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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 />

192

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