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Detector Based Traceability Chain Established at the UME<br />
F.Sametoglu * , O.Bazkir, O.Celikel<br />
TUBITAK-Ulusal Metroloji Enstitusu (UME),<br />
Gebze, 41470, Kocaeli, Turkey<br />
Abstract. In UME, detector based traceability chain for<br />
radiometry and photometry was established in 2003, which<br />
is presented.<br />
1. Introduction<br />
The concept of traceability to a national laboratory is<br />
fundamental to a unified system of metrology. Metrology<br />
institutions establish their own traceability chains and<br />
cross-linkings in measurements depending on primary and<br />
secondary standards. In optical metrology this type of chain<br />
can be established either with source or detectors based<br />
standards. We developed detector-based radiometric and<br />
photometric scales and established traceability chain in<br />
measurements, which is given in Figure 1.<br />
Calibration, Fl<br />
Radiometers<br />
Power Meters<br />
Cryogenic<br />
Radiometer<br />
Absolute Optical Power<br />
Sphere<br />
Radiometer<br />
Absolute Responsivity<br />
Pyroelectrical Radiometer Trap Detector Filter Radiometer<br />
Optical Power<br />
Absolute Responsivity Absolute Responsivity<br />
Spectral Responsivity<br />
Calibration, Rl<br />
Radiometers<br />
Detectors<br />
Meters<br />
Calibration, EV<br />
Photometers<br />
Luxmeters<br />
Si Detectors<br />
Spectral Responsivity<br />
Calibration, IV<br />
Light Sources<br />
Illuminance<br />
Relative Responsivity<br />
Luminous Responsivity<br />
Calibration, RI<br />
Retroreflectors<br />
Cat Eyes<br />
Luminous Intensity<br />
Luminous Intensity<br />
Coefficient<br />
Figure 1. Traceability chain for radiometry and photometry<br />
established at the UME.<br />
2. Absolute Optical power Scale<br />
Filter Radiometer<br />
Spectral Irradiance<br />
Goniometer<br />
Luminous Flux<br />
Integrating Sphere<br />
Luminous Flux<br />
Retroreflection<br />
Coefficient<br />
Luminance<br />
Calibration, RA<br />
Retroreflectors<br />
Cat Eyes<br />
Calibration, Rl<br />
Fiber Optic<br />
Power Meters<br />
Calibration, El<br />
Radiometers<br />
Light Sources<br />
Calibration, FV<br />
Light Sources<br />
Calibration, LV<br />
Luminance Sources<br />
Luminance Meters<br />
Top of chain constitutes the absolute measurement of<br />
optical power (W) measured by using a helium-cooled<br />
electrical-substitution cryogenic radiometer (ESCR).<br />
Intensity stabilized and vertically polarized lasers (He-Ne,<br />
Ar + and Nd:YAG) are used for the realization. The<br />
measurement of optical power at each laser wavelength<br />
was performed using static substitution method by which<br />
optical temperature induced by optical heating is<br />
sandwiched between two electrical temperatures, which are<br />
slightly above and blow the optical temperature, obtained<br />
by electrical heating. Then optical power was obtained by<br />
equating it to the electrical power calculated by<br />
interpolation of an optical and two electrical temperatures<br />
and two electrical powers. Effects of all the parameters like<br />
scattering, window transmittance and imperfect cavity<br />
absorbance on the optical power were examined and the<br />
optical power scale was realized with an expanded<br />
uncertainty of a few parts of 10 4 .<br />
3. Responsivity Scale<br />
Absolute responsivity scale is based on calibration of<br />
homemade reflection type trap detectors, which consist of<br />
three Hamamatsu S1337-11 windowless silicon<br />
photodiodes, against ESCR. The absolute spectral<br />
responsivity scales for optically characterized each trap<br />
detectors were obtained at two steps. In the first step, the<br />
absolute spectral responsivities at the mentioned discrete<br />
laser wavelengths were measured. Then in the second step,<br />
developing the interpolation and extrapolation models for<br />
the internal quantum efficiency and reflectance of detectors<br />
the scale was expanded to 350 - 850 nm wavelength range<br />
with an expanded uncertainty of 0.05 %.<br />
The relative optical power and spectral responsivity<br />
scales from 250 nm to 350 and 850 nm to 2500 nm<br />
wavelength ranges were realized by calibrating the<br />
detectors against another transfer standard called as<br />
electrically calibrated pyroelectric radiometer (ECPR). The<br />
ECPR has flat response pyroelectric detector made from<br />
lithium tantalite crystal, which has permanent dipole<br />
moment. The pyroelectric detector was calibrated against<br />
ESCR and the responsivity scale was realized between 250<br />
and 2500 nm wavelength range with an expanded<br />
uncertainty of 1.74 % by using the spectral reflectance of<br />
coating of pyroelectric detector.<br />
3. Spectral Irradiance Scale<br />
Temperature-controlled home-made filter radiometers<br />
were used in order to realize spectral irradiance scale<br />
between 286 nm and 901 nm wavelength range. Filter<br />
radiometer consists of three element silicon trap detector,<br />
band-pass filters and precision aperture. The temperature<br />
of each radiometer housing including, aperture and filter<br />
can be adjusted from 18 °C to 35 °C range with stability of<br />
better than 0.05 °C using circular thermo-electric Peltier<br />
element. The irradiance scale was realized using the<br />
measurements of aperture area, transmittance of filters and<br />
* Corresponding author. Phone: +902626795000; Fax: +902626795001<br />
E-mail address: ferhat.sametoglu@ume.tubitak.gov.tr<br />
Proceedings NEWRAD, 17-19 October 2005, Davos, Switzerland 331