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ILT 5000 Laboratory Light Meter

A Laboratory Light Meter That Functions as a Radiometer or Photometer

The ILT 5000 is a laboratory light meter that is user-configurable as a radiometer or as a photometer for measuring irradiance (W/m2), illuminance (lux), luminous or radiant intensity (candela or W/sr) as well as the total integrated dose/exposure in joules, J/cm2, lux*seconds and more. Sensors are available off-the-shelf covering the entire UV to NIR range. All systems are NIST calibrated include ISO/IEC 17025:2017 accreditation.

ILT 5000 Laboratory Light Meter Overview, Key Features & Specifications

The ILT 5000 is a laboratory light meter that is user-configurable as a radiometer or as a photometer for measuring irradiance (W/m2), illuminance (lux), luminous or radiant intensity (candela or W/sr) as well as the total integrated dose/exposure in joules, J/cm2, lux*seconds and more. Sensors are available off-the-shelf covering the entire UV to NIR range. All systems are NIST calibrated include ISO/IEC 17025:2017 accreditation.

The ILT 5000 is the replacement for the ILT 1700 light meter. Its smaller size makes it at home in both the laboratory and in the field. Advancements include rapid optical measurements for graphically profiling the output of intense pulse light sources, a broader measurement range, an iPhone app, plus built-in wireless, data storage, and rechargeable batteries. The ILT 5000 also comes with a complementary basic LabView DLL sample code, an extensive API and ILT’s DataLight III light measurement and data collection software.

ILT 5000 Key Features

The ILT 5000 replaces the former ILT 1700 light meter and provides an extended dynamic range of 10 decades.

  • 10-decade dynamic range
  • Compatible with PMT detectors
  • Wireless transmitter built-in
  • Auto-range, auto-dark, auto-sample with user control options
  • 4-20 mA output
  • “Set it & forget it” remote data logging
  • Built in rechargeable battery pack
  • Multi-system simultaneous continuous monitoring
  • LabView compatible
  • NIST-traceable / ISO17025 accredited calibrations
  • Backwards compatible with ILT 1700 SED series detectors
  • Sample rate up to 100Hz, programmable

 

The ILT 5000 can support a wide range of light measurement applications that include audience scanning laser safety, UV sterilisation (UVGI), solar measurements, photoresist & lithography, measurement of optical radiation hazard, phototherapy, photo-degradation, PPF & PPFD plant studies, and many more.

A wide range of interchangeable sensors, input optics, filters and other accessories is available that allows the user to configure their meter as either a radiometer or as a photometer for their particular type of measurement (please see “Sensors” & “Input Optics” tabs).

ILT 5000 Laboratory Light Meter Specifications

Meter Type

User Configurable Light Meter (Radiometer or Photometer)

Spectral Response

Sensor/filter dependent, from 165nm to 40µm

Available Sensors

Silicon, InGaAs, SiC and vacuum photodiodes

 

Thermopile detectors

 

Photomultiplier (PMT) detectors

 

Choice of input optics and filters

Measurements

Sensor/calibration dependent, includes the following parameters:

 

Radiant flux (Watt)

 

Irradiance (W/m2)

 

Radiant intensity (W/sr)

 

Radiance (W/sr.m2)

 

Luminous flux (lumen)

 

Illuminance (lux)

 

Luminous intensity (candela)

 

Luminance (cd/m2)

 

Dose (J/m2)

Sensor Compatibility

All ILT “xxD” series sensors (except SHD models), plus SPF025F/U and SPM068 and MPP series detectors

Measurement Range

100fA – 1mA (10 decades), automatic + manual selection

Sampling Rate

Up to 100Hz, programmable

Capture Functions

Auto-range, auto-dark, auto-sample (with user control options)

Interfaces

USB2 + Wi-Fi

Signal Output

4-20mA

On-Board Data Storage

Internal, up to 16,380 readings can be stored

Calibrations

NIST traceable, ISO 17025 accredited

 

User-defined calibration facility

Dimensions

Approx. 41 x 125 x 175mm (H x W x L)

Power

Built-in rechargeable battery pack

Weight

TBA

Operating Temperature

-40 to 85°C

 

A wide range of interchangeable sensors, input optics, filters and other accessories is available that allows the user to configure their meter as either a radiometer or as a photometer for their preferred measurement. The ILT 5000 is the only light meter in the range that is compatible with high sensitivity photomultiplier tube (PMT) detectors.

