
Triax Series Spectrographs
Affordable Triple Grating, 190 mm Focal Length, Imaging Spectrographs
Available as an imaging spectrograph or a scanning monochromator, HORIBA’s Triax triple grating spectrometer offers maximum versatility, automation, and affordability at a level of optical superiority that our users have come to expect from HORIBA. These spectrometers benefit from HORIBA’s patented and revolutionary triple grating turret assembly that has two independent axis of rotation , controlled by a single stepper motor, to control wavelength position and grating switching. To switch gratings the turret rotates about the center axis, but to scan wavelengths the turret rotates around the front face of the grating to maintain on axis rotation of the grating. These spectrometers also benefit from the highest quality of gratings, also designed and manufactured by HORIBA.
Two configurations to choose from

Manual Slits with single entrance/exit ports (Triax 180)
Automated slits with single entrance and single or dual exit ports (Triax 190)
Benefits
- Low cost triple grating spectrometer
- Patented grating turret design
- Good image quality
- Monochromator or imaging spectrograph
- Optional second exit port (Triax 190 )
- USB interface
Hardware
Monochromator Hardware
Slits
The Triax has the following slit types available
- Automated 2 mm slit (part number MSL-TXB2)
- Automated 7 mm slit (part number MSL-TXB7)
- Fixed entrance and side exit (Triax 190 only, part number MSL-TNFA)
- Fixed exit (part number MSL-TXF)
The Triax automated slits adjustable from 0 to 2 mm opening or 0 to 7 mm opening. A manually adjustable height limiter allows the user to quickly shut or open the light path to 1 mm and 15 mm heights.
You can add accessories to the Triax-series spectrometers to obtain optimum results for a variety of applications. To attach the accessories to the Triax, use the two tapped holes on the body of the slit. These holes are also useful for connecting the Triax with your experiments and equipment. When connecting with the Triax, it is important to know the distance from the mounting face of the slit’s body to the slits.
Note that some custom accessories require removal of the height-limiter assembly in order to be attached to the Triax chassis. To remove the height-limiter assembly, remove the four screws holding the assembly onto the chassis.
Fixed Slit Assembly
The fixed slit assembly can hold different slit inserts ranging in physical size from 0.025 to 2 mm, and for the 1200 g/mm grating the reciprocal linear dispersion of the Triax is 3.53 nm/mm.
Micrometer Adjustable Slit Assembly
Gratings
World Class Diffraction Gratings Manufactured by HORIBA
A Proud Tradition of Excellence
Since the acquisition by HORIBA of Jobin Yvon, a spectroscopy company founded in 1819, HORIBA Scientific has continued to define the leading edge of the Optics of Spectroscopy.
For the last 40 years HORIBA Scientific has taken a leading position in the design, development and manufacture of master and replica diffraction gratings. HORIBA Scientific diffraction gratings are found in both high volume OEM instruments and in world class cutting edge scientific applications. Our pattern of leadership in optics has been hallmarked by the continuing development of both classically ruled and holographic diffraction grating technologies. This led to the introduction in 1967 of the aberration corrected holographic grating and subsequently ion etched and blazed concave and plane holographic gratings.
The Triax series of spectrometers take full advantage of the highest quality of gratings that HORIBA designs and manufactures.
A Vast Array of Choices
There is a wide selection of gratings to choose from depending on optical requirements. Gratings are 32 x 32 mm for the MicroHR. There are three different types of gratings available; classically ruled, holographic, and blazed holographic. There is also a flat mirror that may be ordered for the dual grating turret option.
Ruled gratings | Select for applications where high throughput or low groove density is required, or when working in the infrared. Typically, they have high throughput at the cost of higher stray light. |
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Holographic gratings | Available in higher groove densities for finer resolution requirements and are excellent choices for experiments with laser excitation such as Raman or laser induced photoluminescence. They provide the lowest possible stray light possible, sometimes at the cost of lower throughput. |
Blazed holographic gratings | These gratings have the same advantages as holographic gratings with better throughput. |
Groove Density
Ruled gratings and blazed holographic 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 of the selected grating 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 of the slits.
Unique Triple Grating Turret Assembly
These spectrometers benefit from HORIBA’s patented and revolutionary triple grating turret assembly that has two independent axis of rotation , controlled by a single stepper motor, to control wavelength position and grating switching. To switch gratings the turret rotates about the center axis, but to scan wavelengths the turret rotates around the front face of the grating to maintain on axis rotation of the grating.
Below is a comprehensive list of available gratings for the MicroHR series of spectrometers. Other gratings are also available upon request.
