Add to ORKGElectron lenses for head-on beam-beam compensation will be installed in IP 10 at RHIC. Compensation of the beam-beam effect experienced at IP 8 requires betatron phase advances of {Delta}{psi} = k {center_dot} {pi} between the proton-proton interaction point at IP 8, and the electron lens at IP 10. This paper describes the lattice solutions for both the BLUE and the YELLOW ring to achieve this goal
To compensate the large beam–beam tune spread and beam–beam resonance driving terms in the polarized...
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
Since previous BEAM'06 workshop a year ago, significant progress has been made in the field of beam-...
To apply head-on beam-beam compensation for RHIC, two electron lenses are designed and will be insta...
Beam experiments have been performed in RHIC to determine some key parameters of the RHIC electron l...
Two electron lenses are under construction for RHIC to partially compensate the head-on beam-beam ef...
Two electron lenses (e-lenses) have been in operation during the 2015 RHIC physics run as part of a ...
The luminosity of the eRHIC ring-ring design is limited by the beam-beam effect exerted on the elect...
In this note we calculate the effect of the electron lense solenoids on the proton optics. Electron ...
We are designing two electron lenses (E-lens) to compensate for the large beam-beam tune spread from...
In polarized proton operation the luminosity of RHIC is limited by the head-on beam-beam effect, and...
We designed two electron lenses to apply head-on beam-beam compensation for RHIC; they will be insta...
We are designing two electron lenses (E-lens) to compensate for the large beam-beam tune spread from...
To compensate the large beam-beam tune spread and beam-beam resonance driving terms in the polarized...
Installation of electron lenses for the purpose of head-on beam-beam compensation is foreseen at RHI...
To compensate the large beam–beam tune spread and beam–beam resonance driving terms in the polarized...
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
Since previous BEAM'06 workshop a year ago, significant progress has been made in the field of beam-...
To apply head-on beam-beam compensation for RHIC, two electron lenses are designed and will be insta...
Beam experiments have been performed in RHIC to determine some key parameters of the RHIC electron l...
Two electron lenses are under construction for RHIC to partially compensate the head-on beam-beam ef...
Two electron lenses (e-lenses) have been in operation during the 2015 RHIC physics run as part of a ...
The luminosity of the eRHIC ring-ring design is limited by the beam-beam effect exerted on the elect...
In this note we calculate the effect of the electron lense solenoids on the proton optics. Electron ...
We are designing two electron lenses (E-lens) to compensate for the large beam-beam tune spread from...
In polarized proton operation the luminosity of RHIC is limited by the head-on beam-beam effect, and...
We designed two electron lenses to apply head-on beam-beam compensation for RHIC; they will be insta...
We are designing two electron lenses (E-lens) to compensate for the large beam-beam tune spread from...
To compensate the large beam-beam tune spread and beam-beam resonance driving terms in the polarized...
Installation of electron lenses for the purpose of head-on beam-beam compensation is foreseen at RHI...
To compensate the large beam–beam tune spread and beam–beam resonance driving terms in the polarized...
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
Since previous BEAM'06 workshop a year ago, significant progress has been made in the field of beam-...