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  • - Instrument IntroductionThe FTIR-650 is a Fourier transform infrared spectrometer developed by Tianjin Gangdong Company. It features stable performance, ease of operation, a long service life, and low maintenance costs. Widely used in the pharmaceutical, chemical, petroleum, environmental protection, food, materials, public security, defense, semiconductor, and optical industries, it is an indispensable analytical and testing tool for laboratory research and industrial production. It can serve as a dedicated testing system for free silica in air, a dedicated SiO₂ testing system, a dedicated s...
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Sales Hotline:400-105-3560

After-sales service: 022-83712229 (for physics teaching)

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Tianjin, China

Contact Address:2nd Floor, EF Unit, Building G, Xinmao Technology Park, Huayuan Industrial Park, Tianjin

Name: LRS-5 Confocal Raman Spectrometer
Date:2017-07-19

LRS-5 Confocal Raman Spectrometer

面料: 1、Surface enhancement(SERS) Rhodamine6G Rhodamine 6G (also known as Rose Red 6G, Rhodamine 590, Yellow-Green Basic Rhodamine, also known as Rhodamine 6G) is a chemical substance with the molecular formula C28H31N2O3Cl. It appears as a red or yellowish-brown powder. When dissolved in water, it exhibits a scarlet color with green fluorescence; when dissolved in alcohol, it exhibits a red color with yellow fluorescence or a yellow-red color with green fluorescence. It poses significant hazards to humans and other living organisms. 2、Superconducting materials Yttrium-barium-copper-oxide (abbreviated as YBCO)YBCO is the first material with a superconducting transition temperature above 77 K. It can be used as a magnet in nuclear magnetic resonance imaging, magnetic levitation systems, and Josephson junctions. Its superconducting transition temperature is higher than the boiling point of liquid nitrogen (77 K), allowing it to be cooled using relatively inexpensive liquid nitrogen, whereas previously discovered superconductors required cooling with liquid helium (4.2 K) or liquid hydrogen (20 K).YBCO features a perovskite-defect layered structure consisting of alternating CuO-CuO₂-CuO₂-CuO layers, with the CuO₂ layers capable of deformation and folding. Yttrium atoms are present in the CuO₂ and CuO₂ layers, while BaO layers are located between the CuO and CuO₂ layers.3、Semiconductor MaterialsGallium nitride(GaN) Gallium nitride (GaN) is a compound of nitrogen and gallium. As a direct-bandgap semiconductor, it has been widely used in light-emitting diodes since the 1990s. This compound has a structure similar to zinc blende and exhibits high hardness. With a wide bandgap of 3.4 electronvolts, gallium nitride is suitable for use in high-power, high-speed optoelectronic devices. Gallium arsenide(GaAs) Gallium arsenide (GaAs) is a compound of the elements gallium and arsenic; it is a III-V direct-bandgap semiconductor with a zinc blende crystal structure. Gallium arsenide is used in the manufacture of devices such as microwave frequency integrated circuits, monolithic microwave integrated circuits, infrared light-emitting diodes, laser diodes, solar cells, and optical windows. GaAs is frequently used as a substrate material for the epitaxial growth of other III-V semiconductors, including indium gallium arsenide and aluminum gallium arsenide.4、Polymerpolystyrene(PS) Raman spectrum of polystyrenePolystyrene (PS) resin is an amorphous polymer. The side groups of the polystyrene macromolecular chains consist of benzene rings, and the random arrangement of these bulky benzene ring side groups determines the physicochemical properties of polystyrene. The symmetric ring breathing vibrations of cyclic compounds are often the strongest Raman spectral bands. Therefore, the Raman spectrum of polystyrene (PS) primarily features several vibrational peaks at 618 cm⁻¹, 1000 cm⁻¹ (ring breathing), 1029 cm⁻¹, 1199 cm⁻¹, and 1601 cm⁻¹ (C=C bond in the benzene ring). Nylon(PA) Raman spectrum of nylonThe infrared spectra of different types of nylon are extremely similar, but the skeletal structures formed by different methylene sequences exhibit distinct, strong bands in the Raman spectrum, making them easy to distinguish from one another.
Category:
Type: Raman spectrometer
Model:

- 主要参数

名称

参数

测量方式

定性/半定量检测

激光器(激发波长)

532nm(633nm、785nm可扩展)

光谱范围

50~7000cm-1

光谱分辨率

≤1cm-1

波长精度

≤±1cm-1

灵敏度

可观察到硅的四阶峰

空间分辨率

x/y轴:0.01μm;z轴:0.002μm

(与显微镜的微调齿轮减速比相关)

