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Optical Radiation MeasurementsSpectroradiometric Source MeasurementsTechnical Contact: Do not ship instruments or standards to the mailing address listed below. Contact the technical staff for the shipping address. Mailing Address:
back to top | back to index of optical radiation measurements Requests for the above calibration services are scheduled for completion within 90 days after the receipt of a purchase order and the test device. Spectroradiometric Source Measurements (39010C39060S)The NIST Quality System is based on the International Standard ISO/IEC 17025:1999(E) General requirements for the competence of testing and calibration laboratories. back to top | back to index of optical radiation measurements Spectral Radiance Lamps (39010C)
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| Standard | Wavelength (nm) | Typical
Values (µW cm2 nm1 sr1) |
Relative
Expanded Uncertainty (k = 2)(%) |
|---|---|---|---|
| Tungsten
strip lamp spectral radiance standard |
225 | 0.55 | 1.5 |
| 250 | 3.6 | 1.3 | |
| 350 | 3.0 x 102 | 1.0 | |
| 655 | 1.3 x 104 | 0.6 | |
| 900 | 2.2 x 104 | 0.6 | |
| 1700 | 1.1 x 104 | 0.5 | |
| 2400 | 4.0 x 103 | 0.4 |
| Standard | Wavelength (nm) | Typical
Values (µW cm2 nm1 SR1) |
Relative
Expanded Uncertainty (k = 2)(%) |
|---|---|---|---|
| Integrating
sphere source spectral radiance standard |
300 | 0.40 | 1.1 |
| 500 | 38.0 | 0.5 | |
| 700 | 120.0 | 0.4 | |
| 900 | 150.0 | 0.7 | |
| 1600 | 84.0 | 1.2 | |
| 2400 | 10.0 | 3.0 |
| Standard | Wavelength (nm) | Typical
Values (µW cm2 nm1) |
Relative
Expanded Uncertainty (k = 2)(%) |
|---|---|---|---|
| Tungsten
quartz halogen FEL lamp spectral irradiance standard |
250 | 0.02 | 1.6 |
| 350 | 0.85 | 1.1 | |
| 655 | 17.0 | 0.6 | |
| 900 | 23.0 | 0.5 | |
| 1600 | 12.0 | 0.3 | |
| 2400 | 4.0 | 0.6 |
| Standard | Wavelength (nm) | Typical
Values (µW cm2 nm1) |
Relative
Expanded Uncertainty (k = 2)(%) |
|---|---|---|---|
| Deuterium
arc lamp spectral irradiance standard |
200 | 0.04 | 5.0 |
| 250 | 0.03 | 3.1 | |
| 350 | 0.007 | 3.1 | |
| 400 | 0.005 | 3.1 |
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Figure 7.1 Measurement Uncertainty for NIST Spectral Radiance Calibrations
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Two types of spectral irradiance lamp standards are supplied by NIST. For general applications, tungstenfilament, 1000 W quartzhalogen FEL lamps are calibrated at 31 wavelengths from 250 nm to 2400 nm, or at a reduced set of wavelengths for narrower wavelength ranges. All calibrations are performed at a working distance is 50 cm. For ultraviolet applications, deuteriumarc lamps are calibrated at 21 wavelengths from 200 nm to 400 nm The deuterium lamps are intended primarily for use at wavelengths between 200 nm and 250 nm Although the shape of the spectral distribution of the deuterium lamps is stable over long periods of time, the absolute irradiance varies on the order of 12 % (k = 2). The uncertainty of the absolute irradiance can be reduced by approximately a factor of two by scaling the spectral irradiance of the deuterium lamp to the spectral irradiance of a tungstenfilament quartzhalogen FEL lamp standard over the wavelength range 250 nm to 300 nm, each time the lamp is operated.
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Spectroradiometric calibrations of integrating sphere, blackbody, and lamp sources are performed in the Facility for Automatic Spectral Calibrations (FASCAL). This instrument has the capability of performing spectral radiance measurements from 200 nm to 2500 nm and measuring radiance temperatures from 1050 K to 2700 K with an adjustable spectral bandwidth down to 0.1 nm. Spectral irradiance measurement capability from 200 nm to 2500 nm at flux levels down to 0.01 µWcm2 nm1 is also available. For both spectral radiance and irradiance measurements, a wide variety of sources and measurement geometries are possible. Other special tests requiring the capabilities of FASCAL are also performed, depending on the availability of equipment and personnel.
