نتایج جستجو برای: nlo analysis

تعداد نتایج: 2826398  

2005
W. Slominski H. Abramowicz A. Levy

An NLO photon parton parametrization is presented based on the existing F γ 2 measurements from e +e− data and the low-x proton structure function from ep interactions. Also included in the extraction of the NLO parton distribution functions are the dijets data coming from γp → j1+j2+X. The new parametrization is compared to other NLO parametrizations. TPJU – 2/2005 TAUP 2797-05 March 2005 e-ma...

2013
B. Abelev J. Adam D. Adamová A. M. Adare M. M. Aggarwal G. Aglieri Rinella M. Agnello A. G. Agocs A. Agostinelli Z. Ahammed N. Ahmad A. Ahmad Masoodi I. Ahmed S. A. Ahn S. U. Ahn I. Aimo S. Aiola M. Ajaz A. Akindinov D. Aleksandrov B. Alessandro D. Alexandre A. Alici A. Alkin J. Alme T. Alt V. Altini S. Altinpinar I. Altsybeev C. Alves Garcia Prado C. Andrei A. Andronic V. Anguelov J. Anielski T. Antičić F. Antinori P. Antonioli L. Aphecetche H. Appelshäuser N. Arbor S. Arcelli N. Armesto R. Arnaldi T. Aronsson I. C. Arsene M. Arslandok A. Augustinus R. Averbeck T. C. Awes J. Äystö M. D. Azmi M. Bach A. Badalà Y. W. Baek R. Bailhache R. Bala A. Baldisseri F. Baltasar Dos Santos Pedrosa J. Bán R. C. Baral R. Barbera F. Barile G. G. Barnaföldi L. S. Barnby V. Barret J. Bartke M. Basile N. Bastid S. Basu B. Bathen G. Batigne B. Batyunya P. C. Batzing C. Baumann I. G. Bearden H. Beck C. Bedda N. K. Behera I. Belikov F. Bellini R. Bellwied E. Belmont-Moreno G. Bencedi S. Beole I. Berceanu A. Bercuci Y. Berdnikov D. Berenyi A. A. E. Bergognon R. A. Bertens D. Berzano L. Betev A. Bhasin A. K. Bhati J. Bhom L. Bianchi N. Bianchi C. Bianchin J. Bielčík J. Bielčíková A. Bilandzic S. Bjelogrlic F. Blanco F. Blanco D. Blau C. Blume F. Bock A. Bogdanov H. Bøggild M. Bogolyubsky L. Boldizsár M. Bombara J. Book H. Borel A. Borissov J. Bornschein M. Botje E. Botta S. Böttger E. Braidot P. Braun-Munzinger M. Bregant T. Breitner T. A. Broker T. A. Browning M. Broz R. Brun E. Bruna G. E. Bruno D. Budnikov H. Buesching S. Bufalino P. Buncic O. Busch Z. Buthelezi D. Caffarri X. Cai H. Caines A. Caliva E. Calvo Villar P. Camerini V. Canoa Roman G. Cara Romeo F. Carena W. Carena F. Carminati A. Casanova Díaz J. Castillo Castellanos E. A. R. Casula V. Catanescu C. Cavicchioli C. Ceballos Sanchez J. Cepila P. Cerello B. Chang S. Chapeland J. L. Charvet S. Chattopadhyay S. Chattopadhyay M. Cherney C. Cheshkov B. Cheynis V. Chibante Barroso D. D. Chinellato P. Chochula M. Chojnacki S. Choudhury P. Christakoglou C. H. Christensen P. Christiansen T. Chujo S. U. Chung C. Cicalo L. Cifarelli F. Cindolo J. Cleymans F. Colamaria D. Colella A. Collu M. Colocci G. Conesa Balbastre Z. Conesa del Valle M. E. Connors G. Contin J. G. Contreras T. M. Cormier Y. Corrales Morales P. Cortese I. Cortés Maldonado M. R. Cosentino F. Costa P. Crochet R. Cruz Albino E. Cuautle L. Cunqueiro A. Dainese R. Dang A. Danu K. Das D. Das I. Das A. Dash S. Dash S. De H. Delagrange A. Deloff E. Dénes A. Deppman G. O. V. de Barros A. De Caro G. de Cataldo J. de Cuveland A. De Falco D. De Gruttola N. De Marco S. De Pasquale R. de Rooij M. A. Diaz Corchero T. Dietel R. Divià D. Di Bari C. Di Giglio S. Di Liberto A. Di Mauro P. Di Nezza Ø. Djuvsland