111 research outputs found
Generalized entropy optimized by an arbitrary distribution
- Author
- Publication venue
- 'IOP Publishing'
- Publication date
- 20/11/2002
- Field of study
We construct the generalized entropy optimized by a given arbitrary
statistical distribution with a finite linear expectation value of a random
quantity of interest. This offers, via the maximum entropy principle, a unified
basis for a great variety of distributions observed in nature, which can hardly
be described by the conventional methods. As a simple example, we explicitly
derive the entropy associated with the stretched exponential distribution. To
include the distributions with the divergent moments (e.g., the Levy stable
distributions), it is necessary to modify the definition of the expectation
value.Comment: 10 pages, no figure
Schroedinger equation for joint bidirectional motion in time
- Author
- Aebi R
- Aebi R
- Aharonov Y
- Azizov T Ya
- Azizov T Ya
- Baer M
- Bjorken J D
- Bjorken J D
- Carroll S M
- Chevalley C
- Davies P
- Davies P C W
- Dirac P A M
- Feynman R P
- Frankel T
- G E Hahne
- Gohberg I
- Hahne G E
- Hazewinkel M (ed)
- Juneja O P
- Kaku M
- Konisi G
- Konisi G
- Landsberg P T (ed)
- Levine R D
- Light J C
- Marcus R A
- Miller W H
- Nagy K L
- Nahin P J
- Newton R G
- Novikov I D
- Penrose R
- Penrose R
- Peskin M E
- Pontrjagin L S
- Price H
- Reichenbach H
- Schrödinger E
- Schulman L S
- Schweber S S
- Stannard F R
- Weinberg S
- Wigner E P
- Zeh H-D
- Publication venue
- 'IOP Publishing'
- Publication date
- 19/04/2004
- Field of study
The conventional, time-dependent Schroedinger equation describes only
unidirectional time evolution of the state of a physical system, i.e., forward
or, less commonly, backward. This paper proposes a generalized quantum dynamics
for the description of joint, and interactive, forward and backward time
evolution within a physical system. [...] Three applications are studied: (1) a
formal theory of collisions in terms of perturbation theory; (2) a
relativistically invariant quantum field theory for a system that kinematically
comprises the direct sum of two quantized real scalar fields, such that one
field evolves forward and the other backward in time, and such that there is
dynamical coupling between the subfields; (3) an argument that in the latter
field theory, the dynamics predicts that in a range of values of the coupling
constants, the expectation value of the vacuum energy of the universe is forced
to be zero to high accuracy. [...]Comment: 30 pages, no figures. Related material is in quant-ph/0404012.
Differs from published version by a few added remarks on the possibility of a
large-scale-average negative energy density in spac
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
- Ferencek D
- Ferguson T
- Fernandez M
- Ferrando A
- Ferri F
- Ferro C
- Field RD
- Fields LJ
- Finger M
- Finger M
- Fiore L
- Fiori F
- Fisher M
- Fisk I
- Flacher H
- Flix J
- Florez C
- Flossdorf A
- Flowers K
- Flucke G
- Flugge G
- Foa L
- Focardi E
- Folgueras S
- Fontaine JC
- Ford WT
- Foudas C
- Fouz MC
- Franci D
- Francis B
- Frangenheim J
- Franzoni G
- Frazier R
- Freeman J
- Freudenreich K
- Friedl M
- Friis E
- Frisch B
- Frosali S
- Frueboes T
- Fruhwirth R
- Fu Y
- Fulcher J
- Funk W
- Furic IK
- Futyan D
- Gabathuler K
- Gabella W
- Gaddi A
- Galanti M
- Gallinaro M
- Gallo E
- Gamsizkan H
- Ganjour S
- Gao Y
- Garcia JMV
- Garcia-Abia R
- Garcia-Bellido A
- Garcia-Solis EJ
- Garfinkel AF
- Garrido RGR
- Gartner J
- Gary JW
- Gascon S
- Gasparini F
- Gasparini U
- Gataullin M
- Gaultney V
- Gauthier L
- Gavrilov V
- Gay APR
- Gaz A
- Gebbert U
- Gecse Z
- Geenen H
- Geffert P
- Geiser A
- Gele D
- Genchev V
- Gennai S
- Gentit FX
- Georgiou G
- Geralis T
- Gerbaudo D
- Gerber CE
- Gershtein Y
- Gerwig H
- Geurts FJM
- Ghete VM
- Ghezzi A
- Giacomelli P
- Giammanco A
- Giassi A
- Gibbons LK
- Giffels M
- Gigi D
- Gill K
- Gilmore J
- Giordano D
- Giordano F
- Girgis S
- Giubilato P
- Giunta M
- Giurgiu G
- Givernaud A
- Glege F
- Gleyzer SV
- Glushkov I
- Gninenko S
- Go A
- Gobbo B
- Godang R
- Godinovic N
- Godshalk A
- Goerlach U
- Goh J
- Gokbulut G
- Gokieli R
- Goldberg S
