Lonny berman efac may 10 th 2007
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Lonny Berman EFAC May 10 th 2007. ID Beamline Optics and Damping Wigglers. Outline. Hard x-ray undulator beamline monochromator thermal modelling (silicon and diamond) Hard x-ray undulator beamline mirror modelling Damping wiggler beamline monochromator thermal modelling (silicon)

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Lonny Berman EFAC May 10 th 2007

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Lonny berman efac may 10 th 2007

Lonny BermanEFACMay 10th 2007

ID Beamline Optics and Damping Wigglers



Hard x-ray undulator beamline monochromator thermal modelling (silicon and diamond)

Hard x-ray undulator beamline mirror modelling

Damping wiggler beamline monochromator thermal modelling (silicon)

Damping wigglers: to cant or not to cant

Undulator beamline silicon monochromator

Undulator Beamline Silicon Monochromator

Simulation of “hockey-puck” liquid nitrogen cooled crystal design using 2σ beam size (1.2 mm wide x 0.75 mm high) from U14 superconducting undulator at maximum K, 30 m distance from source, 12.7º Bragg angle (corresponds to 8.9 keV for Si(111)).

Total power = 109 W (unfiltered), 92 W (filtered)

Maximum temperature = 98 K (unfiltered), 94 K (filtered)

Maximum thermal slope error in beam footprint = ±5 µrad (unfiltered), ±4 µrad (filtered)

Courtesy of Viswanath Ravindranath

Performance for longer undulators

Performance for Longer Undulators

4 m long undulator case with filter

4 m Long Undulator Case with Filter

Conclusion: for silicon, there is no better temperature for the illuminated area of the crystal to be at, than 125 K.

Action Item: investigate the use of controls and diagnostics to make sure that this is the temperature of the illuminated area of the crystal.

Using a water cooled diamond

Using a Water-Cooled Diamond

The diamond wafer is 0.5 mm thick and the (111) Bragg reflection is used (Bragg angle is 19.7º at 8.9 keV). Beam size 2.4 mm wide x 1.5 mm high (4σ).

Here, 60% of the incident power is transmitted through the crystal, and the depth dependence of the 40% absorbed power has to be taken into consideration. The transmitted power propagates through a hole in the copper substrate. There is 1 mm of overlap of the diamond wafer and copper substrate all around. A crucial consideration, in such a design, is the thermal contact between the diamond and the substrate.

Courtesy of Paul Montanez

Diamond crystal peformance

Diamond Crystal Peformance

Conclusion: pathways to improvement involve better thermal contact, larger contact area, thinner diamond to absorb less power.

Action Item: watch developments in the field, as the main challenge with diamonds is in obtaining an assured supply of large, good quality crystals.

Lonny berman efac may 10 th 2007

NSLS X25 1 m Long Vertical Focusing Mirror

demag. source,σ’


electron source

size, σ


1 m long dynamically bent palladium coated mirror, fused silica substrate.

X25 Mirror Bender System

X25 Vertical Mirror Parameters

Source to Optic = 23 m

Optic to Focus = 3.5 m

Demag = 6.6:1

measured rms slope = 1.4 μrad


perfect image size fwhm = 3.25 μm

calc. image size incl. fig. err. fwhm = 23 μm


perfect image size fwhm = 1.1 μm

calc. image size incl. fig. err. fwhm = 23 μm

3.5 m

23 m

Courtesy of James Ablett

Lonny berman efac may 10 th 2007

X25 SHADOW Ray-Tracing

X25 Mirror at NSLS-I

X25 Mirror, fwhm = 16.6 μmIdeal Mirror, fwhm = 3.2 μm

vertical [microns]

X25 Mirror

rms slope=1.4 μrad

y [μm]

Ideal Mirror

distance along mirror [cm]


X25 Mirror at NSLS-II

x [mm]

Normalized Intensity

X25 Mirror at NSLS-II

X25 Mirror, ‘width’ ~ 16 μmIdeal Mirror, fwhm = 1.03 μm

vertical [microns]

X25 Mirror

y [μm]

distance along mirror [cm]

Ideal Mirror


x [mm]

Normalized Intensity

Damping wiggler silicon monochromator

Damping Wiggler Silicon Monochromator

We looked at the same crystal design as we used for undulator beams, and studied its performance using different size wiggler beams.