The ILT 5000 light meter is compatible with the following sensors. Detector assemblies comprise the sensor, and usually also include a filter that defines the spectral response, an input optic that defined the type of radiometric or photometric parameter that can be measured and a calibration.

An example of a calibrated detector assembly for illuminance measurements in lux is “SED033/Y/W”. This comprises:

  • SED033/U, a 33mm² uncalibrated silicon photodiode sensor
  • The “Y” photopic filter
  • The “W” cosine diffuser
  • Calibration in lux

ModelMeasurementSpectral ResponseSpectral RangeDetector TypeSize (mm2)CalibrationHousingComments
SCD110/UPhotometricPhotopic400-700nmSilicon5.8UncalibratedWand-style
SCD114/UBlue RadiometricBillirubin @ 450nm422-480nmSilicon5.8UncalibratedWand-styleBilirubin Phototherapy Probe
SCD145/UBlue RadiometricPhototherapy @ 450nm360-525nmSilicon5.8UncalibratedWand-style
SED005/UUV/VIS RadiometricUnfiltered250-675nmGaAsP5.2UncalibratedWand-styleQuartz window
SUD005/UUndefinedUnfiltered250-675nmGaAsP5.2UncalibratedWand-styleQuartz window, underwater version
SED007/UNIR RadiometricUnfiltered850-1700nmInGaAs7.0UncalibratedCylinderical
SUD007/UNIR RadiometricUnfiltered850-1700nmInGaAs7.0UncalibratedCylindericalUnderwater version
SED033/UUndefinedUnfiltered200-1100nmSilicon33.0UncalibratedCylindericalQuartz window
SUD033/UUndefinedUnfiltered200-1100nmSilicon33.0UncalibratedCylindericalQuartz window, underwater version
SED100/UUndefinedUnfiltered200-1100nmSilicon100.0UncalibratedCylindericalQuartz window
SUD100/UUndefinedUnfiltered200-1100nmSilicon33.0UncalibratedCylindericalQuartz window, underwater version
SED185/UVUV RadiometricUnfiltered160-240nmGold cathode vacuum photodiode50.0UncalibratedCylindericalQuartz window, visible blocking
SED220/USolar Blind RadiometricUnfiltered160-320nmVacuum photodiode50.0UncalibratedCylindericalFused silica window, visible blocking
SUD220/USolar Blind RadiometricUnfiltered160-320nmVacuum photodiode50.0UncalibratedCylindericalFused silica window, visible blocking, underwater version
SED240/USolar Blind RadiometricUnfiltered185-320nmVacuum photodiode50.0UncalibratedCylindericalQuartz window, visible blocking
SUD240/USolar Blind RadiometricUnfiltered185-320nmVacuum photodiode50.0UncalibratedCylindericalQuartz window, visible blocking, underwater version
SED/254/UUVC RadiometricUVC @ 254nm249-259nmSilicon3.6UncalibratedCylinderical
SUD254/UUVC RadiometricUVC @ 254nm249-259nmSilicon3.6UncalibratedCylindericalUnderwater version
SED270/UUV RadiometricUnfiltered215-355nmSiC photodiode2.0UncalibratedCylindericalVisible blocking
SUD270/UUV RadiometricUnfiltered215-355nmSiC photodiode2.0UncalibratedCylindericalVisible blocking, underwater version
SED270C/UUVC RadiometricUVC @ 265nm230-280nmSiC photodiode2.0UncalibratedCylindericalVisible blocking
SUD270C/UUVC RadiometricUVC @ 265nm230-280nmSiC photodiode2.0UncalibratedCylindericalVisible blocking, underwater version
SED270B/UUVB RadiometricUVB @ 300-305nm265-325nmSiC photodiode2.0UncalibratedCylinderical
SUD270B/UUVB RadiometricUVB @ 300-305nm265-325nmSiC photodiode2.0UncalibratedCylindericalUnderwater version
SED623/UBroadband RadiometricUnfiltered (flat >700nm)0.2-4.2µmThermopile4.0UncalibratedCylindericalQuartz window
SED624/UBroadband RadiometricUnfiltered (flat >700nm)0.2-40µmThermopile4.0UncalibratedCylindericalKBr window
SPF025F/UVIS/NIR RadianceFlat response filter400-1064nmSilicon1.2UncalibratedPen Probe
SPD025Y/ULuminancePhotopic400-700nmSilicon1.2UncalibratedPen Probe
MPPUVAUVA IrradianceUVA315-390nmSilicon5.8UncalibratedMini Pen ProbeTeflon cosine diffuser, 8mm aperature
MPPNBBUVB IrradianceUVB @ 310-313nm290-330nmGaAsp photodiode5.2UncalibratedMini Pen ProbeTeflon cosine diffuser, 8mm aperature
MPPUVBUVB IrradianceUVB265-320nmSiC photodiode2.0UncalibratedMini Pen ProbeTeflon cosine diffuser, 8mm aperature
SPM068UV/VIS RadiometricUnfiltered230-700nmPhotomultiplier Tube (PMT)N/AUncalibrated
068_01UV/VIS RadiometricUnfiltered230-870nmPhotomultiplier Tube (PMT)N/AUncalibrated