- Goldenzweig P
- Goldstein J
- Golf F
- Gollapinni S
- Golovtsov V
- Golubev N
- Golutvin I
- Gomez G
- Gomez JA
- Gomez JP
- Goncharov M
- Gonzalez JS
- Gonzi S
- Gorski M
- Gotra Y
- Gottschalk E
- Goulianos K
- Gouskos L
- Gouzevitch M
- Govoni P
- Gowdy S
- Grab C
- Grachov O
- Grandi C
- Gras P
- Grassi M
- Gray L
- Gray R
- Graziano A
- Greder S
- Green D
- Gregoire G
- Gregores EM
- Gresele A
- Gribushin A
- Grigelionis I
- Grimes M
- Grishin V
- Gritsan AV
- Grogg KS
- Gronberg J
- Grothe M
- Grunewald M
- Gruschke J
- Gu J
- Guchait M
- Guiducci L
- Guler AM
- Guler Y
- Gulmez E
- Gunthoti K
- Guo S
- Guo Y
- Guo ZJ
- Gupta P
- Gupta R
- Guragain S
- Gurpinar E
- Gurrola A
- Gurtu A
- Gutay L
- Gutsche O
- Haas J
- Hackstein C
- Hadjiiska R
- Hadley NJ
- Hagopian S
- Hagopian V
- Haguenauer M
- Hahn A
- Hahn KA
- Hajdu C
- Halkiadakis E
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- Hall-Wilton R
- Halu A
- Halyo V
- Hammad GH
- Hammer J
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- Hanlon J
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- Hanson G
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- Harkonen J
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- Harris RM
- Hartl C
- Hartley D
- Hartmann F
- Harvey J
- Hashemi M
- Hatakeyama K
- Hatherell Z
- Hauk J
- Haupt J
- Hauser J
- Hays J
- Heath GP
- Heath HF
- Hebbeker T
- Hebda P
- Hegeman J
- Hegner B
- Heikkinen A
- Heindl SM
- Heinrich M
- Heintz U
- Heister A
- Hektor A
- Held H
- Heltsley B
- Henderson C
- Heo SG
- Heracleous N
- Hernandez AS
- Hernandez JM
- Herndon M
- Herve A
- Hesketh G
- Heyburn B
- Heydhausen D
- Hidas D
- Hildreth M
- Hill C
- Hindrichs O
- Hintz W
- Hinzmann A
- Hirosky R
- Hirschauer J
- Hits D
- Hobson PR
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- Hohlmann M
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- Hollingsworth M
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- Honma A
- Hooberman B
- Hoorani HR
- Hopkins W
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- Hormann N
- Horvath D
- Hos I
- Hou WS
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- Huang XT
- Huckvale B
- Hunt A
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- Iaydjiev P
- Ibarguen HAS
- Iglesias LL
- Ignatenko M
- Iiyama Y
- Iles G
- Ille B
- Incandela J
- Ingram Q
- Innocente V
- Iorio AOM
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- Ivanov A
- Ivanov Y
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- Jackson J
- Jafari A
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- Jain S
- Jain S
- James E
- Jang DW
- Janot R
- Janssen X
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- Jarrin EC
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- Joshi U
- Juillot P
- Jun SY
- Jung H
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- Justus C
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- Kachanov V
- Kadastik M
- Kadija K
- Kaestli HC
- Kaftanov V
- Kailas S
- Kalakhety H
- Kalavase P
- Kalinowski A
- Kalogeropoulos A
- Kamenev A
- Kamon T
- Kang S
- Kangal EE
- Kannike K
- Kao KY
- Kao SC
- Kapusi A
- Karaman T
- Karapostoli G
- Karavakis E
- Karchin PE
- Karim M
- Karimaki V
- Karjavin V
- Karmgard DJ
- Kaschube K
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- Kataria SK
- Katkov I
- Katsas P
- Kaufman GN
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- Kaussen G
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- Kaya O
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- Kellogg RG
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- Kesisoglou S
- Khachatryan V
- Khakzad M
- Khalatyan S
- Khalil S
- Khan A
- Khan WA
- Kharchilava A
- Khatiwada R
- Khotilovich V
- Khukhunaishvili A
- Khurshid T
- Kiesenhofer W
- Killewald P
- Kilminster B
- Kim B
- Kim DH
- Kim GN
- Kim H
- Kim H
- Kim JE
- Kim JH
- Kim JY
- Kim M
- Kim TJ
- Kim V
- Kim Y
- Kim Z
- Kinnunen R
- Kirakosyan M
- Kirsanov M
- Klabbers P
- Klanner R
- Klapoetke K
- Klein B
- Klein K
- Kleinwort C
- Klem J
- Klima B
- Klimenko S
- Klimkovich T
- Klingebiel D
- Kluge H
- Klukas J
- Klute M
- Knutsson A
- Ko W
- Koay SA
- Kodolova O
- Kohli JM
- Kokkas P
- Kolb J
- Kolberg T
- Konecki M
