W. Kucewicz
Polish Academy of Sciences
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Featured researches published by W. Kucewicz.
Nuclear Physics | 2005
B. B. Back; M. D. Baker; M. Ballintijn; D.S. Barton; Bruce Becker; Russell Richard Betts; A. A. Bickley; R. Bindel; A. Budzanowski; Wit Busza; A. Carroll; Z. Chai; M.P. Decowski; E. García; T. Gburek; N. George; K. Gulbrandsen; S. Gushue; C. Halliwell; J. Hamblen; A.S. Harrington; M. Hauer; G.A. Heintzelman; C. Henderson; David Jonathan Hofman; R. S. Hollis; R. Holynski; Burt Holzman; A. Iordanova; E. Johnson
This paper describes the conclusions that can be drawn from the data taken thus far with the PHOBOS detector at RHIC. In the most central Au+Au collisions at the highest beam energy, evidence is found for the formation of a very high energy density system whose description in terms of simple hadronic degrees of freedom is inappropriate. Furthermore, the constituents of this novel system are found to undergo a significant level of interaction. The properties of particle production at RHIC energies are shown to follow a number of simple scaling behaviors, some of which continue trends found at lower energies or in simpler systems. As a function of centrality, the total number of charged particles scales with the number of participating nucleons. When comparing Au+Au at different centralities, the dependence of the yield on the number of participants at higher p T (∼4 GeV/c) is very similar to that at low transverse momentum. The measured values of charged particle pseudorapidity density and elliptic flow were found to be independent of energy over a broad range of pseudorapidities when effectively viewed in the rest frame of one of the colliding nuclei, a property we describe as “extended longitudinal scaling”. Finally, the centrality and energy dependences of several observables were found to factorize to a surprising degree.
Physical Review C | 2011
B. Alver; B. B. Back; M. D. Baker; M. Ballintijn; D.S. Barton; R. R. Betts; A. A. Bickley; R. Bindel; A. Budzanowski; W. Busza; A. Carroll; Z. Chai; V. Chetluru; M.P. Decowski; E. García; T. Gburek; N. George; K. Gulbrandsen; S. Gushue; C. Halliwell; J. Hamblen; G.A. Heintzelman; C. Henderson; D. J. Hofman; R. S. Hollis; R. Holynski; B. Holzman; A. Iordanova; E. Johnson; J.L. Kane
Pseudorapidity distributions of charged particles emitted in Au+Au, Cu+Cu, d+Au, and p+p collisions over a wide energy range have been measured using the PHOBOS detector at the BNL Relativistic Heavy-Ion Collider (RHIC). The centrality dependence of both the charged particle distributions and the multiplicity at midrapidity were measured. Pseudorapidity distributions of charged particles emitted with |{eta}|<5.4, which account for between 95% and 99% of the total charged-particle emission associated with collision participants, are presented for different collision centralities. Both the midrapidity density dN{sub ch}/d{eta} and the total charged-particle multiplicity N{sub ch} are found to factorize into a product of independent functions of collision energy, {radical}(s{sub N{sub N}}), and centrality given in terms of the number of nucleons participating in the collision, N{sub part}. The total charged particle multiplicity, observed in these experiments and those at lower energies, assumes a linear dependence of (lns{sub N{sub N}}){sup 2} over the full range of collision energy of {radical}(s{sub N{sub N}})=2.7-200 GeV.
Physical Review Letters | 2001
B. B. Back; W. Kucewicz; Andrzej Olszewski; A. Budzanowski; C. Halliwell; L. Rosenberg; P. Steinberg; M. Reuter; W. Skulski; J.-L. Tang; K. W. Wozniak; C. Henderson; Willis Lin; B. Wyslouch; E. Garcia; C. Reed; I.C. Park; G. van Nieuwenhuizen; A. H. Wuosmaa; Baker; Burt Holzman; C. Vale; G. S. F. Stephans; S. Manly; R. R. Betts; R. Verdier; G.A. Heintzelman; D.S. Barton; P. Sarin; A. Carroll
The charged-particle pseudorapidity density dN(ch)/d eta has been measured for Au+Au collisions at sqrt[s(NN)] = 130 GeV at RHIC, using the PHOBOS apparatus. The total number of charged particles produced for the 3% most-central Au+Au collisions for /eta/<or=5.4 is found to be 4200+/-470. The evolution of dN(ch)/d eta with centrality is discussed, and compared to model calculations and to data from proton-induced collisions. The data show an enhancement in charged-particle production at midrapidity, while in the fragmentation regions, the results are consistent with expectations from pp and pA scattering.
