BSI Cooled High Sensitivity Spectrometers 200-1100nm

Sign In

Show Password Forgot your password?

Sign In
Need a new account?
Register

Register

Forgot your password?
Register
Register your account immediately
Sign In

Retrieve password

Get verification code
submission
Sign In

简体中文 English

Products / Light Analysis /Spectrometers /Fiber Spectrometers (200nm to 5um) /BSI Cooled High Sensitivity Spectrometers 200-1100nm /

BSI Cooled High Sensitivity Spectrometers 200-1100nm

MC Series Overview Knowledge Base Related Products Accessories Order Now!

The MC Series BSI (Backside Illuminated) Cooled High Sensitivity Spectrometer is an optical fiber spectrometer with thermoelectric internal cooling technology. It uses a high-resolution optical platform and has both high resolution and low noise capabilities, making it especially suitable for low-light detection occasions that require long exposure (such as fluorescence Signal detection and Raman signal detection occasions). Complementing the TEC system, the MC Series has an excellent Signal to Noise Ratio, down to 0.41nm FWHM optical resolution, and a SMA905 fiber connector. This is a popular model employed for Angular-Resolved Spectroscopy and Fluorescence/Raman Spectroscopy. The cooled optical fiber spectrometer employs a cooled 2D CCD array with a peak quantum efficiency of 95%.

Up to 1000:1 SNR - the MC Sereis cooled optical fiber spectrometer utilises Hamamatutsu Thermoelectric cooled detector reducing temperatures by up to 40℃ , suppressing the dark current noises and greatly improve the signal to noise ratio

Up to 95% peak quantum efficiency - M Sereis cooled detector fiber spectrometer uses a special back thinning technique where light is introduced from the rear surface to section PN, improving the quantum conversion efficiency, especially the quantum conversion efficiency in the ultraviolet band

Product specifications and Brochures

Product Brochure Link:

Model Wavelength Range	200 - 1100nm
Optical Resolution	Up to 0.25nm based on different slit size and grating
Integration Time	7ms ~ 30min
Dynamic Range	10,000:1
Signal to Noise Ratio	1,000:1 when Saturated
Correction Linearity	>99%
Detector Model	Hamamatsu, S7031, 1044 * 64 pixels, back-illuminated, refrigerated 2d array,
Pixel	1064 x 64
Size / Weight	180.5 × 115.2 × 46.8 mm³ / 1.328kg
Fiber Interface	SMA905 or FC/PC optional
A/D Resolution	16 bits
Data Transmission	USB2.0, RS232
Step Drawings

Configuration Example

364.87 ~ 1044.91 nm / Slit 25 µm / FWHM 0.66 nm @794 nm

MC Series Wavelength, Slit and Optical Resolution Specifications

Model	Wavelength Range	Grating Scribe / Blaze Wavelength	Slit Width
			10 um	25 um	50 um	100 um	200 um
			Optical Resolution FWHM
MC/200-1000	200-1000nm	300/300nm &550nm	1.6nm	1.7nm	1.8nm	3nm	6nm
MC/300-1100	300-1100nm	300/300nm & 550nm	1.6nm	1.7nm	1.8nm	3nm	6nm
MC/400-930	400-930nm	400/500nm	1.4nm	1.5nm	1.6nm	2.6nm	5nm
MC/350-740	350-740nm	600/500nm	0.9nm	1nm	1.2nm	1.6nm	3nm
MC/530-630	530-630nm	1800/500nm	0.25nm	0.3nm	0.4nm	0.5nm	1nm
MC/710-1050	710-1050nm	600/800nm	0.9nm	1nm	1.2nm	1.6nm	3nm
MC/780-1030	780-1030nm	830/900nm	0.55nm	0.6nm	0.7nm	0.95nm	1.8nm

Multi Channel Upgrade Option

Do you need more precise measurements over a broad wavelength range? Our multi-channel spectrometers upgrade option offers a solution. Choose the desired spectrometer wavelength range, and we can integrate them into a single system (up to 4 channels) with single fiber or multi fiber output option. Please contact us for more info.

