Evolution of sexual dimorphism of wing shape in the Drosophila melanogaster subgroup (2009)
Gidaszewski, N.A., Baylac, M., Klingenberg, C.
Background: Sexual dimorphism of body size has been the subject of numerous studies, but few have examined sexual shape dimorphism (SShD) and its evolution. Allometry, the shape change associated...
The GUINEVERE Project for Accelerator Driven System Physics (2009)
Billebaud, A., Baeten, P., Aït Abderrahim, H., Ban, G., Baylac, M., Bergmans, G., ...
The GUINEVERE project is part of the EUROTRANS Integrated Project of the 6th EURATOM Framework Programme. It is mainly devoted to ADS on-line reactivity monitoring validation, sub-criticality...
The GUINEVERE Project for Accelerator Driven System Physics (2009)
Billebaud, A., Baeten, P., Aït Abderrahim, H., Ban, G., Baylac, M., Bergmans, G., ...
The GUINEVERE project is part of the EUROTRANS Integrated Project of the 6th EURATOM Framework Programme. It is mainly devoted to ADS on-line reactivity monitoring validation, sub-criticality...
The GUINEVERE Project for Accelerator Driven System Physics (2009)
Billebaud, A., Baeten, P., Aït Abderrahim, H., Ban, G., Baylac, M., Bergmans, G., ...
The GUINEVERE project is part of the EUROTRANS Integrated Project of the 6th EURATOM Framework Programme. It is mainly devoted to ADS on-line reactivity monitoring validation, sub-criticality...
Burgio, GR, Baylac, M, Heyer, E, Montagutelli, X
To assess the genetic basis of the skull shape variation and morphological integration in mice, we have used a tool based onthe cross between the distantly related mouse species Mus spretus (SEG/Pas...
The GUINEVERE project at the VENUS facility (2008)
Baeten, P., Aït Abderrahim, H., Bergmans, G., Heyse, J., Maes, D., Verboomen, B., ...
The GUINEVERE project at the VENUS facility (2008)
Baeten, P., Aït Abderrahim, H., Bergmans, G., Heyse, J., Maes, D., Verboomen, B., ...
The GUINEVERE project at the VENUS facility (2008)
Baeten, P., Aït Abderrahim, H., Bergmans, G., Heyse, J., Maes, D., Verboomen, B., ...
Vigne, J. D., Bignon, O., Callou, C., Cucchi, T., Mashkour, M., Auffray, J. C., ...
Though the use of geometrics morphometrics analysis is wide spread since at least 15 years in the scope of biological and anthropological sciences, the overwhelming majority of archaeologists still...
Parity-violating electroweak asymmetry in polarized-e p scattering (2007)
Aniol, K.A., Armstrong, D.S., Averett, T., Baylac, M., Burtin, E., Calarco, J., ...
End-to-End Beam Dynamics for CERN LINAC4 (2007)
Lombardi, A, Sargsyan, E, Lanzone, S, Lallement, J B, Bellodi, G, Baylac, M, ...
LINAC 4 is a normal conducting H- linac which aims to intensify the proton flux available for the CERN accelerator complex. This injector is designed to accelerate a 65 mA beam of H- ions up to 160...
This report presents some general characteristics of the main synchrotron dipole magnets designed for the CNAO project. It gives some estimates of field integrals and magnetic field flux using the...
This report presents some general characteristics of the main synchrotron dipole magnets designed for the CNAO project. It gives some estimates of field integrals and magnetic field flux using the...
This report presents some general characteristics of the main synchrotron dipole magnets designed for the CNAO project. It gives some estimates of field integrals and magnetic field flux using the...
Linac4 Technical Design Report (2006)
Arnaudon, L, Baudrenghien, P, Baylac, M, Bellodi, G, Body, Y, Borburgh, J, ...
Linac4 is an H- linear accelerator, intended to replace Linac2 as injector to the PS Booster (PSB). By delivering to the PSB a beam at 160 MeV energy, Linac4 will provide the conditions to double the...
The SPL (II) at CERN, a Superconducting 3.5 GeV H- Linac (2006)
Gerigk, F, Baylac, M, Bellodi, G, Benedico-Mora, E, Body, Y, Caspers, F, ...
A revision of the physics needs and recent progress in the technology of superconducting (SC) RF cavities have triggered major changes in the design of a SC H-linac at CERN. With up to 5MW beam...
