Modular Spectrometers

The TEO-200-X series of FTIR spectrometers represent a low cost Fourier transform infrared spectrometers and employ a number of unique features that ensure high performance from a compact instrument. The 200-X measures just 59 X 39 X 19 cm and is regarded as one of the most compact and versatile infrared FTIR spectrophotometers. The design of the 200-X is unique both in terms of optical design and the software and firmware designed specifically to significantly reduce overall analytical times. The interferometer geometry employs a new compact Michelson self compensating optical system that eliminates many of the optical alignment problems found in conventional type optical interferometers. The 200-X design avoids the use of conventional corner cube optics and dynamic alignment. In practice this means that the instrument can be used in the research laboratory, in any university or college environment and if required, can also be used outside laboratory or in remote locations.

The sample compartment is large and can accommodate all of the normal sample handling requirements relating to FTIR spectroscopy. This unique compartment will also accommodate a wide range of accessories supplied by specialist accessory manufacturers. Overall dimensions are W20 X D26 X H16 cm . The optical axis is 74.5 mm above the base of the sample compartment and there is free space of 90 mm above the optical axis to the underside of the lid.

In order to facilitate the use of more than one beam splitter or detector , provisions have been made to interchange the beam splitter and detector assemblies allowing the 200-X to be used at any wavelength from 15000 to 400 cm-1.

Beam Splitters Range subject to coatings
KBr 7,800 to 380 cm-1
ZnSe 5,000 to 500 cm-1
Fused silica 15,000 to 3,000 cm-1

$ 17,500.00

The Model TEO200 benchtop FTIR spectrometer is a low cost Fourier transform infrared spectrometer that employs a number of unique features to achieve high performance from such a compact size. At just 385x265x160mm , it is one of the most compact FTIR systems on the market today.
The TEO200 is unique in terms of its optical geometry and software/firmware design. The optical geometry is simplified by employing a new and remarkably compact Michelson self compensating optical system that eliminates many of the optical alignment problems found in conventional linear and pendulum type optical interferometers. For example, the TEO200 design avoids the use of conventional corner cube optics and dynamic alignment. In practical terms, the instrument can be used inside a research laboratory, or even as a mobile unit in outside environments. Its software and firmware design is also tightly coordinated which significantly reduces overall data acquisition and computational time.
The sealed, desiccated enclosure of the TEO200 eliminates the need for continuous dry nitrogen purging during operation. Other notable features include an air cooled IR source as oppose to water cooled, and the interferometer mechanical bearing does not require gas supply. There are however, three dry nitrogen gas inlets on the rear of the spectrometer for the purging of the detector compartment, sample compartment, and interferometer compartment from moisture, carbon dioxide and other gases.

Please note that there are a variety of spectral ranges available, depending on the detector-beam splitter choices for the system. The price of the system includes this beam splitter, but it must be specified.
KBr 7,000 to 400 cm-1
ZnSe 5,000 to 500 cm-1
CaF2 10,000 to 1,000 cm-1
Quartz 15,000 to 3,000 cm-1

$ 15,698.00

The TEO-402 is a compact Michelson interferometer module with built-in laser and a broadband IR source. It is designed to be used as a core component in a complete FTIR instrument.
Note that this system does not include a power supply, AD board, or detector.

$ 11,288.00

This option allows the SPS-300 to use both output ports simultaneously. The internal mirror that directs the parallel beam to the converging output is replaced by a large beam splitter which sends half the radiation to the converging output, and the other half to the parallel output.

Please discuss any questions you have regarding the beam splitter, or operating two detectors simultaneously, with your authorized Sciencetech technical sales staff.

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The TEO-402 is a compact Michelson interferometer module with built-in laser and a broadband IR source. It is designed to be used as a core component in a complete FTIR instrument.
Note that this system does not include a power supply, AD board, or detector.

$ 10,238.00

An imaging 1/4m Monochromator/spectrograph. It has f/3.5 aperture and a 2D flat field output for multi-channel use. It has a nominal resolution of 0.15 nm.
Special toroidal mirror makes additional astigmatism correction. This spectrograph provides superior image quality over area 25 mm wide and 12 mm high
The unique layout with mirrors of unequal input and output (200mm and 250 mm) focal length is optimized for minimum coma while allowing high throughput and minimum stray light and vignetting
Please contact a technical sales member to discuss coupling options.
For more information, please see the technical datasheet.

$ 10,020.00

An imaging 1/2 meter monochromator/spectrograph. It has an f/8 aperture and a 2D flat field output for multi-channel use. It has a nominal resolution of 0.1 nm.
Special toroidal mirror makes additional astigmatism correction. This spectrograph provides superior image quality
The unique layout with toroidal mirrors is optimized for minimum coma while allowing high throughput and minimum stray light and vignetting. This option only applies to f/8 triple turrell with 50x50 mm grating holder
Please contact a technical sales member to discuss coupling options.
For more information, please see the technical datasheet.

