F. Jundt

Publication List Details

Period

1966 - 2007

Number

303

Co-Authors

Nuclear Modification Factor for Charged Pions and Protons at Forward Rapidity in Central Au+Au Collisions at 200 GeV (2007)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

We present spectra of charged pions and protons in 0-10% central Au+Au collisions at √sNN = 200 GeV at mid-rapidity (y = 0) and forward pseudorapidity ($\eta$ = 2.2) measured with the BRAHMS...

Rapidity dependence of high $p_T$ suppression at $\sqrt{s_{NN}}$=62.4GeV (2006)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

We present measurements of charged hadron p_T spectra from Au+Au collisions at sqrt(snn)=62.4 GeV for pseudorapidities eta=0, eta=1 and eta=3.2. Around midrapidity (eta=0, eta=1) we find nuclear...

Onset of nuclear matter expansion in Au + Au collisions (2006)

Crochet, P., Rami, F., Gobbi, A., Dona, R., Coffin, J.P., Fintz, P., ...

Using the FOPI detector at GSI Darmstadt, excitation functions of collective flow components were measured for the Au+Au system, in the reaction plane and out of this plane, at seven incident...

Onset of nuclear matter expansion in Au + Au collisions (2006)

Crochet, P., Rami, F., Gobbi, A., Dona, R., Coffin, J.P., Fintz, P., ...

Using the FOPI detector at GSI Darmstadt, excitation functions of collective flow components were measured for the Au+Au system, in the reaction plane and out of this plane, at seven incident...

Onset of nuclear matter expansion in Au + Au collisions (2006)

Crochet, P., Rami, F., Gobbi, A., Dona, R., Coffin, J.P., Fintz, P., ...

Using the FOPI detector at GSI Darmstadt, excitation functions of collective flow components were measured for the Au+Au system, in the reaction plane and out of this plane, at seven incident...

Rapidity dependence of high p_T suppression at sqrt{s_{NN}}=62.4{GeV} (2006)

Arsene, I., Bearden, I. G., Beavis, D., Besliu, C., Budick, B., Bøggild, H., ...

We present measurements of charged hadron p_T spectra from Au+Au collisions at sqrt(snn)=62.4 GeV for pseudorapidities eta=0, eta=1 and eta=3.2. Around midrapidity (eta=0, eta=1) we find nuclear...

Rapidity dependence of high $p_T$ suppression at $\sqrt{s_{NN}}$=62.4GeV (2006)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

We present measurements of charged hadron p_T spectra from Au+Au collisions at sqrt(snn)=62.4 GeV for pseudorapidities eta=0, eta=1 and eta=3.2. Around midrapidity (eta=0, eta=1) we find nuclear...

Centrality dependent particle production at y=0 and y $\sim$ 1 in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

Particle production of identified charged hadrons, $\pi^{\pm}$, $K^{\pm}$, $p$, and $\bar{p}$ in Au+Au collisions at $\sqrt(snn) =$ 200 GeV has been studied as a function of transverse momentum and...

Quark gluon plasma and color glass condensate at RHIC ? The perspective from the BRAHMS experiment (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

We review the main results obtained by the BRAHMS collaboration on the properties of hot and dense hadronic and partonic matter produced in ultrarelativistic heavy ion collisions at RHIC. A...

Charged meson rapidity distributions in central Au+Au collisions at $\sqrt{s_{NN}$ = 200 GeV (2005)

Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., Chasman, C., ...

We have measured rapidity densities $dN/dy$ of $\pi^{\pm}$ and $K^{\pm}$ over a broad rapidity range (-0.1 < y < 3.5) for central Au+Au collisions at $\sqrt{^{s}NN}$ = 200 GeV. These data have...

Measurement of the $K_{L} \to e^{+}e^{-}e^{+} e^{-}$ Decay Rate (2005)

Lai, A, Bearden, I G, Marras, D, Batley, J Richard, Dosanjh, R S, Gershon, T J, ...

The decay rate of the long-lived neutral K meson into the e^+ e^- e^+ e^- final state has been measured with the NA48 detector at the CERN SPS. Using data collected in 1998 and 1999, a total of 200...

Centrality dependence of charged particle pseudorapidity distributions from d+Au collisions at $\sqrt{s_{NN}}$=200 GeV (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

Charged-particle pseudorapidity densities are presented for the d+Au reaction at sqrt{s_{NN}}=200 GeV with -4.2

Forward and midrapidity like-particle ratios from p+p collisions at $\sqrt{s}$ = 200 GeV (2005)

Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., Chasman, C., ...

