scholarly journals Further tests on liquid‐nitrogen‐cooled, thin silicon‐crystal monochromators using a focused wiggler synchrotron beam

1996 ◽  
Vol 67 (9) ◽  
pp. 3350-3350 ◽  
Author(s):  
C. S. Rogers ◽  
D. M. Mills ◽  
P. B. Fernandez ◽  
G. S. Knapp ◽  
M. Wulff ◽  
...  
1995 ◽  
Vol 66 (6) ◽  
pp. 3494-3499 ◽  
Author(s):  
C. S. Rogers ◽  
D. M. Mills ◽  
W.‐K. Lee ◽  
G. S. Knapp ◽  
J. Holmberg ◽  
...  

2019 ◽  
Vol 26 (2) ◽  
pp. 382-385
Author(s):  
Joshua Stimson ◽  
Michael Ward ◽  
John Sutter ◽  
Sofia Diaz-Moreno ◽  
Simon Alcock ◽  
...  

In order to provide adequate cryogenic cooling of both existing and next-generation crystal monochromators, a new approach to produce an optimum thermal interface between the first crystal and its copper heat exchanger is proposed. This will ensure that the increased heat load deposited by higher X-ray powers can be properly dissipated. Utilizing a cylindrical silicon crystal, a tubular copper heat exchanger and by exploiting the differing thermal and mechanical properties of the two, a very good thermal interface was achieved at liquid-nitrogen temperatures. The surface flatness of the diffracting plane at one end of the cylindrical crystal was measured at room temperature while unconstrained. The crystal was then placed into the copper heat exchanger, a slide fit at room temperature, and then cooled to liquid-nitrogen temperature. At −200°C the slide fit became an interference fit. This room-temperature `loose' fit was modelled using finite-element analysis to obtain the desired fit at cryogenic temperatures by prescribing the fit at room temperature. Under these conditions, the diffraction surface was measured for distortion due to thermal and mechanical clamping forces. The total deformation was measured to be 30 nm, an order of magnitude improvement over deformation caused by cooling alone with the original side-clamped design this concept method is set to replace. This new methodology also has the advantage that it is repeatable and does not require macro-scale tools to acquire a nanometre-accuracy mounting.


1971 ◽  
Vol 30 (3) ◽  
pp. 806-810 ◽  
Author(s):  
Tetsuji Nishikawa ◽  
Shiro Suzuki ◽  
Tsuneaki Tsuru ◽  
Kuninori Endo ◽  
Takeshi Katayama ◽  
...  

2004 ◽  
Vol 70 (3) ◽  
Author(s):  
F. Barrué ◽  
M. Chevallier ◽  
D. Dauvergne ◽  
R. Kirsch ◽  
J.-C. Poizat ◽  
...  

2009 ◽  
Vol 17 (1) ◽  
pp. 6-11 ◽  
Author(s):  
Clair Collins ◽  
Neil Rowlands ◽  
Peter Statham ◽  
James Holland

Recent advances in silicon drift detector (SDD) design have set a new benchmark for Energy Dispersive X-ray spectroscopy (EDS). Not only do these detectors offer all the benefits users have come to expect from SDD—high count rates, liquid nitrogen-free analysis and excellent resolution—but large active areas and unique technology allow the user to collect EDS data at normal imaging beam currents and lower accelerating voltages in seconds.Energy Dispersive Spectrometry (EDS) has been used for many years to analyse the chemical composition of materials. Historically, EDS detectors used a bulk silicon crystal drifted with lithium. Although such Si(Li) detectors had exceptionally good performance, they had limited count rate capability and operated at very low temperatures thus requiring cooling with liquid nitrogen.


1996 ◽  
Author(s):  
Carey S. Rogers ◽  
Dennis M. Mills ◽  
Wah Keat Lee ◽  
Patricia B. Fernandez ◽  
Timothy Graber

2013 ◽  
Vol 20 (4) ◽  
pp. 567-580 ◽  
Author(s):  
Lin Zhang ◽  
Manuel Sánchez del Río ◽  
Giulio Monaco ◽  
Carsten Detlefs ◽  
Thomas Roth ◽  
...  

X-ray crystal monochromators exposed to white-beam X-rays in third-generation synchrotron light sources are subject to thermal deformations that must be minimized using an adequate cooling system. A new approach was used to measure the crystal shape profile and slope of several cryogenically cooled (liquid nitrogen) silicon monochromators as a function of beam powerin situand under heat load. The method utilizes multiple angular scans across the Bragg peak (rocking curve) at various vertical positions of a narrow-gap slit downstream from the monochromator. When increasing the beam power, the surface of the liquid-nitrogen-cooled silicon crystal deforms from a concave shape at low heat load to a convex shape at high heat load, passing through an approximately flat shape at intermediate heat load. Finite-element analysis is used to calculate the crystal thermal deformations. The simulated crystal profiles and slopes are in excellent agreement with experiments. The parameters used in simulations, such as material properties, absorbed power distribution on the crystal and cooling boundary conditions, are described in detail as they are fundamental for obtaining accurate results.


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