Mapping行程

3〞×2〞

CCD光谱探测器尺寸

26.6×3.2mm

有效像素

1650×200

像素尺寸

16×16μm

共焦针孔

50μm,150μm,200μm,400μm


  • Product Overview
  • Product Applications
  • Typical User

- Instrument Overview


The LRS-5 Confocal Raman Spectrometer is a research-grade Raman testing instrument equipped with a 3D automated stage. Its true confocal optical path ensures the rapid and accurate acquisition of high-resolution spectral images. The LRS-5 features an optimized optical design to deliver industry-leading sensitivity, achieving diffraction-limited spatial resolution while maintaining high light throughput. Combined with a proprietary software operating system, the Raman testing process is made more convenient, efficient, and user-friendly.


- Product Features


ü True Confocal Imaging Capability


High spatial resolution, coupled with a 3D automated stage, enables point-by-point scanning of a sample’s points, lines, surfaces, and depth, yielding spatial distribution images of the sample’s chemical structure, composition, and physical properties.


ü Superior Performance


All optical components are optimally designed to ensure spatial and spectral resolution reach the diffraction limit. High spectral resolution captures detailed sample information—such as crystallinity integrity, polycrystalline vs. amorphous identification, stress effects, and size effects—making analysis simple and intuitive.


ü High Sensitivity


Capable of detecting silicon’s fourth-order peak.


ü Low Wavenumber Performance


Low-wavenumber performance enables detection of spectral ranges difficult to obtain with conventional spectrometers, thereby characterizing a wider range of sample features


ü High-Sensitivity Detector


Low-noise, high-sensitivity receiver delivers experimental results in a short time


ü Software-Controlled Automatic Variable Aperture


Automatic adjustment of confocal aperture


ü Powerful Software


Software system specifically designed for Raman spectroscopy, enabling not only standard spectral acquisition and analysis but also rapid automatic mapping scanning


Optional Raman database available for rapid identification and analysis


ü Flexible Configuration


Modular design: Customers can select different components and models to best meet their needs and achieve high cost-effectiveness


Multiple Lasers: Multiple excitation wavelengths are available, suitable for various samples and optimized experimental results


Multiple Grating: Multiple gratings are available


ü Functionality Expansion


Raman-AFM Coupling and TERS (Tip-Enhanced Raman Spectroscopy)


- Tianjin Gangdong Technology’s Raman Spectroscopy Milestones

1998 Gangdong Technology launched the LRS-2/3 laser Raman/ Fluorescence Spectrometer, designed for Raman and fluorescence spectroscopy measurements and teaching in physics and chemistry laboratories at higher education institutions


2008 Gangdong Technology launched China’s first micro-area laser Raman spectrometer


2009 Gangdong Technology’s micro-area laser Raman spectrometer passed the technical appraisal organized by the Tianjin Municipal Science and Technology Commission and received the Certificate of Scientific and Technological Achievement Appraisal issued by the Tianjin High-Tech Achievement Transformation Center


2010 Gangdong Technology launched China’s first confocal Raman spectrometer


2011 Gangdong Technology participated in the R&D work for the “National Major Scientific Instrument and Equipment Development Project—Research and Development of Laser Differential Confocal Scanning Imaging and Detection Instruments and Their Applications”


2016 The “Research and Development of Laser Differential Confocal Scanning Imaging and Detection Instruments and Their Applications” project successfully passed the expert panel acceptance review


- Comparison of Raman Spectroscopy and Infrared Spectroscopy


(1) Due to differences in spectral principles, the information provided by the two spectroscopic methods also varies. Certain highly symmetrical functional groups with very low polarity and weak infrared absorption exhibit strong spectral bands in Raman spectroscopy; for example, C-C, C=C, and S-S bonds are particularly suitable for Raman spectroscopic analysis. Infrared spectroscopy is only suitable for determining the side chains and terminal groups of polymers, whereas Raman spectroscopy is more commonly used to study the backbone structure of polymers. Raman spectroscopy and infrared spectroscopy are in a “complementary” relationship.


(2) In many cases, samples do not require pretreatment for Raman testing; samples of polymer materials in any form can be tested directly, and they can even be measured while housed in transparent containers, which is particularly convenient for analyzing liquid samples.


(3) Water exhibits very strong infrared absorption, whereas its Raman scattering is weak, with only a faint peak near 1640 cm⁻¹; therefore, Raman spectroscopy is particularly well-suited for the study of aqueous solutions.




