr
- Boulanger F
- Burigana C
- Butler Rc
- Calabrese E
- Cardoso J-
- Catalano A
- Chiang Hc
- Christensen Pr
- Clements Dl
- Colombi S
- Colombo Lpl
- Combet C
- Crill Bp
- Curto A
- Cuttaia F
- Danese L
- Davis Rj
- de Bernardis P
- de Zotti G
- Delabrouille J
- Dickinson C
- Diego Jm
- Dore O
- Ducout A
- Dupac X
- Elsner F
- Elt Bd
- Ensslin Ta
- Eriksen Hk
- ez-Monteagudo C
- Finelli F
- Forni O
- Frailis M
- Fraisse Aa
- Franceschi E
- Galeotta S
- Galli S
- Ganga K
- Ghosh T
- Giard M
- Giraud-Heraud Y
- Gjerlow E
- Gonzalez-Nuevo J
- Gorski Km
- Gruppuso A
- Gudmundsson Je
- Harrison Dl
- Hern
- Herranz D
- Hildebr
- Hornstrup A
- Hovest W
- Hurier G
- Jaffe Ah
- Jones Wc
- Keihanen E
- Keskitalo R
- Kisner Ts
- Knoche J
- Knox L
- Kunz M
- Kurki-Suonio H
- Lagache G
- Lahteenmaki A
- Lamarre J-
- Lasenby A
- Lattanzi M
- Leonardi R
- Levrier F
- Lilje Pb
- Linden-Vornle M
- Lopez-Caniego M
- Lubin Pm
- M
- Macias-Perez Jf
- Maffei B
- Maggie G
- Maino D
- Mangilli A
- Maris M
- Martin Pg
- Martinez-Gonzalez E
- Masi S
- Matarrese S
- Meinhold Pr
- Melchiorri A
- Mennella A
- Migliaccio M
- Mitra S
- Miville-Deschenes M-
- Moneti A
- Montier L
- Morgante G
- Mortlock D
- Moss A
- Munshi D
- Murphy Ja
- Naselsky P
- Nati F
- Natoli P
- Netterfield Cb
- Norgaard-Nielsen Hu
- Novikov D
- Novikov I
- Olesi N
- Pagano L
- Pajot F
- Paoletti D
- Pasian F
- Patanchon G
- Perdereau O
- Perotto L
- Pettorino V
- Piacentini F
- Piat M
- Pierpaoli E
- Pointecouteau E
- Polenta G
- Pratt Gw
- Rachen Jp
- Reinecke M
- Remazeilles M
- Renault C
- Renzi A
- Ri M
- Ristorcelli I
- Rocha G
- Rosset C
- Rossetti M
- Roudier G
- Rubino-Martin Ja
- Rusholme B
- S
- Santos D
- Savelainen M
- Savini G
- Scott D
- Spencer Ld
- Stolyarov V
- Stompor R
- Sudiwala R
- Sunyaev R
- Sutton D
- Suur-Uski A-
- Sygnet J-
- T Sr
- Tauber Ja
- Terenzi L
- Toffolatti L
- Tomasi M
- Tristram M
- Tucci M
- Tuovinen J
- Valenziano L
- Valiviita J
- Van Tent B
- Vielva P
- Villa F
- W
- Wade La
- Wehus Ik
- Yvon D
- Zacchei A
- Zonca A
- Publication venue
- 'EDP Sciences'
- Publication date
- 01/01/2016
- Field of study
The secondary cosmic microwave background (CMB) B-modes stem from the
post-decoupling distortion of the polarization E-modes due to the
gravitational lensing effect of large-scale structures. These lensing-induced
B-modes constitute both a valuable probe of the dark matter distribution and
an important contaminant for the extraction of the primary CMB B-modes from
inflation. Planck provides accurate nearly all-sky measurements of both the
polarization E-modes and the integrated mass distribution via the
reconstruction of the CMB lensing potential. By combining these two data
products, we have produced an all-sky template map of the lensing-induced
B-modes using a real-space algorithm that minimizes the impact of sky masks.
