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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

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