1. Refurbishment of PHA System on AUG (2010) - SDD from PNDetector -
with cap and Be-Window
in TO8 housing
● Active volume: 10 mm2 x 450 μm
● 30 nm aluminum layer on top and 8 μm Beryllium window in cap
(avoid visible light detection)
● Hole drilled in cap for operation in vacuum (custom request)
● Internal Zr-collimator (3.2 mm diameter)
● Moderate cooling by Peltier cooler (1-stage)
● Energy resolution: 133 Mn-Ka, -20° C, 100kcps, tsh = 1 μs

2. Assembly of AUG PHA-System
- November
SDD screwed on cooled Cu-structure, then socket fixed to SDD

3. First Tests and Calibration on AUG - in-situ X-ray tube source with Cu-anode, 5 mm Be-Filter used -
then I would like to address some physics issues, and discuss
diagnostics requirements & techniques...
then I will go through selected diagnostics in a very brief manner,
addressing....
and finall make some concluding remarks
● strong line at 1.75 keV could be due to anode contamination
by tungsten (filament material)

4. (exponential + gaussians)
In-Situ Calibration of AUG SDD-Detector - by X-ray tube (Cu-Anode, 12 kV) -
red: fitted spectrum
(exponential + gaussians)
first ....
then I would like to address some physics issues, and discuss
diagnostics requirements & techniques...
then I will go through selected diagnostics in a very brief manner,
addressing....
and finall make some concluding remarks

5. Viewing Geometry of PHA on AUG
● PHA line of sight equivalent with
Single Bragg spectrometer LOS
( A-port of sector 1)
● SDD detector at
R = m
z = m
● Distances for etendu calculation:
(etendue defined by pinholes)
detector (coll. Ø = 3.2 mm )
| mm
fixed pinhole (Ø = 0.5 mm )
| mm
variable pinholes (Ø = mm)
| mm
plasma axis (R=1.7 m)
first ....
then I would like to address some physics issues, and discuss
diagnostics requirements & techniques...
then I will go through selected diagnostics in a very brief manner,
addressing....
and finall make some concluding remarks

6. First PHA Measurements on AUG with new Detector - #26116 (800 kA, 3 NBI sources) -
● X-spectrum dominated by line
radiation from highly ionized W
● typically 3 main peaks
in PHA spectra (many lines)
● trade-off between energy
resolution and count-rate
● here: digital filter optimized
for high count-rates
first ....
then I would like to address some physics issues, and discuss
diagnostics requirements & techniques...
then I will go through selected diagnostics in a very brief manner,
addressing....
and finall make some concluding remarks
68 lines from
NIST database

7. X-Ray Line Radiation - AUG #26532 -
pha26532-fit-1.ps
Nonlinear Fit (22 free parameters, red)
(4 exponential and 6x3 gaussian fit parameters)

8. Tungsten X-Ray Line Radiation - AUG #26574, high Te plasma (e-ITB) -
Fe24+
Cr22+
W62-64+
W,Cl,Ar

9. Tungsten X-Ray Line Radiation - AUG #26574, high Te plasma (e-ITB) -
Nonlinear Fit (25 free parameters, red)
(4 exponential and 7x3 gaussian fit parameters)

10. Accidental Ti-Injection - #26117 (800 kA, 3 NBI sources) -
(0.26 nm)
first ....
then I would like to address some physics issues, and discuss
diagnostics requirements & techniques...
then I will go through selected diagnostics in a very brief manner,
addressing....
and finall make some concluding remarks
● similar Ti events in s s s

11. W + Ar X-Ray Line Radiation - AUG #26580, standard H-mode -
Filter:
110 mm Be

12. 2. Strong Argon Events in X-Ray Spectra ... - #26804, 26805, ECRH -
PHA
IONEQ
simulation
● ... but Ar concentration only 2-3∙10-4

13. Te Analysis of Slope of X-Ray Continuum Radiation - #26223 (1 MA, NBI+ECRH+ICRH) -
PHA
first ....
then I would like to address some physics issues, and discuss
diagnostics requirements & techniques...
then I will go through selected diagnostics in a very brief manner,
addressing....
and finall make some concluding remarks