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Damping Wigglers as Sources of Hard X-Rays at NSLS-II

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Hard X-Ray Wiggler Sources at NSLS-II









Oleg Chubar

X-ray source scientist, XFD, NSLS-II

Workshop on Preparation of High-Pressure Beamline Proposal

April 29, 2010

1 BROOKHAVEN SCIENCE ASSOCIATES

Wiggler Impact on NSLS-II Electron Beam Parameters

Two main phenomena associated with the process of Emission of Photons by relativistic Electrons

in High-Energy Electron Storage Rings:

- Radiation Damping (associated with classical emission) tends to reduce Electron Beam Emittance

- Quantum Fluctuations (due to discreteness of the emission “events”) result in the increase

of Electron Beam Emittance and Energy Spread

The “equilibrium” Electron Beam Emittance and Energy Spread is determined by the balance of these

two phenomena.



Basic Parameters of Electron Beam at NSLS-II

Energy 3 GeV

Max. Current 0.5 A



Bare Lattice With With

(without DW) 3 x 7 m DW 8 x 7 m DW If used in dispersion-free

Horizontal Emittance [nm] 2 0.9 0.5 straight sections at NSLS-II,

high-field wigglers would

Relative Energy Spread 0.5 x 10-3 0.89 x 10-3 1.0 x 10-3 further reduce e-beam

Horizontal RMS Size [μm]* 64 / 204 43 / 137 33 / 107 emittance, however would

Horizontal RMS Divergence [μrad]* increase energy spread

31 / 9.8 21 / 6.6 17 / 5.1

Vertical RMS Size [μm]* 4.6 / 8.2 2.9 / 5.2 2.9 / 5.2

Vertical RMS Divergence [μrad]* 4.3 / 2.4 2.7 / 1.5 2.7 / 1.5

* - Low-Beta section / High-Beta section values 2 BROOKHAVEN SCIENCE ASSOCIATES

Spectral Brightness of NSLS-II Sources









3 BROOKHAVEN SCIENCE ASSOCIATES

Spectral Flux of NSLS-II Sources









4 BROOKHAVEN SCIENCE ASSOCIATES

Wiggler Comparisons: Brightness

NSLS-II e-beam

assumed:

I = 0.5 A

εx = 0.55 nm

εy = 8 pm









5 BROOKHAVEN SCIENCE ASSOCIATES

Wiggler Comparisons:

Flux per Unit Horizontal Angle









6 BROOKHAVEN SCIENCE ASSOCIATES

Wiggler Comparisons:

Peak Flux per Unit Solid Angle









7 BROOKHAVEN SCIENCE ASSOCIATES

DW Reference Magnetic and Mechanical Design

Magnetic Design with Side Magnets: 90 mm Period, 1.85 T Peak Field at 12.5 mm Gap (T. Tanabe)

3D Magnetic Model (with reduced number of periods) Calculated Magnetic Field (RADIA)









Side Magnets





Fixed-Gap Conceptual Mechanical Design (proposal of E.Gluskin and E.Trakhtengerg, APS)

3.5 T SC Wiggler of MAX-Lab

The Structure (E. Wallen, Max-Lab)

RADIA model with reduced number of periods

Peak Magnetic Field vs Horizontal Position









Period: 61 mm

Magnetic Gap: 10 mm



Vertical Magnetic Field on the Axis Peak Magnetic Field vs Vertical Position

Example of Commercially-Available Multi-Pole SCW

Figure courtesy of Nikolay Mezentsev (BINP, Novosibirsk, Russia)

Power Output of NSLS-II IDs

Power per Unit Solid Angle

In Horizontal Median Plane In Vertical Median Plane









Total Power:

PDW90≈ 67 kW

PSCW60≈ 34 kW





11 BROOKHAVEN SCIENCE ASSOCIATES

Spectral-Angular Distributions of Emission from

2 x 3.5 m Long DW90 in “Inline” Configuration

Angular Profiles of DW Emission

at Different Photon Energies

Spectral Flux per Unit Solid Angle Horizontal Profiles









FWHM Angular Divergence of DW Emission Vertical Profiles









1/g ≈ 170 μrad

Wiggler Magnetic Fields and Electron Trajectories

DW90 Magnetic Field (RADIA) SCW60









DW90 Modeling Magnetic Field Zoom

Typical perturbations due to

imperfect magnets: ΔB/Bmax~3 x 10-3

(magnet specs: ΔBr/Br <10-2)









Horizontal Trajectory: Angle







Suggested Tolerance for

Horizontal Trajectory in DW:

|x| < 120 μm

(max. allowed deviation from Horizontal Trajectory: Coordinate

“straightness”: 20 μm)

Example of SCW Parametric Optimization

(for SOLEIL High Pressure Beamline)

Spectral Flux Per Unit Horizontal and Vertical Angles

from Wigglers with Different Periods and Peak Fields

at the Constraints on the Total Emitted Power Pmax = 30 kW, and the Total Length L  2 m

E = 2.75 GeV, I = 0.5 A, Sinusoidal Field



Photons/s/0.1%bw/mr2 at  = 50 keV W/mr2 at 20 keV <  < 100 keV









x max = 8 mr x max = 8 mr





x min = 2 mr x min = 2 mr









u  35 mm, Np  44 u  44 mm, Np  42 “Technology Limits” Data taken from:

Bmax  2.85 T Bmax  2.6 T - presentations by N.Mezentsev (BINP) and S.Kubsky (ACCEL)

F  1.6 x 1015 Ph/s/0.1%bw/mr2 F  1.2 x 1015 Ph/s/0.1%bw/mr2 - hybrid wiggler simulations by O.Marcouille

SOLEIL, 2005

In-Vacuum Wiggler W50

On-Axis Flux 3D Magnetic Model

per Unit Solid Angle (reduced number of periods)

[Ph/s/0.1%bw/mrad2]

Photon Energy: 50 keV

Pmax = 25 kW; L = 2 m

O. Marcouille

EPAC2008







Approx. “Technology Curves”

CAD Drawing









On-Axis Magnetic Field

Magnetic Force vs Gap

Example of Spectral Performance of Optimized SCW

(for SOLEIL High Pressure Beamline)



Spectral Flux per Unit Horizontal and Vertical Angles









Ptot  20 kW for all structures Ptot  30 kW, L  2 m for all structures









Wiggler for NSLS-II High Pressure Beamline could be similarly optimized to provide

maximal flux (per unit solid angle) in users’ spectral domain of interest, while satisfying

all accelerator physics constraints.



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