Conceptual design of the SPL II: A high-power superconducting H- linac at CERN (2006)
Baylac, M., Gerigk, F., Benedico Mora, E., Caspers, F., Chel, S., De Conto, J.M., ...
An analysis of the revised physics needs and recent progress in the technology of supreconducting RF cavities have led to major changes in the specification and in the design for a Superconducting...
Error study of CERN Linac 4 (2006)
Baylac, M, De Conto, J M, Froidefond, E, Sargsyan, E
LINAC 4 is a normal conducting H- structure proposed to intensify the proton flux currently available for the CERN accelerator chain. This linac is designed to accelerate a 65 mA beam up to 160 MeV...
Statistical simulations of machine errors for LINAC4 (2006)
Baylac, M, De Conto, J M, Froidefond, E, Sargsyan, E
LINAC 4 is a normal conducting H- linac proposed at CERN to provide a higher proton flux to the CERN accelerator chain. It should replace the existing LINAC 2 as injector to the Proton Synchrotron...
Statistical simulations of machine errors for LINAC4 (2006)
Baylac, M., De Conto, J. M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- linac proposed at CERN to provide a higher proton flux to the CERN accelerator chain. It should replace the existing LINAC 2 as injector to the Proton Synchrotron...
Error study of CERN Linac 4 (2006)
Baylac, M., De Conto, J. M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- structure proposed to intensify the proton flux currently available for the CERN accelerator chain. This linac is designed to accelerate a 65 mA beam up to 160 MeV...
Statistical simulations of machine errors for LINAC4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- linac proposed at CERN to provide a higher proton flux to the CERN accelerator chain. It should replace the existing LINAC 2 as injector to the Proton Synchrotron...
Error study of CERN Linac 4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- structure proposed to intensify the proton flux currently available for the CERN accelerator chain. This linac is designed to accelerate a 65 mA beam up to 160 MeV...
Conceptual design of the SPL II: A high-power superconducting H- linac at CERN (2006)
Baylac, M., Gerigk, F., Benedico Mora, E., Caspers, F., Chel, S., De Conto, J.M., ...
An analysis of the revised physics needs and recent progress in the technology of supreconducting RF cavities have led to major changes in the specification and in the design for a Superconducting...
Statistical simulations of machine errors for LINAC4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- linac proposed at CERN to provide a higher proton flux to the CERN accelerator chain. It should replace the existing LINAC 2 as injector to the Proton Synchrotron...
Error study of CERN Linac 4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- structure proposed to intensify the proton flux currently available for the CERN accelerator chain. This linac is designed to accelerate a 65 mA beam up to 160 MeV...
End-to-end beam dynamics for CERN LINAC4 (2006)
Lombardi, A.M., Sargsyan, E., Lanzone, S., Lallement, J.B., Bellodi, G., Baylac, M., ...
LINAC 4 is a normal conducting H- linac which aims to intensify the proton flux available for the CERN accelerator complex. This injector is designed to accelerate a 65 mA beam of H- ions up to 160...
End-to-end beam dynamics for CERN LINAC4 (2006)
Lombardi, A.M., Sargsyan, E., Lanzone, S., Lallement, J.B., Bellodi, G., Baylac, M., ...
LINAC 4 is a normal conducting H- linac which aims to intensify the proton flux available for the CERN accelerator complex. This injector is designed to accelerate a 65 mA beam of H- ions up to 160...
Statistical simulations of machine errors for LINAC4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- linac proposed at CERN to provide a higher proton flux to the CERN accelerator chain. It should replace the existing LINAC 2 as injector to the Proton Synchrotron...
Error study of CERN Linac 4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- structure proposed to intensify the proton flux currently available for the CERN accelerator chain. This linac is designed to accelerate a 65 mA beam up to 160 MeV...
End-to-end beam dynamics for CERN LINAC4 (2006)
Lombardi, A.M., Sargsyan, E., Lanzone, S., Lallement, J.B., Bellodi, G., Baylac, M., ...
LINAC 4 is a normal conducting H- linac which aims to intensify the proton flux available for the CERN accelerator complex. This injector is designed to accelerate a 65 mA beam of H- ions up to 160...
Statistical simulations of machine errors for LINAC4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- linac proposed at CERN to provide a higher proton flux to the CERN accelerator chain. It should replace the existing LINAC 2 as injector to the Proton Synchrotron...
Error study of CERN Linac 4 (2006)
Baylac, M., De Conto, J.M., Froidefond, E., Sargsyan, E.