- Kong DJ
- Konig S
- Konigsberg J
- Konstantinov D
- Kopecky A
- Korablev A
- Korpela A
- Kortelainen MJ
- Korytov A
- Kossov M
- Kotlinski D
- Kotov K
- Kousouris K
- Kovalskyi D
- Kovitanggoon K
- Koybasi O
- Kozhuharov V
- Kozlov G
- Kraan A
- Krajczar K
- Kramer L
- Krammer M
- Krasnikov N
- Kravchenko I
- Kreczko L
- Kreis B
- Kress M
- Kress T
- Kreuzer P
- Kroeger R
- Krofcheck D
- Krokhotin A
- Krolikowski J
- Kropivnitskaya A
- Krpic D
- Krucker D
- Krutelyov V
- Krychkine V
- Kubik A
- Kubota Y
- Kuessel Y
- Kuhr T
- Kukartsev G
- Kumar A
- Kumar A
- Kunori S
- Kuo CM
- Kurca T
- Kurt R
- Kuznetsov V
- Kuznetsova E
- Kwan S
- Kyberd P
- Kypreos T
- Kyriakis A
- Laasanen AT
- Lacaprara S
- Lacroix F
- Lae CK
- Laird E
- Lamichhane R
- Lampen T
- Lanaro A
- Lander R
- Landsberg G
- Lanev A
- Lange D
- Lange J
- Lange W
- Langenegger U
- Lannon K
- Lanske D
- Lariccia R
- Lassila-Perini K
- Laszlo A
- Lath A
- Lawson P
- Lazaridis C
- Lazic D
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- Wissing C
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- Wood JS
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- Wright D
- Wrochna G
- Wu JH
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- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
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- Xu M
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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
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- Zheng Y
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- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- 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
Hawking Radiation from Higher-Dimensional Black Holes
- Author
- A Casanova
- A Chamblin
- A Flachi
- A Ishibashi
- A Peltola
- AA Starobinskii
- AC Ottewill
- AL Fitzpatrick
- AS Cornell
- AS Majumdar
- AS Majumdar
- B Cuadros-Melgar
- B Kleihaus
- BL Hu
- C Galfard
- C Herdeiro
- CM Harris
- CM Harris
- D Karasik
- D-C Dai
- D-C Dai
- DC Dai
- DK Park
- DN Page
- DN Page
- DN Page
- E Jung
- E Jung
- E Newman
- E Seidel
- ED Fackerell
- EW Leaver
- FR Tangherlini
- G Aad
- G Aad
- G Aad
- G Duffy
- G Kofinas
- G Kofinas
- GL Landsberg
- H Kodama
- H Kodama
- H Kodama
- H Kudoh
- H Kudoh
- H Yoshino
- HS Reall
- HT Cho
- I Antoniadis
- J Doukas
- J Grain
- JA Frost
- JB Hartle
- JL Synge
- JN Goldberg
- K Murata
- L Randall
- L Randall
- M Anber
- M Bruni
- M Casals
- M Casals
- M Casals
- M Casals
- M Casals
- M Casals
- M Durkee
- M Govender
- M Heydari-Fard
- M Visser
- M Wang
- MA Rubin
- MA Rubin
- MK Parikh
- MOP Sampaio
- MOP Sampaio
- N Arkani-Hamed
- N Arkani-Hamed
- N Dadhich
- N Kaloper
- N Kaloper
- N Tanahashi
- N Tanahashi
- P Figueras
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Kanti
- P Nicolini
- PC Argyres
- R Brout
- R Casadio
- R Casadio
- R Emparan
- R Emparan
- R Emparan
- R Emparan
- R Emparan
- R Gregory
- R Gregory
- R Gregory
- R Gregory
- R Guedens
- R Parentani
- R Schutzhold
- RA Konoplya
- RC Myers
- S Abdolrahimi
- S Abdolrahimi
- S Chatrchyan
- S Chatrchyan
- S Creek
- S Creek
- S Creek
- S Creek
- S Creek
- S Dimopoulos
- S Hossenfelder
- S Massar
- S Shankaranarayanan
- S Tomizawa
- SA Teukolsky
- SA Teukolsky
- SB Giddings
- SC Park
- SD Mathur
- SM Christensen
- SM Christensen
- SW Hawking
- SW Hawking
- T Damour
- T Tanaka
- UH Gerlach
- V Cardoso
- V Cardoso
- V Frolov
- V Khachatryan
- VP Frolov
- VP Frolov
- VP Frolov
- WG Unruh
- Y Decanini
- Y Sendouda
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/04/2014
- Field of study
We review the quantum field theory description of Hawking radiation from evaporating black holes and summarize what is known about Hawking radiation from black holes in more than four space-time dimensions. In the context of the Large Extra Dimensions scenario, we present the theoretical formalism for all types of emitted fields and a selection of results on the radiation spectra. A detailed analysis of the Hawking fluxes in this case is essential for modelling the evaporation of higher-dimensional black holes at the LHC, whose creation is predicted by low-energy models of quantum gravity. We discuss the status of the quest for black-hole solutions in the context of the Randall-Sundrum brane-world model and, in the absence of an exact metric, we review what is known about Hawking radiation from such black holes