Figure 7.2 Measurement Uncertainty for NIST Spectral Irradiation Calibrations.
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Realization of the National Institute of Standards and Technology detectorbased spectral irradiance scale, H. W. Yoon, C. E. Gibson, and P. Y. Barnes, Applied Optics 41 (28), 5879-5890 (2002).
Longterm Temporal Stability of the National Institute of Standards and Technology Spectral Irradiance Scale Determined with Absolute Filter Radiometers, H. W. Yoon, and C. E. Gibson, Applied Optics 41 (28), 5872-5878 (2002).
Understanding Your Calibration Sources is the Key to Making Accurate Spectroradiometric Measurements, H. W. Yoon, and C. E. Gibson, OE Magazine, 48, (July 2001).
Comparison of the absolute detectorbased spectral radiance assignment with the current NISTassigned spectral radiance of tungstenstrip lamps, H. W. Yoon, and C. E. Gibson, Metrologia 37, 429432 (2000).
A CCPR international comparison of spectral radiance measurements in the airultraviolet, R. P. Lambe, R. D. Saunders, C. E. Gibson, and J. Hollandt, Metrologia 37 (1), 5154 (2000).
Results of a NIST/VNIIOFI comparison of spectralradiance measurements, R. D. Saunders, C. E. Gibson, K. D. Meilenz, V. I. Sapritsky, K. A. Sudarev, and B. B. Khlevnoy, Metrologia 3, 449 (1995).
The New International Temperature Scale of 1990 and its Effect on Radiometric, Photometric, and Colorimetric Measurements and Standards, K .D. Mielenz, R. D. Saunders, A. C. Parr, and J. J. Hsia, CIE Proc. 22nd Session Melbourne 1991 no. 91, (1991).
Results of a CCPR Intercomparison of Spectral Irradiance Measurements by National Laboratories, J. H. Walker, R. D. Saunders, J. K. Jackson, and K. D. Mielenz, J. Res. Natl. Inst. Stand. Technol. 96, 647 (1991).
The 1990 NIST Scales of Thermal Radiometry, K. D. Mielenz, R. D. Saunders, A. C. Parr, and J. J. Hsia, J. Res. Natl. Inst. Stand. Technol. 95 (6), 621629 (1990).
Spectroradiometric Determination of the Freezing Temperature of Gold, K. D. Mielenz, R. D. Saunders and J. Shumaker, J. Res. Natl. Inst. Stand. Technol., 95 (1), 4967 (Jan.Feb. 1990).
The International Temperature Scale of 1990 (ITS90), H. PrestonThomas, Metrologia 27, 2310 (1990).
NBS Measurement Services: Spectral Irradiance Calibrations, J. H. Walker, R. D. Saunders, J. K. Jackson, and D. A. McSparron, Natl. Bur. Stand. (U.S.), Spec. Publ. 25020 (Sept. 1987).
NBS Measurement Services: Spectral Radiance Calibrations, J. H. Walker, R. D. Saunders, and A. T. Hattenburg, Natl. Bur. Stand. (US), Spec. Publ. 2501 (Jan. 1987).
Spectral irradiance standard for the ultraviolet: the deuterium lamp, R. D. Saunders, W. R. Ott, and J. M. Bridges, Appl. Opt. 17, 593 (1978).
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Technical Contacts:
Jeanne M. Houston
(39071C39081S)
Tel: 301/9752327
E-mail: jeanne.houston@nist.gov
Thomas C. Larason
(39080S, 39081S, 39100S)
Tel: 301/9752334
E-mail: thomas.larason@nist.gov
George Eppeldauer
(39090S)
Tel: 301/9752338
E-mail: george.eppeldauer@nist.gov
Do not ship instruments or standards to the mailing address listed below. Contact the technical staff for the shipping address.
