Consisting of a unique arc lamp housing tightly coupled to a 0.2 meter monochromator, the Tunable KiloArc™ Illuminator is a self aligned illuminator that generates hundreds of milliwatts of intensity and offers the versatility of continuous wavelength and bandwidth selection. The wavelength can be set manually or, for ultimate flexibility, it can be scanned under computer control. The Tunable KiloArc™ Illuminator could not be easier to operate. The system is air cooled and requires no ozone venting. Simply push the start button and dial the wavelength and bandpass of output that you require. It’s that easy!
Arc Lamp Hardware
Lamp Housing
You would have to buy 6 old style vertical lamp housings to deliver the same number of photons that a KiloArc™ delivers to a single point!
At the heart of every OBB KiloArc™ is a proprietary on-axis ellipsoidal reflector. Our reflectors collect up to 70% of the radiant energy from the arc lamp, versus only 12% for typical condenser systems in vertical lamp housings. The ellipse literally wraps around the arc lamp, collecting 5 to 6 times more output power than from a conventional system.

The arc source is located at one focus points of the ellipse, and the radiation is reflected by the ellipse to the secondary focus which is actually outside of the KiloArc™. Since the light is brought to a focus by reflection rather than refraction (through a lens), there are less losses from absorption or lens-surface back-reflection. This design is so efficient that an OBB Lamp housing can deliver up to 11 times more optical power into a given smaller area than a conventional lamp housing.
Our ellipsoidal reflectors are proprietary in design and the coating used. They are NOT electro-formed reflectors, which can distort with heat, and can degrade within months. Our proprietary design ensures that distortion of the critical ellipsoid cannot occur as the lamp reaches its operating temperature. This ensures thermal stability of focus. The coating ensures reasonably long operating life, typically 2–3 years.
The KiloArc™ ellipsoidal reflector is an f/4 reflector. The f/# is important when considering matching the KiloArc™ source to some other components like, fiber optics, liquid light guides or monochromators. However f/# for an ellipsoidal reflector is not an indicator of light collection as it is in a simple lens design. The shape and size of the ellipsoidal reflector determines how much light is collected from the lamp arc. The f/# only determines the focal cone angle.
The KiloArc™ is air cooled. However since the system uses ozone free lamps, there is no ozone or venting requirements, although there is an exhaust hose adapter if you want to vent the warm air out of a lab.
The OBB KiloArc™ is a sealed arc lamp housing with a quartz window through which the focused light is delivered. Below is the spectral transmission curve for the quartz window.
Quartz Spectral Transmision Curve

Lamp
Unique Quick Release Self Aligning Lamp Replacement.

You have a choice of two lamps depending on the spectral output that you require; xenon or mercury-xenon. The lamps are provided as a complete pre-aligned assembly which includes a cooling fin and a quick release self aligning connector. Of course you may order both types of lamps as they are interchangeable.
The xenon gas used in the lamp provides continuous spectra from 180 nm to 2,500 nm at varying intensities (refer to spectral output graph). The mercury-xenon provides more of a line spectra (refer to spectral output graph). The spectral curves for xenon and mercury-xenon are normalized (relative intensities) therefore, although you cannot tell from the curves, the mercury-xenon lamp actually has greater intensities than the xenon lamp at it’s various peaks. Refer to specifications web page for detailed spectral characteristics of these two lamps.
The KiloArc™ uses ozone free quartz lamps which cut off the deep UV below 240 nm.
Typical lamp lifetime is 1,500 hrs. The lamp lifetime is highly dependent on operating conditions. Lamps should not be operated above their rated wattage (1,000 W).
Lamp Spectrum Band Pass Intensity Charts
Xenon Lamp Spectrum

Xenon Intensity Chart
Wavelength |
% output |
Wavelength |
% output |
Wavelength |
%output |
Wavelength |
% output |
| 250-300 |
2.489 |
750-800 |
4.682 |
1250-1300 |
0.896 |
1750-1800 |
0.345 |
| 300-350 |
3.540 |
800-850 |
8.914 |
1300-1350 |
0.705 |
1800-1850 |
0.306 |
| 350-400 |
4.577 |
850-900 |
6.284 |
1350-1400 |
0.931 |
1850-1900 |
0.306 |
| 400-450 |
5.245 |
900-950 |
6.788 |
1400-1450 |
0.919 |
1900-1950 |
0.306 |
| 450-500 |
5.626 |
950-1000 |
5.848 |
1450-1500 |
1.118 |
1950-2000 |
0.268 |
| 500-550 |
5.214 |
1000-1050 |
2.871 |
1500-1550 |
0.701 |
2000-2050 |
0.345 |
| 550-600 |
5.729 |
1050-1100 |
1.953 |
1550-1600 |
0.513 |
2050-2100 |
0.230 |
| 600-650 |
6.472 |
1100-1150 |
1.402 |
1600-1650 |
0.515 |
2100-2150 |
0.230 |
| 650-700 |
5.649 |
1150-1200 |
1.593 |
1650-1700 |
0.552 |
2150-2200 |
0.230 |
| 700-750 |
4.862 |
1200-1250 |
0.846 |
1700-1750 |
0.428 |
TOTAL |
100.000 |
Mercury/Xenon Lamp Spectrum