Ruled Gratings
Groove Density L/mm | Blaze Wavelength | Recommended Spectral Range | Blaze Angle | Part Numbers |
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300 nm | 150-600 nm | 17°27' | 510 01 330 | |
500 nm | 250-850 nm | 26°45' | 510-02-330 | |
630 nm | 350-850 nm | 34°32' | 510 03 330 | |
250 nm | 150-500 nm | 8°38' | 510-04-330 | |
330 nm | 200-700 nm | 11°25' | 510-05-330 | |
400 nm | 200-800 nm | 13°53' | 510-06-330 | |
500 nm | 250-950 nm | 17°27' | 510-07-330 | |
630 nm | 350-1200 nm | 22°12' | 510 08 330 | |
750 nm | 400-1200 nm | 26°45' | 510-09-330 | |
1µm | 500-1200 nm | 36°52' | 510-10-330 | |
350 nm | 200-700 nm | 9°00' | 510 91 330 | |
550 nm | 250-1100 nm | 14°30' | 510-93-330 | |
1.5 µm | 600-1700 nm | 42°27' | 510-97-330 | |
300 nm | 200-600 nm | 5°10' | 510-11-330 | |
400 nm | 250-800 nm | 6°54' | 510-12-330 | |
500 nm | 250-1000 nm | 8°38' | 510-13-330 | |
750 nm | 400-1500 nm | 13°00' | 510-14-330 | |
1µm | 500-1700 nm | 17°27' | 510-15-330 | |
1.5 µm | 750-2400 nm | 26°45' | 510-16-330 | |
2 µm | 1000-2400 nm | 36°52' | 510-17-330 | |
300 | 250 nm | 150-500 nm | 2°09' | 510-50-330 |
500 nm | 300-950 nm | 4°18' | 510-18-330 | |
600 nm | 350-1300 nm | 5°10' | 510-19-330 | |
1 µm | 700-2000 nm | 8°38' | 510-20-330 | |
2 µm | 1100-4500 nm | 17°27' | 510-21-330 | |
3 µm | 1700-5000 nm | 26°45' | 510-22-330 | |
4 µm | 2000-5000 nm | 36°52' | 510-23-330 | |
500 nm | 250-950 nm | 2°09' | 510-49-330 | |
1-2 µm | 800-2300 nm | 5°10' | 510-24-330 | |
2 µm | 1200-4000 nm | 8°38' | 510-25-330 | |
4 µm | 2.2 - 9 um | 17°27' | 510-26-330 | |
5 µm | 3.5 - 10 um | 22°01' | 510-27-330 | |
150 | 6 µm | 4 - 10 um | 26°45' | 510 28 330 |
150 | 8 µm | 5 - 10 um | 36°52' | 510 29 330 |
120 | 2-5 µm | 1.7 - 4.5 um | 8°39' | 510-30-330 |
5 µm | 3 - 10 um | 17°27' | 510-31-330 | |
7-5 µm | 4.5 - 12 um | 26°45' | 510-32-330 | |
450 nm | 250-950 nm | 1°17' | 510-48-330 | |
3 µm | 1.7 - 6 um | 8°38' | 510 33 330 | |
6 µm | 3 - 13 um | 17°27' | 510 34 330 | |
9 µm | 5 - 14.5 um | 26°45' | 510 35 330 | |
75 | 4 µm | 2 - 8 um | 8°38' | 510-36-330 |
8 µm | 5.5 - 17 um | 17°27' | 510 37 330 | |
12 µm | 8 - 19 um | 26°45' | 510-38-330 | |
10 µm | 7.5 - 13 um | 17°27' | 510-39-330 | |
15 µm | 9 - 24 um | 26°45' | 510-40-330 | |
50 | 6 µm | 3 - 12 um | 8°38' | 510-41-330 |
50 | 12 µm | 8 - 22 um | 17°27' | 510-42-330 |
50 | 18 µm | 11 - 28 um | 26°45' | 510-43-330 |
50 | 24 µm | 15 - 30 um | 36°52' | 510-44-330 |
40 | 22-5 µm | 14 - 30 um | 26°45' | 510 45 330 |
30 | 30 µm | N/A | 26°45' | 510 46 330 |
20 | 45 µm | N/A | 26°45' | 510 47 330 |
Holographic Gratings
Groove Density L/mm | Recommended Spectral Range | Part Numbers |
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150-400 nm | 520-07-330 | |
3000 | 250-450 nm | 520-09-330 |
300-600 nm | 520-12-330 | |
170-500 nm | 520-13-330 | |
100-300 nm | 520 14 330 | |
450-650 nm | 520 15 330 | |
190-650 nm | 520 16 330 | |
150-450 nm | 520 17 330 | |
2000 | 100-300 nm | 520 18 330 |
450-850 nm | 520 -19 -330 | |
190-700 nm | 520 -20 -330 | |
150-450 nm | 520 -21 -330 | |
1800 | 100-300 nm | 520 22 330 |
400-1200 nm | 520 -24 -330 | |
190-700 nm | 520 -25 -330 | |
150-450 nm | 520 -26 -330 | |
400-1300 nm | 520 -29 -330 | |
150-450 nm | 520 30 330 | |
250-800 nm | 520 -32 -330 | |
400-1200 nm | 520 33 330 |
Blazed Holographic Gratings
Groove Density L/mm | Blaze Wavelength | Recommended Spectral Range | Part Number |
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250 nm | 190-600 nm | 530-13-330 | |
330 nm | 200-600 nm | 530-11-330 | |
400 nm | 300-600 nm | 530-15-330 | |
1800 | 500 nm | 450-850 nm | 530 19 330 |
250 nm | 180-650 nm | 530-20-330 | |
400 nm | 250-850 nm | 530-18-330 | |
250 nm | 190-450 nm | 530-25-330 | |
330 nm | 240-800 nm | 530-22-330 | |
500 nm | 300-1000 nm | 530-24-330 | |
630 nm | 400-1200 nm | 530-27-330 | |
750 nm | 500-1200 nm | 530-28-330 | |
900 nm | 600-1200 nm | 530-50-330 | |
900 nm | 700-1700 nm | 530-60-330 | |
850 nm | 700-1700 nm | 530-66-330 | |
500 nm | 300-1000 nm | 530-29-330 | |
1000 nm | 700-1750 nm | 530 34 330 |
Diffraction Grating Calculator
The Diffraction Grating Calculator below can be used to determine the various optical performance specifications of HORIBA spectrometers when used in conjunction with selected spectroscopy cameras, point detectors and various grating alternatives. It is a very useful tool with pull down selections of all of our current spectrometers, cameras and gratings.
