We present an approach for compensating adverse effects of the detector solenoid in the SuperB Interaction Region (IR). We place compensating solenoids around the IR quadrupole magnets to reduce the magnetic fields nearly to zero. This allows more operational headroom for superconducting IR magnets and avoids saturation of ferric IR magnets. We place stronger compensating solenoids between IR magnets to reverse the magnetic field direction. This allows adjusting the total integrated solenoid field to zero, which eliminates coordinate plane rotation and reduces vertical beam displacements in the IR
This paper presents analysis of detector solenoid effects on primary disrupted beam in the ILC 14 mr...
In order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact Line...
bstract 1.1 General Assembly Layout The beam dynamics of superconducting (SC) heavy-ion inacs operat...
The SUPER-B detector solenoid has a strong 1.5 T field in the Interaction Region (IR) area, and its ...
The PEP-II experimental detector includes a strong 1.5 T solenoid field in the interaction region (I...
We examine the emittance dilution due to synchrotron radiation in the fringing fields at the end of ...
In this paper, we discuss the optics effects of the realistic detector solenoid field on beam size a...
This paper presents a method for compensating the vertical orbit change through the interaction regi...
Commissioning the compensation system of the solenoid in the BaBar detector presents a challenging p...
To achieve high luminosity, the target vertical beam size at the TESLA interaction point is 5 nm. Th...
The main sources of linear coupling in the interaction re-gions (IRS) of the Relativistic Heavy Ion ...
Future linear colliders may require a nonzero crossing angle between the two beams at the interactio...
Solenoid field (a), can be confined by the return path outer coil (b), and shield coil at the apertu...
Compensation of the effect of strong solenoidal magnetic fields on particle beams is studied. In e+e...
The beam dynamics of superconducting (SC) heavy-ion linacs operating in the velocity range below 0.4...
This paper presents analysis of detector solenoid effects on primary disrupted beam in the ILC 14 mr...
In order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact Line...
bstract 1.1 General Assembly Layout The beam dynamics of superconducting (SC) heavy-ion inacs operat...
The SUPER-B detector solenoid has a strong 1.5 T field in the Interaction Region (IR) area, and its ...
The PEP-II experimental detector includes a strong 1.5 T solenoid field in the interaction region (I...
We examine the emittance dilution due to synchrotron radiation in the fringing fields at the end of ...
In this paper, we discuss the optics effects of the realistic detector solenoid field on beam size a...
This paper presents a method for compensating the vertical orbit change through the interaction regi...
Commissioning the compensation system of the solenoid in the BaBar detector presents a challenging p...
To achieve high luminosity, the target vertical beam size at the TESLA interaction point is 5 nm. Th...
The main sources of linear coupling in the interaction re-gions (IRS) of the Relativistic Heavy Ion ...
Future linear colliders may require a nonzero crossing angle between the two beams at the interactio...
Solenoid field (a), can be confined by the return path outer coil (b), and shield coil at the apertu...
Compensation of the effect of strong solenoidal magnetic fields on particle beams is studied. In e+e...
The beam dynamics of superconducting (SC) heavy-ion linacs operating in the velocity range below 0.4...
This paper presents analysis of detector solenoid effects on primary disrupted beam in the ILC 14 mr...
In order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact Line...
bstract 1.1 General Assembly Layout The beam dynamics of superconducting (SC) heavy-ion inacs operat...