Triax Series

Short Focal Length Triple Grating Imaging Spectrographs

Short Focal Length Triple Grating Imaging Spectrographs

Affordable 190 nm focal length imaging spectrometers offering maximum versatility and automation

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)
Segment: Scientific
Division: Custom Spectroscopy Solutions
Base product
Manufacturing Company: HORIBA Scientific
  • 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

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. 

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

1800

300 nm

150-600 nm

17°27'

510 01 330

1800

500 nm

250-850 nm

26°45'

510-02-330

1800

630 nm

350-850 nm

34°32'

510 03 330

1200

250 nm

150-500 nm

8°38'

510-04-330

1200

330 nm

200-700 nm

11°25'

510-05-330

1200

400 nm

200-800 nm

13°53'

510-06-330

1200

500 nm

250-950 nm

17°27'

510-07-330

1200

630 nm

350-1200 nm

22°12'

510 08 330

1200

750 nm

400-1200 nm

26°45'

510-09-330

1200

1µm

500-1200 nm

36°52'

510-10-330

900

350 nm

200-700 nm

9°00'

510 91 330

900

550 nm

250-1100 nm

14°30'

510-93-330

900

1.5 µm

600-1700 nm

42°27'

510-97-330

600

300 nm

200-600 nm

5°10'

510-11-330

600

400 nm

250-800 nm

6°54'

510-12-330

600

500 nm

250-1000 nm

8°38'

510-13-330

600

750 nm

400-1500 nm

13°00'

510-14-330

600

1µm

500-1700 nm

17°27'

510-15-330

600

1.5 µm

750-2400 nm

26°45'

510-16-330

600

2 µm

1000-2400 nm

36°52'

510-17-330

300

250 nm

150-500 nm

2°09'

510-50-330

300

500 nm

300-950 nm

4°18'

510-18-330

300

600 nm

350-1300 nm

5°10'

510-19-330

300

1 µm

700-2000 nm

8°38'

510-20-330

300

2 µm

1100-4500 nm

17°27'

510-21-330

300

3 µm

1700-5000 nm

26°45'

510-22-330

300

4 µm

2000-5000 nm

36°52'

510-23-330

150

500 nm

250-950 nm

2°09'

510-49-330

150

1-2 µm

800-2300 nm

5°10'

510-24-330

150

2 µm

1200-4000 nm

8°38'

510-25-330

150

4 µm

2.2 - 9 um

17°27'

510-26-330

150

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

120

5 µm

3 - 10 um

17°27'

510-31-330

120

7-5 µm

4.5 - 12 um

26°45'

510-32-330

100

450 nm

250-950 nm

1°17'

510-48-330

100

3 µm

1.7 - 6 um

8°38'

510 33 330

100

6 µm

3 - 13 um

17°27'

510 34 330

100

9 µm

5 - 14.5 um

26°45'

510 35 330

75

4 µm

2 - 8 um

8°38'

510-36-330

75

8 µm

5.5 - 17 um

17°27'

510 37 330

75

12 µm

8 - 19 um

26°45'

510-38-330

60

10 µm

7.5 - 13 um

17°27'

510-39-330

60

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

3600

150-400 nm

520-07-330

3000

250-450 nm

520-09-330

2400

300-600 nm

520-12-330

2400

170-500 nm

520-13-330

2400

100-300 nm

520 14 330

2000

450-650 nm

520 15 330

2000

190-650 nm

520 16 330

2000

150-450 nm

520 17 330

2000

100-300 nm

520 18 330

1800

450-850 nm

520 -19 -330

1800

190-700 nm

520 -20 -330

1800

150-450 nm

520 -21 -330

1800

100-300 nm

520 22 330

1200

400-1200 nm

520 -24 -330

1200

190-700 nm

520 -25 -330

1200

150-450 nm

520 -26 -330

600

400-1300 nm

520 -29 -330

600

150-450 nm

520 30 330

150

250-800 nm

520 -32 -330

150

400-1200 nm

520 33 330

Blazed Holographic Gratings

Groove Density L/mm

Blaze Wavelength

Recommended Spectral Range

Part Number

2400

250 nm

190-600 nm

530-13-330

2400

330 nm

200-600 nm

530-11-330

2400

400 nm

300-600 nm

530-15-330

1800

500 nm

450-850 nm

530 19 330

1800

250 nm

180-650 nm

530-20-330

1800

400 nm

250-850 nm

530-18-330

1200

250 nm

190-450 nm

530-25-330

1200

330 nm

240-800 nm

530-22-330

1200

500 nm

300-1000 nm

530-24-330

1200

630 nm

400-1200 nm

530-27-330

1200

750 nm

500-1200 nm

530-28-330

1200

900 nm

600-1200 nm

530-50-330

950

900 nm

700-1700 nm

530-60-330

900

850 nm

700-1700 nm

530-66-330

600

500 nm

300-1000 nm

530-29-330

600

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.

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.

LabSpec

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

 

 

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)
26.7 cm (L) x 23.5 cm (W) x 18.7 cm (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.

Raman and Resonance Raman Spectroscopy of Enzymes
Raman and Resonance Raman Spectroscopy of Enzymes
The TRIAX and iHR series spectrometers used in Raman system configurations provide superior imaging performance with no re-diffracted light and maximized optical throughput.
Low Temperature Macro Photoluminescence and PLE System
Low Temperature Macro Photoluminescence and PLE System
The FluoroLog-3® system makes an ideal turnkey macro PL / PLE system. The large format sample chamber allows the easy installation of a standard helium cryostat for low temperature studies.
Photoluminescence and Photoreflectance
Photoluminescence and Photoreflectance
As a result of rapid development in semiconductor manufacturing, many types of optoelectronic devices such as laser diodes, LEDs, and high-electron-mobility transistors (HEMTs) are now fabricated by epitaxial-growth methods.
Photoluminescence of Semiconductors
Photoluminescence of Semiconductors
Photoluminescence spectroscopy (PL) is a powerful optical method used for characterizing materials. PL can be used to find impurities and defects in silicon and group III-V element semiconductors, and to determine semiconductor band-gaps.
Triax Series Specification Sheet
CategoryDocuments
Size 0.25 MB
FiletypePDF

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