Add to ORKGIn polarized proton operation the luminosity of RHIC is limited by the head-on beam-beam effect, and methods that mitigate the effect will result in higher peak and average luminosities. Two electron lenses, one for each ring, are being constructed to partially compensate the head-on beam-beam effect in the two rings. An electron lens consists of a low energy electron beam that creates the same amplitude dependent transverse kick as the proton beam. We discuss design considerations and present the main parameters
In this note we summarize the calculated particle loss of a proton bunch in the presence of head-on ...
Electron lenses are under construction for installation in RHIC in order to mitigate the head-on bea...
The luminosity of the eRHIC ring-ring design is limited by the beam-beam effect exerted on the elect...
In polarized proton operation, the performance of the Relativistic Heavy Ion Collider (RHIC) is limi...
Two electron lenses are under construction for RHIC to partially compensate the head-on beam-beam ef...
In polarized proton operation, the performance of the Relativistic Heavy Ion Collider (RHIC) is limi...
To compensate the beam-beam tune spread and beam-beam resonance driving terms in the polarized proto...
In polarized proton operation the RHIC performance is limited by the head-on beam-beam effect. To ov...
Beam experiments have been performed in RHIC to determine some key parameters of the RHIC electron l...
To compensate the large beam-beam tune spread and beam-beam resonance driving terms in the polarized...
Two electron lenses (e-lenses) have been in operation during the 2015 RHIC physics run as part of a ...
To compensate the large beam–beam tune spread and beam–beam resonance driving terms in the polarized...
International audienceTwo electron lenses (e-lenses) have been in operation during the 2015 RHIC phy...
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
To apply head-on beam-beam compensation for RHIC, two electron lenses are designed and will be insta...
In this note we summarize the calculated particle loss of a proton bunch in the presence of head-on ...
Electron lenses are under construction for installation in RHIC in order to mitigate the head-on bea...
The luminosity of the eRHIC ring-ring design is limited by the beam-beam effect exerted on the elect...
In polarized proton operation, the performance of the Relativistic Heavy Ion Collider (RHIC) is limi...
Two electron lenses are under construction for RHIC to partially compensate the head-on beam-beam ef...
In polarized proton operation, the performance of the Relativistic Heavy Ion Collider (RHIC) is limi...
To compensate the beam-beam tune spread and beam-beam resonance driving terms in the polarized proto...
In polarized proton operation the RHIC performance is limited by the head-on beam-beam effect. To ov...
Beam experiments have been performed in RHIC to determine some key parameters of the RHIC electron l...
To compensate the large beam-beam tune spread and beam-beam resonance driving terms in the polarized...
Two electron lenses (e-lenses) have been in operation during the 2015 RHIC physics run as part of a ...
To compensate the large beam–beam tune spread and beam–beam resonance driving terms in the polarized...
International audienceTwo electron lenses (e-lenses) have been in operation during the 2015 RHIC phy...
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
To apply head-on beam-beam compensation for RHIC, two electron lenses are designed and will be insta...
In this note we summarize the calculated particle loss of a proton bunch in the presence of head-on ...
Electron lenses are under construction for installation in RHIC in order to mitigate the head-on bea...
The luminosity of the eRHIC ring-ring design is limited by the beam-beam effect exerted on the elect...