A wide range of interchangeable sensors, input optics, filters and other accessories is available that allows the user to configure their meter as either a radiometer or as a photometer for their preferred measurement.

The input optics attached to the photodetector define the type of measurements that can be made. There are four measurement types that you can make with your light meter: the total radiant flux (Watt); the flux per unit area received, called the irradiance (W/m2); the flux emitted per unit solid angle, called the radiant intensity (W/sr); and the flux emitted per unit area per unit solid angle, called the radiance (W/sr.m2). For photometric measurements, the equivalent parameters are luminous flux (lumen), illuminance (lumen/m2 = lux), luminous intensity (lumen/sr = candela) and luminance (cd/m2).

TypeModelDescriptionComment
DiffuserPDPolycarbonate domed diffuser for VIS applications, 400 -700nm, 42mm OD
DiffuserWQuartz (1.024″ dia) wide-eye diffuser with internal dome, 200-2100nm, 42mm OD
DiffuserWUW diffuser with sealant and o-rings to allow submersion in liquids. 42mm diameter OD
DiffuserTDTeflon (21.5mm dia) dome diffuser, 200-700nm, 42mm OD
DiffuserQTTeflon (0.43” dia) diffuser with protective quartz window, 200-700nm, 42mm OD
DiffuserQT-#mmQT diffuser with aperture to measure smaller light spots. Available with 1, 3, 5 or 7mm apertures, 200-700nm
DiffuserA313Quartz (0.43″ dia) flat multi-layer diffuser, 200-2100nm, 42mm OD
DiffuserA313-#mmA313 diffuser with aperture to measure smaller light spots. Available with  1,3,5 or 7 mm apertures, 200-2100 nm
DiffuserTTeflon (0.5″ dia) diffuser in threaded filter ring.  With mating threads to allow add. optical components to attach. 42mm OD
DiffuserRAA4Right angle adapter/diffuser (0.27″ dia) with mini integrating sphere, 0.61″ dia x 0.44″ tallDesigned for use with SMA-905 fibre optics
DiffuserRAA4XRight angle adapter/diffuser (0.27” dia) with x10 attenuation, mini integrating sphere, 0.61” dia by 0.44” tallDesigned for use with SMA-905 fibre optics
DiffuserRAA5XMini right angle adapter/diffuser (0.25″ dia) with internal integrating sphere, 0.46 x 0.47 x 0.84″Designed for use with SMA-905 fibre optics
DiffuserA2Silica chips in a filter ring to be combined with W or WU for use on fiber optics. Requires MPS2354P2XD  to connect to fibreDesigned for use with SMA-905 fibre optics
DiffuserW5EMiniature cosine correcting diffuser with 6.35mm OD and ~10.92mm length. Threads directly onto SMA905 fibre
Laser Power AdaptorHNK15Narrow beam adapter, eliminates alignment errors.  15mm openingUsed for testing small spots of light and or collimated beams
Laser Power AdaptorK1515mm aperture and targeting aidUsed for testing small spots of light and or collimated beams
Laser Power AdaptorK99mm aperture and targeting aidUsed for testing small spots of light and or collimated beams
Fibre OpticFFO600SC1m 600µm solid core, low solar, patchcord, Kevlar jacketTo connect input optics to a sensor via an SMA patchcord
Fibre OpticFFO600FCPC1m 600µm solid core, low solar, patchcord, Kevlar jacket, FCPC to SMA-905To connect input optics to a sensor via an SMA patchcord
Fibre OpticFFO600SCW-33m 600µm solid core, patchcord, Kevlar jacket, submersibleTo connect input optics to a sensor via an SMA patchcord
Fibre OpticFFOSMA2UV1000Add description
Robert Yeo:
From website: SMA2/UV1000/1100N/SQLK6.0mm/2 Fiber Optic, UV 1000/1100 nm
To connect input optics to a sensor via an SMA patchcord