We present a measurement of pi-\pi+, K-/K+ and pbar/p from p+p collisions at sqrt(s) = 20 0GeV over the rapidity range 0

Recent results from the BRAHMS experiment at RHIC (2005)

Staszel, P., Arsene, I., G. Bearden, I., Beavis, D., Besliu, C., Budick, B., ...

We present the results obtained by the BRAHMS experiment at the Relativistic Heavy Ion Collider (RHIC) for three colliding systems, namely: Au + Au, d + Au and p + p at $sqrt{s_nn}$. The main focus...

Centrality dependent particle production at y=0 and y $\sim$ 1 in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

Particle production of identified charged hadrons, $\pi^{\pm}$, $K^{\pm}$, $p$, and $\bar{p}$ in Au+Au collisions at $\sqrt(snn) =$ 200 GeV has been studied as a function of transverse momentum and...

Forward and midrapidity like-particle ratios from p+p collisions at $\sqrt{s}$ = 200 GeV (2005)

Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., Chasman, C., ...

We present a measurement of pi-\pi+, K-/K+ and pbar/p from p+p collisions at sqrt(s) = 20 0GeV over the rapidity range 0

Quark gluon plasma and color glass condensate at RHIC ? The perspective from the BRAHMS experiment (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

We review the main results obtained by the BRAHMS collaboration on the properties of hot and dense hadronic and partonic matter produced in ultrarelativistic heavy ion collisions at RHIC. A...

Centrality dependence of charged particle pseudorapidity distributions from d+Au collisions at $\sqrt{s_{NN}}$=200 GeV (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

Charged-particle pseudorapidity densities are presented for the d+Au reaction at sqrt{s_{NN}}=200 GeV with -4.2

Charged meson rapidity distributions in central Au+Au collisions at $\sqrt{s_{NN}$ = 200 GeV (2005)

Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., Chasman, C., ...

We have measured rapidity densities $dN/dy$ of $\pi^{\pm}$ and $K^{\pm}$ over a broad rapidity range (-0.1 < y < 3.5) for central Au+Au collisions at $\sqrt{^{s}NN}$ = 200 GeV. These data have...

Recent results from the BRAHMS experiment at RHIC (2005)

Staszel, P., Arsene, I., G. Bearden, I., Beavis, D., Besliu, C., Budick, B., ...

We present the results obtained by the BRAHMS experiment at the Relativistic Heavy Ion Collider (RHIC) for three colliding systems, namely: Au + Au, d + Au and p + p at $sqrt{s_nn}$. The main focus...

Centrality dependent particle production at y=0 and y $\sim$ 1 in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

Particle production of identified charged hadrons, $\pi^{\pm}$, $K^{\pm}$, $p$, and $\bar{p}$ in Au+Au collisions at $\sqrt(snn) =$ 200 GeV has been studied as a function of transverse momentum and...

Forward and midrapidity like-particle ratios from p+p collisions at $\sqrt{s}$ = 200 GeV (2005)

Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., Chasman, C., ...

We present a measurement of pi-\pi+, K-/K+ and pbar/p from p+p collisions at sqrt(s) = 20 0GeV over the rapidity range 0

Quark gluon plasma and color glass condensate at RHIC ? The perspective from the BRAHMS experiment (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

We review the main results obtained by the BRAHMS collaboration on the properties of hot and dense hadronic and partonic matter produced in ultrarelativistic heavy ion collisions at RHIC. A...

Centrality dependence of charged particle pseudorapidity distributions from d+Au collisions at $\sqrt{s_{NN}}$=200 GeV (2005)

Arsene, I., Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

Charged-particle pseudorapidity densities are presented for the d+Au reaction at sqrt{s_{NN}}=200 GeV with -4.2

Charged meson rapidity distributions in central Au+Au collisions at $\sqrt{s_{NN}$ = 200 GeV (2005)

Bearden, I.G., Beavis, D., Besliu, C., Budick, B., Boggild, H., Chasman, C., ...

We have measured rapidity densities $dN/dy$ of $\pi^{\pm}$ and $K^{\pm}$ over a broad rapidity range (-0.1 < y < 3.5) for central Au+Au collisions at $\sqrt{^{s}NN}$ = 200 GeV. These data have...