Dijet azimuthal decorrelations in pp collisions at √s = 7TeV
- 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
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- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
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- Andreev V
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- Wissing C
- Wittich P
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- Womersley WJ
- Won S
- Wood D
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu JH
- Wu W
- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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 L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- American Physical Society
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Measurements of dijet azimuthal decorrelations in pp collisions at √s=7 TeV using the CMS detector at the CERN LHC are presented. The analysis is based on an inclusive dijet event sample corresponding to an integrated luminosity of 2.9 pb-1. The results are compared to predictions from perturbative QCD calculations and various Monte Carlo event generators. The dijet azimuthal distributions are found to be sensitive to initial-state gluon radiation
Search for dijet resonances in 7 TeV pp collisions at CMS
- Author
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- Abbiendi G
- Abbrescia M
- Abdel-Basit A
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
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- Baden A
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- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
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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 2.9 pb-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)
Measurement of the B+ production cross section in pp collisions at √s = 7 TeV
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
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- Yilmaz Y
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- Zeuner WD
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- Ziebarth EB
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- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Measurements of the total and differential cross sections dσ/dpTB and dσ/dyB for B+ mesons produced in pp collisions at √s=7 TeV are presented. The data correspond to an integrated luminosity of 5.8 pb-1 collected by the CMS experiment operating at the LHC. The exclusive decay B+→J/ψK+, with J/ψ→μ+μ-, is used to detect B+ mesons and to measure the production cross section as a function of pTB and yB. The total cross section for pTB>5 GeV and |yB|<2.4 is measured to be 28.1±2.4±2.0±3.1 μb, where the first uncertainty is statistical, the second is systematic, and the last is from the luminosity measurement
Transverse-momentum and pseudorapidity distributions of charged hadrons in pp collisions at √s=7 TeV
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- Abbiendi G
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- 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 √s=7 TeV 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/dη||η|<0.5=5.78±0.01(stat)±0.23(syst) for non-single-diffractive events, higher than predicted by commonly used models. The relative increase in charged-particle multiplicity from √s=0.9 to 7 TeV is [66.1±1.0(stat)±4.2(syst)]%. The mean transverse momentum is measured to be 0.545±0.005(stat)±0.015(syst) GeV/c. The results are compared with similar measurements at lower energies
Search for supersymmetry in pp collisions at 7 TeV in events with jets and missing transverse energy
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- Abbiendi G
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- Yilmaz Y
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- Yun JC
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- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Zhang L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- Elsevier
