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Dive into the research topics where Dieter Roehrich is active.

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Featured researches published by Dieter Roehrich.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000

The STAR level-3 trigger system

C. Adler; J. Berger; M. DeMello; T. Dietel; D. Flierl; J. M. Landgraf; J. S. Lange; M. J. Levine; A. Ljubicic; J. M. Nelson; Dieter Roehrich; R. Stock; C. Struck; P. Yepes

Abstract The STAR Level-3 trigger issues a trigger decision upon a complete online reconstruction of Au+Au collisions at relativistic heavy ion collider energies. Central interactions are processed up to a rate of 50 s −1 including a simple analysis of physics observables. The setup of the processor farm and the event reconstruction as well as experiences and the proposed trigger algorithms are described.


Physical Review C | 2002

System, centrality, and transverse mass dependence of two-pion correlation radii in heavy ion collisions at 11.6A and 14.6A GeV/c

L. Ahle; Y. Akiba; K. Ashktorab; M. D. Baker; D. R. Beavis; P. Beery; H.C. Britt; B. Budick; J. Chang; C. Chasman; Z. Chen; C. Y. Chi; Y.Y. Chu; V. Cianciolo; B. A. Cole; J. Costales; H. J. Crawford; J. B. Cumming; R. Debbe; J. C. Dunlop; W. Eldredge; J. Engelage; S. Y. Fung; E. Garcia; M. Gonin; S. Gushue; H. Hamagaki; L. F. Hansen; R. Hayano; S. Hayashi

Two-pion correlation functions are analyzed at mid-rapidity for three systems (14.6 A-GeV Si+Al, Si+Au, and 11.6 A-GeV Au+Au), seven distinct centrality conditions, and different kT bins in the range 0.1--0.5 GeV/c. Source reference frames are determined from fits to the Yano-Koonin source parameterization. Bertsch-Pratt radius parameters are shown to scale linearly with both number of projectile and total participants as obtained from a Glauber model calculation. A finite emission duration that increases linearly with system/centrality is also reported. The mT dependence of the Bertsch-Pratt radii is measured for the central Si+Au and Au+Au systems. The system/centrality dependence is investigated separately for both high and low mT regions.


Physical Review Letters | 1996

Production of phi mesons in central 28Si+196Au collisions at 14.6A GeV/c.

Y. Akiba; D. R. Beavis; P. Beery; H.C. Britt; B. Budick; C. Chasman; Z. Chen; C. Y. Chi; Y.Y. Chu; Cianciolo; B. A. Cole; J.B. Costales; H. J. Crawford; J.B. Cumming; R. Debbe; J. Engelage; S. Y. Fung; M. Gonin; S. Gushue; H. Hamagaki; O. Hansen; R. Hayano; S. Hayashi; S. Homma; H. Kaneko; J. H. Kang; S. Kaufman; W. L. Kehoe; K. Kurita; R.J. Ledoux

Production of the {phi} meson in central Si+Au collisions has been measured by E859 at the Brookhaven Alternating Gradient Synchrotron by selecting events with identified K{sup +}K{sup -} pairs. The mass and width of the {phi}, obtained from the invariant mass distribution of kaon pairs, are consistent with those of free f mesons. The transverse mass and rapidity distributions are presented. The inverse slope parameter for an exponential fit to the invariant transverse mass distribution is 179{+-}10{+-}17 MeV.


Physical Review Letters | 1994

Transverse Energy Production in {sup 208}Pb+Pb Collisions at 158 GeV per Nucleon

T. Alber; H. Appelshaeuser; J. Baechler; J. Bartke; H. Bialkowska; F. Bieser; Bloomer; C. O. Blyth; R. Bock; C. Bormann; F.P. Brady; R. Brockmann; P. Buncic; H.L. Caines; D. Cebra; P. Chan; G.E. Cooper; J. G. Cramer; P.B. Cramer; P. Csato; I. Derado; J. Dunn; V. Eckardt; F. Eckhardt; S. Euler; M.I. Ferguson; H.G. Fischer; Z. Fodor; P. Foka; P. Freund