Computer Control
In addition to wavelength control the MicroHR has an optional automated turret control and automated control of the optional internal five position filter wheel.
There are multiple software platforms to choose from for spectrometer control and acquisition.
HORIBA’s world renowned software platform, LabSpec is ideal for most Raman and photoluminescence applications. It offers advanced capabilities, with expert functionality, control and flexibility. LabSpec is the first choice for most spectrometer customers. | |
SynerJY™ | SynerJY™ software is a fully integrated data acquisition and data analysis program for spectroscopic systems. It is selected for custom spectroscopy configurations not suitable for LabSpec. |
LabVIEW™ | LabVIEW VI’s are now available for the complete line of instrumentation from the Optical Spectroscopy Division, allowing users to work with the LabVIEW™ development package from National Instruments. This option requires proficiency with LabVIEW™ programing. |
SDK | Software Development Kits (SDK’s) are available for programmers who wish to write their own software control of HORIBA spectrometers. This option absolutely requires proficiency with programing |
Accessories
Compatible Optical Building Blocks
The Triax series spectrograph is one of many inter-connectable Optical Building Blocks available from HORIBA Scientific. These Optical Building Blocks can be ordered together to form a subassembly or even a complete custom spectroscopy solution.
C-Mount Adapter
The Triax series can be provided with ational C-Mount coupler accessory for the exit port that allows it to be coupled to cameras that use a C-Mount thread. It can also be equipped with an entrance side C-Mount coupler so that it can be directly attached to a microscope with an appropriate C-Mount detection port.
Fiber Light GuidesWe offer a selection of fiber optic and liquid light guides to choose from depending on the application. Lens based fiber-coupler with f/# matching optics for SMA and ferrule (part number 220F, or 220F-AFC for FC Mount fibers). | ||
Direct fiber-coupler with no optics for 10 mm and 0.25″ ferrule with thumbscrew x-y adjusters, (part number AFO-XY) Mirror based fiber-coupler for 10 mm ferrule (part number J23078640). Contact us for information about SMA and FC adapters. Simple fiber-adapter for 0.25″ ferrule (part number 120F). |
Internal Filter WheelsThe optional internal filter wheel (part number J450629) mounts at the entrance port of the Triax spectrometer and includes a blank window, 400 nm, 700 nm, 1000 nm LP filters. 2 mm filter thickness only. |
Optical ChoppersIf you would like to use an optical chopper with your spectrograph/monochromator, then we have a number of solutions. To learn more click here. |
Single Channel Detectors
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Spectroscopy Cameras
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Broad Band Light Sources
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Sample Compartment
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Specifications
Specifications | |
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Focal length | 0.19 meters |
Entrance aperture ratio | f/3.9 |
Grating size | 50 mm × 50 mm |
Image magnification at the exit | 1.00 |
Scanning range with 1200 gr/mm grating | 0–1400 nm |
Multichannel coverage (over 30 mm) | 106 nm with 1200 gr/mm grating |
Focal plane | 30 mm wide × 12 mm high |
Spectral dispersion with 1200 gr/mm grating | 3.53 nm/mm |
Spectral resolution as a scanning monochromator with 1200 gr/mm grating | 0.3 nm |
Wavelength positioning accuracy | ± 0.3 nm |
Wavelength repeatability | ± 0.06 nm |
Wavelength drive step size for 1200 gr/mm grating | 0.06 nm |
Dimensions | 10.5" (L) x 9.25" (W) x 7.35" (H) |
Weight (approx.) | 25.4 lbs (11.5 kg) |
*All specifications with 1200 gr/mm grating, array with 26 micron pixels
** 400 nm
Specifications subject to change without notice.