$ 10,000.00

In the 9072DS, the grating in the second monochromator is arranged such that it reverses the spectral dispersion of the first monochromator. This leads to a spectrally homogenized beam at the output port of the second monochromator and greatly reduced stray light, ideal for spectroradiometry, Raman or UV measurements of solar radiation.
The arrangement of the 9072DS allows it to act either as a tunable bandpass filter or a tunable notch filter. Arranged as a tunable bandpass filter the bandpass of the device is determined by the width of an intermediate slit. When arranged as a tunable notch filter the width of the notch is determined by the physical width of an opaque notch placed at the intermediate slit position.
The 9072DS can also be used to pass or filter out several selected wavelengths by using a custom intermediate multi-slit mask instead of a single width intermediate slit.

One SS-80 slit is included, which can be attached to either the input or output port. A second slit can be added to the order if desired.
The fixed intermediate slit or notch filter is not included in the 9072DS and can be selected from any of Sciencetech's SF-series of fixed slits and added to the order. A custom multi-slit mask can be added to the order upon request.
Gratings and grating holders are not included. The 9072DS accommodates 30 × 30 mm gratings, with up to three gratings per turret. Two of each selected grating must be purchased to fill both monochromators. One grating holder is required for each grating.

$ 9,524.00

In the 9072DA, the inbound light is dispersed by the first grating then passed through a fixed intermediate slit where stray light is rejected and then spectrally dispersed again by the second grating.

The double dispersion of the double additive monochromators results in a doubling of the dispersion of a single monochromator, leading to better optical resolution. The bandpass is half that of a single 9072 monochromator.

One SS-80 slit is included, which can be attached to either the input or output port. A second slit can be added to the order if desired.
The fixed slit is not included in the 9072DA and can be selected from any of Sciencetech's SF-series of fixed slits and added to the order.
Gratings and grating holders are not included. The 9072DA accommodates 30 × 30 mm gratings, with up to three gratings per turret. Two of each selected grating must be purchased to fill both monochromators. One grating holder is required for each grating.

$ 9,524.00

The Sciencetech 9057F is a fast half meter motorized Czerny-Turner monochromator (and spectrograph) with an f/5.9 aperture. This is a "faster" model with larger optics for higher light throughput compared to the standard 9057 with f/8 aperture. Both models utilize a computer controlled motorized turret for automatic grating and wavelength selection. The regular 9057 model supports up to three 50 x 50mm gratings whereas the larger optics 9057F model supports up to two 64 x 64mm (clear aperture) gratings.
Please refer to the technical datasheet for more specifications.

$ 8,562.00

The 9057 is a half meter monochromator and spectrograph with an f/8 aperture. This system is a Czerny-Turner design optimized to reduce aberrations.
This monochromator supports up to three 50x50mm gratings on a computer controlled turret. It includes a single input slit by default; please select appropriate output mounting (slit, detector or CCD mounting, etc...) when ordering.
A fast version of the 9057, the 9057F, operates with 64x64mm gratings and offers better throughput with the same optical pathlength. Please discuss with your Sciencetech technical sales staff member to find if the 9057F is a better choice for your particular application.

$ 8,082.00

The Sciencetech 9055F is a 250 mm focal length modified Czerny-Turner monochromator, with a flat field output for spectrograph use. This is designed as a faster version of the 9055 with larger optics for higher light throughput and f/2.5 aperture. All 9055Fs have a computer controlled, motorized turret for automatic grating and wavelength selection. Both input and output ports are situated on the front faceplate of the monochromator/spectrograph, and the system includes one adjustable SS80 slit at the input port. The 9055F supports up to two 64 x 64 mm (clear aperture) gratings.
Please see technical datasheet for further information.

$ 7,530.00

The Sciencetech 9055 is a 250mm asymmetric focal length modified Czerny-Turner monochromator. It has a flat field output for use as a spectrograph. This model has an f/3.5 aperture (for the "Fast" version with f/2.5, please see the 9055F). It has a computer-controlled interchangeable turret for automatic grating and wavelength selection.
Both the input and output ports are located on the front faceplate of the monochromator, and the system includes one SS80 slit at the input port. CE compliant.

It Includes a Sci-Mono, a Windows based software module with a simple graphical user interface for controlling Sciencetech stepping monochromator wavelength selection. SciMono is provided free of charge with a Sciencetech motorized monochromator when SciSpec software has not been purchased.

Sciencetech Software (Sci-Spec) is available at an additional cost. It is a standalone data acquisition and allows controlling the monochromator by itself.

This system does not include gratings or a host computer. If you require any of these components, please speak with your technical sales staff member.

Refer to the technical datasheet for additional information.

$ 7,020.00

Sciencetech manufactures grid polarizing beam-splitters for use in the far-infrared and terahertz spectral regions. These beamsplitters divide the incoming beam according to its polarization. The beam-splitter consist of very fine parallel aluminum lines spaced 4 µm apart on a thin mylar substrate. It has the widest spectral range with a higher frequency cut-off than that of other polarizers that work in the near-millimeter wavelength range.
This particular model is 5" (12.5cm) diameter, and is the largest standard size of the IR beam-splitter polarizer Sciencetech offers. For larger or smaller sizes, or for a full list of technical specifications, please speak with your authorized Sciencetech technical sales staff member.

