First set of data after the BS02, started on 9 Feb. Testing was restarted on 12 April 2016 with the day03 data. Testing restarted again on 9 May with int time cals.
The rough response test will also allow us to look for other straylight issues we might miss with the laser lines (more IR?).
All the raw data files and their images , Table of KEYWORDS variable |
Page Number |
Link |
Description |
Date |
1.01 |
|
Oriel lamp- All tracks and track 7 only and Laser data track 8 only every 50 nm |
Feb 9, 2016 |
1.02 |
|
Laser data track 8 only - fill in day 1 data and closer look at 2nd order signal on UV end |
Feb 9, 2016 |
Data testing restarted on 12 April |
1.03 |
|
Solar data - looking at a grey plaque for each track individually |
Apr 12, 2016 |
Data restarted again with cfg02 = 1st ever shutter block & controller installed,
and with the new LabJack aux data acq running |
1.04 |
Day 04 - 9 May Raw Data , Table |
Int time calibration data - test run - track 7 only one lamp level |
May 10, 2016 |
1.05 |
Day 05 - 10 May Raw Data , Table |
Int time calibration - full run, used lamp voltages to reduce light (but this will not be spectrally flat, color temp change) |
May 11, 2016 |
1.06 |
Day 06 - 11 May Raw Data , Table |
Int time calibration - redo using shutter between lamp and sphere (no color temp change) |
May 12, 2016 |
1.07 |
Day 07 - 12 May Raw Data , Table |
Int time calibration - redo of day 6 but with track 7 only and lamp levels going from low to high |
May 17, 2016 |
1.08 |
Day 08 - 18 May Raw Data , Table |
Int time calibration - Track 1 and 14 to see how is compares to track 7 single track - not used |
May 18, 2016 |
1.09 |
Day 09 - 19 May Raw Data , Table |
Int time calibration - Track 1 and 14 to see how is compares to track 7 single track - repeat of day 8 |
May 19, 2016 |
1.10 |
Day 10 - 26 May Raw Data , Table |
In time cal Habauzit method - The radiance was changed along with the exposure time to keep the number of counts approximately constant |
May 26, 2016 |
1.11 |
Day 11 - 28 May Raw Data , Table |
Linearity Habauzit method - all scans @ 1 sec exposure time while varying
the output of the integrating sphere |
May 28, 2016 |
|
Day 01 - Oriel data- All tracks and track 7 only and Laser data track 8 only every 50 nm |
2.01 |
|
Track selection using the day 1 lamp data |
Feb 10, 2016 |
2.02 |
Track selection - edge2edge |
Track selection using the day 1 lamp data - Edge to Edge tracks |
Feb 10, 2016 |
2.03 |
Wave cal |
Wavelength calibration from the 1 day lasers |
Feb 10, 2016 |
2.04 |
Cross Track |
Looking at Cross Track |
Feb 10, 2016 |
2.05 |
Light leaks |
Looking for ambient light leaks (none found) |
Feb 10, 2016 |
2.06 |
Track movement check |
Comparing the Resonon lamp data to the Hawaii lamp data |
Feb 10, 2016 |
2.07 |
Laser data |
Looking at all the laser data |
Feb 10, 2016 |
2.08 |
lamp data fun |
Lamp data comparing partial and full track data |
Feb 10, 2016 |
2.09 |
Track def and movement |
Looking at track definitions and how track movement affects each |
Feb 12, 2016 |
2.10 |
rel track response |
Using uncaled lampdata and ol420L10.txt lamp data to get a VERY rough idea of in-track relative response & mult MOBY data |
Feb 17, 2016 |
|
|
|
|
Day 02 - Laser data track 8 only - fill in day 1 data and closer look at 2nd order signal on UV end |
3.01 |
Laser data |
Day 2 laser data only |
Feb 11, 2016 |
3.02 |
0-30 pixel feature search |
Looking for the 0-30 pixel feature in the laser data |
Apr 6, 2016 |
3.03 |
Ghosting check |
Checking to see if light from track 1 is showing up on track 14 in the UV |
Jan 22, 2018 |
Day 03 - Solar data looking at a grey plaque for each track individually |
4.01 |
Solar data |
Solar data for each track |
Apr 12, 2016 |
4.02 |
Closer look |
A Closer look at the new features in the Solar data (track 8 and 5) |