The case shown here is based on a beam size of 3.6 mm wide x 2.25 mm high at 30 m from the 7 m long damping wiggler source (original design), Si(111) at 8.9 keV (Bragg angle 12.7º).

Total power = 475 W

Maximum temperature = 125 K

Maximum thermal slope error in beam footprint = ±6.6 µrad, not bad!

Courtesy of Viswanath Ravindranath

Damping wiggler mono using bigger beam

Damping Wiggler Mono Using Bigger Beam

We also looked at the case of a beam size twice as large in the horizontal and vertical directions, i.e. 7.2 mm wide x 4.5 mm high.

Total power = 1.77 kW

Maximum temperature = 355 K

Maximum thermal slope error in beam footprint = ±300 µrad

Notice that the temperature rise in this case is no longer concentrated right at the beam footprint. The crystal is too small in size to handle the power.

Conclusion: bigger beams require bigger crystals with bigger cooling interfaces.

Courtesy of Viswanath Ravindranath

Lonny berman efac may 10 th 2007

Damping Wigglers: To Cant or Not to Cant

  • Multiple yet independent damping wiggler beamlines may be accommodated in individual straight sections, either by viewing different off-axis portions of the same damping wiggler fan, or by viewing on-axis radiation emissions from separate wigglers which are canted by a few milliradians with respect to each other.

  • The larger the canting angle, the larger the impact on the emittance of the ring. E.g. if two 3.5 m long wigglers canted by 2 mrad with respect to each other are installed in each of these 8 straight sections, then the emittance increases by 8%.

Critical Energy Dependence Across Each Canted Wiggler Radiation Fan

For each fan:

Ec = Ec,max(1-[ө/өmax]2)1/2

өmax = K/γ

Ec (keV)

2 mrad

10.8 keV







ө (mrad)

Lonny berman efac may 10 th 2007

Flux Variation Across Wiggler Fan

Courtesy of Steve Hulbert

Flux Conclusion: canted damping wigglers offer no advantages for flux-dependent applications except at the highest photon energies, as compared with viewing the fan at even 1.5 mrad off-axis horizontally.

Lonny berman efac may 10 th 2007

Brightness is a Different Matter

Brightness Conclusion: when viewed at 1 mrad off-axis horizontally, the horizontal source size of a 7 m long damping wiggler will appear to be 7 mm wide, diminishing the brightness by a factor of ~20, relative to on-axis viewing.

Insertion device codes do not handle this effect correctly, but it has been empirically observed at the X25 wiggler:

Lonny Berman and Zhijian Yin (1997)

If brightness is an important consideration for a damping wiggler source, it must be viewed on-axis. The only means to achieve this, for two completely independent beamlines, is to implement canted damping wigglers.



Existing liquid nitrogen cooled silicon crystal design will handle NSLS-II undulator beams, with attention to temperature control

For water-cooled diamond crystals to be effective in NSLS-II undulator beams, attention to crystal size and thermal contact is necessary

Small mirror figure errors can introduce structure into an NSLS-II undulator focused beam as well as blur image

Liquid nitrogen cooled silicon crystal designed for an NSLS-II undulator beam could handle a damping wiggler beam with dimensions of ~4-5 mm; larger size beams will need to be handled by larger size crystals

Canted damping wigglers pose no advantage for flux-dependent applications (compared with off-axis views of a single wiggler), but will be necessary for brightness-dependent applications if more than one independent beamline per damping wiggler straight section is desired

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