Fibre OpticFFO400UVIR1m 400µm, patchcord, SMA905, BX, 250-2500nmTo connect input optics to a sensor via an SMA patchcord
Fibre OpticFFO2501Add description
Robert Yeo:
Bndl-0.5m-56×200/220/245 LSHOH sealed at both ends for water immersion; 200 deg C max operating temperature
To connect input optics to a sensor via an SMA patchcord
Fibre OpticFFO12-SSolid tubing, rated 300 deg C, patchcord, rigid, 12″ longTo connect input optics to a sensor via an SMA patchcord
Fibre OpticFFO18-SSolid tubing, rated 300 deg C, patchcord, rigid, 18″ longTo connect input optics to a sensor via an SMA patchcord
Fibre OpticP11-2Fiber, 600 micron LSHOH, 1.97″To connect input optics to a sensor via an SMA patchcord
Fibre OpticP11-4Fiber, 600 micron LSHOH, 3.97″To connect input optics to a sensor via an SMA patchcord
Fibre OpticPIN4Contact luminance probe, fibre optic light guideRequires P6/SMA adapter
Filter RingA310Filter ring, mounts filters 25mm dia. upto 7mm thick, with 1 ¼”-24 threads
Filter RingA311Filter ring, mounts filters 25mm dia. upto 4mm thick, with 1 ¼”-24 threads
Filter RingMPS235600XDFilter ring, mounts filters 12.7mm dia. up to 4mm thick, with 1 ¼”-24 threads
Filter RingMPS235500XDFilter ring, mounts filters 12.7mm dia. up to 7mm thick, with 1 ¼”-24 threads
Right Angle ProbeRAMP12High temperature right angle probe, up to 300°CRequires P6/SMA adapter
Right Angle ProbeRAMP18High temperature right angle probe, up to 300°CRequires P6/SMA adapter
HoodHHood, internally baffled to reduce stray light and field of view.  Accepts std input optics & filtersBest for distance 25′ or less
HoodH2Hood, occlusion, with internal surface painted flat black to minimise internal reflectionsFor beam candela measurement on small light sources
LensL30-1Lens, for effective intensity of flash sources at a distance greater than 25 feet
LensRLens, radiance/luminance, 1.5° FOV
LensR1.7Lens, radiance/luminance, 1.7mrad
LensR11Lens, radiance/luminance, 11.0mrad
LensR2Lens, radiance/luminance, 2.0° FOVDesigned for use with SMA-905 fibre optics
LensR3Lens, radiance/luminance, small spot at fixed 500mm working distanceDesigned for use with SMA-905 fibre optics
AdaptorP2Adaptor, 4.3mm ID
AdaptorP6Adaptor, 12.5mm ID
AdaptorP6/SMAAdaptor, SMA-905 Designed for use with SMA-905 fibre optics
ApertureSHM30727P##Detector aperture for irradiance/illuminance measurements. Sizes (##) 1.0, 2.0, 3.0, 3.2, 4.3, 5.0 & 7.0mm dia.
Integrating SphereINS50Integrating sphere, 2″ dia, 0.276″ input port, SMA-905 adaptor to attach fibreDesigned for use with SMA-905 fibre optics
Integrating SphereINS125Integrating sphere, 5″ dia, 3 ports (2 x 20mm, 1 x 40mm)

A wide range of interchangeable sensors, input optics, filters and other accessories is available that allows the user to configure their meter as either a radiometer or as a photometer for their preferred measurement.

A photodetector would typically be fitted with an optical filter which modifies the inherent spectral response of the sensor. For a radiometer to measure the amount of monochromatic light, you only need to know the calibrated spectral response of the photodiode at the relevant wavelengths. If the light source is anything other than monochromatic (which is the case for all light sources except lasers), a radiometer with bare photodiode cannot yield absolute radiometric measurements. A “radiometric” filter can be fitted to the photodiode that normalises the response over a limited wavelength range, typically ±10% from 450-950nm, which provides a partial solution.