The cross-correlation of this template with an observed (primordial and
secondary) B-mode map can be used to measure the lensing B-mode power
spectrum at multipoles up to 2000. In particular, when cross-correlating with
the B-mode contribution directly derived from the Planck polarization maps,
we obtain lensing-induced B-mode power spectrum measurement at a significance
level of 12Ď, which agrees with the theoretical expectation derived
from the Planck best-fit ÎCDM model. This unique nearly all-sky
secondary B-mode template, which includes the lensing-induced information
from intermediate to small (10â˛ââ˛1000) angular scales, is
delivered as part of the Planck 2015 public data release. It will be
particularly useful for experiments searching for primordial B-modes, such as
BICEP2/Keck Array or LiteBIRD, since it will enable an estimate to be made of
the lensing-induced contribution to the measured total CMB B-modes.Comment: 20 pages, 12 figures; Accepted for publication in A&A; The B-mode map
is part of the PR2-2015 Cosmology Products; available as Lensing Products in
the Planck Legacy Archive http://pla.esac.esa.int/pla/#cosmology; and
described in the 'Explanatory Supplement'
https://wiki.cosmos.esa.int/planckpla2015/index.php/Specially_processed_maps#2015_Lensing-induced_B-mode_ma
Measurement of the t(t)over-bar production cross section in the dilepton channel in pp collisions at âs=8 TeV
- Author
- Abdelalim AA
- Adam W
- Adler Volker
- Alda WL
- Alderweireldt S
- Alves GA
- Antunovic Z
- Asawatangtrakuldee C
- Assran Y
- Attikis A
- Avila C
- Ban Y
- Bansal M
- Bansal S
- Basegmez S
- Beernaert Kelly
- Beliy N
- Beluffi C
- Benucci Leonardo
- Bergauer T
- Bernardes CA
- Besancon M
- Bian JG
- Blekman F
- Blyweert S
- Brigljevic V
- Bruno G
- Caebergs T
- Caillol C
- Carvalho W
- Castello R
- Caudron A
- Ceard L
- Chatrchyan S
- Chen GM
- Chen HS
- Chen M
- Chinellato J
- Cimmino Anna
- Clerbaux B
- Cornelis T
- Costantini Silvia
- Couderc F
- Custodio A
- D'Hondt J
- Da Costa EM
- Da Silva WLP
- Da Silveira GG
- Damiao DD
- Daubie E
- De Lentdecker G
- De Souza SF
- De Wolf EA
- Delaere C
- Dias FA
- Diblen SS
- Dildick Sven
- Dimitrov A
- Dragicevic M
- du Pree T
- Du R
- Eerola P
- Elgammal S
- Ero J
- Fabjan C
- Favart D
- Favart L
- Fedi G
- Figueiredo DM
- Finger M
- Finger M
- Florez C
- Forthomme L
- Friedl M
- Fruhwirth R
- Garcia Guillaume
- Garcia JMV
- Gay APR
- Genchev V
- Ghete VM
- Giammanco A
- Glushkov I
- Godinovic N
- Gomez JP
- Gonzalez JS
- Gregores EM
- Guo Y
- Hadjiiska R
- Hammad GH
- Harkonen J
- Hartl C
- Heracleous N
- Hollar J
- Hormann N
- Hrubec J
- Iaydjiev P
- Janssen X
- Jeitler M
- Jez P
- Jiang CH
- Kadastik M
- Kadija K
- Kalogeropoulos A
- Kamel AE
- Karimaki V
- Keaveney J
- Khachatryan V
- Kiesenhofer W
- Kim TJ
- Kinnunen R
- Klein Benjamin
- Knunz V
- Knutsson A
- Komm M
- Kortelainen MJ
- Kovac M
- Kozhuharov V
- Krammer M
- Kratschmer I
- Lampen T
- Lassila-Perini K
- Lehti S
- Lelas D
- Lellouch Jeremie
- Lemaitre V
- Leonard A
- Li Q
- Li W
- Liang D
- Liang S
- Liao J
- Liko D
- Linden T
- Litov L
- Liu S
- Lowette S
- Luetic J
- Luukka P
- Luyckx S
- Maenpaa T
- Maes M
- Mahmoud MA
- Malbouisson H
- Malek M
- Manganote EJT
- Mao Y
- Marage PE
- Marinov A
- Marono MV
- Martins CD
- Martins MC
- Martins T
- Mavromanolakis G
- McCartin Joseph
- Mekterovic D
- Meng X
- Mercadante PG
- Mikulec I
- Militaru O
- Mohammadi A
- Montoya CAC
- Moreno BG
- Morovic S
- Mossolov V
- Mousa J
- Mucibello L
- Mundim L
- Muntel M
- Murumaa M
- Nicolaou C
- Nogima H
- Novaes SF
- Nuttens C
- Ocampo Rios Alberto Andres
- Ochesanu S
- Olbrechts A
- Padula SS
- Pagano D
- Pavlov B
- Peltola T
- Pereira AV
- Pernie L
- Petkov P
- Pin A
- Piotrzkowski K
- Piperov S
- Plestina R
- Pol ME
- Polic D
- Popov A
- Ptochos F
- Puljak I
- Qian SJ
- Quertenmont L
- Rabady D
- Radi A
- Rahbaran B
- Raidal M
- Razis PA
- Rebane L
- Reis T
- Rodozov M
- Rohringer H
- Roland B
- Rougny R
- Ryckbosch Dirk
- Sanabria JC
- Santaolalla J
- Santoro A
- Schofbeck R
- Selvaggi M
- Seva T
- Shumeiko N
- Sierra LFC
- Sigamani Michael
- Sirunyan AM
- Souza MHG
- Strauss J
- Strobbe Nadja
- Strom D
- Sultanov G
- Sznajder A
- Tao J
- Taurok A
- Tavernier S
- Thomas L
- Thyssen Filip
- Tiko A
- Tikvica L
- Tomei TRFP
- Treberer-Treberspurg W
- Tumasyan A
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tuuva T
- Tytgat Michael
- Van Doninck W
- Van Haevermaet H
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Remortel N
- Van Spilbeeck A
- Vander Velde C
- Vanlaer P
- Villella I
- Voutilainen M
- Vutova M
- Walsh SinĂŠad Mary
- Waltenberger W
- Wang D
- Wang J
- Wang X
- Wang Z
- Wendland L
- Wulz CE
- Yazgan Efe
- Zaganidis Nikolaos
- Zhang L
- Zou W
- Publication venue
- Publication date
- 01/01/2014
- Field of study
The top-antitop quark (t (t) over bar) production cross section is measured in proton-proton collisions at root s = 8 TeV with the CMS experiment at the LHC, using a data sample corresponding to an integrated luminosity of 5.3 fb(-1). The measurement is performed by analysing events with a pair of electrons or muons, or one electron and one muon, and at least two jets, one of which is identified as originating from hadronisation of a bottom quark. The measured cross section is 239 +/- 2 (stat.) +/- 11 (syst.) +/- 6 (lum.) pb, for an assumed top-quark mass of 172.5 GeV, in agreement with the prediction of the standard model
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
- Berry D
- Berry E
- 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
- Boldizsar L
- Bolla G
- Bolognesi S
- 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
- Bose T
- Bostock F
- Botta C
- Boucerneur M
- Boudoul G
- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Broccolo G
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmuller O
- Buege V
- Buehler M
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burelo ED
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Caballero IG
