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BSI High Sensitivity UV Spectrometer 200-1100nm

M Series BSI High Sensitivity UV Enhanced Spectrometer (Backside Illuminated) utilizes Hamamatsu area array backside-illuminated CCD, and its UV sensitivity is increased by about 7 times compared to an ordinary spectrometer. At the same time, it uses 280 & 760nm double blazed grating, equipped with LVF anti-high-order filter, based on a 100.0mm focal length optical platform. It provides a balanced sensitivity and higher resolution in the full spectrum of 200~1100nm, which is suitable for a variety of Spectrometers for scientific research applications.

Key Product Highlights

Peak 70% UV response - utilizes Hamamatsu back-thinned CCD and have over 70% quantum efficiency in the ultraviolet 200nm, which is very suitable for Broad-spectrum measurement including ultraviolet band;


64x2048 Super large sensing surface

super-large sensing area CCD, which sensitivity is further improved by 4 times as compared to the ordinary 14-line pixel CCD;

 

200-1100nm Full spectrum coverage- 

M Series use optical platform with a focal length of 100.0mm which is suitable for full spectrum detection at 200~1100nm, covering the entire photosensitive area of the detector while increasing the resolution by 10%.


Application Highlights 

Jewellery / Ore Spectroscopy

Desktop Raman Spectroscopy

Desktop LIBS

Transparent reflection/ Absorption spectrum 

Fluorescence spectrum measurement  

Microscopic spectroscopy 






Product specifications and Brochures

Product Brochure Link:  

Detection Range

200 ~ 1100nm, depending on the grating

Optical Resolution

The highest 0.2nm (FWHM), based on 1800 line grating and 10μm slit, 

Detector

Hamamatsu, S10420, 64×2048 pixels, 64-line area array back-illuminated

Eliminate High-order Diffraction

3 kinds of front and 4 kinds of post filter options to eliminate ghost lines in the spectrum

Optical Platform

Focal length 100.0mm, f-number 4.5,   symmetrical cross CT light path

Integration Time

10ms ~ 120s, dark noise saturation over 120s

Dynamic Range

5,000:1, more than twice better than similar products, which is good for weaker signal detection

Signal-to-noise Ratio

800:1 (when saturated)

Stray Light

<0.1% @ 600nm

Correction Linearity

> 99%

Step Drawings



Configuration Example


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


M Series Wavelength, Slit and Optical Resolution Option

ModelWavelength RangeGrating Scribe / Blaze WavelengthSlit Width
10 um25 um50 um100 um200 um
Optical Resolution FWHM
M/200-1100200-1100nm300/300nm & 550nm1nm1.3nm1.8nm3nm6nm
M/400-1000400-1000nm400 /500nm1.4nm1.5nm1.6nm2.6nm5nm
M/350-800350-800nm600 /500nm0.8nm1nm1.2nm1.6nm3nm
M/530-640530-640nm1800 /500nm0.2nm0.3nm0.4nm0.5nm1nm
M/710-1100710-1100nm600 /800nm0.8nm1nm1.2nm1.6nm3nm
M/780-1060785-1060nm830 /900nm0.38nm0.45nm0.6nm0.95nm1.8nm



Product Size



Photonic Crystal Sensor Measurement


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Figure 1, Reflectance spectra of TPEP-SiO2 anti-structure photonic crystals during the absorption-desorption 

process of different vapours

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 Figure 2,Different concentrations of TPEP-SiO2 vapor reflectance spectra 

 and the repeatability of adsorption-desorption

This experiment is carried out by placing the prepared TPEP-SiO2, (Tetraphenylethene polymer-SiO2 inverse opal) anti-structure photonic crystals in tetrahydrofuran and acetone vapor respectively and observed the changes in the reflectance spectrum over time during the adsorption and analysis of the measured photonic crystals (Figure 1). In addition, it can be observed in Figure 2 that the red shift of the band gap was caused by different concentrations of steam by changing the content of tetrahydrofuran and acetone in the steam. From the test results, the photonic crystal prepared in the experiment will undergo red shift when absorbing tetrahydrofuran and acetone vapor, and the degree of red shift is related to the concentration of organic matter in the absorbed vapor. The forbidden band of the photonic crystal will gradually return to its position before absorption after absorbing the organic gas in the air.