A radiometer can also be equipped with a filter that limits or adapts the spectral response and these are typically used in safety or medical applications where certain wavelengths are more dangerous or more efficacious than others. Examples of this are measuring the safety of UVC light sources, measuring the erythemal effectiveness of a UVB source and measuring blue phototherapy lights used for the treatment of bilirubin (jaundice in new-borns).

A photometer is similar to a radiometer, but the photodiode is equipped with a special filter that modifies the spectral sensitivity of the detector/filter combination so as to match as closely as possible that of the human vision system, defined at the CIE spectral luminous efficiency for photopic vision (“photopic” response). The photopic response of the human eye strongly favours green coloured light, with blue and red light being perceived as less intense. Thus, a photopic sensor ranks the brightness of light sources in close agreement to how the human vision system would perceive them.

Mounted in threaded (1 1/4-24 thread) black anodized rings, all filters may be repeatedly interchanged on any SED, SEL, and SHD detector. Unmounted filters and empty filter rings are also available.

Filter TypePurposeDescription
APhotoresist filterProvides an ‘A’ response (320-475nm) with silicon detectors
ACT5Actinic germicidal filterProvides an expanded actinic response or effective germicidal/bactericidal response when used with SED (SEL) 240 detector; also gives UV actinic hazard response curve per ACGIH
T2ACT5Actinic germicidal filter / diffuserCompries ACT5 actinic filter with T2X cosine diffuser
BPhotoresist filterProvides a ‘B’ response (326-401nm) with silicon detectors
BASBilirubin action spectrum filterA blue light filter that imparts a Bilirubin action spectrum onto a silicon detector
FUVCFar UV filterAn interference filter with centre wavelength at 230nm, used to block longer wavelengths for testing excimer 222nm UVGI lamps
FFlat response filterA “radiometric” filter that imparts a nominally flat spectral response when used with a silicon detector
HMR-1Hot mirrorAn IR-rejecting hot mirror, can be combined with the F filter for a flatter VIS response
NS185Narrowband UV filterAn interference filter with centre wavelength of 185nm
NSXXXNarrowband UV filterAn interference filter with bandpass of 10nm and centre wavelengths of 254, 280, 313, 335, 350 & 365nm
NSXXXCustom narrowband filterAn interference filter with custom centre wavelengths in UV, VIS & NWIR bands
NDFSS102Neutral density filter setA set of UV-IR attenuating filters mounted to fit SED (also: SEL/SHD/SL) detectors. QNDS1, QNDS2 and QNDS3 included
PAR-1Photosynthetically active radiation filterA filter tailored to be combined with silicon detectors. Combined quantum response is spectrally flat in the visible range.
QNDS1Neutral density filterQuartz filter with 10 times attenuation (10% transmittance)
QNDS2Neutral density filterQuartz filter with 100 times attenuation (1% transmittance)
QNDS3Neutral density filterQuartz filter with 1000 times attenuation (0.1% transmittance)
SCSXXXSharp cut-off filterGlass, longwave-pass filters. 60% transmittance. Cut-off wavelengths available are 280, 365, 395, 440, 465, 490, 520, 530, 545, 590, 605, 622, 650, 695, 740, 780, 810 & 830nm
BLUEBlue hazard filterFilter mounted for use with silicon detectors
TFRDFar red colour filterFilter mounted for use with silicon detectors
TREDRed colour filterFilter mounted for use with silicon detectors
TLS312Narrowband UVB filterNarrowband filter for use with GaAsP detectors, for TL-01 lamp measurement
UVAPhototherapy filterA filter, when combined with a silicon detector, produces a UVA response from 315 to 390nm (10% transmittance)
UVB-1Phototherapy filterA filter, when combined with a solar blind vacuum photodiode, produces a response from 265 to 332nm
UVB-2Phototherapy filterA filter set that includes both shortwave-pass and longwave-pass filters to block UVC and UVA. Passes light from 280-310nm
UVFFlat response UV filterA filter that imparts a flat response onto the 005 series UV-Visible GaAsP detector over a range of ~350-405nm (full range 275-450nm)
WBSXXXWideband filterMounted glass filters with center wavelength at XXXnm. Note that many WBS filters cannot be used with silicon sensors due to a secondary response in the IR, so they are typically sold with the SED (SEL)005. Centre wavelengths available are 320, 350, 375, 400, 405, 440, 460, 465, 480 & 520nm
Y4Photopic filterA filter, when combined with a silicon detector, matches the CIE standard photopic observer function. F1′ of 1.6% when used with SED033 and SED100 detectors
ZCIEScotopic filterA filter, when combined with a silicon detector, matches the CIE standard scotopic observer function
ZPMScotopic filterA filter, when combined with the SCM068-1 PMT, matches the CIE standard scotopic observer function