Apr 12, 2016 |
Day 04 - Int time calibration data - test run |
5.01 |
int cal correction |
Int time check using Iris to reduce lamp levels - ADU/pix - calibration |
|
Day 05 - Int time calibration data - full run, used lamp voltages to reduce light (but this will not be spectrally flat, color temp change) |
6.01 |
cross track SLC |
Using the lamp data to look at cross track SLC |
May 17, 2016 |
6.02 |
int cal correction |
Int time check using Iris to reduce lamp levels - ADU/pix (ony high lamp levels) |
May 20, 2016 |
Day06 - Int time calibration data - redo using shutter between lamp and sphere (no color temp change) |
7.01 |
int cal (ADU/pix/sec) |
Int time check using Iris to reduce lamp levels - ADU/pix/sec |
May 12, 2016 |
7.02 |
int cal (ADU/pix) |
Int time check using Iris to reduce lamp levels - ADU/pix |
May 12, 2016 |
7.03 |
int cal correction |
Int time check using Iris to reduce lamp levels - ADU/pix - calibration |
May 16, 2016 |
Day07 - Int time calibration data - redo of day 6 but with only track 7 on |
8.01 |
int cal correction |
Int time check using Iris to reduce lamp levels - ADU/pix - calibration |
May 16, 2016 |
8.02 |
int cal comp |
Comparison of day 6 and 7 with 5th order poly fit to the data |
May 17, 2016 |
Day08 - Int time calibration data - track 1 and 14 - not used |
9.01 |
|
|
May 16, 2016 |
Day09 - Int time calibration data - redo of day 8 track1 and 14 |
10.01 |
int cal correction |
Int time check using Iris to reduce lamp levels - ADU/pix - calibration |
May 16, 2016 |
Day10 - In time cal the Habauzit method - The radiance was changed along with the exposure time to keep the number of counts approximately constant |
11.01 |
int cal Habauzit |
Int time using Habauzit method as sanity check on int cals from previous days |
May 26, 2016 |
Day11 - Linearity Habauzit method - all scans @ 1 sec exposure time while varying
the output of the integrating sphere |
12.01 |
linearity Habauzit |
Linearity using Habauzit method - but with a lamp and not a laser |
May 31, 2016 |
|
|
|
|
|
|
|
|
|
DATA PLOTS that cover many days |
100.01 |
All laser data |
Looking at all the laser data so far (day 1 and 2) |
Feb 11, 2016 |
100.02 |
All int cal |
Looking at all the integration time cal data (day 4-9) |
May 20, 2016 |
100.03 |
All int cal - clean |
Second look at the int cal data, fewer tracks and regressions (day 4-9) |
May 25, 2016 |
100.04 |
int cal regress |
Looking at regressions of the int cal data |
May 25, 2016 |
|
|
|
|
DAY 1 EMAIL from Mike |
Hi Steph,
If you are up to it, there are some BS02cfg01 data in ftp1/Mike/HI-2016-01/
I just ran the Oriel incandescent lamp with all 14 FOs at the
exit port of the 12" Spectralon sphere.
The alignment was VERY rough! See the photos.
I took 5x backgrounds with the sphere lamp light off, then
I took 5x ambients = sphere light off, then
I took 5x signals = sphere light on.
Then I found FO# 8 and coupled it alone to the sphere. See photos.
I took 5x signals = sphere light on, then
I took 1x ambient = sphere light off, then
I took 1x background
All data were collected at 0.5 sec exposure, 4x gain,
speeds= 4.25 usec Vert, 3 MHz @ 16 bit Horiz,
35/35 ms shutter delays,
CCD was -40 degC.
I think I messed up the exposure time setting though, because
at the end it looked like the max sig was ~1.5e4 ADU, but the readout plot
was showing 4e4 ADU when I was scanning (?) -
I am still having trouble running the SOLIS software...
There were no Aux data collected.
Now I'm going to try to run thru a set of laser lines with FO# 8 only.
Good Luck, MF
-------------------------------------------------------------
Hi Steph,
I just scanned 11 laser lines, at 300 : 50 : 800 nm,
for at total of 22 files = sig & bac,
all with FO# 8 only.
There is a pg. 2 of 2 log sheet for this.
There are no more photos.
That's it for today/tonight.