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon A
- Cali IA
- Callner J
- Calvo E
- Camanzi B
- Caminada L
- Campagnari C
- Campbell A
- Campderros JD
- Camporesi T
- Cankocak K
- Cano E
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carroll R
- Cartiglia N
- Carvalho W
- Castaldi R
- Castello R
- Castro A
- Castro E
- Caudron J
- Cavallari F
- Cavallo FR
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cebra D
- Cepeda M
- Cerati GB
- Cerci S
- Cerizza G
- Cerminara G
- Cerny K
- Ceron C
- Cerrada M
- 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
- Chen WT
- Chen Y
- Chen Z
- Cheng TL
- Chertok M
- Chetluru V
- Cheung HWK
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Choi M
- Choi S
- Choi Y
- 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
- Conte E
- Conway J
- Cooper SI
- Cortabitarte RV
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- 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
- Dolen J
- Dominguez A
- Dominik W
- Dorigo T
- Dorney B
- Doroba K
- Dosselli U
- Dozen C
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- Dubinin M
- Duda M
- Dudero PR
- Dudko L
- Dugad S
- Duggan D
- Dumanoglu I
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dusinberre E
- Dutta D
- Dutta S
- Dutta V
- Dyulendarova M
- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
- Eerola P
- Efron J
- Eggert N
- El Mamouni H
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elvira VD
- Enderle H
- Engh D
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erhan S
- Ero J
- Ershov A
- Esen S
- Eshaq Y
- Eskew C
- Eskut E
- Etesami SM
- Eugster J
- Eusebi R
- Evangelou I
- Evans D
- Everaerts P
- Everett A
- Fabbri F
- Fabbri F
- Fabbricatore P
- Fabbro B
- Fabjan C
- Fabozzi F
- Faccioli P
- Fahim A
- Falkiewicz A
- Fanfani A
- Fano L
- Fantasia C
- Fanzago F
- Farrell C
- Fasanella D
- Fassi F
- Faure JL
- Favaro C
- Favart D
- Fay J
- Fehling D
- Feindt M
- Felcini M
- Feld L
- Ferapontov A
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- Zoeller MH
- 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 CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta MV
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
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- Zhokin A
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- Ziebarth EB
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
- Abbrescia M
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- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yucel M
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zeinali M
- Zeise M
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zheng Y
- Zhokin A
- Zhu RY
- Zhukov V
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- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
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- Wissing C
- Wittich P
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- Woehri HK
- Wolf M
- Wolf R
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- Won S
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- Worm SD
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- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- 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
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- 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
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- 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
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yoo J
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- Yumiceva F
- Yun JC
- Zabel J
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- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
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- Zhu RY
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
- Abbrescia M
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- Acosta JG
- Acosta MV
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- Adam W
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- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
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- Ahuja S
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- Akgun B
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- Akin IV
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- Alexander J
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- Anagnostou G
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
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- Ziebarth EB
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Capiluppi P
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- Castaldi R
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- Civinini C
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- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
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- Colling D
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- Cortezon EP
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- Costantini S
- Costanza F
- Coughlan JA
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- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cushman P
- Cussans D
- Custodio A
- 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
- Dabrowski A
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
- Davids M
- Davies G
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
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- de Fatis TT
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- De Gruttola M
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- De La Cruz-Burelo E
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- De Mattia M
- de Monchenault GH
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- Deisher A
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- del Arbol PMR
- Del Re D
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
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