Author(s): Margetis, S.; Alber, T.; Appelshauser, H.; Bachler, J.; Bartke, J.; Bialkowska, H.; Bieser, F.; Bloomer, M.A.; Blyth, C.O.; Bock, R.; Bormann, C.; Brady, F.P.; Brockmann, R.; Buncic, P.; Caines, H.L.; Cebra, D.; Chan, P.; Cooper, G.E.; Cramer, J.G.; Cramer, P.B.; Csato, P.; Derado, I.; Dunn, J.; Eckardt, V.; Eckhardt, F.; Euler, S.; Ferguson, M.I.; Fischer, H.G.; Fodor, Z.; Foka, P.; Freund, P.; Fuchs, M.; Gal, J.; Gasdzicki, M.; Gladysz, E.; Grebieszkow, J.; Gunther, J.; Harris, J.W.; Heck, W.; Hegyi, S.; Hill, L.A.; Huang, I.; Howe, M.A.; Igo, G.; Irmscher, D.; Jacobs, P.; Jones, P.G.; Kadija, K.; Kecskemeti, J.; Kowalski, M.; Kuhmichel, A.; Lsdiuk, B.; Margetis, S.; Mitchell, J.W.; Mock, A.; Nelson, J.M.; Odyniec, G.J.; Palinkas, J.; Palla, G.; Panagiotou, A.D.; Petridis, A.; Piper, A.; Poskanzer, A.M.; Prindle, D.J.; Puhlhofer, F.; Rauch, W.; Renfordt, R.; Retyk, W.; Ritter, Hans G.; Rohrich, D.; Rudolph, H.; Runge, K.; Sandoval, A.; Sann, H.; Schafer, E.; Schmitz, N.; Schonfelder, S.; Seyboth, P.; Seyerlein, J.; Sikler, F.; Skrzypczak, E.; Stock, R.; Stroebele, H.; Szentpetery, I.; Sziklai, J.


Contrast Media & Molecular Imaging | 2015

Multimodal approach to assess tumour vasculature and potential treatment effect with DCE-US and DCE-MRI quantification in CWR22 prostate tumour xenografts

Natalia Arteaga-Marrero; Cecilie Brekke Rygh; Jose Francisco Mainou-Gomez; Kim Nylund; Dieter Roehrich; J Heggdal; P Matulaniec; Odd Helge Gilja; Rolf K. Reed; Lena Svensson; Nataliya Lutay; Dag Rune Olsen

The aim of this study was to compare intratumoural heterogeneity and longitudinal changes assessed by dynamic contrast-enhanced ultrasound (DCE-US) and dynamic contrast-enhanced magnetic resonance imaging (DCE-MRI) in prostate tumour xenografts. In vivo DCE-US and DCE-MRI were obtained 24 h pre- (day 0) and post- (day 2) radiation treatment with a single dose of 7.5 Gy. Characterization of the tumour vasculature was determined by Brix pharmacokinetic analysis of the time-intensity curves. Histogram analysis of voxels showed significant changes (p < 0.001) from day 0 to day 2 in both modalities for kep , the exchange rate constant from the extracellular extravascular space to the plasma, and kel , the elimination rate constant of the contrast. In addition, kep and kel values from DCE-US were significantly higher than those derived from DCE-MRI at day 0 (p < 0.0001) for both groups. At day 2, kel followed the same tendency for both groups, whereas kep showed this tendency only for the treated group in intermediate-enhancement regions. Regarding kep median values, longitudinal changes were not found for any modality. However, at day 2, kep linked to DCE-US was correlated to MVD in high-enhancement areas for the treated group (p = 0.05). In contrast, correlation to necrosis was detected for the control group in intermediate-enhancement areas (p < 0.1). Intratumoural heterogeneity and longitudinal changes in tumour vasculature were assessed for both modalities. Microvascular parameters derived from DCE-US seem to provide reliable biomarkers during radiotherapy as validated by histology. Furthermore, DCE-US could be a stand-alone or a complementary technique.


Proceedings of 9th International Conference on Large Scale Applications and Radiation Hardness of Semiconductor Detectors — PoS(RD09) | 2010

Radiation tolerance of an SRAM based FPGA used in a large tracking detector

K. Røed; J. Alme; D. Fehlker; M. Richter; K. Ullaland; H. Helstrup; Dieter Roehrich

A reconfiguration solution has been implemented in order to correct Single Event Upsets (SEUs) in the configuration memory of an FPGA. This FPGA is in charge of data readout of a large tracking detector and will operate in a radiation exposed environment. It is therefore important to reduce the probability of experiencing functional failures caused by SEUs. Correct implementation of the reconfiguration solution is validated by irradiation and fault injection tests. The results of these tests are presented along with tests that show how this solution can be combined with an additional mitigation approach to effectively reduce the functional failure rate.


Acta Radiologica | 2018

Radiation treatment monitoring with DCE-US in CWR22 prostate tumor xenografts

Natalia Arteaga-Marrero; Jose Francisco Mainou-Gomez; Cecilie Brekke Rygh; Nataliya Lutay; Dieter Roehrich; Rolf K. Reed; Dag Rune Olsen

