Here - PMOD/WRC
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Here - PMOD/WRC
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Relative Signal<br />
1.0E+01<br />
1.0E+00<br />
1.0E-01<br />
1.0E-02<br />
1.0E-03<br />
1.0E-04<br />
1.0E-05<br />
1.0E-06<br />
1.0E-07<br />
light are significant in the wings for measurements of all<br />
three LEDs. After the stray-light correction, the errors are<br />
reduced more than one order of magnitude, which<br />
corresponds to a reduction of measurement error in<br />
chromaticity coordinates (x, y) from 0.01 (original) to less<br />
than 0.001 (after correction) for the green LED.<br />
1.0E+01<br />
1.0E+00<br />
1.0E-01<br />
1.0E-08<br />
200 300 400 500 600 700 800<br />
Wavelength (nm)<br />
Measured Sig Corrected Sig 1 count level<br />
Relative Signal<br />
1.0E-02<br />
1.0E-03<br />
1.0E-04<br />
1.0E-05<br />
Figure 2. An example of the stray-light correction for a laser<br />
source measurement. Thick solid line: measured raw signals<br />
from the array spectrometer; thin symbol line: stray-light<br />
corrected signals; horizontal dashed line: one-count level of the<br />
15-bit array spectroradiometer.<br />
<br />
Improvement in measurement uncertainty<br />
The stray-light correction can significantly reduce the<br />
errors in both the calibration of an array spectroradiometer<br />
and measurements of test sources. Figure 3 shows plots of<br />
the raw output signal, the stray-light corrected ‘true’ signal,<br />
and the percentage of the stray-light signal relative to the<br />
‘true’ signal for a calibration of an array spectrometer<br />
system with stray light of 10 -4 , using an incandescent<br />
standard lamp. The stray-light signals are significant<br />
compared to the ‘true’ signals below 400 nm. The error<br />
without correction reaches 30 % of the ‘true’ signal at 350<br />
nm. By applying the stray-light correction, the<br />
spectroradiometer errors arising from stray light in the<br />
measurement of the standard lamp are reduced<br />
significantly below 400 nm.<br />
Relative Signal<br />
1.0E+01<br />
1.0E+00<br />
1.0E-01<br />
1.0E-02<br />
1.0E-03<br />
1.0E-04<br />
0<br />
300 400 500 600 700 800<br />
Wavelength (nm)<br />
Raw Signal Corrected Signal Stray-light Signal (%)<br />
Figure 3. Stray-light correction for calibration of the spectral<br />
responsivity of an array spectrometer system. Thick solid line:<br />
raw output signal from the spectrograph; thin solid line:<br />
stray-light corrected ‘true’ signal; thick symbol line: percentage<br />
of stray-light signal relative to the ‘true’ signal.<br />
Correction for stray light is critical when measuring<br />
test sources that have dissimilar spectra compared to that<br />
of the calibration source. As an example, an array<br />
spectroradiometer was used to measure the color of a blue<br />
LED, a green LED, and a red LED. The measurement<br />
results are shown in Figure 4. Errors arising from stray<br />
100<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
Stray-light Signal (%)<br />
1.0E-06<br />
1.0E-07<br />
200 300 400 500 600 700 800<br />
Blue raw<br />
Green raw<br />
Red raw<br />
Wavelength (nm)<br />
Blue corrected<br />
Green corrected<br />
Red corrected<br />
Figure 4. Stray-light corrections for measurements of a blue, a<br />
green, and a red LEDs. Thick solid line: measured raw signals<br />
from the spectrograph; thin symbol line: stray-light corrected<br />
signals.<br />
<br />
Conclusion<br />
A stray-light correction matrix has been developed for<br />
spectrometers to perform a simple, fast correction of<br />
stray-light errors in measured raw signals. This approach<br />
corrects stray-light errors using a simple matrix<br />
multiplication, which can be readily incorporated in an<br />
instrument’s software for real-time stray-light correction.<br />
After the correction was applied, stray-light errors were<br />
reduced by one to two orders of magnitude, to a level less<br />
than 10 -5 of the measured signal of broad-band sources,<br />
equivalent to less than one count of the 15-bit-resolution<br />
instrument. The principle of the stray-light correction can<br />
be used to correct other types of errors resulting from<br />
different mechanisms, for example, fluorescence of optical<br />
materials used in a spectrometer system. By correcting<br />
spectroradiometers for stray light, significant reductions in<br />
overall measurement uncertainties are expected in<br />
colorimetry (as shown in the LED example), radiometry,<br />
photometry, spectroscopy, and other areas where these<br />
instruments are commonly used.<br />
The theory, the validation, and the example<br />
applications of the stray-light correction matrix approach<br />
will be presented.<br />
References<br />
Brown, S. W., Johnson, B. C., Feinholz, M. E., Yarbrough, M. A.,<br />
Flora, S. J., Lykke, K. R., and Clark, D. K., Stray light<br />
correction algorithm for spectrographs, Metrologia, 40,<br />
S81-83, 2003.<br />
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