Product Size

Software Interface

Main software user interface

1.Detection Panel (Function menu and operation buttons)

2.Device Panel (Device list and paremeter settings)

3.Spectral Window (Spectral curve display and spectral window management)

4.Spectral Recording Panel (Spectral curve selection and naming)

Key Spectral processing feature

● Wavelength Smoothing

● Defluoresence

● Substract the background signal

● Rransmission and reflection measurement

● Absobance measurement

● Multi measurement with different timing

For detail software user manual please Click here

Because of the limited number of pixels in the spectrometer detector, there is a situation where only a few pixels make up a single spectral peak at the high spectral resolution, resulting in an unsmoothed peak, as shown in the figure below.

The figure shows an example of a drift in the peak position due to the temperature drift of the spectrometer at different temperatures for the same spectral peak. The spectral peaks are not symmetrical because the number of pixels that make up the spectral peaks is small, and the highest pixel of the spectral peak is shifted by one pixel from do to right under the effect of temperature drift.

At this point, we have two ways to evaluate the drift of this peak position.

1. Look at the position of the highest pixel point. Obviously, the peak position is shifted by one pixel, which translates to about 0.15 nm.

2. Fit the peaks before and after the drift and find the peak point of the fit, which is between two pixels. The drift of the fitted peak point is about 0.07nm

So which of these two methods is the right one? We believe that the second one is correct and reflects the true drift of the peak position. The reasons are as follows.

1. The high resolution leads to a low sampling rate of the pixels of the spectral peaks, and directly looking at the shape of the pixels together does not reflect the actual shape of the peaks.

2. The spectral peaks are physically closer to the symmetric distribution, and the drift of the peak position does not cause the peak shape to change.

3. By fitting all the pixels that make up the spectral peaks, the peak shape obtained is closer to the physical reality of the peaks.

Therefore, using the fitted peak shape to determine the peak position and evaluate the drift of the spectrometer is the correct method.

In practice, is it all necessary to do so? It depends on the situation.

If 1. The spectral resolution is low, and the sampling rate of the spectral peaks is high, i.e., it takes more pixel points to compose a peak, and these pixel points themselves are connected into a smoother and more symmetrical peak shape, then you can directly find the position of the highest pixel, or between two pixels, and confirm the peak position by visual evaluation.

2. With High spectral resolution and the need to know precisely the peak value, the above fitting method is needed. The fitting can be done by Spline algorithm, or by Gaussian or Lorentzian fitting, and the reader can choose according to the spectral nature of the sample under test. If you don't know how to choose, use Spline.

Name	Model	Wavelength Range	Detector	Resolution	Noise Ratio	Dynamic Range
High Resolution Spectrometer	L Sereis	200-1100nm	Hamamatsu，S11639，2048 pixels	<1nm customizable	500:1	2000:1
High Resolution Spectrometer	H Series	200-1100nm	Hamamatsu，S11639，2048 pixels	<1nm customizable	500:1	2000:1
Back Illuminated Spectrometer	M Series	200-1100nm	Hamamatsu，S10420，64×2048 pixels	<1nm customizable	800:1	5000:1
Hi Sensitivity Cooled Spectrometer	MC Serie	200-1100nm	Hamamatsu，S7031，64×1044 pixels	<1nm customizable	1000:1	10000:1
Handheld Raman System	RM	785/1064nm	Band Range 200-3200cm^-1/ 200-2500cm^-1	6 - 8 cm^-1
Portable Tabletop Raman System	RMT EZ	785nm	Band Range 200-3200cm^-1	7 cm^-1 typical
Portable Tabletop Raman System	RMT	532/785/1064nm	Band Range 200-3200cm^-1/200-1800cm^-1	8 - 9 cm^-1 typical
NIR Spectrometer	NIR Series	900-2500nm	Hamamatsu, G9203	3-10nm	15000:1	15000:1
MWIR Spectrometer	MWIR Series	1-5um	PbS or PbSe 256 pixels	10-30nm	20 RMS

	Laser Scanning Confocal Microscope
	Wide Field Raman Microscope
	Fluorescence / Photoluminescence Microscope,

Accessories

For more information on customized accessories, please contact us info@simtrum.com

