Spectralon Reflective Coating Standard,( Zenith White and Gold Coating available)
1.5" diameter entrance/exit port (1), 1" diameter application ports (3) (90 degree, North Pole and 180 degree)
Additional Ports and reduction of ports possible
Internal baffle on 90 deg port

$ 3,681.00

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$ 730.00

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$ 730.00

Active Area: 13mm^2 (3.6 x 3.6mm)
Rise Time: 10ns @20V
NEP: 1.2 x 10^(-14) W/Hz^(1/2) @ 900nm, 20V
Dark Current: 20nA @ 20V
Junction capacitance: 40pF @ 10V

$ 320.00

Active Area: 100mm^2 (10 x 10mm)
Rise Time: 150ns
NEP: 1.5 x 10^(-14) W/Hz^(1/2) @ 960nm
Dark Current: 200pA @ 5V
Junction capacitance: 380pF @ 5V

$ 320.00

Material: Si
Wavelength Range: 350-1100
Detector Size: 3.6 x 3.6mm
Gain (Fixed): 8 x 10 dB steps
Bandwidth Range: DC - 17MHz
NEP: 2.1x10^(-12) to 7.7x10^(-11) W/Hz^(1/2)

$ 650.00

Material: Si
Wavelength Range: 350-1100
Detector Size: 0.8mm diameter
Gain (Fixed): 100kV/A
Bandwidth Range: DC - 50MHz
NEP: 6.5x10^(-11) W/Hz^(1/2)

$ 800.00

Material: Si
Wavelength Range: 200-1100
Detector Size: 1.0mm diameter
Gain (Fixed): 10kV/A
Bandwidth Range: DC - 150MHz
NEP: 5.5x10^(-11) W/Hz^(1/2)

$ 632.00

Active Area: 13mm^2 (3.6 x 3.6mm)
Wavelength Range: 350-1100nm
Rise Time: 14ns
NEP: 1.6x10^(-14) W/Hz^(1/2)
Dark Current: 0.35nA
Junction Capacitance: 40pF

$ 560.00

Rise/Fall Time: 14 ns
Active Area: 13mm^2 (3.6 x 3.6mm)
NEP: 1.6E-14 W/Hz^(1/2)
Dark Current: 0.35 nA
Material: UV-enhanced Si
Junction Capacitance: 40pF @5V

$ 360.00

Rise/Fall Time: 450ns/45ns
Responsivity: 0.50 A/W
Active Area: Diameter = 9mm
NEP: 5.5E-14 W/Hz^(1/2)@5V
Dark Current: 1.0uA@5V
Material: UV-enhanced Si
Junction Capacitance: 1.75nF @0V

$ 620.00

Rise/Fall Time: 10ns
Active Area: 13mm^2 (3.6x3.6mm)
NEP: 1.2x10^(-14) W/Hz^(1/2)
Dark Current: 0.3nA
Material: Si
Junction Capacitance: 65pF @5V

$ 360.00

Rise/Fall Time: 45ns
Active Area: 100mm^2 (Diameter = 11.0mm)
NEP: 5.5x10^(-14) W/Hz^(1/2)
Dark Current: 1.0uA
Material: Si
Junction Capacitance: 1.75nF @0V

$ 290.00

Class: BBA, ASTM E927-19
Target Size: 152 mm diameter
Working Distance: 900 mm
Collimation: 3 degrees, half angle
Power Supply: 611-1.6k (included)
Lamp: 1600 W Xenon Arc Lamp, Ozone free (included)
Air Mass Filter: AM1.5G (included)

Sciencetech is pleased to offer the SS-1.6kW solar simulator. This model is free of chromatic aberration and uses a fully reflective design to create uniformity on target, maximizing UV throughput. The SS-1.6kW includes air-cooled arc lamp housing, 1600 W ozone free xenon bulb, and adjustable power supply with igniter.

This solar simulator has one filter holder for Sciencetech's FT style filters. AM1.5G air mass filter included. For other options (i.e. AM0), please speak to a Sciencetech Representative. Other filters such as dichroic filters and bandpass filters are available for further modification of the spectrum.

This instrument features standard horizontal operation, but vertical operation is optional (please see Sciencetech's DFS-SS, 160-8016).

Class AAA available upon request. Please speak with your authorized Sciencetech Representative for further details and a full range of options.

Requires 220-240V/ 50/60Hz, 12.1-9.0A, Fused 15A, 250V
This system includes 1 IEC 60320 C19 compatible power cable. Region-specific version must be selected at the time of placing an order (see product 491-9003).

$ 48,999.00

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

$ 17,399.00

The IRE-12 a coiled filament operating at approximately 900 degrees Celsius when powered with 10 watts. The radiating element is a coil of resistance wire which has a high emissivity in the Infrared spectral region. The coil is supported by a grooved cylindrical substrate of alumina, resulting in the windings being electrically insulated from each other. This contributes to a more uniform radiating source. The unit does not require operation in a sealed atmosphere. The header is fabricated from cold-rolled steel. The support pins are hermetically sealed in glass.

$ 263.00

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
CaF2 10,000 to 1,000 cm-1
Quartz 15,000 to 3,000 cm-1

$ 16,999.00

This is an external transmission and reflectance sample chamber that can be mated to an output port of the SPS-series FTIRs. This sample chamber allows small samples (such as cuvettes or thin films) to be studied in both reflection and transmission. The sample chamber shares the vacuum environment with the FTIR, but an optional window or vacuum gate (sold separately) allows the chamber to be isolated from the FTIR. The sample chamber utilizes reflective aspheric optics with gold coating for excellent far infrared and terahertz operation.

Contact for Pricing

This is an SMA fiber coupler (FC style also available) with an interface flange mount to the input port of a Sciencetech monochromator or spectrograph (fiber not included). Please note two versions are available. One version is for the Sciencetech 9030 monochromator which utilizes its own slit interface flange design. The other version is for all other Sciencetech Series 9000 and 8000 monochromators and spectrographs which use a common slit interface flange design. With an FIB1 at the input port, a slit (fixed or adjustable) is not necessary as the width of the input fiber typically defines the input slit width. Please note that this fiber connection does not address the f number matching issue between the fiber and the monochromator or spectrograph. Hence if it is used at the input port of the monochromator or spectrograph, significant light loss can be expected with the fiber having an f number closer to 1. If this is an issue, please speak to a Sciencetech Applications Specialist about using a condensing lens assembly with the FIB4 or FIB5 instead

$ 220.00

Liquid Helium Cooled Bolometers are 10^2 to 10^4 (two to four orders magnitude) more sensitive than room temperature pyro-electric detectors
Liquid Helium Cooled 1.6K
5u - 2000u spectral range
Liquid Nitrogen required in outer jacket (dual stage cooling)
2.5 mm diameter diamond absorber
0.5" F/3.8 diameter condensing cone as input optics
Preamp circuitry generates +/-14V max
5" Diameter Dewar Included

Filterwheel Position #1 - Long pass 5micron cut-on
Position #2 - Wedged P13 filter (13micron cut-on long pass)
Position #3 - Wedged C103 filter (103 micron cut-on long pass filter)
Wedged Diamond window Diameter = 25.0mm

$ 54,340.00