Luck, MF |
DAY 2 EMAIL from Mike |
Hi Steph,
Today's BS02 data are FTPing now.
There were no Aux data collected.
There were 3 log sheets.
There were 36 laser lines scanned.
All had bac & sig scans, first & last had amb scans.
All were via bare FO#8 & Ekspla.
All had same camera setup as yesterday / Day1.
I spent some time trying to pin down the 2nd order signal,
via laser lines between 339 to 360 nm.
The rest of today's lines fill in Ken's request for "300-800, every 25 or 50 nm or so". |
DAY 3 EMAIL from Mike - restarted data collection!!! |
Hello Steph,
The BS01 is in the mail to Miami, so we are back to testing the BS02!
I just did some more renaming, in /ftp1/Mike/HI-2016-01/doc
I made all BS2*.* into BS02*.* - i.e. bee ess zero two.
In there is now from today BS02cfg01_log_06.jpg
There is a new dir = /ftp1/Mike/HI-2016-01/BS2cal/day03
( and I renamed day1 & day2 dirs to day01 & day02 ).
Today I got the aux logging for BS02.
I think the connector for %RH might be flakey -
I saw the Volt-in drop out when I bumped it...
I used the long M259 Es FO#700 before Terry installs it in M261.
FO#700 bare tip was pointed at the gray plaque under somewhat
cloudy skys, then each of the 14x FOs from the BS02 bundle were
connected to the other end, and I scanned sig & bac at somewhat
differing exposure times to keep ~50k ADU signal. So there are
14x sig,bac scan pairs, plus one amb at the end called #14.
I bet you know what to look for via this data set right?
Aloha, MF |
DAY 4 EMAIL from Mike - restarted data collection!!! AGAIN |
Hello again,
I did not get very far tonight, but I did collect some data, from BS02cfg02, where cfg02 = 1st ever shutter block & controller installed,
and with the new LabJack aux data acq running.
I setup the incandescent lamp with the 12 inch Spectralon sphere,
sphere had full-open 5 inch diameter exit port. There was a TEC'ed
photodiode monitor on the sphere, read via Keithly DVM @ micro-Amp
auto-scale setting. I only ran through exposure times from 1.5 sec
down to 0.035 sec (i.e. the 35 ms shutter-delay floor). And I only
collected signal scans via Trk7 (i.e. only one shutter open).
I have some more bugs to work out with the setup tomorrow, but then
maybe we can start making LOTS of data again!
Aloha, MF
|
DAY 4 EMAIL from Mike - new aux data acquisition/logging system |
Hi Steph,
I have a new aux data acquisition/logging system for you to figure out !
This is using a LabJack DAQ, which is what Mark used to control the shutter block,
and what Art has been using for other A/D kine.
I apologize beforehand because I know it will take some work for your data processing.
I wrote up a "manual" <attached: Aux_data_via_LabJack_for_MOBY-Refresh(rev1).pdf> and collected a short test file <attached: aux2016050601=test.dat>
I think you should have all the conversion pieces to get degC & %RH data out (?),
because the hardware pieces have all been used before. The internal Resonon
degC & %RH you know aboot. The ambient degC & %RH probe is what we used
with the FISH. The extra external degC is what we used to monitor the fiber splitter
last time we did splitter stuffs. There is one change, the DAQ has a 5 Volt power supply,
and this is used to power the %RH probes (i.e. not the 3.3 Vdc we have been using
for the internal Resonon %RH). And, the same 5 Vdc source is used to get a measurable
Voltage out of the thermistors (instead of the directly measured Ohms from thermistors
we've been collection lately) - this may sound confusing, but you/we did this for the
FISH aux data via a National Instruments DAQ. There is an equation in the "manual" for how to convert the measured thermistor Voltage back to thermistor Ohms.
Once you have Ohms then you convert to degC via the Steinhart-Hart eqn/coefficents.
I am going to take my laptop into the water hut and try running the BSxxcfgyy tonight
with this new aux system. I want to start an integration time experiment. We'll see
how far I get tonight.
Aloha, MF
|
DAY 5 EMAIL from Mike |
Hi Steph,
I had to change the name on the aux file from yesterday -
it was missing a zero at/near the end.
Tonight I started by re-running the same same scans as last night =
only T7 open, with same exposure times, 1.5 thru 0.035 sec,
to see if this is repeatable.