Model No.	Type	Wavelength	Core Diameter	Length	# of Fiber	Connector
I1000-S/S-L2	Optic Fiber	360~2500 nm	1000 μm	2 m	1	SMA905-SMA905
V1000-S/S-L2		200 ~ 1100 nm	1000μm	2 m	1	SMA905-SMA905
DV600-S/S-L2		190~1100 nm	600μm	2 m	1	SMA905-SMA905
I600-S/S-L2		360~2500 nm	600μm	2 m	1	SMA905-SMA905
V600-S/S-L2		200 ~ 1100 nm	600μm	2 m	1	SMA905-SMA905
DV400-S/S-L2		190~1100 nm	400μm	2 m	1	SMA905-SMA905
I400-S/S-L2		360~2500 nm	400μm	2 m	1	SMA905-SMA905
V400-S/S-L2		200 ~ 1100 nm	400μm	2 m	1	SMA905-SMA905
DV200-S/S-L2		190~1100 nm	200μm	2 m	1	SMA905-SMA905
I200-S/S-L2		360~2500 nm	200μm	2 m	1	SMA905-SMA905
V200-S/S-L2		200 ~ 1100 nm	200μm	2 m	1	SMA905-SMA905
DV100-S/S-L2		190~1100 nm	100μm	2 m	1	SMA905-SMA905
I100-S/S-L2		360~2500 nm	100μm	2 m	1	SMA905-SMA905
V100-S/S-L2		200 ~ 1100 nm	100μm	2 m	1	SMA905-SMA905
I1000-Y*2-S/S-L2	Bifurcated Fiber, Y-bundle : 2 fibers	360~2500nm	1000μm	2 m	A-2nos, B1-1nos, B2-1nos	A-SMA905 / B1-SMA905 / B2-SMA905
V1000-Y*2-S/S-L2		200 ~ 1100 nm	1000μm	2 m	A-2nos, B1-1nos, B2-1nos	A-SMA905 / B1-SMA905 / B2-SMA905
DV600-Y*7-S/S-L2		190~1100 nm	600μm	2 m	A-7nos, B1-1nos, B2-6nos	A-SMA905 / B1-SMA905 / B2-SMA905
I600-Y*7-S/S-L2		360~2500nm	600μm	2 m	A-7nos, B1-1nos, B2-6nos	A-SMA905 / B1-SMA905 / B2-SMA905
DV600-1*7-S/S-L2	Multi-core Fiber	190~1100 nm	600μm	2 m	7	SMA905-SMA905
I600-1*7-S/S-L2	Multi-core Fiber	360~2500nm	600μm	2	7	SMA905-SMA905

	Integrating Sphere Wavelength 250 - 2500 nm Output port customizable Black anodized aluminum alloy housing		Gold Coated Integrating Spheres Wavelength 1000 - 5000 nm Electrochemically plated diffuse reflective film coating
	Halogen Light Source Wavelength 360 - 2500 nm Long lifetime, typically 10,000 hours SMA905 output connector		Deuterium UV Light Source Wavelength 190 - 400 nm Long lifetime, typically 1500 hours SMA905 output connector
	Sample Holder with Mounting for Transmittance Measurement		Sample Holder with Mounting for Reflectance Measurement
	Cuvette Holders		Optical Mount for Transmittance and Reflectance Sample Measurement
	Fiber Optic Attenuator Wavelength 200 - 2500 nm Adjustable slit for attenuation		Fiber Collimator Wavelength 185 - 2500 nm Numerical aperture 0.22 - 0.37 NA, fiber core diameter ≥ 100 µm

We are here for you!


Drop us an email at info@simtrum.com to get the Best Price today.		Want more technical information? Click Here for the professional Customized System/ Solutions.


Don't have time to search the products one by one? No worries. you can download the full range of SIMTRUM Product Line Cards. Click it now.		Want to stay closer to the Market Dynamics and Technological Developments? Just take 5 seconds to Sign In as a member of SIMTRUM, we will bring you the most up-to-date news. (Sign in button on the top right of the screen).

Search Reset

	Availability	Reference Price (USD)
MC/200-1000 High Sensitivity Cooled Spectrometer, MC-series, Wavelength: 200-1000nm	4-6 Weeks	$13900.00
MC/300-1100 High Sensitivity Cooled Spectrometer, MC-series, Wavelength: 300-1100nm	4-6 Weeks	$13900.00
MC/400-930 High Sensitivity Cooled Spectrometer, MC-series, Wavelength: 400-930nm	4-6 Weeks	$12255.00
MC/350-740 High Sensitivity Cooled Spectrometer, MC-series, Wavelength: 350-740nm	4-6 Weeks	$12255.00
MC/530-630 High Sensitivity Cooled Spectrometer, MC-series, Wavelength: 530-630nm	4-6 Weeks	$12255.00
MC/710-1050 High Sensitivity Cooled Spectrometer, MC-series, Wavelength: 710-1050nm	4-6 Weeks	$12255.00
MC/780-1030 High Sensitivity Cooled Spectrometer, MC-series, Wavelength: 780-1030nm	4-6 Weeks	$12255.00