A. Dobrin T. Dobrowolski B. Dönigus O. Dordic A. K. Dubey A. Dubla L. Ducroux P. Dupieux A. K. Dutta Majumdar G. D Erasmo D. Elia D. Emschermann H. Engel B. Erazmus H. A. Erdal D. Eschweiler B. Espagnon M. Estienne S. Esumi D. Evans S. Evdokimov G. Eyyubova D. Fabris J. Faivre D. Falchieri A. Fantoni M. Fasel D. Fehlker L. Feldkamp D. Felea A. Feliciello G. Feofilov A. Fernández Téllez E. G. Ferreiro A. Ferretti A. Festanti J. Figiel M. A. S. Figueredo S. Filchagin D. Finogeev F. M. Fionda E. M. Fiore E. Floratos M. Floris S. Foertsch P. Foka S. Fokin E. Fragiacomo A. Francescon U. Frankenfeld U. Fuchs C. Furget M. Fusco Girard J. J. Gaardhøje M. Gagliardi A. Gago M. Gallio D. R. Gangadharan P. Ganoti C. Garabatos E. Garcia-Solis C. Gargiulo I. Garishvili J. Gerhard M. Germain A. Gheata M. Gheata B. Ghidini P. Ghosh P. Gianotti P. Giubellino E. Gladysz-Dziadus P. Glässel L. Goerlich R. Gomez P. González-Zamora S. Gorbunov S. Gotovac L. K. Graczykowski R. Grajcarek A. Grelli C. Grigoras A. Grigoras V. Grigoriev A. Grigoryan S. Grigoryan B. Grinyov N. Grion J. F. Grosse-Oetringhaus J.-Y. Grossiord R. Grosso F. Guber R. Guernane B. Guerzoni M. Guilbaud K. Gulbrandsen H. Gulkanyan T. Gunji A. Gupta R. Gupta K. H. Khan R. Haake Ø. Haaland C. Hadjidakis M. Haiduc H. Hamagaki G. Hamar L. D. Hanratty A. Hansen J. W. Harris A. Harton D. Hatzifotiadou S. Hayashi A. Hayrapetyan S. T. Heckel M. Heide H. Helstrup A. Herghelegiu G. Herrera Corral N. Herrmann B. A. Hess K. F. Hetland B. Hicks B. Hippolyte Y. Hori P. Hristov I. Hřivnáčová M. Huang T. J. Humanic D. Hutter D. S. Hwang R. Ichou R. Ilkaev I. Ilkiv M. Inaba E. Incani G. M. Innocenti C. Ionita M. Ippolitov M. Irfan V. Ivanov M. Ivanov O. Ivanytskyi A. Jachołkowski C. Jahnke H. J. Jang M. A. Janik P. H. S. Y. Jayarathna S. Jena R. T. Jimenez Bustamante P. G. Jones H. Jung A. Jusko S. Kalcher P. Kaliňák T. Kalliokoski A. Kalweit J. H. Kang V. Kaplin S. Kar A. Karasu Uysal O. Karavichev T. Karavicheva E. Karpechev A. Kazantsev U. Kebschull R. Keidel B. Ketzer S. A. Khan M. M. Khan P. Khan A. Khanzadeev Y. Kharlov B. Kileng S. Kim D. W. Kim D. J. Kim B. Kim T. Kim M. Kim M. Kim J. S. Kim S. Kirsch I. Kisel S. Kiselev A. Kisiel G. Kiss J. L. Klay J. Klein C. Klein-Bösing A. Kluge M. L. Knichel A. G. Knospe M. K. Köhler T. Kollegger A. Kolojvari V. Kondratiev N. Kondratyeva A. Konevskikh V. Kovalenko M. Kowalski S. Kox G. Koyithatta Meethaleveedu J. Kral I. Králik F. Kramer A. Kravčáková M. Krelina M. Kretz M. Krivda F. Krizek M. Krus E. Kryshen M. Krzewicki V. Kucera Y. Kucheriaev T. Kugathasan C. Kuhn P. G. Kuijer I. Kulakov J. Kumar P. Kurashvili A. B. Kurepin A. Kurepin A. Kuryakin S. Kushpil V. Kushpil M. J. Kweon Y. Kwon P. Ladrón de Guevara C. Lagana Fernandes I. Lakomov R. Langoy C. Lara A. Lardeux S. L. La Pointe P. La Rocca R. Lea M. Lechman S. C. Lee G. R. Lee I. Legrand J. Lehnert R. C. Lemmon M. Lenhardt V. Lenti I. León Monzón P. Lévai S. Li J. Lien R. Lietava S. Lindal V. Lindenstruth C. Lippmann M. A. Lisa H. M. Ljunggren D. F. Lodato P. I. Loenne V. R. Loggins V. Loginov D. Lohner C. Loizides K. K. Loo X. Lopez E. López Torres G. Løvhøiden X.-G. Lu P. Luettig M. Lunardon J. Luo G. Luparello C. Luzzi P. M. Jacobs R. Ma

