To increase luminosity in the Relativistic Heavy Ion Collider's (RHIC's) polarized proton 250 GeV operations, we are considering reducing {beta}* to 0.65 m at the interaction points (IPs), and increasing bunch intensity. The new working point near the 2/3 integer will used on the ramp to preserve polarization. In addition, we plan to adjust the betatron-phase advances between IP6 and IP8 to (k+1/2)*{pi} so to lower the dynamic beta-beat from the beam-beam interaction. The effects of all these changes will impact the dynamic aperture, and hence, it must be evaluated carefully. In this article, we present the results of tracking the dynamic aperture with the proposed lattices
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
Dynamic aperture evaluation of the proposed lattices for the RHIC 2009 polarized proton ru
The Future Circular Collider (FCC) design study aims to develop possible circular colliders in the p...
In this article we numerically evaluate the dynamic apertures of the proposed lattices for the comin...
In this note we carry out dynamic aperture calcuations to understand the lifetime difference between...
In the article we evaluate the dynamic apertures of the proposed lattices for the coming Relativisti...
With the updated multipole magnet eld errors in the interaction regions (IRs), detailed dynamic aper...
With the updated multipole magnet field errors in the interaction regions (IRs), detailed dynamic ap...
In the preparation for the 2011 RHIC 250 GeV polarized proton (pp) run, both experiment and simulati...
The Relativistic Heavy Ion Collider (RHIC) operation as the polarized proton collider presents uniqu...
To achieve the RHIC polarized proton enhanced luminosity goal of 150.10{sup 30} cm{sup -2}sec{sup -}...
The further improvement of RHIC luminosity performance requires more precise understanding of the RH...
After providing collisions of polarized protons at a beam energy of 100 GeV since 2001, the Relativi...
The further improvement of RHIC luminosity performance requires more precise understanding of the RH...
The Relativistic Heavy Ion Collider (RHIC) as the first high energy polarized proton collider has b...
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
Dynamic aperture evaluation of the proposed lattices for the RHIC 2009 polarized proton ru
The Future Circular Collider (FCC) design study aims to develop possible circular colliders in the p...
In this article we numerically evaluate the dynamic apertures of the proposed lattices for the comin...
In this note we carry out dynamic aperture calcuations to understand the lifetime difference between...
In the article we evaluate the dynamic apertures of the proposed lattices for the coming Relativisti...
With the updated multipole magnet eld errors in the interaction regions (IRs), detailed dynamic aper...
With the updated multipole magnet field errors in the interaction regions (IRs), detailed dynamic ap...
In the preparation for the 2011 RHIC 250 GeV polarized proton (pp) run, both experiment and simulati...
The Relativistic Heavy Ion Collider (RHIC) operation as the polarized proton collider presents uniqu...
To achieve the RHIC polarized proton enhanced luminosity goal of 150.10{sup 30} cm{sup -2}sec{sup -}...
The further improvement of RHIC luminosity performance requires more precise understanding of the RH...
After providing collisions of polarized protons at a beam energy of 100 GeV since 2001, the Relativi...
The further improvement of RHIC luminosity performance requires more precise understanding of the RH...
The Relativistic Heavy Ion Collider (RHIC) as the first high energy polarized proton collider has b...
In this note we summarize the calculated 10{sup 6} turn dynamic apertures with the proposed head-on ...
Dynamic aperture evaluation of the proposed lattices for the RHIC 2009 polarized proton ru
The Future Circular Collider (FCC) design study aims to develop possible circular colliders in the p...