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Dive into the research topics where C. Del Papa is active.

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Featured researches published by C. Del Papa.


Physics Letters B | 1992

A measurement of σtot (γp) at √s=210 GeV

M. Derrick; D. Krakauer; S. Magill; B. Musgrave; J. Repond; K. Sugano; R. W. Stanek; R. L. Talaga; J. L. Thron; F. Arzarello; R. Ayed; G. Barbagli; G. Bari; M. Basile; L. Bellagamba; D. Boscherini; G. Bruni; P. Bruni; Gc Romeo; G. Castellini; M. Chiarini; L. Cifarelli; F. Cindolo; F. Ciralli; A. Contin; S. D'Auria; C. Del Papa; F. Frasconi; P. Giusti; G. Iacobucci

Abstract The total photoproduction cross section is determined from a measurement of electroproduction with the ZEUS detector at HERA. The Q 2 values of the virtual photons are in the range 10 −7 Q 2 −2 GeV 2 . The γp total cross section in the γp centre of mass energy range 186–233 GeV is 154 ± 16 (stat.) ± 32 (syst.) μ b.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2001

The ATLAS Silicon Pixel Sensors

M. S. Alam; A. Ciocio; K. Einsweiler; J. Emes; M. Gilchriese; A Joshi; S. Kleinfelder; R. Marchesini; F McCormack; O Milgrome; N Palaio; F Pengg; J. Richardson; G. Zizka; M. Ackers; A Andreazza; G. Comes; P. Fischer; M. Keil; V Klasen; T Kuhl; S. Meuser; W. Ockenfels; B. Raith; J. Treis; N. Wermes; C. Gößling; F. Hügging; J. Wüstenfeld; R. Wunstorf

Prototype sensors for the ATLAS silicon pixel detector have been developed. The design of the sensors is guided by the need to operate them in the severe LHC radiation environment at up to several hundred volts while maintaining a good signal-to-noise ratio, small cell size, and minimal multiple scattering. The ability to be operated under full bias for electrical characterization prior to attachment of the readout integrated circuit electronics is also desired.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995

Performance of a new ohmic contact for GaAs particle detectors

M. Alietti; C. Canali; A. Castaldini; A. Cavallini; A. Cetronio; C. Chiossi; S. D'Auria; C. Del Papa; C. Lanzieri; F. Nava; P. Vanni

Abstract In recent papers, we have investigated, within the context of the RD-8 experiment, the behaviour as a function of bias of the active region of particle detectors made by Alenia SpA on semi-insulating liquid encapsulated Czochralski gallium arsenide: the active region width depends linearly on the bias voltage. The diodes were found to break down as soon as the field reached the back ohmic contact. This suggested that the ohmic contact was injecting holes into the diode, therefore we have decided to develop a new, non-injecting, non-alloyed ohmic contact. This new contact allows us to go far beyond, five times, the voltage bias necessary to have a fully active detector. The higher voltage reached by the detectors helps us improve the charge collection efficiency, up to more than 95% for alphas and more than 90% for beta (mips) particles and X-rays, giving a more stable operation of the detectors. For the first time we can explore the characteristics of a GaAs detector beyond the voltage needed for it to be completely active.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1990

A preliminary study of GaAs solid-state detectors for high-energy physics

R. Bertin; S. D'Auria; C. Del Papa; F. Fiori; B. Lisowski; V. O'Shea; P.G. Pelfer; K. M. Smith; A. Zichichi

Abstract The first phase of a study of GaAs as a base material for solid-state detectors has been completed. The main motivation behind this study is the greater radiation resistance of integrated circuits made of GaAs (compared with Si). Many diodes, of different sizes and shapes but built with the same technique, have been tested electrically and as detectors, using α sources and minimum-ionizing particles. The tests show that these devices work with a full detection effeciency, although there is evidence for trapping of a fraction of the charge produced by the particle inside the semiconductor.


Physics Letters B | 1978

A measurement of inclusive π0 production at large pT from p-p collisions at the CERN ISR

A.L.S. Angelis; B.J. Blumenfeld; L. Camilleri; T. J. Chapin; R. L. Cool; C. Del Papa; L. Di Lella; Z. Dimcovski; R. J. Hollebeek; L.M. Lederman; D.A. Levinthal; J. T. Linnemann; L. Lyons; N. Phinney; B.G. Pope; Stephen H. Pordes; A.F. Rothenberg; A. M. Segar; J. Singh-Sidhu; A. M. Smith; M. J. Tannenbaum; R. A. Vidal; J.S. Wallace-Hadrill; T.O. White; J. M. Yelton

Abstract The inclusive cross section for larger p T π 0 production near 90° in p-p collisions at the CERN ISR is presented for centre-of-mass energies 30.7, 53.1 and 62.4 GeV. The data are inconsistent with scaling of the form p T − n F ( x T ), with constant n or with n allowed to depend on x T = 2p T / s . For s = 53.1 and 62.4 GeV , the value of n found for 3.5 p T c is n = 8.0 ± 0.5, in agreement with previous experiments. However, for 7.5 p T c the value becomes n = 5.1 ± 0.4.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002

A measurement of Lorentz angle and spatial resolution of radiation hard silicon pixel sensors