The rapidity and centrality dependence of nuclear modification factors at RHIC - what does bulk particle production tell us about the nuclear medium ? (2004)

Arsene, I., Bearden, G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

The BRAHMS experiment at RHIC has measured the production of charged hadrons as a function of pseudorapidity and transverse momentum in Au+Au, d + Au, and p+p collisions at a common energy of...

The rapidity and centrality dependence of nuclear modification factors at RHIC - what does bulk particle production tell us about the nuclear medium ? (2004)

Arsene, I., Bearden, G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

The BRAHMS experiment at RHIC has measured the production of charged hadrons as a function of pseudorapidity and transverse momentum in Au+Au, d + Au, and p+p collisions at a common energy of...

The rapidity and centrality dependence of nuclear modification factors at RHIC - what does bulk particle production tell us about the nuclear medium ? (2004)

Arsene, I., Bearden, G., Beavis, D., Besliu, C., Budick, B., Boggild, H., ...

The BRAHMS experiment at RHIC has measured the production of charged hadrons as a function of pseudorapidity and transverse momentum in Au+Au, d + Au, and p+p collisions at a common energy of...

Detector and Front-end electronics for ALICE and STAR silicon strip layers (2000)

Arnold, L, Baudot, J, Coffin, J P, Guillaume, G, Higueret, S, Jundt, F, ...

Detector modules consisting of Silicon Strip Detector (SSD) and Front End Electronics (FEE) assembly have been designed in order to provide the two outer layers of the ALICE Inner Tracker System...

TAB Bonded SSD Module for the STAR and ALICE Trackers (2000)

Lutz, Jean Robert, Arnold, L, Baudot, J, Bonnet, D, Coffin, J P, Germain, M, ...

Presentation made at LEB99, 20-24 September 1999A novel compact detector module has been produced by the "IReS"-"Subatech"-"Thomson-CSF-Detexis" collaboration. It includes a Double-Sided (DS) Silicon...

Abundance of Delta resonances in $^{58}$Ni + $^{58}$Ni collisions between 1 and 2 AGeV (1999)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

Charged pion spectra measured in 58Ni-58Ni collisions at 1.06, 1.45 and 1.93 AGeV are interpreted in terms of a thermal model including the decay of Delta resonances. The transverse momentum spectra...

Abundance of Delta resonances in $^{58}$Ni + $^{58}$Ni collisions between 1 and 2 AGeV (1999)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

Charged pion spectra measured in 58Ni-58Ni collisions at 1.06, 1.45 and 1.93 AGeV are interpreted in terms of a thermal model including the decay of Delta resonances. The transverse momentum spectra...

Abundance of Delta resonances in $^{58}$Ni + $^{58}$Ni collisions between 1 and 2 AGeV (1999)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

Charged pion spectra measured in 58Ni-58Ni collisions at 1.06, 1.45 and 1.93 AGeV are interpreted in terms of a thermal model including the decay of Delta resonances. The transverse momentum spectra...

Stopping and radial flow in central $^{58}$Ni + $^{58}$Ni collisions between 1A and 2A GeV (1999)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

The production of charged pions, protons and deuterons has been studied in central collisions of 58Ni on 58Ni at incident beam energies of 1.06, 1.45 and 1.93 AGeV. The dependence of...

$K^+$ production in the reaction $^{58}$Ni + $^{58}$Ni at incident energies from 1 to 2 A GeV (1999)

Best, D., Herrmann, N., Hong, B., Kirejczyk, M., Ritman, J., Wisniewski, K., ...

Semi-inclusive triple differential multiplicity distributions of positively charged kaons have been measured over a wide range in rapidity and transverse mass for central collisions of $^{58}$Ni with...

Azimuthal anisotropies as stringent test for nuclear transport models (1999)

Crochet, P., Rami, F., Dona, R., Coffin, J.P., Fintz, P., Guillaume, G., ...

Azimuthal distributions of charged particles and intermediate mass fragments emitted in Au+Au collisions at 600AMeV have been measured using the FOPI facility at GSI-Darmstadt. Data show a strong...

$K^+$ production in the reaction $^{58}$Ni + $^{58}$Ni at incident energies from 1 to 2 A GeV (1999)

Best, D., Herrmann, N., Hong, B., Kirejczyk, M., Ritman, J., Wisniewski, K., ...

Semi-inclusive triple differential multiplicity distributions of positively charged kaons have been measured over a wide range in rapidity and transverse mass for central collisions of $^{58}$Ni with...

