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Rehak, M.

Paper Title Page
MO6PFP006 Design of the NSLS II High Order Multipole Correctors* 139
 
  • M. Rehak, J. Bengtsson, G. Danby, J.W. Jackson, J. Skaritka, C.J. Spataro
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


Feasibility studies for two families of corrector magnets for NSLS-II are presented. The first family of magnets are generalizations of figure eight quadrupoles using rotationally symmetric breaks in the return yoke to fit in available space. Properties specific to figure eight magnet are identified. The second type of magnet is a combined sextupole/dipole trim.

 
MO6PFP007 Design and Measurement of the NSLS II Quadrupole Prototypes 142
 
  • M. Rehak, A.K. Jain, J. Skaritka, C.J. Spataro
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


The design and measurement of the NSLS-II ring quadrupoles prototypes are presented. These magnets are part of a larger prototype program described in [1]. Advances in software, hardware, and manufacturing have led to some new level of insight in the quest for the perfect magnet design. Three geometric features are used to minimize the first three allowed harmonics by way of optimization. Validations through measurement and confidence levels in calculations are established.

 
MO6PFP009 Design and Measurement of the NSLS II Correctors 148
 
  • G. Danby, J.W. Jackson, A.K. Jain, M. Rehak, O. Singh, J. Skaritka, C.J. Spataro
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


Discrete corrector magnets are used for the 230 horizontal and vertical steering magnets in the NSLS-II storage ring. A unique design incorporates both dipole and skew quad correctors for(DC) steering in the same magnet. Separate AC (orbit feedback) correctors have also been designed. Comparison with alternate designs are presented as well as prototype measurements

 
MO6PFP010 Design and Measurement of the NSLSII Sextupoles 151
 
  • C.J. Spataro, A.K. Jain, M. Rehak, J. Skaritka
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


The Sextupole magnets for the National Synchrotron Light Source (NSLS-II) have stringent performance requirements. These magnets have a faceted pole profile departing from the classic shape due to constraint imposed by the vacuum tube. Three different geometric features were used as parameters to minimize unallowed harmonics. Prototypes were measured and have confirmed the good field quality.

 
MO6PFP008 The Design and Construction of NSLS-II Magnets 145
 
  • J. Skaritka, J. Bengtsson, G. Danby, G. Ganetis, W. Guo, R.C. Gupta, J.W. Jackson, A.K. Jain, S.L. Kramer, S. Krinsky, Y. Li, W. Meng, B. Nash, S. Ozaki, M. Rehak, S. Sharma, C.J. Spataro, F.J. Willeke
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


NSLS-II is a new state-of-the-art medium energy synchrotron light source designed to deliver world leading brightness and flux with top-off operation for constant output. Design and engineering of NSLS-II began in 2005 and the beginning of construction and operations are expected to start in 2009 and 2015, respectively. The energy of the machine is 3Gev and the circumference 792 m. The chosen lattice requires tight on magnetic field tolerances for the ring magnets. These magnets have been designed with 3D Opera software. The required multipole field quality and alignment preclude the use of multifunctional sextupoles, leading to discrete corrector magnets in the storage ring. The corrector magnets are multifunctional and will provide horizontal and vertical steering as well as skew quadrupole. This paper describes the dipoles, quadrupoles, sextupoles, and corrector magnets design and prototyping status of the NSLS-II.

 
TU5RFP009 NSLS-II Pulsed Magnet Design Considerations 1105
 
  • R. Heese, R.P. Fliller, R. Meier, B. Parker, M. Rehak, T.V. Shaftan, F.J. Willeke, P. Zuhoski
    BNL, Upton, Long Island, New York
  • E. Weihreter
    BESSY GmbH, Berlin
 
 

NSLS-II injection system contains 13 pulsed magnets and their power supplies for injection in and extraction from the booster and injection in the storage ring. Requirement of having injection process transparent for the NSLS-II users translates into challenging specifications for the pulsed magnet design. To keep the beam jitter within 10% of radiation source size, relative kicker mismatch must be kept on 10-5 level and residual vertical field must be below few gauss in amplitude. In this paper we discuss specifications for the pulsed magnets, their preliminary design and parameters' tolerances.

 
TU5RFP012 Alternative Designs of the NSLS-II Injection Straight Section 1114
 
  • T.V. Shaftan, R.P. Fliller, R. Heese, E.D. Johnson, R. Meier, M. Rehak, F.J. Willeke
    BNL, Upton, Long Island, New York
  • E. Weihreter
    BESSY GmbH, Berlin
 
 

The NSLS-II is a state of the art 3 GeV synchrotron light source that is being developed at BNL. The 9.3 meter long injection straight section of NSLS-II storage ring currently fits a conventional injection set-up that consists of four kickers producing a closed bump together with a DC septum and a pulsed septum. In this paper we analyze alternative options based on: a) injection via a pulsed sextupole and b) injection with a Lambertson septum. We discuss dynamics of the injected and stored beams and, consequently, magnet specifications and tolerances. In conclusion we summarize advantages and drawbacks of each injection scheme.

 
TH6PFP016 Numerical Based Linear Model for Dipole Magnets 3732
 
  • Y. Li, S. Krinsky, M. Rehak
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by U.S. DOE, Contract No.DE-AC02-98CH10886


In this paper, we discuss an algorithm for constructing a numerical linear optics model for dipole magnets from a 3D field map. The difference between the numerical model and K. Brown’s analytic approach is investigated and clarified. It was found that the optics distortion due to the dipoles’ fringe focusing must be properly taken into account to accurately determine the chromaticities. In NSLS-II, there are normal dipoles with 35-mm gap and dipoles for infrared sources with 90-mm gap. This linear model of the dipole magnets is applied to the NSLS-II lattice design to match optics parameters between the DBA cells having dipoles with different gaps.