- Publication date
- 01/01/2011
- 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 @ 2011 ElsevierA search for supersymmetry with R-parity conservation in proton-proton collisions at a centre-of-mass energy of 7 TeV is presented. The data correspond to an integrated luminosity of 35 inverse picobarns collected by the CMS experiment at the LHC. The search is performed in events with jets and significant missing transverse energy, characteristic of the decays of heavy, pair-produced squarks and gluinos. The primary background, from standard model multijet production, is reduced by several orders of magnitude to a negligible level by the application of a set of robust kinematic requirements. With this selection, the data are consistent with the standard model backgrounds, namely t t-bar, W + jet and Z + jet production, which are estimated from data control samples. Limits are set on the parameters of the constrained minimal supersymmetric extension of the standard model. These limits extend those set previously by experiments at the Tevatron and LEP colliders.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)
Search for supersymmetry in pp collisions at 7 TeV in events with jets and missing transverse energy
- 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
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- Piroue R
- Pivarski J
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- Plestina R
- Pol ME
- Polatoz A
- Polese G
- Polic D
- Poll A
- Pollack B
- Pompili A
- Pooth O
- Popescu S
- Pordes R
- Pozdnyakov A
- Pozzobon N
- Prescott C
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Pugliese G
- Puigh D
- Puljak I
- Punz T
- Qazi S
- Qian SJ
- Quan X
- Quast G
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- Radburn Smith BC
- Radicci V
- Ragazzi S
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- Rahmat R
- Raics P
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- Rakness G
- Ralich R
- Ralph D
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- Raspereza A
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- Razis PA
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- Redaelli N
- Redjimi R
- Redondo I
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- Reithler H
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- ROLANDI LUIGI
- Romano E
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- Romero A
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- Rommerskirchen T
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- Savin A
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- Scheurer A
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- Wickens J
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- Wigmans R
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- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Wohri HK
- Wolf R
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- Won S
- Wood D
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu JH
- Wu W
- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- 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 L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A search for supersymmetry with R-parity conservation in proton-proton collisions at a centre-of-mass energy of 7 TeV is presented. The data correspond to an integrated luminosity of 35 pb(-1) collected by the CMS experiment at the LHC. The search is performed in events with jets and significant missing transverse energy, characteristic of the decays of heavy, pair-produced squarks and gluinos. The primary background, from standard model multijet production, is reduced by several orders of magnitude to a negligible level by the application of a set of robust kinematic requirements. With this selection, the data are consistent with the standard model backgrounds, namely t (t) over bar, W + jet and Z + jet production, which are estimated from data control samples. Limits are set on the parameters of the constrained minimal supersymmetric extension of the standard model. These limits extend those set previously by experiments at the Tevatron and LEP colliders. (C) 2011 CMS Collaboration
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