Azimuthal anisotropies as stringent test for nuclear transport models (1999)

Crochet, P., Rami, F., Dona, R., Coffin, J.P., Fintz, P., Guillaume, G., ...

Azimuthal distributions of charged particles and intermediate mass fragments emitted in Au+Au collisions at 600AMeV have been measured using the FOPI facility at GSI-Darmstadt. Data show a strong...

Stopping and radial flow in central $^{58}$Ni + $^{58}$Ni collisions between 1A and 2A GeV (1999)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

The production of charged pions, protons and deuterons has been studied in central collisions of 58Ni on 58Ni at incident beam energies of 1.06, 1.45 and 1.93 AGeV. The dependence of...

$K^+$ production in the reaction $^{58}$Ni + $^{58}$Ni at incident energies from 1 to 2 A GeV (1999)

Best, D., Herrmann, N., Hong, B., Kirejczyk, M., Ritman, J., Wisniewski, K., ...

Semi-inclusive triple differential multiplicity distributions of positively charged kaons have been measured over a wide range in rapidity and transverse mass for central collisions of $^{58}$Ni with...

Azimuthal anisotropies as stringent test for nuclear transport models (1999)

Crochet, P., Rami, F., Dona, R., Coffin, J.P., Fintz, P., Guillaume, G., ...

Azimuthal distributions of charged particles and intermediate mass fragments emitted in Au+Au collisions at 600AMeV have been measured using the FOPI facility at GSI-Darmstadt. Data show a strong...

Stopping and radial flow in central $^{58}$Ni + $^{58}$Ni collisions between 1A and 2A GeV (1999)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

The production of charged pions, protons and deuterons has been studied in central collisions of 58Ni on 58Ni at incident beam energies of 1.06, 1.45 and 1.93 AGeV. The dependence of...

Central collisions of Au on Au at 150, 250 and 400 A.MeV (1999)

Reisdorf, W., Best, D., Gobbi, A., Herrmann, N., Hildenbrand, K.D., Hong, B., ...

Collisions of Au on Au at incident energies of 150, 250 and 400 A MeV were studied with the FOPI-facility at GSI Darmstadt. Nuclear charge (Z 16) and velocity of the products were detected with full...

Central collisions of Au on Au at 150, 250 and 400 A.MeV (1999)

Reisdorf, W., Best, D., Gobbi, A., Herrmann, N., Hildenbrand, K.D., Hong, B., ...

Collisions of Au on Au at incident energies of 150, 250 and 400 A MeV were studied with the FOPI-facility at GSI Darmstadt. Nuclear charge (Z 16) and velocity of the products were detected with full...

Central collisions of Au on Au at 150, 250 and 400 A.MeV (1999)

Reisdorf, W., Best, D., Gobbi, A., Herrmann, N., Hildenbrand, K.D., Hong, B., ...

Collisions of Au on Au at incident energies of 150, 250 and 400 A MeV were studied with the FOPI-facility at GSI Darmstadt. Nuclear charge (Z 16) and velocity of the products were detected with full...

Identification of baryon resonances in central heavy-ion collisions at energies between 1 and 2 AGeV (1998)

Eskef, M., Pelte, D., Goebels, G., Haefele, E., Herrmann, N., Korolija, M., ...

The mass distributions of baryon resonances populated in near-central collisions of Au on Au and Ni on Ni are deduced by defolding the $p_t$ spectra of charged pions by a method which does not depend...

Stopping and radial flow in central $^{58}$Ni + $^{58}$Ni collisions between 1A and 2A GeV (1998)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

The production of charged pions, protons and deuterons has been studied in central collisions of 58Ni on 58Ni at incident beam energies of 1.06, 1.45 and 1.93 AGeV. The dependence of...

Identification of baryon resonances in central heavy-ion collisions at energies between 1 and 2 AGeV (1998)

Eskef, M., Pelte, D., Goebels, G., Haefele, E., Herrmann, N., Korolija, M., ...

The mass distributions of baryon resonances populated in near-central collisions of Au on Au and Ni on Ni are deduced by defolding the $p_t$ spectra of charged pions by a method which does not depend...

Stopping and radial flow in central $^{58}$Ni + $^{58}$Ni collisions between 1A and 2A GeV (1998)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

The production of charged pions, protons and deuterons has been studied in central collisions of 58Ni on 58Ni at incident beam energies of 1.06, 1.45 and 1.93 AGeV. The dependence of...

