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Cross sections for e(+)p neutral current deep inelastic scattering have been measured at a center-of-mass energy of roots=318 GeV with the ZEUS detector at HERA using an integrated luminosity of 63.2 pb(-1). The double-differential cross section, d(2)sigma/dxdQ(2), is presented for 200 GeV(2)<Q(2)<30 000 GeV(2) and for 0.005<x<0.65. The single-differential cross sections dsigma/dQ(2), dsigma/dx and dsigma/dy are presented for Q(2)>200 GeV(2). The effect of Z-boson-exchange is seen in dsigma/dx measured for Q(2)>10 000 GeV(2). The data presented here were combined with ZEUS e(+)p neutral current data taken at roots=300 GeV and the structure function F(2)(em) was extracted. All results agree well with the predictions of the Standard Model.
Cross sections for e(+)p neutral current deep inelastic scattering have been measured at a center-of-mass energy of roots=318 GeV with the ZEUS detector at HERA using an integrated luminosity of 63.2 pb(-1). The double-differential cross section, d(2)sigma/dxdQ(2), is presented for 200 GeV(2)<Q(2)<30 000 GeV(2) and for 0.005<x<0.65. The single-differential cross sections dsigma/dQ(2), dsigma/dx and dsigma/dy are presented for Q(2)>200 GeV(2). The effect of Z-boson-exchange is seen in dsigma/dx measured for Q(2)>10 000 GeV(2). The data presented here were combined with ZEUS e(+)p neutral current data taken at roots=300 GeV and the structure function F(2)(em) was extracted. All results agree well with the predictions of the Standard Model.
Cross sections for e(+)p neutral current deep inelastic scattering have been measured at a center-of-mass energy of roots=318 GeV with the ZEUS detector at HERA using an integrated luminosity of 63.2 pb(-1). The double-differential cross section, d(2)sigma/dxdQ(2), is presented for 200 GeV2<Q(2)<30 000 GeV2 and for 0.005<x<0.65. The single-differential cross sections dsigma/dQ(2), dsigma/dx and dsigma/dy are presented for Q(2)>200 GeV2. The effect of Z-boson-exchange is seen in dsigma/dx measured for Q(2)>10 000 GeV2. The data presented here were combined with ZEUS e(+)p neutral current data taken at roots=300 GeV and the structure function F-2(em) was extracted. All results agree well with the predictions of the Standard Model. RI De Pasquale, Salvatore/B-9165-2008; Wing, Matthew/C-2169-2008; Doyle, Anthony/C-5889-2009; collins-tooth, christopher/A-9201-2012; Ferrando, James/A-9192-2012; Gladilin, Leonid/B-5226-2011; Golubkov, Yury/E-1643-2012
High-Q(2) neutral current cross sections in e(+)p deep inelastic scattering at root s=318 GeV
Cross sections for e(+)p neutral current deep inelastic scattering have been measured at a center-of-mass energy of roots=318 GeV with the ZEUS detector at HERA using an integrated luminosity of 63.2 pb(-1). The double-differential cross section, d(2)sigma/dxdQ(2), is presented for 200 GeV(2)200 GeV(2). The effect of Z-boson-exchange is seen in dsigma/dx measured for Q(2)>10 000 GeV(2). The data presented here were combined with ZEUS e(+)p neutral current data taken at roots=300 GeV and the structure function F(2)(em) was extracted. All results agree well with the predictions of the Standard Model.
Cross sections for e(+)p neutral current deep inelastic scattering have been measured at a center-of-mass energy of roots=318 GeV with the ZEUS detector at HERA using an integrated luminosity of 63.2 pb(-1). The double-differential cross section, d(2)sigma/dxdQ(2), is presented for 200 GeV(2)<Q(2)<30 000 GeV(2) and for 0.005<x<0.65. The single-differential cross sections dsigma/dQ(2), dsigma/dx and dsigma/dy are presented for Q(2)>200 GeV(2). The effect of Z-boson-exchange is seen in dsigma/dx measured for Q(2)>10 000 GeV(2). The data presented here were combined with ZEUS e(+)p neutral current data taken at roots=300 GeV and the structure function F(2)(em) was extracted. All results agree well with the predictions of the Standard Model.
Cross sections for e(+)p neutral current deep inelastic scattering have been measured at a center-of-mass energy of roots=318 GeV with the ZEUS detector at HERA using an integrated luminosity of 63.2 pb(-1). The double-differential cross section, d(2)sigma/dxdQ(2), is presented for 200 GeV2<Q(2)<30 000 GeV2 and for 0.005<x<0.65. The single-differential cross sections dsigma/dQ(2), dsigma/dx and dsigma/dy are presented for Q(2)>200 GeV2. The effect of Z-boson-exchange is seen in dsigma/dx measured for Q(2)>10 000 GeV2. The data presented here were combined with ZEUS e(+)p neutral current data taken at roots=300 GeV and the structure function F-2(em) was extracted. All results agree well with the predictions of the Standard Model. RI De Pasquale, Salvatore/B-9165-2008; Wing, Matthew/C-2169-2008; Doyle, Anthony/C-5889-2009; collins-tooth, christopher/A-9201-2012; Ferrando, James/A-9192-2012; Gladilin, Leonid/B-5226-2011; Golubkov, Yury/E-1643-2012
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.11770/144360
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.