LINAC 4 is a normal conducting H- structure proposed to intensify the proton flux currently available for the CERN accelerator chain. This linac is designed to accelerate a 65 mA beam up to 160 MeV...
Laveissiere, G., Degrande, N., Jaminion, S., Jutier, C., Todor, L., Di Salvo, R., ...
We have made the first measurements of the virtual Compton scattering process via the e p -> e p gamma exclusive reaction at Q**2 = 1 GeV**2 in the nucleon resonance region. The cross section is...
Laveissiere, G., Todor, L., Degrande, N., Jaminion, S., Jutier, C., Di Salvo, R., ...
We report a Virtual Compton Scattering study of the proton in Hall A at the Thomas Jefferson National Accelerator Facility at low CM energies. We have determined the structure functions...
Effects of atomic hydrogen and deuterium exposure on high polarization GaAs photocathodes (2005)
Baylac, M., Adderley, P., Brittian, J., Clark, J., Day, T., Grames, J., ...
Strained-layer GaAs and strained-superlattice GaAs photocathodes are used at Jefferson Laboratory to create high average current beams of highly spin-polarized electrons. High electron yield, or...
Effects of atomic hydrogen and deuterium exposure on high polarization GaAs photocathodes (2005)
Baylac, M., Adderley, P., Brittian, J., Clark, J., Day, T., Grames, J., ...
Strained-layer GaAs and strained-superlattice GaAs photocathodes are used at Jefferson Laboratory to create high average current beams of highly spin-polarized electrons. High electron yield, or...
Effects of atomic hydrogen and deuterium exposure on high polarization GaAs photocathodes (2005)
Baylac, M., Adderley, P., Brittian, J., Clark, J., Day, T., Grames, J., ...
Strained-layer GaAs and strained-superlattice GaAs photocathodes are used at Jefferson Laboratory to create high average current beams of highly spin-polarized electrons. High electron yield, or...
Effects of atomic hydrogen and deuterium exposure on high polarization GaAs photocathodes (2005)
Baylac, M., Adderley, P., Brittian, J., Clark, J., Day, T., Grames, J., ...
Strained-layer GaAs and strained-superlattice GaAs photocathodes are used at Jefferson Laboratory to create high average current beams of highly spin-polarized electrons. High electron yield, or...
Parity-violating electroweak asymmetry in polarized-e p scattering (2004)
Aniol, K.A., Armstrong, D.S., Averett, T., Baylac, M., Burtin, E., Calarco, J., ...
Laveissiere, G., Todor, L., Degrande, N., Jaminion, S., Jutier, C., Di Salvo, R., ...
We report a Virtual Compton Scattering study of the proton in Hall A at the Thomas Jefferson National Accelerator Facility at low CM energies. We have determined the structure functions...
Laveissiere, G., Degrande, N., Jaminion, S., Jutier, C., Todor, L., Di Salvo, R., ...
We have made the first measurements of the virtual Compton scattering process via the e p -> e p gamma exclusive reaction at Q**2 = 1 GeV**2 in the nucleon resonance region. The cross section is...
Basic instrumentation for Hall A at Jefferson Lab (2004)
Alcorn, J., Anderson, B.D., Aniol, K.A., Annand, J.R.M., Auerbach, L., Arrington, J., ...
Parity-violating electroweak asymmetry in polarized-e p scattering (2004)
Aniol, K.A., Armstrong, D.S., Averett, T., Baylac, M., Burtin, E., Calarco, J., ...
Laveissiere, G., Todor, L., Degrande, N., Jaminion, S., Jutier, C., Di Salvo, R., ...
We report a Virtual Compton Scattering study of the proton in Hall A at the Thomas Jefferson National Accelerator Facility at low CM energies. We have determined the structure functions...
Laveissiere, G., Degrande, N., Jaminion, S., Jutier, C., Todor, L., Di Salvo, R., ...
We have made the first measurements of the virtual Compton scattering process via the e p -> e p gamma exclusive reaction at Q**2 = 1 GeV**2 in the nucleon resonance region. The cross section is...
Basic instrumentation for Hall A at Jefferson Lab (2004)
Alcorn, J., Anderson, B.D., Aniol, K.A., Annand, J.R.M., Auerbach, L., Arrington, J., ...
Laveissiere, G., Degrande, N., Jaminion, S., Jutier, C., Todor, L., Di Salvo, R., ...
Exclusive electroproduction of pi0 mesons on protons in the backward hemisphere has been studied at Q2=1.0 GeV2 by detecting protons in the forward direction in coincidence with scattered electrons...