Identification of baryon resonances in central heavy-ion collisions at energies between 1 and 2 AGeV (1998)

Eskef, M., Pelte, D., Goebels, G., Haefele, E., Herrmann, N., Korolija, M., ...

The mass distributions of baryon resonances populated in near-central collisions of Au on Au and Ni on Ni are deduced by defolding the $p_t$ spectra of charged pions by a method which does not depend...

Identification of baryon resonances in central heavy-ion collisions at energies between 1 and 2 AGeV (1998)

Eskef, M., Pelte, D., Goebels, G., Haefele, E., Herrmann, N., Korolija, M., ...

The mass distributions of baryon resonances populated in near-central collisions of Au on Au and Ni on Ni are deduced by defolding the $p_t$ spectra of charged pions by a method which does not depend...

Identification of baryon resonances in central heavy-ion collisions at energies between 1 and 2 AGeV (1998)

Eskef, M., Pelte, D., Goebels, G., Haefele, E., Herrmann, N., Korolija, M., ...

The mass distributions of baryon resonances populated in near-central collisions of Au on Au and Ni on Ni are deduced by defolding the $p_t$ spectra of charged pions by a method which does not depend...

Abundance of Delta Resonances in 58Ni+58Ni Collisions between 1 and 2 AGeV (1997)

Hong, FOPI Collaboration: B., Herrmann, N., Ritman, J. L., Best, D., Gobbi, A., Hildenbrand, K. D., ...

Charged pion spectra measured in 58Ni-58Ni collisions at 1.06, 1.45 and 1.93 AGeV are interpreted in terms of a thermal model including the decay of Delta resonances. The transverse momentum spectra...

Onset of nuclear matter expansion in Au+Au collisions (1997)

Crochet, Philippe, Rami, F, Gobbi, A, Donà, R, Coffin, J P, Fintz, P, ...

Using the FOPI detector at GSI Darmstadt, excitation functions of collective flow components were measured for the Au+Au system, in the reaction plane and out of this plane, at seven incident...

Charged pion production in Au on Au collisions at 1 AGeV (1997)

Pelte, D., Haefele, E., Best, D., Goebels, G., Herrmann, N., Pinkenburg, C., ...

Charged pions are measured with the $4\pi$ detector $FOPI$ at $GSI$ using the Au on Au reaction at 1.06 AGeV bombarding energy. The pion multiplicities $n_{\rm \pi}$ increase with the number of...

Proton-proton correlations in central collisions of Ni + Ni at 1.93 A.GeV and the space-time extent of the emission source (1997)

Kotte, R., Biegansky, J., Moesner, J., Neubert, W., Plettner, C., Wohlfarth, D., ...

Small-angle correlations of proton pairs produced in central Ni+Ni collisions at a beam energy of 1.93 A · GeV are investigated with the FOPI detector system at GSI Darmstadt. Simultaneous...

Charged pions from Ni on Ni collisions between 1 and 2 AGeV (1997)

Pelte, D., Eskef, M., Goebels, G., Hafele, E., Herrmann, N., Korolija, M., ...

Charged pions from Ni + Ni reactions at 1.05, 1.45 and 1.93 AGeV are measured with the FOPI detector. The mean $\pi^{\pm}$ multiplicities per mean number of participants increase with beam energy, in...

Abundance of Delta resonances in $^{58}$Ni + $^{58}$Ni collisions between 1 and 2 AGeV (1997)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

Charged pion spectra measured in 58Ni-58Ni collisions at 1.06, 1.45 and 1.93 AGeV are interpreted in terms of a thermal model including the decay of Delta resonances. The transverse momentum spectra...

Onset of nuclear matter expansion in Au + Au collisions (1997)

Crochet, P., Rami, F., Gobbi, A., Dona, R., Coffin, J.P., Fintz, P., ...

Using the FOPI detector at GSI Darmstadt, excitation functions of collective flow components were measured for the Au+Au system, in the reaction plane and out of this plane, at seven incident...

$K^+$ production in the reaction $^{58}$Ni + $^{58}$Ni at incident energies from 1 to 2 A GeV (1997)

Best, D., Herrmann, N., Hong, B., Kirejczyk, M., Ritman, J., Wisniewski, K., ...

Semi-inclusive triple differential multiplicity distributions of positively charged kaons have been measured over a wide range in rapidity and transverse mass for central collisions of $^{58}$Ni with...

Azimuthal anisotropies as stringent test for nuclear transport models (1997)

Crochet, P., Rami, F., Dona, R., Coffin, J.P., Fintz, P., Guillaume, G., ...