MC/780-1030 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)

0.6

50um Slit Optical Resolution (nm)

0.7

Integration Time

7ms-30min

MC/710-1050 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)

50um Slit Optical Resolution (nm)

1.2

Integration Time

7ms-30min

DV600-1*7-S/S-L2 - Parameter

I600-1*7-S/S-L2 - Parameter

I600-Y*7-S/S-L2 - Parameter

DV600-Y*7-S/S-L2 - Parameter

V1000-Y*2-S/S-L2 - Parameter

I1000-Y*2-S/S-L2 - Parameter

V100-S/S-L2 - Parameter

I100-S/S-L2 - Parameter

DV100-S/S-L2 - Parameter

V200-S/S-L2 - Parameter

I200-S/S-L2 - Parameter

DV200-S/S-L2 - Parameter

V400-S/S-L2 - Parameter

I400-S/S-L2 - Parameter

DV400-S/S-L2 - Parameter

V600-S/S-L2 - Parameter

I600-S/S-L2 - Parameter

DV600-S/S-L2 - Parameter

V1000-S/S-L2 - Parameter

Company
About us Contact us Worldwide Location
Light Analysis
Spectrometers Hyperspectral Camera Power meters Beam Profiler
Microscope
Confocal Microscope Raman Microscope Microscopy Stages TCSPC Solution
Light Sources
Fiber lasers Fiber Amplifier Diode Lasers Incoherent Light
Imaging
sCMOS Camera SW/MW/LW IR Cameras Infrared Pyrometer Microscope Cameras
Optics
Nonlinear Crystals Thz Components Waveplate Objective Lens

Sign In

Register

Retrieve password

BSI Cooled High Sensitivity Spectrometers 200-1100nm | SIMTRUM

MC/780-1030 - Parameter

MC/710-1050 - Parameter

DV600-1*7-S/S-L2 - Parameter

I600-1*7-S/S-L2 - Parameter

I600-Y*7-S/S-L2 - Parameter

DV600-Y*7-S/S-L2 - Parameter

V1000-Y*2-S/S-L2 - Parameter

I1000-Y*2-S/S-L2 - Parameter

V100-S/S-L2 - Parameter

I100-S/S-L2 - Parameter

DV100-S/S-L2 - Parameter

V200-S/S-L2 - Parameter

I200-S/S-L2 - Parameter

DV200-S/S-L2 - Parameter

V400-S/S-L2 - Parameter

I400-S/S-L2 - Parameter

DV400-S/S-L2 - Parameter

V600-S/S-L2 - Parameter

I600-S/S-L2 - Parameter

DV600-S/S-L2 - Parameter

V1000-S/S-L2 - Parameter

I1000-S/S-L2 - Parameter

MC/530-630 - Parameter

MC/350-740 - Parameter

MC/400-930 - Parameter

MC/300-1100 - Parameter

MC/200-1000 - Parameter

MC/780-1030 - Download

MC/710-1050 - Download

DV600-1*7-S/S-L2 - Download

I600-1*7-S/S-L2 - Download

I600-Y*7-S/S-L2 - Download

DV600-Y*7-S/S-L2 - Download

V1000-Y*2-S/S-L2 - Download

I1000-Y*2-S/S-L2 - Download

V100-S/S-L2 - Download

I100-S/S-L2 - Download

DV100-S/S-L2 - Download

V200-S/S-L2 - Download

I200-S/S-L2 - Download

DV200-S/S-L2 - Download

V400-S/S-L2 - Download

I400-S/S-L2 - Download

DV400-S/S-L2 - Download

V600-S/S-L2 - Download

I600-S/S-L2 - Download

DV600-S/S-L2 - Download

V1000-S/S-L2 - Download

I1000-S/S-L2 - Download

MC/530-630 - Download

MC/350-740 - Download

MC/400-930 - Download

MC/300-1100 - Download

MC/200-1000 - Download

Accessories