soft x-ray absorption and coherence analysis
DESCRIPTION
Soft X-ray Absorption and Coherence Analysis. Gabriel Weil Stanford Synchrotron Radiation Laboratory Northwestern University. Outline. Intro to Coherence and LCLS Experiment Overview: Testing Non-Redundant Array Method Against Double Pinhole Data Raw Data: Images from CCD camera - PowerPoint PPT PresentationTRANSCRIPT
Soft X-ray Absorption and Coherence Analysis
Gabriel Weil
Stanford Synchrotron Radiation Laboratory
Northwestern University
Outline
Intro to Coherence and LCLS Experiment Overview: Testing Non-Redundant
Array Method Against Double Pinhole Data Raw Data: Images from CCD camera Analysis: What to look for in the pictures Results / Conclusions: Coherence Function Aside: Absorption Experiment
What is Coherence?
Temporal: how uniform is the frequency? – measured with monochromator
Spatial: measured / detected with Young’s double slit experiment – visibility of interference fringes
A. Schawlow, Sci. Am. 219, 120 (1968)
source
Motivation: Use on LCLSUltrafast Lensless Imaging Motivation: Use on LCLSUltrafast Lensless Imaging Motivation: Use on LCLS LCLS will produce single-shot pulses with LCLS will produce single-shot pulses with
unprecedented intensity and transverse coherenceunprecedented intensity and transverse coherence Need to be able to measure transverse coherence Need to be able to measure transverse coherence
function within timescale of pulsefunction within timescale of pulse Double pinhole method requires multiple Double pinhole method requires multiple
measurements measurements not feasible on LCLS not feasible on LCLS Non-Redundant Array (NRA) method potentially Non-Redundant Array (NRA) method potentially
solves this problemsolves this problem
Double Pinhole Standard method of measuring coherence –
based on Young’s double slit experiment Produces visible interference assuming coherence
and uniform intensity in regionsource
Beamline Optics
AreaDetector
CCD
7 μm
Photon Energy: 420 eV
Double Pinhole Images
Double Pinhole Images
Non-Redundant Array (NRA)
Designed to provide complete coherence picture with a single measurement
Produces an observed interference pattern that represents the convolution ideal interference pattern with the spatial coherence function
NRA Au mask with aperture separation distances from 0.5 to 12 µm and 900 nm thickness
NRA Images
100% Relative Intensity
12.7 % Relative Intensity
5.0 % Relative Intensity
Analysis
Double pinhole:
NRA: Image is convolution of ideal diffraction pattern with spatial coherence function – need to deconvolve to extract coherence
Convolution is multiplication in Fourier space:
minmax
minmax
II
IIV
dtCItCI )()())(*(
ResultsVisibility vs. Distance at three aperture settings
(Percentage of Maximum Intensity Setting)
0
0.2
0.4
0.6
0.8
1
1.2
0 2 4 6 8
Pinhole Seperation (μm)
Fri
ng
e V
isib
ilit
y
5.0% Io
12.7% Io
2.4 % Io
100% Io
ResultsVisibility vs Distance at Undulator Peak and Blue
Edge
0
0.2
0.4
0.6
0.8
1
1.2
0 2 4 6 8
Pinhole speration (μm)
Vis
ibil
ity
Blue Edge
Undulator Peak
Absorption Experiment
Purpose was to determine cause of ‘leaking’ radiation
Samples were sputtered Au films of thickness typical to other 5-2 experiments
Tested against control evaporated Au films of comparable thickness
Results
Some dependence on gold microstructure, but small compared to deviation from theoretical values
Due to size of deviation there are probably higher harmonics being detected – this needs further study