Azimuthal distributions of charged particles and intermediate mass fragments emitted in Au+Au collisions at 600AMeV have been measured using the FOPI facility at GSI-Darmstadt. Data show a strong...

Central collisions of Au on Au at 150, 250 and 400 A.MeV (1997)

Reisdorf, W., Best, D., Gobbi, A., Herrmann, N., Hildenbrand, K.D., Hong, B., ...

Collisions of Au on Au at incident energies of 150, 250 and 400 A MeV were studied with the FOPI-facility at GSI Darmstadt. Nuclear charge (Z 16) and velocity of the products were detected with full...

Charged pion production in Au on Au collisions at 1 AGeV (1997)

Pelte, D., Haefele, E., Best, D., Goebels, G., Herrmann, N., Pinkenburg, C., ...

Charged pions are measured with the $4\pi$ detector $FOPI$ at $GSI$ using the Au on Au reaction at 1.06 AGeV bombarding energy. The pion multiplicities $n_{\rm \pi}$ increase with the number of...

Proton-proton correlations in central collisions of Ni + Ni at 1.93 A.GeV and the space-time extent of the emission source (1997)

Kotte, R., Biegansky, J., Moesner, J., Neubert, W., Plettner, C., Wohlfarth, D., ...

Small-angle correlations of proton pairs produced in central Ni+Ni collisions at a beam energy of 1.93 A · GeV are investigated with the FOPI detector system at GSI Darmstadt. Simultaneous...

Charged pions from Ni on Ni collisions between 1 and 2 AGeV (1997)

Pelte, D., Eskef, M., Goebels, G., Hafele, E., Herrmann, N., Korolija, M., ...

Charged pions from Ni + Ni reactions at 1.05, 1.45 and 1.93 AGeV are measured with the FOPI detector. The mean $\pi^{\pm}$ multiplicities per mean number of participants increase with beam energy, in...

Abundance of Delta resonances in $^{58}$Ni + $^{58}$Ni collisions between 1 and 2 AGeV (1997)

Hong, B., Herrmann, N., Ritman, J.L., Best, D., Gobbi, A., Hildenbrand, K.D., ...

Charged pion spectra measured in 58Ni-58Ni collisions at 1.06, 1.45 and 1.93 AGeV are interpreted in terms of a thermal model including the decay of Delta resonances. The transverse momentum spectra...

Onset of nuclear matter expansion in Au + Au collisions (1997)

Crochet, P., Rami, F., Gobbi, A., Dona, R., Coffin, J.P., Fintz, P., ...

Using the FOPI detector at GSI Darmstadt, excitation functions of collective flow components were measured for the Au+Au system, in the reaction plane and out of this plane, at seven incident...

$K^+$ production in the reaction $^{58}$Ni + $^{58}$Ni at incident energies from 1 to 2 A GeV (1997)

Best, D., Herrmann, N., Hong, B., Kirejczyk, M., Ritman, J., Wisniewski, K., ...

Semi-inclusive triple differential multiplicity distributions of positively charged kaons have been measured over a wide range in rapidity and transverse mass for central collisions of $^{58}$Ni with...

Azimuthal anisotropies as stringent test for nuclear transport models (1997)

Crochet, P., Rami, F., Dona, R., Coffin, J.P., Fintz, P., Guillaume, G., ...

Azimuthal distributions of charged particles and intermediate mass fragments emitted in Au+Au collisions at 600AMeV have been measured using the FOPI facility at GSI-Darmstadt. Data show a strong...

Central collisions of Au on Au at 150, 250 and 400 A.MeV (1997)

Reisdorf, W., Best, D., Gobbi, A., Herrmann, N., Hildenbrand, K.D., Hong, B., ...

Collisions of Au on Au at incident energies of 150, 250 and 400 A MeV were studied with the FOPI-facility at GSI Darmstadt. Nuclear charge (Z 16) and velocity of the products were detected with full...

Charged pions from Ni on Ni collisions between 1 and 2 AGeV (1997)

Pelte, D., Eskef, M., Goebels, G., Hafele, E., Herrmann, N., Korolija, M., ...

Charged pions from Ni + Ni reactions at 1.05, 1.45 and 1.93 AGeV are measured with the FOPI detector. The mean $\pi^{\pm}$ multiplicities per mean number of participants increase with beam energy, in...