Then I did the same exp times with all tracks illuminated.
To see if the number of tracks illuminated affects the exp time cal.
Then I continued with all tracks on, for longer exp times,
which meant stepping down the lamp voltage twice. When I had to change the lamp voltage I scanned sig & bac
at both the high & low lamp voltages, keeping the exp time same,
so we can calculate a spectral ratio to "adjust" the
lamp spectra from high to low across the lamp voltage change.
I think you might have run through this game before yes?
If this makes no sense let me know!
FileZilla & the www are complete junk tonight! <100 kB/s, >10 crashes...
I think I may have sent you a version of this aux doc yesterday
that was missing the end of pg. 1 descrip of the time stamp?
<attached: Aux_data_via_LabJack_for_MOBY-Refresh(rev1).pdf>
MF
|
DAY 5 EMAIL from Mike - new aux file fomrat and conversion |
Hi Steph,
The HTM2500LF was used as the external/ambient %RH & degC with the FISH = 1 with Blue & 1 red Red, inside the big black box house for both instruments.
Attached here is the manual <HTM25X0LF(revC).pdf>,
where pg.4 bottom equation is how to get %RH, with temperature compensation,
and my notes for pg.6 of same manual <%RH_&_NTCthermistor_06.png> which shows the eqn you need to convert thermistor Ohms to K & degC,
and my Steinhart-Hart regression coefficients for Ohms to degC<HTM2500LF_Steinhart-Hart.jpg> = coef's on pg.6 notes.
I'm going to try to dig up my MATLAB code for FISH aux,
because it seems to me there should be a Vin somewhere in the %RH eqn -
i.e. should Vout be a function of Vin ?
Maybe not, because manual pg.2 says Supply Voltage = 4.75 to 5.25 Vdc...
One (more) detail I forgot to note:
for HI-2016-01 ambient the HTM2500LF S/N = 122702-37.
Which I don't think really matters much, but I'll add that to the pdf writeup.
If I have time I'll try to add all the conversion equations & coefficients to the pdf!
MF |
DAY 5 EMAIL from Mike - new aux file fomrat and conversion |
I kinda knew this, but here are the spectral ratios for the 2x lamp Voltage changes ... which are not very flat ...
<attached: C:\data\2016\HI-2016-01\BS02cal\plots>
THat PLot I SEnt YEsterday, with the day5 10V/6V & 6V/3V spectral ratios was not correct.
It turns out one needs to ratio Net Signal (my yesterday plot ratioed Signals).
Here is the Net Signal ratio plot ... with the PD monitor ratios overplotted ...
<attached: HI-2016-01_day5_MF.png>

|
DAY 6 EMAIL from Mike |
Hi Steph,
FileZilla is running 3x faster tonight, only 2x crashes so far...
I added an iris between the lamp and the sphere today,
so we shall see if the 2x step-downs in output level are
more spectrally flat than last night...
And, I used a different input port on the integrating sphere
for the Oriel incandescent lamp + iris. This port has a small
internal baffle. This port was meant to be an input port for
a fiber optic. So there is the chance that the output port
uniformity might be better (?).
Otherwise, I repeated the all-track data from last night:
1x aux file, 2x log sheets, 26x sig&bac scans, 2x amb scans.
I also took 3x photos of the Oriel lamp setup.
MF |
DAY 6 EMAIL from Mike - updated AUX documnet |
Thank you! I am going to have to think aboot this some... MF
P.S. here is the aux doc updated w/ HTM S/N & "Ambient" naming.
<attached: Aux_data_via_LabJack_for_MOBY-Refresh(rev2).pdf> |
DAY 5-6 EMAIL from Mike - graphs |
Hi Steph,
THat PLot I SEnt YEsterday, with the day5 10V/6V & 6V/3V spectral ratios was not correct. It turns out one needs to ratio Net Signal (my yesterday plot ratioed Signals).
Here is the Net Signal ratio plot ... with the PD monitor ratios overplotted ...<attached: HI-2016-01_day5_MF.png>
And here is same for day6 via iris changes to dim the sphere output <attached: HI-2016-01_day6_MF.png>
For Day6, it would seem that we could be averaging spectral pixels ~300:900 to get an estimate of the Net Signal change to compare with the exposure time change.