Differential cross sections of charged particles in inelastic pp collisions as a function of pT have been measured at [Formula: see text] at the LHC. The pT spectra are compared to NLO-pQCD calculations. Though the differential cross section for an individual [Formula: see text] cannot be described by NLO-pQCD, the relative increase of cross section with [Formula: see text] is in agreement with...

2008
Stefano Frixione Bryan R. Webber

This is the user’s manual of MC@NLO 3.4. This package is a practical implementation, based upon the HERWIG event generator, of the MC@NLO formalism, which allows one to incorporate NLO QCD matrix elements consistently into a parton shower framework. Processes available in this version include the hadroproduction of single vector and Higgs bosons, vector boson pairs, heavy quark pairs, single to...

2012
Hua Xing Zhu Chong Sheng Li Ding Yu Shao Jian Wang C.-P. Yuan

We present a theoretical framework for systematically calculating next-to-leading order (NLO) QCD effects to various experimental observables in models with massive COVB in a model independent way at hadron colliders. Specifically, we show the numerical results for the NLO QCD corrections to total cross sections, invariant mass distribution and AFB of top quark pairs production mediated by a ma...

2005
Stefano Frixione Bryan R. Webber

This is the user’s manual of MC@NLO 3.1. This package is a practical implementation, based upon the HERWIG event generator, of the MC@NLO formalism, which allows one to incorporate NLO QCD matrix elements consistently into a parton shower framework. Processes available in this version include the hadroproduction of single vector and Higgs bosons, vector boson pairs, heavy quark pairs, lepton pa...

2008
Stefano Frixione Bryan R. Webber

This is the user’s manual of MC@NLO 3.4. This package is a practical implementation, based upon the HERWIG event generator, of the MC@NLO formalism, which allows one to incorporate NLO QCD matrix elements consistently into a parton shower framework. Processes available in this version include the hadroproduction of single vector and Higgs bosons, vector boson pairs, heavy quark pairs, single to...

2005
V. S. Fadin R. Fiore

Details of the calculation of the non-forward BFKL kernel at next-to-leading order (NLO) are offered. Specifically we show the calculation of the two-gluon production contribution. This contribution was the last missing part of the kernel. Together with the NLO gluon Regge trajectory, the NLO contribution of one-gluon production and the contribution of quark-antiquark production which were foun...

2011
Oksana Nadtoka

The new photochromic polymers based on methacrylic azoesters were synthesized. The azobenzene side chains of obtained polymers contain different groups of both acceptor and donor nature as well as flexible alkyl spacer. The third order nonlinear optical susceptibilities (χ<3>) of the studied solutions were measured by degenerating four wave mixing (DFWM) method. As a result, the enhancement of ...

2012
Javier Adur Vitor B. Pelegati Andre A. de Thomaz Mariana O. Baratti Diogo B. Almeida L. A. L. A. Andrade Fátima Bottcher-Luiz Hernandes F. Carvalho Carlos L. Cesar

BACKGROUND Nonlinear optical (NLO) microscopy techniques have potential to improve the early detection of epithelial ovarian cancer. In this study we showed that multimodal NLO microscopies, including two-photon excitation fluorescence (TPEF), second-harmonic generation (SHG), third-harmonic generation (THG) and fluorescence lifetime imaging microscopy (FLIM) can detect morphological and metabo...

1998
Thomas R. Cundari Henry A. Kurtz Tie Zhou

Nonlinear optical (NLO) properties of transition metal complexes are studied using quantum chemical calculations. By comparison with all electron calculations, effective core potentials have been shown to be competent for the calculation of NLO properties as long as the valence basis sets are comparable. While overall the basis set effects are important for calculation of NLO properties, they a...

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