Charged pions from Ni on Ni collisions between 1 and 2 AGeV (1997)

Pelte, D., Eskef, M., Goebels, G., Hafele, E., Herrmann, N., Korolija, M., ...

Charged pions from Ni + Ni reactions at 1.05, 1.45 and 1.93 AGeV are measured with the FOPI detector. The mean $\pi^{\pm}$ multiplicities per mean number of participants increase with beam energy, in...

Charged pions from Ni on Ni collisions between 1 and 2 AGeV (1997)

Pelte, D., Eskef, M., Goebels, G., Hafele, E., Herrmann, N., Korolija, M., ...

Charged pions from Ni + Ni reactions at 1.05, 1.45 and 1.93 AGeV are measured with the FOPI detector. The mean $\pi^{\pm}$ multiplicities per mean number of participants increase with beam energy, in...

On the transverse momentum distribution of strange hadrons produced in relativistic heavy ion collisions (1995)

Ritman, J.L., Herrmann, N., Best, D., Alard, J.P., Amouroux, V., Bastid, N., ...

Particles with strange quark content produced in the system 1.93 AGeV $^{58}$Ni on $^{58}$Ni have been investigated at GSI Darmstadt with the FOPI detector system. The correlation of these produced...

On the transverse momentum distribution of strange hadrons produced in relativistic heavy ion collisions (1995)

Ritman, J.L., Herrmann, N., Best, D., Alard, J.P., Amouroux, V., Bastid, N., ...

Particles with strange quark content produced in the system 1.93 AGeV $^{58}$Ni on $^{58}$Ni have been investigated at GSI Darmstadt with the FOPI detector system. The correlation of these produced...

On the transverse momentum distribution of strange hadrons produced in relativistic heavy ion collisions (1995)

Ritman, J.L., Herrmann, N., Best, D., Alard, J.P., Amouroux, V., Bastid, N., ...

Particles with strange quark content produced in the system 1.93 AGeV $^{58}$Ni on $^{58}$Ni have been investigated at GSI Darmstadt with the FOPI detector system. The correlation of these produced...

On the transverse momentum distribution of strange hadrons produced in relativistic heavy ion collisions (1995)

Ritman, J.L., Herrmann, N., Best, D., Alard, J.P., Amouroux, V., Bastid, N., ...

Particles with strange quark content produced in the system 1.93 AGeV $^{58}$Ni on $^{58}$Ni have been investigated at GSI Darmstadt with the FOPI detector system. The correlation of these produced...

On the transverse momentum distribution of strange hadrons produced in relativistic heavy ion collisions (1995)

Ritman, J.L., Herrmann, N., Best, D., Alard, J.P., Amouroux, V., Bastid, N., ...

Particles with strange quark content produced in the system 1.93 AGeV $^{58}$Ni on $^{58}$Ni have been investigated at GSI Darmstadt with the FOPI detector system. The correlation of these produced...

Entropy production in the Au + Au reaction between 150 and 800 A MeV (1993)

Kuhn, C., Konopka, J., Coffin, J.P., Cerruti, C., Fintz, P., Guillaume, G., ...

The entropy per nucleon (S/A) has been extracted for the Au [(150—800)A MeV] + Au reaction by using the phase I setup of the 4 pi facility at GSI, Darmstadt. The entropy has been obtained from the...

Entropy production in the Au + Au reaction between 150 and 800 A MeV (1993)

Kuhn, C., Konopka, J., Coffin, J.P., Cerruti, C., Fintz, P., Guillaume, G., ...

The entropy per nucleon (S/A) has been extracted for the Au [(150—800)A MeV] + Au reaction by using the phase I setup of the 4 pi facility at GSI, Darmstadt. The entropy has been obtained from the...

Entropy production in the Au + Au reaction between 150 and 800 A MeV (1993)

Kuhn, C., Konopka, J., Coffin, J.P., Cerruti, C., Fintz, P., Guillaume, G., ...

The entropy per nucleon (S/A) has been extracted for the Au [(150—800)A MeV] + Au reaction by using the phase I setup of the 4 pi facility at GSI, Darmstadt. The entropy has been obtained from the...

Entropy production in the Au + Au reaction between 150 and 800 A MeV (1993)

Kuhn, C., Konopka, J., Coffin, J.P., Cerruti, C., Fintz, P., Guillaume, G., ...

The entropy per nucleon (S/A) has been extracted for the Au [(150—800)A MeV] + Au reaction by using the phase I setup of the 4 pi facility at GSI, Darmstadt. The entropy has been obtained from the...