Mailing Address:
National Institute of Standards and Technology
100 Bureau Drive, Stop 8441
Gaithersburg, MD 208998441
Fax: 301/8695700
| Service
ID Number |
Description of Services | Fee ($) |
|---|---|---|
| 39071C | UV Silicon Photodiodes | 4402 |
| 39072C | Recalibration of UV Silicon Photodiodes | 3355 |
| 39073C | Visible to NIR Silicon Photodiodes | 4494 |
| 39074C | Recalibration of Visible to NIR Silicon Photodiodes | 3355 |
| 39075S | Special Tests of NIR Photodiodes | At Cost |
| 39077C | UV to NearInfrared Silicon Photodiodes (Hamamatsu S2281) | 5332 |
| 39078C |
Recalibration of UV to NearInfrared Silicon Photodiodes (Hamamatsu S13371010BQ or S2281) |
4193 |
| 39080S | Special Tests of Radiometric Detectors | At Cost |
| 39081S | Special Tests of Photodetector Responsivity Spatial Uniformity | At Cost |
| 39090S | Special Tests of IR Detectors | At Cost |
| 39100S | Special Tests of Irradiance Detectors | At Cost |
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This laboratory's quality system is based on the ANSI/NCSL Z54011994 standard and the ISO/IEC Guide 25.
NIST will supply the customer with a UDT Sensors, Inc. model UV100 silicon photodiode characterized in the ultraviolet (UV) spectral region. The UV silicon photodiode includes the measured spectral responsivity [A/W] from 200 nm to 500 nm in 5 nm steps. The 1 cm2 photosensitive area of the photodiodes is underfilled for the measurements with a beam of diameter 1.5 mm. The spectral responsivity is measured at radiant power levels of less than 20 µW. The bandpass of the measurement is 3 nm The spatial uniformity of responsivity over the photosensitive area is also measured at 350 nm
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Recalibration of UV silicon photodiodes previously supplied by NIST under (39071C) is performed by measuring spectral responsivity from 200 nm to 500 nm
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NIST will supply the customer with a Hamamatsu model S2281 (previously a Hamamatsu S13371010BQ) windowed silicon photodiode characterized in the visible to nearIR spectral region. The spectral responsivity of the photodiode is measured from 350 nm to 1100 nm in 5 nm steps. The 1 cm2 photosensitive area is underfilled for the measurements with a beam of diameter 1.1 mm. The spectral responsivity is measured at radiant power levels of less than 1 µW. The bandpass of the measurement is 4 nm The spatial uniformity of responsivity over the photosensitive area is also measured at 500 nm
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Recalibration of visible to nearinfrared silicon photodiodes previously supplied by NIST under (39073C) is performed by measuring spectral responsivity from 350 nm to 1100 nm The spectral range can be extended to 200 nm for an additional fee (use Test # 39078C).
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Special tests of customersupplied NIR photodiodes are performed by measuring spectral responsivity from 700 nm to 1800 nm A 1.1 mm diameter beam is centered on and underfills the photosensitive area. The spectral responsivity is measured at radiant power levels of less than 1 µW. The bandpass of the measurement is 4 nm Customers should communicate with Thomas Larason to discuss details before submitting a formal request.
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NIST will supply customers with a Hamamatsu model windowed silicon photodiode characterized in the UV to nearIR spectral region. The spectral responsivity of the photodiode is measured from 200 nm to 1100 nm in 5 nm steps. The 1 cm2 photosensitive area of the photodiode is underfilled for the measurements. The spectral responsivity is measured with a beam of diameter 1.5 mm from 200 nm to 400 nm at radiant power levels of less than 20 µW. The bandpass of the measurement is 3 nm From 405 nm to 1100 nm the spectral responsivity is measured with a beam of diameter 1.1 mm in the 400 nm to 1800 nm spectral region at power levels less than 1 µW. The bandpass of the measurement is 4 nm in this spectral region. The spatial uniformity of responsivity over the photosensitive area is also measured at 500 nm
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Recalibration of silicon photodiodes previously supplied by NIST (under 39077C or 39073C) is performed by measuring spectral responsivity from 200 nm to 1100 nm
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Special tests of radiometric detectors generally used in the ultraviolet, visible, and infrared regions of the spectrum can be performed. Detector characteristics that can be determined in this special test include spectral responsivity and quantum efficiency (electrons per photon). For example, detectors responsivity can be measured between 193 nm and 1800 nm at power levels less than 4.0 µW. The relative expanded uncertainty is dependent on the wavelength and the individual item measured. Since special tests of this type are unique, details of the tests should be discussed with Thomas Larason before submitting a formal request.