Mercury/Xenon Intensity Chart
Wavelength |
% output |
Wavelength |
% output |
Wavelength |
%output |
Wavelength |
% output |
| 260-270 |
2.205 |
380-390 |
0.538 |
500-510 |
0.199 |
800-900 |
3.186 |
| 270-280 |
2.678 |
390-400 |
0.488 |
510-520 |
0.199 |
900-1000 |
2.947 |
| 280-290 |
2.877 |
400-410 |
2.862 |
520-530 |
0.199 |
1000-1100 |
3.942 |
| 290-300 |
4.231 |
410-420 |
0.304 |
530-540 |
0.249 |
1100-1200 |
3.544 |
| 300-310 |
3.883 |
420-430 |
0.319 |
540-550 |
3.325 |
1200-1300 |
2.190 |
| 310-320 |
5.730 |
430-440 |
5.207 |
550-560 |
1.563 |
1300-1400 |
4.580 |
| 320-330 |
0.538 |
440-450 |
0.498 |
560-570 |
0.249 |
1400-1500 |
2.091 |
| 330-340 |
1.572 |
450-460 |
0.199 |
570-580 |
3.463 |
1500-1600 |
2.449 |
| 340-350 |
0.448 |
460-470 |
0.199 |
580-590 |
4.908 |
1600-1700 |
2.051 |
| 350-360 |
0.886 |
470-480 |
0.199 |
590-600 |
0.521 |
1700-1800 |
2.190 |
| 360-370 |
8.403 |
480-490 |
0.229 |
600-700 |
3.467 |
1800-1900 |
1.990 |
| 370-380 |
1.473 |
490-500 |
0.483 |
700-800 |
2.041 |
1900-2000 |
1.990 |
Power Supply
The KiloArc™ illuminator has a dedicated 1,000 watt power supply and igniter built into it. The power supply is a high efficiency switch-mode type supply. It is rated at 1,200 watts to ensure that it is not operated at the limit of its range. This provides better stability and longer lifetime when operated at 1,000 W. The KiloArc™ has triple shielding and electronic filtering to ensure that there is no RF transmitted or radiated out of the illuminator to interfere with sensitive equipment, like computers.
Igniter
The internal igniter provides a 45 KV pulse for reliable lamp ignition. Ignition noise can disrupt, or even destroy, sensitive equipment in the vicinity of an arc lamp during start-up. This can be quite a concern in a crowded lab environment. OBB Engineers carefully designed and tested the KiloArc’s triple shielding housing and electronic filtering to ensure that there is no RF transmitted or radiated out of the illuminator
KiloArc™ Power Supply and Igniter Specifications |
Input
|
210–240 V AC 50/60 Hz |
| Starting |
45 kV starting pulse |
| Power Rating |
800–1200 watts (adjustable) — recommended 800–1000 watts |
| Output Volts Compliance |
17–23 VDC |
Output Current Limit
|
70 A rms |
Smart Features
There are two LED indicators on the back, one called the “STATUS” which shows the modes of operation: cool down, stand by, or error. The other is an ERROR indication. It senses problems and displays error codes when they occur.
Particular considerations were paid to safety. The lamp chamber and power supply are constantly monitored for heat, as well as the airflow for cooling. If there are problems the lamp will shut down automatically and you will receive an appropriate error message. If the access door to the lamp is loose or open the lamp will turn off, or not ignite..
We tried to make the operation as fool proof, safe and reliable as possible, making the KiloArc™ ideal for commercial applications.
Mounting Information
In case you wanted to mount the KiloArc™ the following are the mounting options on the base plate of the supply:

Set of Feet
The KiloArc™ comes without feet on a level plate. In case you want to operate it on a surface that requires leveling, we can provide you with a set of four adjustable feet.