Now I will look at your day6 plots!
MF

|
EMAIL from Mike - Initial integration time calibration methods and equations |
Hi Steph,
I think it might be wise to re-run day6 with only 1-trk illuminated, because there looks like some trk-to-trk diff at short exp times...
This is where errorbars might offer some insight into whether these
differences are significant - I'm thinking about this kind of plot <attached: m4int_BvsR_04jun07_3.png> where one can see that each of the 4x int cals for MOS204 had noise, and flyers,
then you try to fit a regression line and see if the individual points +- their error
are significantly different from the best-fit. In our case here, we would check
if there is really need a separate exp time cal needed for each track...
I suppose I could also change up the exposure times to fill in gaps some...
And I suppose I could reverse the order and run from low-light/long-exposure
through high-light/short-exposure...
Then we can compare day6 T7 bright-to-dim versus day7 only-T7 dim-to-bright...
MF

|
DAY 7 EMAIL from Mike - updated AUX documnet |
Hello again,
Last email for today - I promise !
Day07 data are heading your way.
Same physical setup as Day06.
Only Trk7 = open,
from dim light to bright light
3x brightness steps via 3x iris settings
from 100 sec to 0.035 sec exposure times
trying to repeat some from day4,5,6 plus some new ones.
2x log sheets, 1x aux file, 31 sig & bac scans,
62 total files, total size: 130,527,360 bytes.
Smoking fast inter webs tonight!
(oops, it just slowed down by 4x...)
(and now it did crasht...)
Aloha, MF
|
EMAIL from Mike - integration time calibration methods and equations |
Hi Steph,
Sorry this took all day to answer - I had to go back to my MOS204 notes to remember what I had done in the past and I fought with several errors (and there are at least
two more errors I found that remain un-fixed right now...).
In that plot I sent of the different fits running through the error bars for MOS204,
those fits were via TableCurve 2D - otherwise I do a 5th order regression on log-log data (!)
It looks like this has been my (approximate) int time cal processing approach for MOS2:
1.) get Net Signal ADU from lites & darks
2.) apply MOS2 thermal correction to NetSignal ADU (via TT7 temperatures)
3.) get NetSignal avg & std for BSG pix 200:500, and RSG pix 650:1000 (or other stable pix range)
4.) find the aperture-change lamp-step functions for BSG & RSG
ex. 2007 post-M236 MOS204cfg11 <attached: m4_int_1.png>
5.) compare avg+/-std BSG & RSG step functions vs expected from aperture-wheel-ratios (or monitor ratios)
5.) find spectral NetSignal ADU ratios (1024 pix) relative to 1 sec int time
... some scans will need adjustment via step-function to normalize to 1 sec lamp range ...
... these "adjustments" can be via avg or via full spectral step-functions ...
6.) get RelativeNetSignal avg & std for BSG pix 200:500, and RSG pix 650:1000
(NOTE: this std does NOT include any uncertainty from the lites & darks (i.e. SNR), but it should !)
7.) plot
> plot([-1.5 2.5],[1 1],'k'),hold on
> errorbar(log10(nomInt), avg_RelNetSigBSG./nomInt, std_RelNetSigBSG./nomInt, 'b')
> errorbar(log10(nomInt), avg_RelNetSigRSG./nomInt ,std_RelNetSigRSG./nomInt, 'r')
> xlabel('LOG10[ nominal int time ( sec ) ]'), ylabel('cal / nominal')
7.1.) compare the BSG & RSG, and typically average together to have one int time cal for both...
... AVG = avg( avgBSG avgRSG ) & STD = avg( stdBSG stdRSG )
8.) combine AVG & STD from cal #xx with all previous cals
9.) 5th order regression of "log10" data
> xdata = log10( [ cal01_nominalIntTimeSec cal02_nominalIntTimeSec ... calxx_nominalIntTimeSec ] )
> ydata = log10( [ cal01_AVGRelNetSig cal02_AVGRelNetSig ... calxx_AVGRelNetSig ] )
> myregres % 1=poly, 5=order == Dr. B.'s regress() + my tweaks
ex. MOS204 cal01 ... cal07:
Polynomial Regression: Order = 5
-------------------------------------------
i B(i) Sb(i) F(i)
0 -7.5234e-004 3.6172e-004 4.3260e+000
1 9.8470e-001 6.5196e-004 2.2812e+006
2 2.3619e-002 1.0620e-003 4.9457e+002
3 -2.1780e-002 4.3328e-004 2.5269e+003
4 9.9042e-003 5.7558e-004 2.9609e+002
5 -1.6044e-003 1.6413e-004 9.5558e+001
r^2 1.0000
Std Error of Estimate 0.0020
N 105
Degrees of Freedom 99
10.) overplot 5th order log-log regression vs errorbar() for each individual cal
... ex. <attached: m4int_regress_16May2016.png>
Clear as mud right?
