Several modifications are described in the AGS accelerator complex for accelerating and extracting polarized proton beams. To maintain polarization during the acceleration cycle, several fast pulsed quadrupole magnets were installed around the AGS ring. A significant increase in momentum from 16.5 GeV/c, achieved in July, 84 is expected in 1985. (AIP)Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/87594/2/45_1.pd
This paper contains a brief discussion of the AGS polarized beam work in the 1980’s. It also suggest...
The Brookhaven Relativistic Heavy Ion Collider (RHIC) provides the unique opportunity to collide pol...
There are many experimental elementary particle objectives which are uniquely achievable with polari...
The unexpected importance of high energy spin effects and the success of the ZGS in correcting many ...
As the first hadron accelerator and collider consisting of two independent superconducting rings RHI...
At the AGS an intense polarized proton beam was for the first time successfully accelerated to 22 Ge...
The RHIC spin design goal assumes 2 × 1011 pro-ton/bunch with 70 % polarization. As the injector to ...
The acceleration of polarized beams in circular accelerators is complicated by the numerous depolari...
High energy polarized beam collisions will open up the unique physics opportunities of studying spin...
We have studied the feasibility of polarized proton acceleration in rhe J-PARC accelerator facility,...
To achieve high energy polarized proton collisions polarized beams first have to be accelerated whic...
Description on parts of the polarized ion source itself is given in 1975 UTTAC Annual Report. Polari...
To meet the requirements of new experiments in high energy physics and nuclear physics, a fast cycli...
The acceleration of polarized proton beams in circular accelerators is complicated by the presence o...
Dual partial snake scheme has been used for the Brookhaven AGS (Alternating Gradient Synchrotron) po...
This paper contains a brief discussion of the AGS polarized beam work in the 1980’s. It also suggest...
The Brookhaven Relativistic Heavy Ion Collider (RHIC) provides the unique opportunity to collide pol...
There are many experimental elementary particle objectives which are uniquely achievable with polari...
The unexpected importance of high energy spin effects and the success of the ZGS in correcting many ...
As the first hadron accelerator and collider consisting of two independent superconducting rings RHI...
At the AGS an intense polarized proton beam was for the first time successfully accelerated to 22 Ge...
The RHIC spin design goal assumes 2 × 1011 pro-ton/bunch with 70 % polarization. As the injector to ...
The acceleration of polarized beams in circular accelerators is complicated by the numerous depolari...
High energy polarized beam collisions will open up the unique physics opportunities of studying spin...
We have studied the feasibility of polarized proton acceleration in rhe J-PARC accelerator facility,...
To achieve high energy polarized proton collisions polarized beams first have to be accelerated whic...
Description on parts of the polarized ion source itself is given in 1975 UTTAC Annual Report. Polari...
To meet the requirements of new experiments in high energy physics and nuclear physics, a fast cycli...
The acceleration of polarized proton beams in circular accelerators is complicated by the presence o...
Dual partial snake scheme has been used for the Brookhaven AGS (Alternating Gradient Synchrotron) po...
This paper contains a brief discussion of the AGS polarized beam work in the 1980’s. It also suggest...
The Brookhaven Relativistic Heavy Ion Collider (RHIC) provides the unique opportunity to collide pol...
There are many experimental elementary particle objectives which are uniquely achievable with polari...
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