 Up-Conversion Of Fluorescence Nanocomposites


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Figure 3, Spectral and temperature characterization results of csUCNP@C nanocomposite materials and experimental verification of photothermal therapy in vivo


This experiment is done by combining the temperature-responsive up-conversion luminescent material with the photothermal nanomaterial and detected the microscopic temperature of the photothermal nanomaterial through the change of the luminescence signal. In order to prove the feasibility of the experiment, the spectrum and temperature of the csUCNP@C nanocomposite are characterized, the related characteristics of the two are studied, and photothermal treatment experiments on mouse tumour tissues are conducted (Figure 3). For the detection of the spectrum in the experiment, a portable spectrometer  from Compound Optics was used (Figure 3a). Experiments have found that in a specific temperature range, the logarithm of the intensity ratio at 525nm and 545nm is linear with the inverse of temperature (Figure 3b), and the light intensity at 545nm is inversely proportional to temperature (Figure 3e). During the photothermal process, the increase in microscopic temperature is much greater than the change in macroscopic temperature. After experimental optimization, the experiment results achieved selective killing of individual cells under low-power density light excitation. In addition, they used up-conversion luminescence to monitor the microscopic temperature of tumour-bearing mice, and implemented feedback-type tumour photothermal killing, achieving high-precision photothermal therapy under mild conditions (Figure cf).


Lens Quality Inspection Of handphone


iphone 2.png

Iphone.png

Figure 1, Transmittance spectrum curve


This experimental setup is based on our spectrometer), It has a built-in deuterium halogen light source, a fiber collimator and a near-infrared fiber transmission spectrum measurement system, which allows our spectrometer to measure the transmission spectrum of the IR ink window of the mobile phone accurately. In Figure 1, the top left picture shows the transmittance spectrum curve of the IR ink window tested using L Series, while the right picture is tested using the H Series. It can be seen from the figure that the transmittance of IR ink in the visible light part is less than 10%, and the transmittance in the near-infrared band (900~1050nm) is greater than 70%. This is due to the signal-to-noise ratio (SNR) which is relatively poor in the band greater than 1000nm. In addition, the weaker optical signal measured in this band, results in the spectrometer's SNR not being fully utilized. By replacing the L Series with the better performing H Series , the SNR of this band will be improved significantly.       


 Genernal Lens Quality Inspection


Spectacle.png 



This experimental setup is based on general purpose spectrometer, built with a R3 integrating sphere measuring stand, deuterium halogen light source, fiber collimator and ultraviolet fiber. The built-up transmission spectrum measurement system allows our spectrometer to measure the transmittance of the standard praseodymium and neodymium lenses. The spectrometer was calibrated to meet necessary indicators of the national standard and technical specifications which allows quick and easy tests on transmission ratio of spectacle lens and related materials. The test result uses the recommended configuration to measure the transmittance of the standard lens, and the interpolation method (origin) calculates the corresponding standard transmittance in the spectral curve, resulting in the wavelength interval being 10nm. 


Chlorophyll Spectral Analysis


Chlorophyll.jpgFigure 3, Chlorophyll absorption spectrum

This experimental setup is based on general purpose spectrometer, built with deuterium halogen light source, and ultraviolet fiber. The absorption spectrum measurement system allows our spectrometer to analyze cuvette holder R4. In Figure 3, it shows the chlorophyll spectrum of the leaves of Scirpus sylvestris measured by our spectrometer. Since no further organic solvent extraction is used, the spectral peaks of chlorophyll a and chlorophyll b in the chloroplast pigment are superimposed to a certain extent, but chlorophyll a and chlorophyll can still be marked at the maximum absorption peak of chlorophyll b. The use of our spectrometer allows for quick measurement of chlorophyll spectrum of the plants. Further analysis conducted for chlorophyll absorption spectrum can determine its level.





 Agriculture Greenhouse Irradiance Measurement


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                          Figure 4, Plant photosynthesis absorption spectrum          

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                          Figure 5, the transmittance spectrum of the double glass film


Plant photosynthetic pigments have the strongest absorption of blue and red light and the highest utilization rate. Therefore, the solar spectrum is in the range of 400~520nm (blue) and 610~720nm (red), which is most conducive for plant growth. The light transmittance of the double-glass thin-film modules used in the roof of the photovoltaic greenhouse is tested to ensure that the shielding of the thin-film modules does not affect the growth of the crops inside. If the transmittance of the thin film is low, the roof thin-film solar panels and ordinary transparent glass can be used. LED lights was used to supplement the spectrum required by plants to achieve the light environment for growth. In this case, the spectrometer was used to detect the transmittance of the double-glass thin film module, and the obtained spectrum is shown in figure 5. It can be seen from figure 5, that the dual-glass thin film module has blocked UV light. The transmittance of blue light which is required for plant growth is low, and the transmittance of red light is about 15%, which is sufficient for plant growth, and it can also be supplemented according to its needs during production. At the same time, the thin film component has a high transmittance of infrared light, which is conducive to the maintenance of heat in the greenhouse to maintain off-season temperature difference. The use of our Spectrometers allows efficient detection of transmittance from greenhouse film, which benefits greenhouse building inspections to allow better light supplementation in the greenhouse.