Background Longitudinal monitoring of potential radiotherapy treatment effects can be determined by dynamic contrast-enhanced ultrasound (DCE-US). Purpose To assess functional parameters by means of DCE-US in a murine subcutaneous model of human prostate cancer, and their relationship to dose deposition and time-frame after treatment. A special focus has been placed to evaluate the vascular heterogeneity of the tumor and on the most suitable data analysis approach that reflects this heterogeneity. Material and Methods In vivo DCE-US was acquired 24 h and 48 h after radiation treatment with a single dose of 7.5 Gy and 10 Gy, respectively. Tumor vasculature was characterized pixelwise using the Brix pharmacokinetic analysis of the time-intensity curves. Results Longitudinal changes were detected (P < 0.001) at 24 h and 48 h after treatment. At 48 h, the eliminating rate constant of the contrast agent from the plasma, kel, was correlated (P ≤ 0.05) positively with microvessel density (MVD; rτ = 0.7) and negatively with necrosis (rτ = –0.6) for the treated group. Furthermore, Akep, a parameter related to transcapillary transport properties, was also correlated to MVD (rτ = 0.6, P ≤ 0.05). Conclusion DCE-US has been shown to detect vascular changes at a very early stage after radiotherapy, which is a great advantage since DCE-US is non-invasive, available at most hospitals, and is low in cost compared to other techniques used in clinical practice.


Physical Review Letters | 2010

Elliptic Flow of Charged Particles in Pb-Pb Collisions at {radical}(s{sub NN})=2.76 TeV

K. Aamodt; Ø. Djuvsland; D. Fehlker; Ø. Haaland; Ming Huang; K. Kanaki; A. Klovning; D. T. Larsen; J. Lien; L. Liu; P. I. Loenne; J. Nystrand; M. Richter; Dieter Roehrich; C.H. Stokkevåg; A. Szostak; K. Ullaland; G. Øvrebekk; B. Wagner

We report the first measurement of charged particle elliptic flow in Pb-Pb collisions at sqrt[S(NN)] =2.76 TeV with the ALICE detector at the CERN Large Hadron Collider. The measurement is performed in the central pseudorapidity region (|η|<0.8) and transverse momentum range 0.2<p t<5.0 GeV/c. The elliptic flow signal v₂, measured using the 4-particle correlation method, averaged over transverse momentum and pseudorapidity is 0.087 ± 0.002(stat) ± 0.003(syst) in the 40%-50% centrality class. The differential elliptic flow v₂ p t reaches a maximum of 0.2 near p t =3 GeV/c. Compared to RHIC Au-Au collisions at sqrt[S(NN)] 200 GeV, the elliptic flow increases by about 30%. Some hydrodynamic model predictions which include viscous corrections are in agreement with the observed increase.


Proceedings of the 31st International Conference on High Energy Physics Ichep 2002 | 2003

Results from the BRAHMS experiment at RHIC

D. Röhrich; Ian Gardner Bearden; D. R. Beavis; C. Besliu; Y. Blyakhman; J. Brzychczyk; B. Budick; H. Bøggild; C. Chasman; Christian Holm Christensen; P. Christiansen; J. Cibor; R. Debbe; E. Enger; J. J. Gaardhøje; M. Germinario; K. Grotowski; K. Hagel; Ole Hansen; A.K. Holme; H. Ito; E. Jakobsen; A. Jipa; J.I. Jordre; F. Jundt; C.E. Jørgensen; R. Karabowicz; T Keutgen; E.J. Kim; T. Kozik

Abstract Results from the BRAHMS collaboration for Au+Au collisions at √ S NN = 200 GeV are presented, focussing on the measurement of the net-proton rapidity distribution, the determination of the pseudorapidity distribution of charged particles and on the rapidity distributions of pions and kaons.


Physical Review Letters | 1996

Production ofφMesons in CentralS28i+A196uCollisions at14.6AGeV/c

Y. Akiba; D. R. Beavis; P. Beery; H.C. Britt; B. Budick; C. Chasman; Z. Chen; C. Y. Chi; Y.Y. Chu; V. Cianciolo; B. A. Cole; J.B. Costales; H. J. Crawford; J.B. Cumming; R. Debbe; J. Engelage; S. Y. Fung; M. Gonin; S. Gushue; H. Hamagaki; O. Hansen; R. Hayano; S. Hayashi; S. Homma; H. Kaneko; J. H. Kang; S. Kaufman; W. L. Kehoe; K. Kurita; R.J. Ledoux

Production of the {phi} meson in central Si+Au collisions has been measured by E859 at the Brookhaven Alternating Gradient Synchrotron by selecting events with identified K{sup +}K{sup -} pairs. The mass and width of the {phi}, obtained from the invariant mass distribution of kaon pairs, are consistent with those of free f mesons. The transverse mass and rapidity distributions are presented. The inverse slope parameter for an exponential fit to the invariant transverse mass distribution is 179{+-}10{+-}17 MeV.

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D. R. Beavis

Brookhaven National Laboratory

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R. Debbe

Brookhaven National Laboratory

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S. Y. Fung

University of California

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H. J. Crawford

University of California

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J. Engelage

University of California

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O. Hansen

Brookhaven National Laboratory

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