Laveissiere, G., Degrande, N., Jaminion, S., Jutier, C., Todor, L., Di Salvo, R., ...
Exclusive electroproduction of pi0 mesons on protons in the backward hemisphere has been studied at Q2=1.0 GeV2 by detecting protons in the forward direction in coincidence with scattered electrons...
Laveissiere, G., Degrande, N., Jaminion, S., Jutier, C., Todor, L., Di Salvo, R., ...
Exclusive electroproduction of pi0 mesons on protons in the backward hemisphere has been studied at Q2=1.0 GeV2 by detecting protons in the forward direction in coincidence with scattered electrons...
Basic instrumentation for Hall A at Jefferson Lab (2004)
Alcorn, J., Anderson, B.D., Aniol, K.A., Annand, J.R.M., Auerbach, L., Arrington, J., ...
The instrumentation in Hall A at the Thomas Jefferson National Accelerator Facility was designed to study electro-and photo- induced reactions at very high luminosity and good momentum and angular...
Baylac, M., Burtin, E., Cavata, C., Escoffier, S., Frois, B., Lhuillier, D., ...
A Compton polarimeter has been installed in Hall A at Jefferson Laboratory. This letter reports on the first electron beam polarization measurements performed during the HAPPEX experiment at an...
Compton scattering off polarized electrons with a high finess Fabry-Perot cavity at JLab (2001)
Falletto, N., Authier, M., Bardin, G., Baylac, M., Boyer, M., Bugeon, F., ...
Compton scattering off polarized electrons with a high finess Fabry-Perot cavity at JLab (2001)
Falletto, N., Authier, M., Bardin, G., Baylac, M., Boyer, M., Bugeon, F., ...
Measurement of the neutral weak form-factors of the proton (1999)
Aniol, K.A., Armstrong, D.S., Baylac, M., Burtin, E., Calarco, J., Cates, G.D., ...
We have measured the parity-violating electroweak asymmetry in the elastic scattering of polarized electrons from the proton. The kinematic point (theta_lab = 12.3 degrees and Q^2=0.48 (GeV/c)^2) is...
Measurement of the neutral weak form-factors of the proton (1999)
Aniol, K.A., Armstrong, D.S., Baylac, M., Burtin, E., Calarco, J., Cates, G.D., ...
We have measured the parity-violating electroweak asymmetry in the elastic scattering of polarized electrons from the proton. The kinematic point (theta_lab = 12.3 degrees and Q^2=0.48 (GeV/c)^2) is...
Measurement of the neutral weak form-factors of the proton (1999)
Aniol, K.A., Armstrong, D.S., Baylac, M., Burtin, E., Calarco, J., Cates, G.D., ...
We have measured the parity-violating electroweak asymmetry in the elastic scattering of polarized electrons from the proton. The kinematic point (theta_lab = 12.3 degrees and Q^2=0.48 (GeV/c)^2) is...
Measurement of the neutral weak form-factors of the proton (1999)
Aniol, K.A., Armstrong, D.S., Baylac, M., Burtin, E., Calarco, J., Cates, G.D., ...
We have measured the parity-violating electroweak asymmetry in the elastic scattering of polarized electrons from the proton. The kinematic point (theta_lab = 12.3 degrees and Q^2=0.48 (GeV/c)^2) is...
Measurement of the neutral weak form-factors of the proton (1999)
Aniol, K.A., Armstrong, D.S., Baylac, M., Burtin, E., Calarco, J., Cates, G.D., ...
We have measured the parity-violating electroweak asymmetry in the elastic scattering of polarized electrons from the proton. The kinematic point (theta_lab = 12.3 degrees and Q^2=0.48 (GeV/c)^2) is...
Basic instrumentation for Hall A at Jefferson Lab
Alcorn, J., Anderson, B.D., Aniol, K.A., Annand, J.R.M., Auerbach, L., Arrington, J., ...
The instrumentation in Hall A at the Thomas Jefferson National Accelerator Facility was designed to study electro-and photo- induced reactions at very high luminosity and good momentum and angular...
Basic instrumentation for Hall A at Jefferson Lab
Alcorn, J., Anderson, B.D., Aniol, K.A., Annand, J.R.M., Auerbach, L., Arrington, J., ...
The instrumentation in Hall A at the Thomas Jefferson National Accelerator Facility was designed to study electro-and photo- induced reactions at very high luminosity and good momentum and angular...