NameModelWavelength RangeDetectorResolutionNoise RatioDynamic Range

High Resolution Spectrometer

L Sereis200-1100nmHamamatsu,S11639,2048 pixels<1nm customizable500:12000:1

High Resolution Spectrometer

H Series200-1100nmHamamatsu,S11639,2048 pixels<1nm customizable500:12000:1

Back Illuminated Spectrometer

M Series200-1100nmHamamatsu,S10420,64×2048 pixels<1nm customizable800:15000:1

Hi Sensitivity Cooled Spectrometer 

MC Serie200-1100nmHamamatsu,S7031,64×1044 pixels<1nm customizable1000:110000:1

Handheld Raman System 

RM785/1064nm

Band Range 

200-3200cm-1/ 200-2500cm-1

6 - 8 cm-1

Portable Tabletop Raman System

RMT EZ785nmBand Range  200-3200cm-1
7 cm-1  typical

Portable Tabletop Raman System

RMT532/785/1064nm

Band Range 

200-3200cm-1/200-1800cm-1

8 - 9 cm-1 typical


Cooled NIR Spectrometer 

N Series900-2200nmHamamatsu, G11477up to 8nm
@10um slit width
15000:115000:1

MWIR Spectrometer 

MWIR Series1-5umPbS or PbSe  256 pixels10-30nm20 RMS

Imaging Spectrometer 


240 -1100nm2046 x 1542, 2448 x 2048, 5472 x 34780.44 to 0.66nm


Accessories

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

Model   No.TypeWavelengthCore DiameterLength# of FiberConnector
I1000-S/S-L2Optic Fiber360~2500 nm1000 μm2 m1SMA905-SMA905
V1000-S/S-L2200 ~ 1100 nm1000μm2 m1SMA905-SMA905
DV600-S/S-L2190~1100 nm600μm2 m1SMA905-SMA905
I600-S/S-L2360~2500 nm600μm2 m1SMA905-SMA905
V600-S/S-L2200 ~ 1100 nm600μm2 m1SMA905-SMA905
DV400-S/S-L2190~1100 nm400μm2 m1SMA905-SMA905
I400-S/S-L2360~2500 nm400μm2 m1SMA905-SMA905
V400-S/S-L2200 ~ 1100 nm400μm2 m1SMA905-SMA905
DV200-S/S-L2190~1100 nm200μm2 m1SMA905-SMA905
I200-S/S-L2360~2500 nm200μm2 m1SMA905-SMA905
V200-S/S-L2200 ~ 1100 nm200μm2 m1SMA905-SMA905
DV100-S/S-L2190~1100 nm100μm2 m1SMA905-SMA905
I100-S/S-L2360~2500 nm100μm2 m1SMA905-SMA905
V100-S/S-L2200 ~ 1100 nm100μm2 m1SMA905-SMA905
I1000-Y*2-S/S-L2

Bifurcated Fiber,

 Y-bundle : 2 fibers

360~2500nm1000μm2 mA-2nos, B1-1nos, B2-1nosA-SMA905 / B1-SMA905 / B2-SMA905
V1000-Y*2-S/S-L2200 ~ 1100 nm1000μm2 mA-2nos, B1-1nos, B2-1nosA-SMA905 / B1-SMA905 / B2-SMA905
DV600-Y*7-S/S-L2190~1100 nm600μm2 mA-7nos, B1-1nos, B2-6nosA-SMA905 / B1-SMA905 / B2-SMA905
I600-Y*7-S/S-L2360~2500nm600μm2 mA-7nos, B1-1nos, B2-6nosA-SMA905 / B1-SMA905 / B2-SMA905
DV600-1*7-S/S-L2Multi-core Fiber190~1100 nm600μm2 m7SMA905-SMA905
I600-1*7-S/S-L2360~2500nm600μm27SMA905-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 MeasurementSample Holder with Mounting for Reflectance Measurement
Cuvette HoldersOptical 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

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Compare Model Drawings & Specs Availability Reference Price
(USD)
M/200-1100
Back-Illuminated Spectrometer, M-Series, Wavelength: 200-1100nm
4-6 Weeks Request for quote
M/400-1000
Back-Illuminated Spectrometer, M-Series, Wavelength: 400-1000nm
4-6 Weeks Request for quote
M/350-800
Back-Illuminated Spectrometer, M-Series, Wavelength: 350-800nm
4-6 Weeks Request for quote
M/530-640
Back-Illuminated Spectrometer, M-Series, Wavelength: 530-640nm
4-6 Weeks Request for quote
M/710-1100
Back-Illuminated Spectrometer, M-Series, Wavelength: 710-1100nm
4-6 Weeks Request for quote
M/780-1060
Back-Illuminated Spectrometer, M-Series, Wavelength: 785-1060nm
4-6 Weeks Request for quote