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The optional external light source port upgrade provides both a motorized turning mirror and the flange for the input port so that users can couple external light sources (e.g. glowbar, Gunn diode, synchrotron) into the SPS-300. The motorized mirror switches inputs between the SPS-300 internal mercury lamp and external light source. Additional optics and chambers may be required to focus the external light source into the SPS-300.

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Sciencetech manufactures grid polarizing beam-splitters for use in the far-infrared and terahertz spectral regions. These beamsplitters divide the incoming beam according to its polarization. The beam-splitter consist of very fine parallel aluminum lines spaced 4 µm apart on a thin mylar substrate. It has the widest spectral range with a higher frequency cut-off than that of other polarizers that work in the near-millimeter wavelength range.
This particular model is 4" (10cm) diameter, and is the second largest size of the IR beam-splitter polarizer Sciencetech offers. For larger or smaller sizes, or for a full list of technical specifications, please speak with your authorized Sciencetech technical sales staff member.

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The 9030DS consists of two 100 mm scanning monochromators placed in series in subtractive mode. Bandpass is determined by the width of an intermediate slit, but the 9030DS has a net output dispersion of zero because the monochromators are optically coupled so that the dispersion of the second grating cancels that of the first. This leads to homogenized wavelengths at the output port - there is no spectrum, only a single undispersed slit image - which allows the unit to act as a tunable bandpass or notch filter.

Stray light of all sorts is drastically reduced in a double monochromator, and in the 9030DS it is further minimized by the use of concave holographic gratings. It is ideal for applications where stray light is a problem - where there may be a strong scattered background, such as in spectroradiometry, Raman or UV measurements of solar radiation.

The 9030DS can be used as a tunable notch filter to remove one particular wavelength while allowing all others over the bandpass to pass through, making it an ideal instrument to pre-filter out the strong laser excitation wavelength in a Fluorescence or Raman system so that the weaker output signals can be observed.

The 9030DS is a fully integrated unit with the two diffraction gratings coupled mechanically for accurate positioning, adjusted manually using a thumb-wheel. A variety of fixed slit widths is available. It can be upgraded to be motorized and controlled by a computer with the 9030 Motorized Upgrade. Only one motor and drive unit is required for both monochromators, enabling control via Sciencetech Sci-Mono Active-X library or full featured Sci-Spec software.

The Model 9030DS can also be used to pass or filter out several selected wavelengths by using a custom intermediate multi-slit mask instead of a single width intermediate slit. Mirror coatings have been chosen for this model to enhance performance in the UV-VIS region. Please contact a Sciencetech Applications Specialist for such custom wavelength filtering.

$ 4,628.00

The 9030DA double additive monochromator consists of two 9030 monochromators placed in series. Stray light is drastically reduced in a double monochromator, and in the 9030DA it is further minimized by the use of concave holographic gratings. The inbound light is dispersed by the first grating and again by the second. Both gratings rotate simultaneously in the same direction, and in the DA the monochromators are coupled so that the dispersion is double that of a single 9030 monochromator. Bandpass is half of the corresponding 9030 monochromator for the same output slit, and resolution using a 100 µm slit is 0.4 nm.
Mirror coatings have been chosen for this model to enhance performance in the UV-VIS region.

$ 4,628.00

The 9030DA double additive monochromator consists of two 9030 monochromators placed in series. Stray light is drastically reduced in a double monochromator, and in the 9030DA it is further minimized by the use of concave holographic gratings. The inbound light is dispersed by the first grating and again by the second. Both gratings rotate simultaneously in the same direction, and in the DA the monochromators are coupled so that the dispersion is double that of a single 9030 monochromator. Bandpass is half of the corresponding 9030 monochromator for the same output slit, and resolution using a 100 µm slit is 0.4 nm.
This includes one set of standard slits, but the grating must be selected/specified separately.
Mirror coatings have been chosen for this model to enhance performance in the VIS-NIR region.

$ 4,628.00

The 9030DS consists of two 100 mm scanning monochromators placed in series in subtractive mode. Bandpass is determined by the width of an intermediate slit, but the 9030DS has a net output dispersion of zero because the monochromators are optically coupled so that the dispersion of the second grating cancels that of the first. This leads to homogenized wavelengths at the output port - there is no spectrum, only a single undispersed slit image - which allows the unit to act as a tunable bandpass or notch filter.
Stray light of all sorts is drastically reduced in a double monochromator, and in the 9030DS it is further minimized by the use of concave holographic gratings. It is ideal for applications where stray light is a problem - where there may be a strong scattered background, such as in spectroradiometry, Raman or UV measurements of solar radiation.
This price includes a standard set of slits including a standard intermediate (inverted) slit, but does not include gratings. We also offer customized intermediate (inverted) slits; please speak with your authorized Sciencetech technical support staff member.
Please see technical datasheet for additional information.

$ 4,628.00