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Special tests consisting of measuring the relative changes in responsivity across the photosensitive area (spatial uniformity) can be performed for customersupplied photodetectors. The uniformity is typically measured at a single wavelength in 0.5 mm spatial increments with a beam diameter of 1.5 mm in the 193 nm to 400 nm spectral region at power levels less than 20 µW, and a beam of diameter 1.1 mm in the 400 nm to 1800 nm spectral region at power levels less than 1 µW. Customers should communicate with Thomas Larason to discuss details before submitting a formal request.
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Special tests of customersupplied ambient temperature infrared detectors can be performed in the 2 µm to 20 µm wavelength range. Measurements at longer wavelength are possible, and may be provided to customers having special requirements. The special tests include spectral power and irradiance responsivity and spatial response measurements. The standard configuration uses a 1.3 mm diameter monochromatic beam to underfill the active area of the detector with an /# between /4 and /8. The monochromator output beam is chopped (~ 39 Hz) and has a radiant power ranging from 1 µW at a wavelength of 4 µm to ~ 10 nW at 18 µm. The optical bandpass of the measurement is ~ 1 % of the test wavelength. Customers should contact George Eppeldauer to discuss details before submitting a formal request or to get information on extended measurement capability.
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Special tests of irradiance detectors generally used in the ultraviolet, visible, and nearinfrared regions of the spectrum can be performed. Irradiance responsivity of detectors can be measured between 193 nm and 1800 nm at power levels less than 200 µW/cm2. The spectral irradiance responsivity of a detector can be determined expressed in the unit amperes·mm2 per watt [A·mm2/W]. The relative expanded uncertainty is dependent on the wavelength and the individual item measured. Since special tests of this type are unique, details of the tests should be discussed with Thomas Larason before submitting a formal request.
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Table 7.2 Detector Measurement Services Uncertainties
| Wavelength [nm] |
UV 100 (UV) | S1337 (Visible) |
GE (NIR) | InGaAs (NIR) |
|---|---|---|---|---|
| 200 | 3.8 | 3.8 | ||
| 250 | 1.3 | 1.3 | ||
| 300 | 1.3 | 1.3 | ||
| 350 | 1.8 | 1.8 | ||
| 400 | 1.5 | 1.5 | ||
| 450 | 0.38 | 0.24 | ||
| 500 | 0.38 | 0.22 | ||
| 550 | 0.20 | |||
| 600 | 0.20 | |||
| 650 | 0.20 | |||
| 700 | 0.20 | 0.46 | 0.38 | |
| 750 | 0.22 | 0.42 | 0.36 | |
| 800 | 0.22 | 0.68 | 0.54 | |
| 850 | 0.22 | 0.44 | 0.44 | |
| 900 | 0.22 | 0.50 | 0.40 | |
| 950 | 2.6 | 1.2 | 1.3 | |
| 1000 | 1.7 | 0.9 | 0.9 | |
| 1050 | 2.7 | 0.9 | 0.9 | |
| 1100 | 4.2 | 0.52 | 0.50 | |
|
1150 |
0.8 | 0.8 | ||
| 1200 | 1.4 | 1.5 | ||
| 1250 | 0.9 | 0.9 | ||
| 1300 | 0.9 | 0.9 | ||
| 1350 | 0.9 | 0.9 | ||
| 1400 | 1.2 | 1.2 | ||
| 1450 | 0.9 | 0.9 | ||
| 1500 | 1.0 | 1.0 | ||
| 1550 | 1.1 | 1.1 | ||
| 1600 | 1.4 | 1.3 | ||
| 1650 | 1.1 | 1.0 | ||
| 1700 | 1.7 | 2.2 | ||
| 1750 | 2.6 | 2.7 | ||
| 1800 | 3.4 | 4.2 |
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Table 7.3. NIST Spectroradiometric Detector Measurement Services
| Service ID No. | Item of Test | Range | Relative
Expanded Uncertainty (k = 2) |