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

M/780-1060 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)
0.45

50um Slit Optical Resolution (nm)
0.6

Integration Time
10ms-120s

M/710-1100 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)
1

50um Slit Optical Resolution (nm)
1.2

Integration Time
10ms-120s

M/530-640 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)
0.3

50um Slit Optical Resolution (nm)
0.4

Integration Time
10ms-120s

M/350-800 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)
1

50um Slit Optical Resolution (nm)
1.2

Integration Time
10ms-120s

M/400-1000 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)
1.5

50um Slit Optical Resolution (nm)
1.6

Integration Time
10ms-120s

M/200-1100 - Parameter

Wavelength (nm)

25um Slit Optical Resolution (nm)
1.3

50um Slit Optical Resolution (nm)
1.8

Integration Time
10ms-120s

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

M/780-1060 - Download

M/710-1100 - Download

M/530-640 - Download

M/350-800 - Download

M/400-1000 - Download

M/200-1100 - Download

Accessories

Compare Model Drawings & Specs Availability Reference Price
(USD)
I1000-S/S-L2
Optic Fiber, Wavelength 360-2500 nm, Number of Fiber 1nos, Core Diameter 1000 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
V1000-S/S-L2
Optic Fiber, Wavelength 200-1100 nm, Number of Fiber 1nos, Core Diameter 1000 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
DV600-S/S-L2
Optic Fiber, Wavelength 190-1100 nm, Number of Fiber1nos, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905, Package 5.5 Blue armored tubing
2-3 Weeks Request for quote
I600-S/S-L2
Optic Fiber, Wavelength 360-2500 nm, Number of Fiber 1nos, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
V600-S/S-L2
Optic Fiber, Wavelength 200-1100 nm, Number of Fiber 1nos, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
DV400-S/S-L2
Optic Fiber, Wavelength 190-1100 nm, Number of Fiber 1nos, Core Diameter 400 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
I400-S/S-L2
Optic Fiber, Wavelength 360-2500 nm, Number of Fiber 1nos, Core Diameter 400 um, Length 2M, Connector SMA905-SMA905, Package 5.5 blue armored tubing
2-3 Weeks Request for quote
V400-S/S-L2
Optic Fiber, Wavelength 200-1100 nm, Number of Fiber 1nos, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905, Package 5.5 blue armored tubing
2-3 Weeks Request for quote
DV200-S/S-L2
Optic Fiber, Wavelength 190-1100 nm, Number of Fiber 1nos, Core Diameter 200 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
I200-S/S-L2
Optic Fiber, Wavelength 360-2500 nm, Number of Fiber 1nos, Core Diameter 200 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
V200-S/S-L2
Optic Fiber, Wavelength 200-1100 nm, Core Number 1nos, Core Diameter 200 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
DV100-S/S-L2
Optic Fiber, Wavelength 190-1100 nm, Core Number 1nos, Core Diameter 100 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
I100-S/S-L2
Optic Fiber, Wavelength 360-2500 nm, Core Number 1nos, Core Diameter 100 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
V100-S/S-L2
Optic Fiber, Wavelength 200-1100 nm, Core Number 1nos, Core Diameter 100 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
I1000-Y*2-S/S-L2
Bifurcated Fiber, Y-bundle: 2 fibers , Wavelength 360-2500 nm, Core Diameter 1000 um, Length 2M, Connector SMA905-SMA905, Package 6.0 armored tubing
2-3 Weeks Request for quote
V1000-Y*2-S/S-L2
Bifurcated Fiber, Y-bundle: 2 fibers, Wavelength 200-1100 nm, Core Diameter 1000 um, Length 2M, Connector SMA905-SMA905, Package 6.0 armored tubing
2-3 Weeks Request for quote
DV600-Y*7-S/S-L2
Bifurcated Fiber, Y-bundle: 7 fibers, Wavelength 190-1100 nm, Core Number A-7nos, B1-1nos, B2 - 6nos, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905,Package PVC
2-3 Weeks Request for quote
I600-Y*7-S/S-L2
Bifurcated Fiber, Y-bundle: 2 fibers , Wavelength 360-2500 nm, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
I600-1*7-S/S-L2
Multi-core Fiber, Wavelength 360-2500 nm, Number of Fiber 7nos, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote
DV600-1*7-S/S-L2
Multi-core Fiber, Wavelength 190-1100 nm, Core Number 7nos, Core Diameter 600 um, Length 2M, Connector SMA905-SMA905, Package PVC
2-3 Weeks Request for quote