The ILT 5000 is a light meter that can be user-configured as both a radiometer and a photometer. Other types of light meter are colorimeters, spectrometers and spectroradiometers, which all measure the amount of light but they operate in fundamentally different ways and have advantages and disadvantages.

Radiometers, Photometers & Colorimeters

Radiometers and photometers consist of a photodetector, an electrical readout and a calibration. The spectral response of a photodiode varies with the wavelength of the incident radiation. This means that 1 W/m2 of irradiance at 350nm in the UV will produce a different electrical current compared to 1 W/m2 of red light at 650nm.

The photodetector would typically be fitted with an optical filter which modifies the inherent spectral response of the sensor. For a radiometer to measure the amount of monochromatic light, you only need to know the calibrated spectral response of the photodiode at the relevant wavelengths. If the light source is anything other than monochromatic (which is the case for all light sources except lasers), a radiometer with bare photodiode cannot yield absolute radiometric measurements. A “radiometric” filter can be fitted to the photodiode that normalises the response over a limited wavelength range, typically ±10% from 450-950nm, which provides a partial solution.

A radiometer can also be equipped with a filter that limits or adapts the spectral response and these are typically used in safety or medical applications where certain wavelengths are more dangerous or more efficacious than others. Examples of this are measuring the safety of UVC light sources, measuring the erythemal effectiveness of a UVB source and measuring blue phototherapy lights used for the treatment of bilirubin (jaundice in new-borns).

A photometer is similar to a radiometer, but the photodiode is equipped with a special filter that modifies the spectral sensitivity of the detector/filter combination so as to match as closely as possible that of the human vision system, defined at the CIE spectral luminous efficiency for photopic vision (“photopic” response). The photopic response of the human eye strongly favours green coloured light, with blue and red light being perceived as less intense. Thus, a photopic sensor ranks the brightness of light sources in close agreement to how the human vision system would perceive them.

A colorimeter is a type of photometer that combines three of four photodiodes each with a filter that closely matches the tristimulus response of the eye (the XYZ or XRXBYZ tristimulus colour matching functions). A colorimeter measures the emitted colour of the light source under test, and reports this as tristimulus values, as CIE chromaticity coordinates and as correlated colour temperature (CCT) values or as a dominant wavelength. The Y filter of a colorimeter is the same as the photopic filter in a photometer, hence a “tristimulus” colorimeter can also function as a photometer.

Spectrometers & Spectroradiometers

Whereas radiometers, photometers and colorimeters employ photodiodes with special filters, a spectroradiometer measures what is called the spectral power of the light source, which is the amount of light at each wavelength. The spectral response of the spectroradiometer is calibrated at each wavelength, which therefore avoids the error that arises from measuring the irradiance of broadband light sources with unfiltered radiometers (or even radiometers equipped with normalising filters).

From the measured spectral power, the desired radiometric, photometric or colorimetric metrics can be calculated. A spectroradiometer avoids the potentially significant errors that filtered photometers and colorimeters suffer from where the spectral response of the filtered sensor doesn’t exactly match that of the target observer, for example the photopic response of the eye. This is an important consideration; a high-quality photometer may have a average spectral mismatch (the f1’ factor) to the photopic observer of 5% over the 380-780nm visible light band, but can still yield errors of 50% or more when used to measure blue or red LEDs, for example.

A spectroradiometer is the name given to a spectrometer that is equipped with appropriate collection optics and an absolute calibration. A spectrometer is an optical instrument that employs a diffraction grating that physically separates the incident light into its component wavelengths. Each discrete wavelength is imaged onto an array photodetector, which allows for the recording of a spectral power distribution instantaneously.

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