|---|---|---|---|
| 39071C | UV Silicon Photodiodes (UDT UV 100) | 200 nm to 500 nm | 0.4 % to 3.8 % |
| 39072C | Retest of UV Silicon Photodiodes | 200 nm to 500 nm | 0.4 % to 3.8 % |
| 39073C | Visible to NIR Silicon Photodiodes (Hamamatsu S2281) | 350 nm to 1100 nm | 0.2 % to 4.2 % |
| 39074C | Retest
of Visible to NIR Silicon Photodiodes (Hamamatsu S13371010BQ or S2281) |
350 nm to 1100 nm | 0.2 % to 4.2 % |
| 39075S | Special Tests of NIR Photodiodes | 700 nm to 1800 nm | 0.4 % to 4 % * |
| 39077C | Ultraviolet
to NearInfrared Silicon Photodiodes (Hamamatsu S2281) |
200 nm to 1100 nm | 0.2 % to 4.2 % |
| 39078C | Retest
of Ultraviolet to NearInfrared Silicon Photodiodes (Hamamatsu S2281) |
200 nm to 1100 nm | 0.2 % to 4.2 % |
| 39080S | Special Tests of Radiometric Detectors | 193 nm to 1800 nm | 0.2 % to 5 % * |
| 39081S | Special Tests of Photodetector Responsivity Spatial Uniformity | 193 nm to 1800 nm | 0.0024 % to 0.05 % * |
| 39090S | Special Tests of IR Detectors | 2 µm to 5.4 µm 5.4 µm to 20 µm |
~1.5 % to ~5 % |
| 39100S | Special Tests of Irradiance Detectors | 193 nm to 1800 nm | 4 % to 13 % * |
* Depends on photodetector and signal level.
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The new ultraviolet responsivity scale based on cryogenic radiometry at Synchroton Ultraviolet Radiation Facility III, P. S. Shaw, T. C. Larason, R. Gupta, S. W. Brown, R. E. Vest, and K. R. Lykke, Review of Scientific Instruments, 72, (5), (May 2001).
OptoMechanical and Electric Design of a TunnelTrap Si Radiometer, G. Eppeldauer and D. Lynch, J. Res. Natl. Inst. Stand. Technol. 105(6), 813828 (2000).
Improved NearInfrared Spectral Responsivity Scale, P. S. Shaw, T. C. Larason, R. Gupta, S. W. Brown and K. R. Lykke, J. Res. Natl. Inst. Stand. Technol. 105(5), 689 (2000).
NIST Measurement Services: Spectroradiometric Detector Measurements: Part I Ultraviolet Detectors and Part II Visible to NearInfrared Detectors, T. C. Larason, S. S. Bruce, and A. C. Parr, Natl. Inst. Stand. Technol. (US), Spec. Publ. 25041, (1998).
NIST Measurement Services: Spectroradiometric Detector Measurements: Part III Infrared Detectors, A. L. Migdall and G. Eppeldauer, Natl. Inst. Stand. Technol. (US), Spec. Publ. 25042, (1998).
National Institute of Standards and Technology highaccuracy cryogenic radiometer, T. R. Gentile, J. M. Houston, J. E. Hardis, C. L. Cromer, and A. C. Parr, Appl. Opt. 35, 10561068 (1996).
Realization of a scale of absolute spectral response using the National Institute of Standards and Technology highaccuracy cryogenic radiometer, T. R. Gentile, J. M. Houston, and C. L. Cromer, Appl. Opt. 35, 43924403 (1996).
A National Measurement System for Radiometry, Photometry, and Pyrometry Based upon Absolute Detectors, A. C. Parr, Natl. Inst. Stand. Technol. (US), Tech. Note 1421 (1996).
Developing Quality System Documentation Based on ANSI/NCSL Z54011994 The Optical Technology Division's Effort, S. S. Bruce and T. C. Larason, Natl. Inst. Stand. Technol. (US), Internal Report 5866 (1996).
High Accuracy Measurement of Aperture Area Relative to a Standard Known Aperture, J. B. Fowler and G. Dezsi, J. Res. Natl. Inst. Stand. Technol. 100(3), 277283, (1995).
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Calibration Group, NIST,
100 Bureau Drive, Stop 2300, Gaithersburg, MD 20899-2300
Telephone: 301-975-2092, Fax: 301-869-3548, E-Mail: calibrations@nist.gov
Date created: 06/30/1999
Last updated: 02/02/2006