Entropy production in the Au + Au reaction between 150 and 800 A MeV (1993)

Kuhn, C., Konopka, J., Coffin, J.P., Cerruti, C., Fintz, P., Guillaume, G., ...

The entropy per nucleon (S/A) has been extracted for the Au [(150—800)A MeV] + Au reaction by using the phase I setup of the 4 pi facility at GSI, Darmstadt. The entropy has been obtained from the...

Vies moyennes de niveaux de 53Mn excités par la réaction 50Cr (α, pγ)53Mn (1979)

Fintz, P., Riedinger-Ordoñez, I., Guillaume, G., Jundt, F., Gallmann, A.

Les propriétés électromagnétiques du noyau 53Mn sont étudiées à l'aide de la réaction 50Cr(α, pγ)53Mn à Eα = 14,5 MeV. Les rayonnements γ sont détectés en coïncidence...

Vies moyennes de niveaux de 53Mn excités par la réaction 50Cr (α, pγ)53Mn (1979)

Fintz, P., Riedinger-Ordoñez, I., Guillaume, G., Jundt, F., Gallmann, A.

Les propriétés électromagnétiques du noyau 53Mn sont étudiées à l'aide de la réaction 50Cr(α, pγ)53Mn à Eα = 14,5 MeV. Les rayonnements γ sont détectés en coïncidence...

Vies moyennes de niveaux de 53Mn excités par la réaction 50Cr (α, pγ)53Mn (1979)

Fintz, P., Riedinger-Ordoñez, I., Guillaume, G., Jundt, F., Gallmann, A.

Les propriétés électromagnétiques du noyau 53Mn sont étudiées à l'aide de la réaction 50Cr(α, pγ)53Mn à Eα = 14,5 MeV. Les rayonnements γ sont détectés en coïncidence...

Vies moyennes de niveaux de 53Mn excités par la réaction 50Cr (α, pγ)53Mn (1979)

Fintz, P., Riedinger-Ordoñez, I., Guillaume, G., Jundt, F., Gallmann, A.

Les propriétés électromagnétiques du noyau 53Mn sont étudiées à l'aide de la réaction 50Cr(α, pγ)53Mn à Eα = 14,5 MeV. Les rayonnements γ sont détectés en coïncidence...

LE "MULTIPÔLEMÈTRE". APPLICATION A L'ÉTUDE DE TRANSITIONS ÉLECTROMAGNÉTIQUES (1966)

Gorodetzky, S., Gallmann, A., Coffin, J., Frick, G., Jundt, F.

Un spectromètre magnétique à image intermédiaire du type Siegbahn-Slätis a été transformé en vue de la détermination de la multipolarité de transitions électromagnétiques. Nous avons...

LE "MULTIPÔLEMÈTRE". APPLICATION A L'ÉTUDE DE TRANSITIONS ÉLECTROMAGNÉTIQUES (1966)

Gorodetzky, S., Gallmann, A., Coffin, J., Frick, G., Jundt, F.

Un spectromètre magnétique à image intermédiaire du type Siegbahn-Slätis a été transformé en vue de la détermination de la multipolarité de transitions électromagnétiques. Nous avons...

LE "MULTIPÔLEMÈTRE". APPLICATION A L'ÉTUDE DE TRANSITIONS ÉLECTROMAGNÉTIQUES (1966)

Gorodetzky, S., Gallmann, A., Coffin, J., Frick, G., Jundt, F.

Un spectromètre magnétique à image intermédiaire du type Siegbahn-Slätis a été transformé en vue de la détermination de la multipolarité de transitions électromagnétiques. Nous avons...

A switch region determines the cell type-specific positive or negative action of YY1 on the activity of the human papillomavirus type 18 promoter.

Bauknecht, T, Jundt, F, Herr, I, Oehler, T, Delius, H, Shi, Y, ...

YY1 is a zinc finger transcription factor which acts as either a repressor or an activator dependent on the promoter context. YY1 is a potent activator of the genuine human papillomavirus type 18...

A switch region determines the cell type-specific positive or negative action of YY1 on the activity of the human papillomavirus type 18 promoter.

Bauknecht, T, Jundt, F, Herr, I, Oehler, T, Delius, H, Shi, Y, ...

YY1 is a zinc finger transcription factor which acts as either a repressor or an activator dependent on the promoter context. YY1 is a potent activator of the genuine human papillomavirus type 18...