- 主要参数

名称

参数

测量方式

定性/半定量检测

激光器(激发波长)

532nm(633nm、785nm可扩展)

光谱范围

50~7000cm-1

光谱分辨率

≤1cm-1

波长精度

≤±1cm-1

灵敏度

可观察到硅的四阶峰

空间分辨率

x/y轴:0.01μm;z轴:0.002μm

(与显微镜的微调齿轮减速比相关)

Mapping行程

3〞×2〞

CCD光谱探测器尺寸

26.6×3.2mm

有效像素

1650×200

像素尺寸

16×16μm

共焦针孔

50μm,150μm,200μm,400μm


1、Surface enhancement(SERS

 LRS-5  共焦显微拉曼光谱仪

Rhodamine6G

 LRS-5  共焦显微拉曼光谱仪

Rhodamine 6G (also known as Rose Red 6G, Rhodamine 590, Yellow-Green Basic Rhodamine, also known as Rhodamine 6G) is a chemical substance with the molecular formula C28H31N2O3Cl. It appears as a red or yellowish-brown powder. When dissolved in water, it exhibits a scarlet color with green fluorescence; when dissolved in alcohol, it exhibits a red color with yellow fluorescence or a yellow-red color with green fluorescence. It poses significant hazards to humans and other living organisms.


 

2、

Superconducting materials


 LRS-5  共焦显微拉曼光谱仪

 LRS-5  共焦显微拉曼光谱仪

Yttrium-barium-copper-oxide (abbreviated as YBCO)


YBCO is the first material with a superconducting transition temperature above 77 K. It can be used as a magnet in nuclear magnetic resonance imaging, magnetic levitation systems, and Josephson junctions. Its superconducting transition temperature is higher than the boiling point of liquid nitrogen (77 K), allowing it to be cooled using relatively inexpensive liquid nitrogen, whereas previously discovered superconductors required cooling with liquid helium (4.2 K) or liquid hydrogen (20 K).


YBCO features a perovskite-defect layered structure consisting of alternating CuO-CuO₂-CuO₂-CuO layers, with the CuO₂ layers capable of deformation and folding. Yttrium atoms are present in the CuO₂ and CuO₂ layers, while BaO layers are located between the CuO and CuO₂ layers.


3、

Semiconductor Materials


Gallium nitride

(GaN)

 LRS-5  共焦显微拉曼光谱仪

LRS-5  共焦显微拉曼光谱仪

Gallium nitride (GaN) is a compound of nitrogen and gallium. As a direct-bandgap semiconductor, it has been widely used in light-emitting diodes since the 1990s. This compound has a structure similar to zinc blende and exhibits high hardness. With a wide bandgap of 3.4 electronvolts, gallium nitride is suitable for use in high-power, high-speed optoelectronic devices.


 

Gallium arsenide

(GaAs)

 LRS-5  共焦显微拉曼光谱仪

LRS-5  共焦显微拉曼光谱仪

Gallium arsenide (GaAs) is a compound of the elements gallium and arsenic; it is a III-V direct-bandgap semiconductor with a zinc blende crystal structure. Gallium arsenide is used in the manufacture of devices such as microwave frequency integrated circuits, monolithic microwave integrated circuits, infrared light-emitting diodes, laser diodes, solar cells, and optical windows. GaAs is frequently used as a substrate material for the epitaxial growth of other III-V semiconductors, including indium gallium arsenide and aluminum gallium arsenide.


4、

Polymer


polystyrene

(PS)

 LRS-5  共焦显微拉曼光谱仪

Raman spectrum of polystyrene


Polystyrene (PS) resin is an amorphous polymer. The side groups of the polystyrene macromolecular chains consist of benzene rings, and the random arrangement of these bulky benzene ring side groups determines the physicochemical properties of polystyrene. The symmetric ring breathing vibrations of cyclic compounds are often the strongest Raman spectral bands. Therefore, the Raman spectrum of polystyrene (PS) primarily features several vibrational peaks at 618 cm⁻¹, 1000 cm⁻¹ (ring breathing), 1029 cm⁻¹, 1199 cm⁻¹, and 1601 cm⁻¹ (C=C bond in the benzene ring).


 

Nylon

(PA)

 LRS-5  共焦显微拉曼光谱仪

Raman spectrum of nylon


The infrared spectra of different types of nylon are extremely similar, but the skeletal structures formed by different methylene sequences exhibit distinct, strong bands in the Raman spectrum, making them easy to distinguish from one another.



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