4-Inch Exhaust Hose Adaptor
The KiloArc™ does not generate harmful levels of ozone (less than a typical copier). It does generate some heat. Therefore venting is not a requirement, but if you do desire to vent the exhaust from the KiloArc™, select this option.
IR Absorbing Water Filter
The KiloArc™ light source is coupled to a monochromator with a light tight adapter tube which contains an IR absorbing water filter. The IR absorbing water filter is used to protect the optical elements in the monochromator from the very intense IR heat delivered by the KiloArc™ illuminator. These cylindrical metal devices are filled with water or some other IR absorbing liquid, such as copper sulfate, and have two quartz windows on either end to allow light to transmit through the absorbing solution. The cylindrical walls are water jacketed to allow cooling water to be circulated around the IR absorbing solution itself to keep it from overheating.
The standard IR absorbing water filter that comes with the Tunable KiloArc™ is made of aluminum which can be used with distilled water as the absorbing solution. There is an optional stainless steel filter that can be filled with distilled water, copper sulfate other IR absorbing liquids.
Distilled water is an excellent UV-Vis-NIR transmitter and IR absorber. It will transmit most of the light above 200 nm and absorb almost 100% of the light above 1,000 nm.
There is an optional filter mount that can be attached to the output side of either IR absorbing water filter to allow for multiple 2” square filters to be held.
Monochromator Hardware
This extremely rugged monochromator is built from a single solid metal casting that includes the base plate, optical mounts and all four sides of the unit. Inside the monochromator has extensive baffles to reduce stray light. There is an entrance and exit baffle box at the entrance and exit silts, as well as a center baffle that separates the input side from the exit side of the monochromator.
The monochromator has four optional ports that can be utilized for two inputs and two outputs. In the standard configuration it comes with one entrance and one exit port. This gives you a choice of four different input/output geometries:
180° Straight Line – with folding mirrors on entrance and exit
90° Right Angle – with folding mirror on the exit side
90° Left Angle – with folding mirror on the entrance side
360° – with no folding mirrors
 |
 |
180° Straight Line |
90° Right Angle |
 |
 |
90° Left Angle |
360° |
You can also elect as an option to have two entrance ports or two exit ports. This option adds an appropriate flipping mirror(s) and slit assemblies. The flipping mirror is manually switched to receive light from either entrance port, or to deliver light to either exit port depending on the configuration.
 |
 |
 |
Dual Exit Ports |
Dual Entrance Ports |
Dual Entrance and Exit Ports |
Slits
The monochromator slits are continuously adjustable manual slits with micrometers for adjustment. The slits also have a digital readout of the physical slit size selected. The slit housing also has a manually sliding shutter to quickly shut off or open the light path. This manual shutter has a variable height adjustment to allow you to adjust the allowable slit height.
Gratings
There is a wide selection of gratings to choose from depending on the optical requirements. All gratings are 50 x 50 mm flat gratings. The Ruled gratings have better optical throughput and Holographic gratings have improved stray light characteristics. Ruled gratings have two fundamental parameters to choose from; the groove density, expressed in grooves (or lines) per millimeter, and the blaze angle which nominally refers to the peak reflectance wavelength expressed in nanometers.
The groove density affects the resolution and mechanical scanning range of the monochromator. Below is a reference chart showing the affect groove density has on the mechanical scanning range of the monochromator as well as the reciprocal linear dispersion.
Groove Density |
Mechanical Scanning Range (nm) |
Reciprocal Linear Dispersion (nm/mm) |
| 2,400 g/mm |
0 to 550 nm |
2 nm/mm |
| 1,200 g/mm |
0 to 1,100 nm |
4 nm/mm |
| 600 g/mm |
0 to 2,200 nm |
8 nm/mm |
| 300 g/mm |
0 to 4,400 nm |
16 nm/mm |
150 g/mm |
0 to 8,800 nm |
32 nm/mm |
An optional dual grating mount allows you to select two different gratings, say to optimize throughput in different wavelength ranges. The gratings are positioned back to back and a switch dial is available at the top of the monochromator to manually choose which grating is to be used.
Below is a list of our standard gratings. Other gratings are also available upon request.
Available Gratings
Part # |
Description |
Grating Curve |
| 200 |
600 g/mm, 1,250 nm blaze |
Download Curve |
| 201 |
1,200 g/mm 300 nm blaze |
Download Curve |
| 202 |
1,200 g/mm 400 nm blaze |
Download Curve |
| 203 |
1,200 g/mm, 500 nm blaze |
Download Curve |
| 204 |
Holographic grating 300–800 nm |
Download Curve |
| 205 |
75 g/mm 10.0 µm blaze |
Download Curve |
| 206 |
150 g/mm, 4.0 µm blaze |
Download Curve |
| 207 |
300 g/mm, 2.0 µm blaze |
Download Curve |
| 209 |
600 g/mm, 750 nm blaze |
Download Curve |
| 211 |
600 g/mm 1.0 µm blaze |
Download Curve |
| 212 |
1,200 g/mm, 600 nm blaze |
Download Curve |
| 213 |
1,200 line/mm, 750 nm blaze |
Download Curve |
Wavelength Control
The monochromator wavelength is controlled with a manual dial and readout. The readout is designed to be in true wavelength in nanometers for the 1,200 g/mm grating. For other gratings you have to multiply the dial readout by a factor depending on the actual grating resolution. For example with the 600 g/mm grating you multiply the digital readout by 2 to arrive at the true wavelength position of the monochromator.
Programmable Computer Control
An optional computer control accessory is available. It includes a stepper motor assembly, an MD-1000 USB motor controller interface box and a LabVIEW* driver for computer control of the monochromator wavelength with LabVIEW software from National Instruments.
A very simple software package is also provided by OBB to remotely select the wavelength and control the shutter. Requires Windows 2000 or Windows XP operating system.
Software Screen Shots
Click to enlarge
*LabVIEW is a trade mark of National Instruments
For more information on the Tunable KiloArc™ visit the Tunable KiloArc™ Specifications page. |