MF

|
Day 08 EMAIL from Mike |
Hi Steph,
I re-ran the exp time game again again tonight, with trk#1 & 14 on. There are 2x log sheets, 1x aux file, and 35x sig & bac scans.
I repeated most day7 exp times and tried to fill in a couple holes.
I had a problem when I started log sheet pg.2-of-2, for scan #19 -
I got confused with the 0.9 & 0.8 sec scans at the bright-lite setting...
I may not have gotten scan #18 at 1 sec ?
So at the end I repeated the 1.0 sec scan as scan #35.
Sorry for any confusion there...
Aloha, MF
On 18-May-2016 18:56, Stephanie Flora wrote:
Mike
I have been looking at the data and I think is there is another issue. I think file 17 was done at the same level as file number 35, not at the middle level. When I ratio 17 and 35 to get the step down correction ratio it is 1. I am going to a thesis defense then I will be back to figure this out.
Steph
I think you are correct:
scan #17 @ 1.0 sec should have been collected at the mid-level-lamp setting,
but it is the same as scan #35 @ 1.0 sec, collected at the high-level lamp setting,
and both scans #18,19 were @ 0.9 sec, high-level lamp.
I managed to not collect the cross-step scan at the mid-level lamp.
Last night I was afraid I did something like that.
Theoretically we could use the PD monitor levels to get the mid-to-bright lamp step-factor...
Maybe suppose I should repeat this again tonight - correctly...
I'll probably go from short-exposure / bright-lamp to long-exp / dim-lamp so as
to not EXACTLY drive myself mad.
|
Day 09 EMAIL from Mike |
Hi Steph,
Tonight, for day09, I repeated last night's day08 data set,
with (hopefully) correct exposure timing control =
34x sig & bac scans + 2x log sheets + 1x aux file.
Thanks, MF
|
Pre Day 10 EMAIL from Mike |
Hi Steph,
Looking again at the Habauzit 2003 MOS Bench Unit paper, I was thinking maybe we could try two more things before
giving up with present BS02 setup:
Fig.5, Linearity
keeping exposure time at 1 sec
while varying sphere radiance level
to collect images with low counts up to high counts
Fig.6, Exposure Time
varying exposure time from low to high seconds
while also varying sphere radiance level
to keep the number of counts ~constant in order to
eliminate possible nonlinear effects
The Habauzit Fig.6 approach should be a sanity check
of what we have been doing up to now,
which did not keep constant ADU and hence convolved
any linearity effect.
Both of these approaches directly rely on the sphere monitor
for normalization - but, we do not really know much
aboot our sphere monitor, except that much of the
previous exp time step-factors seem to agree:
change-in-ADU vs change-in-PD (micro Amp DC).
So, I got close last night to writing a logger for the
PD monitor (i.e. LabVIEW reader for the Keithley 6517B electrometer),
so we will have (another) ASCII timeseries of PD level
(something I started thinking aboot in summer 2014).
MF
|
Day 10 EMAIL from Mike |
Hi Steph,
We have more BS data !
I did 2x test scans to check the FITS time stamps "DATE" & "FRAME",
by starting a 60 sec and a 1 sec exposure signal scan at precisely know
computer times ( i.e. as close as I could get to a *:00 sec & *:30 sec start times )
and, just as you thought, DATE == FRAME == start-of-exposure-time.
I ran the new LabVIEW VI to log PhotoDiode Monitor current,
to log filename = pdmon2016052601.txt. I wrote down approximate
PD microAmps as I took scans as a check against what was logging
to the file, but my program flashes the Keithley DVM front panel
and it is hard to read PD levels. I ran the logger at 200 msec dT.
