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quantitative lamp measurements for photoresist processes, general<br />

lamp evaluation, qua<strong>li</strong>ty control, surface color measurements,<br />

photochemistry and photobiology.<br />

INNOVATIVE OPTICS<br />

The measurement optics of the LI-1800 has three major components<br />

— a filter wheel, holographic grating monochromator, and<br />

a si<strong>li</strong>con detector. The filter wheel contains seven order-sorting<br />

filters which e<strong>li</strong>minate second order harmonics and enhance<br />

stray <strong>li</strong>ght rejection by filtering out radiation that is not in the<br />

same spectral region as that being measured. The filter wheel<br />

also has a black target that serves as a dark reference for each<br />

scan.<br />

The dispersing element is a holographic grating monochromator<br />

which is available in two wavelength ranges; 300-850 nm with a<br />

4 nm bandwidth and 300-1100 nm with a 6 nm bandwidth.<br />

Optional monochromator s<strong>li</strong>ts are also available for changing the<br />

bandwidth and sensitivity to meet your app<strong>li</strong>cation.<br />

The monochromator is driven by a precision stepping motor<br />

under control of the internal microcomputer. Wavelength drive<br />

intervals are user selectable at 1, 2, 5 or 10 nm. The LI-1800’s<br />

high efficiency si<strong>li</strong>con detector and autoranging electronics<br />

allow scanning rates of over 30 nm per second.<br />

INTERNAL MICROCOMPUTER<br />

The heart of the LI-1800 system is the internal microcomputer<br />

which controls scanning and the collection, reduction and storage<br />

of data. Communication with the LI-1800 is accomp<strong>li</strong>shed<br />

using the 1800-01A Portable Terminal or any other RS-232<br />

terminal or computer. The LI-1800 is easy to use, yet powerful.<br />

A menu of simple commands covers all facets of operation from<br />

scanning to data output.<br />

SIMPLIFIED SCANNING<br />

Scanning is accomp<strong>li</strong>shed by one command; however, the<br />

LI-1800 lets you specify several parameters to get the scan you<br />

want, including wavelength <strong>li</strong>mits, wavelength drive interval,<br />

and the number of scans to average. Averaging scans provides<br />

accurate data under conditions of fluctuating radiation. Multiple<br />

scan averaging also improves sensitivity (signal to noise ratio) in<br />

low radiation conditions, since it reduces the noise level by a<br />

factor approaching the square root of the number of scans.<br />

After each scan the LI-1800 stores your data in its internal RAM<br />

memory. Standard memory in the LI-1800 is 256K bytes and is<br />

expandable to 512K bytes. The standard 256K memory typically<br />

holds 200 scans from 300-1100 nm (2 nm steps) or 530 scans<br />

from 400-700 nm.<br />

DATA REDUCTION<br />

The LI-1800’s built-in data reduction routines calculate irradiance,<br />

radiance, CIE chromaticity coordinates, illuminance,<br />

luminance, photon flux density, the ratio of spectral irradiance in<br />

two regions of a scan, and more. A data file can also be plotted<br />

on the 6000-03B Plotter/Printer using the LI-1800’s plotting<br />

routine.<br />

SPECIFICATIONS<br />

Holographic Grating Monochromator Options<br />

LI-1800/12 LI-1800/22<br />

Wavelength Range: 300-850 nm 300-1100 nm<br />

Standard Bandwidth<br />

(1/2 mm s<strong>li</strong>ts): 4 nm 6 nm<br />

Wavelength Accuracy: ± 1.5 nm ± 2 nm<br />

Wavelength<br />

Repeatabi<strong>li</strong>ty: ± 0.5 nm ± 0.5 nm<br />

Linear Dispersion: 8 nm/mm 12 nm/mm<br />

Grating:<br />

1200 grooves/mm 800 grooves/mm<br />

Automatic<br />

Filter Wheel: 6 filters 7 filters<br />

Noise Equivalent Irradiance<br />

(Standard cosine receptor, W cm -2 nm -1 )<br />

300-850 nm 300-1100 nm<br />

300 nm 6 × 10 -8 7 × 10 -8<br />

350 nm 4 × 10 -8 4 × 10 -8<br />

400 nm 2.5 × 10 -8 1.5 × 10 -8<br />

500-800 nm 8 × 10 -9 8 × 10 -9<br />

800-850 nm 2.5 × 10 -8 —<br />

800-1040 nm — 6 × 10 -9<br />

1100 nm — 1.5 × 10 -8<br />

Noise Equivalent Irradiance<br />

(1800-11 Remote Cosine Receptor, W cm -2 nm -1 )<br />

300-850 nm 300-1100 nm<br />

350 nm 2 × 10 -7 2 × 10 -7<br />

400 nm 1 × 10 -7 7 × 10 -8<br />

500-800 nm 3 × 10 -8 3.5 × 10 -8<br />

800-850 nm 1 × 10 -8 —<br />

800-1040 nm — 3 × 10 -8<br />

1100 nm — 6 × 10 -8<br />

NOTE: NEI is the noise of the instrument detector and amp<strong>li</strong>fier expressed in<br />

terms of the irradiance necessary to generate a detector output of an equivalent<br />

size. NEI values given are for standard 1/2 mm s<strong>li</strong>ts. Changing to 1 mm s<strong>li</strong>ts<br />

typically increases the sensitivity and reduces the NEI 3 to 4 times. The 1/4 mm<br />

s<strong>li</strong>ts decrease the sensitivity and increase the NEI 3 to 4 times.<br />

Maximum Irradiance Levels (W cm -2 nm -1 )<br />

300-400 nm 5 × 10 -3<br />

400-1000 nm > 1 × 10 -3<br />

Maximum irradiance levels are for 1/2 mm s<strong>li</strong>ts with standard<br />

teflon cosine receptor and filters.<br />

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