I. Gorelov; Grant Gorfine; M. R. Hoeferkamp; S. Seidel; A. Ciocio; K. Einsweiler; M. Gilchriese; A Joshi; S. Kleinfelder; R. Marchesini; O Milgrome; N Palaio; F Pengg; J. Richardson; G. Zizka; M. Ackers; P. Fischer; M. Keil; S. Meuser; T. Stockmanns; J. Treis; N. Wermes; C. Gößling; F. Hügging; J. Wüstenfeld; R. Wunstorf; Dario Barberis; R. Beccherle; M. Cervetto; Giovanni Darbo

Silicon pixel sensors developed by the ATLAS collaboration to meet LHC requirements and to withstand hadronic irradiation to fluences of up to


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992

GaAs solid state detectors for particle physics

S.P. Beaumont; R. Bertin; C.N. Booth; C. Buttar; L. Carraresi; F. Cindolo; M. Colocci; F. Combley; S. D'Auria; C. Del Papa; M. Dogru; M. Edwards; F. Fiori; F. Foster; A. Francescato; Y. Hou; P.A. Houston; B.K. Jones; J.G. Lynch; B. Lisowski; J. Matheson; F. Nava; M. Nuti; V. O'Shea; P.G. Pelfer; C. Raine; J. Santana; I.J. Saunders; P. Seller; P.H. Sharp

10^{15} n_eq/cm^{2}


Physics Letters B | 1978

A Measurement of Inclusive pi0 Production at Large p(T) from p p Collisions at the CERN ISR

Aris L S Angelis; R. J. Hollebeek; T.O. White; D. A. Levinthal; T. J. Chapin; James Linnemann; A. M. Smith; Leon M. Lederman; R. A. Vidal; J. M. Yelton; C. Del Papa; S. Pordes; N. Phinney; L. Camilleri; A. Rothenberg; Z. Dimcovski; B. G. Pope; L. Di Lella; R. L. Cool; L. Lyons; J.S. Wallace-Hadrill; Barry Blumenfeld; Michael J. Tannenbaum; A. M. Segar; J. Singh-Sidhu

have been evaluated using a test beam facility at CERN providing a magnetic field. The Lorentz angle was measured and found to alter from 9.0 deg. before irradiation, when the detectors operated at 150 V bias at B=1.48 T, to 3.1 deg after irradiation and operating at 600 V bias at 1.01 T. In addition to the effect due to magnetic field variation, this change is explained by the variation of the electric field inside the detectors arising from the different bias conditions. The depletion depths of irradiated sensors at various bias voltages were also measured. At 600 V bias 280 micron thick sensors depleted to ~200 micron after irradiation at the design fluence of 1 10^{15} 1 MeV n_eq/cm2 and were almost fully depleted at a fluence of 0.5 * 10^{15} 1 MeV n_eq/cm2. The spatial resolution was measured for angles of incidence between 0 deg and 30 deg. The optimal value was found to be better than 5.3 micron before irradiation and 7.4 micron after irradiation.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1991

The ZEUS vertex detector: Design and prototype test

C. Alvisi; G. Anzivino; F. Arzarello; G. Barbagli; G. Bari; M. Basile; L. Bellagamba; D. Boscherini; G. Bruni; P. Bruni; U. Camerini; G. Cara Romeo; G. Castellini; M. Chiarini; L. Cifarelli; F. Cindolo; F. Ciralli; A. Contin; M. Costa; S. D'Auria; C. Del Papa; S. De Pasquale; F. Fiori; A. Forte; F. Frasconi; P. Giusti; G. Iacobucci; G. Laurenti; B. Lisowski; G. Maccarrone

Abstract We report on progress with Schottky diode and p-i-n diode GaAs detectors for minimum ionising particles. The radiation hardness and potential speed of simple diodes is shown to be more than competitive with silicon detector. A discussion is given of the present understanding of the charge transport mechanism in the detectors since it influences their charge collection efficiency. Early results from microstrip detectors are also described.


Physics Letters B | 1979

A measurement of the production of massive e+e− pairs in proton-proton collisions at √s = 62.4 GeV

A.L.S. Angelis; H. J. Besch; B.J. Blumenfeld; L. Camilleri; T.J. Chapin; R.L. Cool; C. Del Papa; L. Di Lella; Z. Dimčovski; R. J. Hollebeek; L.M. Lederman; D.A. Levinthal; J.T. Linnemann; C. B. Newman; N. Phinney; B.G. Pope; Stephen H. Pordes; A. Rothenberg; R. W. Rusack; A. M. Segar; J. Singh-Sidhu; A. M. Smith; M.J. Tannenbaum; R. A. Vidal; J.S. Wallace-Hadrill; J. M. Yelton; K. K. Young

Abstract The inclusive cross section for larger p T π 0 production near 90° in p-p collisions at the CERN ISR is presented for centre-of-mass energies 30.7, 53.1 and 62.4 GeV. The data are inconsistent with scaling of the form p T − n F ( x T ), with constant n or with n allowed to depend on x T = 2p T / s . For s = 53.1 and 62.4 GeV , the value of n found for 3.5 p T c is n = 8.0 ± 0.5, in agreement with previous experiments. However, for 7.5 p T c the value becomes n = 5.1 ± 0.4.

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A. Contin

University of Bologna

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M. Basile

University of Bologna

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R. Nania

Wayne State University

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P. Giusti

University of Bologna

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F. Cindolo

Austrian Academy of Sciences

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D. E. Dorfan

University of California

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