Physical Review C | 2005
B. B. Back; W. Kucewicz; A. Iordanova; A. Budzanowski; C. Halliwell; Andrzej Olszewski; L. Rosenberg; P. Steinberg; M. Reuter; W. Skulski; J.-L. Tang; K. Wozniak; C. Henderson; Willis Lin; B. Wyslouch; E. García; C. Reed; A. A. Bickley; M. Nguyen; G. van Nieuwenhuizen; Baker; I.C. Park; G. S. F. Stephans; S. Manly; R.R. Betts; M. Ballintijn; R. Verdier; Marguerite Tonjes; G.A. Heintzelman; D.S. Barton
This paper describes the measurement of elliptic flow for charged particles in Au+Au collisions at sqrt(sNN)=200 GeV using the PHOBOS detector at the Relativistic Heavy Ion Collider (RHIC). The measured azimuthal anisotropy is presented over a wide range of pseudorapidity for three broad collision centrality classes for the first time at this energy. Two distinct methods of extracting the flow signal were used in order to reduce systematic uncertainties. The elliptic flow falls sharply with increasing eta at 200 GeV for all the centralities studied, as observed for minimum-bias collisions at sqrt(sNN)=130 GeV.
Physical Review Letters | 2002
B. B. Back; W. Kucewicz; A. Iordanova; A. Budzanowski; C. Halliwell; A. Olszewski; L. Rosenberg; P. Steinberg; M. Reuter; W. Skulski; J.-L. Tang; G. Roland; C. Henderson; Willis Lin; B. Wyslouch; E. García; C. Reed; I.C. Park; G. van Nieuwenhuizen; K. Wozniak; Baker; B. Holzman; C. Vale; R. Teng; G.S.F. Stephans; S. Manly; R. R. Betts; R. Verdier; D.S. Barton; P. Sarin
This paper describes the measurement of collective flow for charged particles in Au+Au collisions at sqrt{s_NN}} = 130 GeV using the PHOBOS detector at the Relativistic Heavy Ion Collider (RHIC). An azimuthal anisotropy is observed in the charged particle hit distribution in the PHOBOS multiplicity detector. This anisotropy is presented over a wide range of pseudorapidity (eta) for the first time at this energy. The size of the anisotropy (v_{2}) is thought to probe the degree of equilibration achieved in these collisions. The result here,averaged over momenta and particle species, is observed to reach 7% for peripheral collisions at mid-rapidity, falling off with centrality and increasing |eta|. Data are presented as a function of centrality for |eta|<1.0 and as a function of eta, averaged over centrality, in the angular region -5.0<eta<5.3. These results call into question the common assumption of longitudinal boost invariance over a large region of rapidity in RHIC collisions.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993
N. Bingefors; H. Borner; R. Boulter; M. Caccia; V. Chabaud; H. Dijkstra; P. Eerola; E. Gross; R. Horisberger; L. Hubbeling; B. Hyams; M. Karlsson; G. Maehlum; K. Ratz; I. Roditi; J. Straver; W. Trischuk; P. Weilhammer; Y. Dufour; P. Bruckman; Pawel Jalocha; P. Kapusta; M. Turala; A. Zalewska; J. Lindgren; R. Orava; K. Osterberg; C. Ronnqvist; H. Saarikko; J.P. Saarikko
The DELPHI Microvertex detector, which has been in operation since the start of the 1990 LEP run, consists of three layers of silicon microstrip detectors at average radii of 6.3, 9.0 and 11.0 cm. The 73728 readout strips, oriented along the beam, have a total active area of 0.42 m2. The strip pitch is 25 μm and every other strip is read out by low power charge amplifiers, giving a signal to noise ratio of 15:1 for minimum ionizing particles. On-line zero suppression results in an average data size of 4 kbyte for Z0 events. After a mechanical survey and an alignment with tracks, the impact parameter uncertainty as determined from hadronic Z0 decays is well described by (69pt)2 + 242 μm, with pt in GeV/c. For the 45 GeV/c tracks from Z0 → μ− decays we find an uncertainty of 21 μm for the impact parameter, which corresponds to a precision of 8 μm per point. The stability during the run is monitored using light spots and capacitive probes. An analysis of tracks through sector overlaps provides an additional check of the stability. The same analysis also results in a value of 6 μm for the intrinsic precision of the detector.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
V. Chabaud; P. Collins; H. Dijkstra; J. J. Gomez Y Cadenas; R. Keranen; S. Masciocchi; W. Trischuk; P. Weilhammer; Y. Dufour; R. Brenner; R. Orava; K. Osterberg; C. Ronnqvist; H. Saarikko; J.P. Saarikko; T. Tuuva; M. Voutilainen; J. Blocki; P. Bruckman; J. Godlewski; Pawel Jalocha; W. Kucewicz; H. Palka; A. Zalewska; B. Bouquet; F. Couchot; B. D'Almagne; F. Fulda-Quenzer; P. Rebecchi; Phillip Allport
The silicon strip microvertex detector of the DELPHI experiment at the CERN LEP collider has been recently upgraded from two coordinates (RΦ only) to three coordinates reconstruction (RΦ and z). The new Microvertex detector consists of 125 952 readout channels, and uses novel techniques to obtain the third coordinate. These include the use of AC coupled double sided silicon detectors with strips orthogonal to each other on opposite sides of the detector wafer. The routing of signals from the z strips to the end of the detector modules is done with a second metal layer on the detector surface, thus keeping the material in the sensitive area to a minimum. Pairs of wafers are daisy chained, with the wafers within each pair flipped with respect to each other in order to minimize the load capacitance on the readout amplifiers. The design of the detector and its various components are described. Results on the performance of the new detector are presented, with special emphasis on alignment, intrinsic precision and impact parameter resolution. The new detector has been taking data since spring of 1994, performing up to design specifications.