I tried to repeat the Trk7 exposure time cal by the Habauzit 2003 method: "The radiance was changed along with the exposure time to keep
the number of counts approximately constant in order to eliminate
any possible nonlinear effects." So we should follow their data
processing description for Fig.6: "The averaged number of counts,
normalized to the monitor signal, was divided by the exposure time.
This result was then normalized by the count rate at 1 s to get a value
y(t) for each exposure time t."
However, it must be noted that we have no idea how linear is the
response of our PD monitor!
(PD = Labsphere D8-SI-100-TE + TEC = SphereOptics)
The "approximately constant number of counts" was 40k max,
but this was at 1 sec exp time, so there are no times < 1sec.
I think this could be remedied by starting with a brighter
lamp Voltage, and keeping max signals ~30k ADU...
Good Luck with this one! MF
|
Day 10 EMAIL #2from Mike |
Hi Steph,
I think I agree with your day10 plot,
although I get a slightly different answer <attached: HI-2016-01_day10_MF_1.png>
Here is my modified-Habauzit data processing approach:
The background image was subtracted from signal image, and counts were
averaged over spatial pixels 455:503 for Track#7 (ADU/pix). The spectral
net signal counts were divided by the exposure time (ADU/pix/sec), then
normalized to the count rate at 1 sec, and averaged over spectral pixels 200:900.
This result was then normalized to the monitor signal averaged over the exposure time.
So, from this I now have an avg & std of the PD mon over each exposure time,
and, over pix 200:900 I have an avg & std ADU/pix/sec relative to 1 sec,
from which I will try tomorrow to to combine uncertainties, from the std's,
to put errorbars on the dots...
( I guess I also have a spectral avg & std for the track over the spatial pixels... )
I think the PD mon log file helps! And the PD levels in the file agree with
what I was writing down from the Keithley front panel, so that is encouraging!
MF

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Day 11 EMAIL from Mike |
Hi Stphaine,
There are Day11 data headed your ftp way:
1x aux file + 1x pdmon file + 2x log sheet scans +
31x sig/bac sets = Habauzit 2003 linearity check,
with all scans @ 1 sec exposure time while varying
the output of the integrating sphere via open/closing
the iris on the Oriel incandescent lamp.
I am not certain if we are checking the linearity of the BS02
or if we are checking the linearity of the PhotoDiode monitor?
But it will be interesting to try to reproduce Habauzit Fig.5!
I did 7x repeats at the highest-radiance / open-iris setting
over the course of the 31 scan sets. This should tell us
something aboot the stability of this setup - I wish I had done
more 1 sec repeats last night for the exposure time check...
Looking back at my MOS int time cals, in the more recent ones
I started repeating the nominal / 1 sec scans VERY OFTEN to
try to remove any time drift of the setup during the run.
Happy LONG weekend, MF
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Day 11 EMAIL 2 from Mike |
Hi Steph,
Thanks! I was just trying to figure out how get the Habauzit Fig.5 & Eq.4 uncertainties...
I like that Steve used the Poisson sqrt( N ) estimate for delta Si !
Are your black lines linear fits ? Maybe you could show the a & b coefficients, and the r^2 & SE & N numbers?
Another thought I had for a helpful plot would be residuals from a linear fit...
I bet they might show some leftover curvature...
One other thing that might clean up the x/y axis a bit is if we show
micro Amps instead of Amps for the PD Monitor... ( or maybe not.. )
MF
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Day 11 EMAIL 3 from Mike |
Here's an example of what I was thinking r.e. micro Amps - ex. xlabel() which eliminates the 10^-8 exponentiation clutter.<attached: HI-2016-01_day11_MF_1.png> These %Std's for N=5 PD points seem encouraging to me!
I was guessing at the 200 msec data logging rate.
I think the Keithley could go faster if we need but I I'd need to understand
the autoranging which slows it down the way I'm using it now.
I just sent Labsphere an email inquiring aboot the spectral range of said PD...

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Day 11 EMAIL 4 from Mike |
I'm getting something like this:
<attached: HI-2016-01_day11_MF_2.png>
where the unc is DOMINATED by the std for 11x pix 870:880
i.e. the std for the 5x PD mon Amps are ~10x to 200x less than
than the std for the 11x relative net signals in ADU/pix/sec / A
I will want to check what I am doing here again tomorrow !

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