Physics Letters B | 2004
B. B. Back; M. D. Baker; D.S. Barton; R. R. Betts; M. Ballintijn; A. A. Bickley; R. Bindel; A. Budzanowski; W. Busza; A. Carroll; M.P. Decowski; E. García; N. George; K. Gulbrandsen; S. Gushue; C. Halliwell; J. Hamblen; G.A. Heintzelman; C. Henderson; D. J. Hofman; R. S. Hollis; R. Holynski; B. Holzman; A. Iordanova; E. Johnson; J.L. Kane; J. Katzy; N. Khan; W. Kucewicz; P. Kulinich
We present transverse momentum distributions of charged hadrons produced in Au+Au collisions at sqrt(s_NN) = 200 GeV. The spectra were measured for transverse momenta p_T from 0.25 to 4.5 GeV/c in a rapidity range of 0.2 < y_pi < 1.4. The evolution of the spectra is studied as a function of collision centrality, from 65 to 344 participating nucleons. The results are compared to data from proton-antiproton collisions and Au+Au collisions at lower RHIC energies. We find a significant change of the spectral shape between proton-antiproton and peripheral Au+Au collisions. Comparing peripheral to central Au+Au collisions, we find that the yields at high p_T exhibit approximate scaling with the number of participating nucleons, rather than scaling with the number of binary collisions.
Physical Review C | 2004
B. B. Back; M. D. Baker; M. Ballintijn; D.S. Barton; R. R. Betts; A. A. Bickley; R. Bindel; A. Budzanowski; W. Busza; A. Carroll; M.P. Decowski; E. García; N. George; K. Gulbrandsen; S. Gushue; C. Halliwell; J. Hamblen; G.A. Heintzelman; C. Henderson; D. J. Hofman; R. S. Hollis; R. Holynski; B. Holzman; A. Iordanova; E. Johnson; J.L. Kane; J. Katzy; N. Khan; W. Kucewicz; P. Kulinich
The centrality dependence of the midrapidity charged particle multiplicity in Au+Au collisions at sqrt(s_NN) = 19.6 and 200 GeV is presented. Within a simple model, the fraction of hard (scaling with number of binary collisions) to soft (scaling with number of participant pairs) interactions is consistent with a value of x = 0.13 +/- 0.01(stat) +/- 0.05(syst) at both energies. The experimental results at both energies, scaled by inelastic p(pbar)+p collision data, agree within systematic errors. The ratio of the data was found not to depend on centrality over the studied range and yields a simple linear scale factor of R_(200/19.6) = 2.03 +/- 0.02(stat) +/- 0.05(syst).
Physical Review Letters | 2003
B. B. Back; M. D. Baker; D.S. Barton; R. R. Betts; M. Ballintijn; A. A. Bickley; R. Bindel; A. Budzanowski; W. Busza; A. Carroll; M.P. Decowski; E. García; N. George; K. Gulbrandsen; S. Gushue; C. Halliwell; J. Hamblen; G.A. Heintzelman; C. Henderson; D. J. Hofman; R. S. Hollis; R. Holynski; B. Holzman; A. Iordanova; E. Johnson; J.L. Kane; J. Katzy; N. Khan; W. Kucewicz; P. Kulinich
We have measured the ratios of antiparticles to particles for charged pions, kaons, and protons near mid-rapidity in central Au+Au collisions at sqrt[s(NN)] = 130 GeV. We observe / = 1.00+/-0.01(stat)+/-0.02(syst), / = 0.91+/-0.07(stat)+/-0.06(syst), and / = 0.60+/-0.04(stat)+/-0.06(syst). The / and / ratios give a consistent estimate of the baryo-chemical potential mu(B) of 45 MeV, a factor of 5-6 smaller than in central Pb+Pb collisions at sqrt[s(NN)] = 17.2 GeV.