Cerium-doped Lutetium Yttrium Orthosilicate or LYSO(Ce) scintillator has the advantages of high light output, high density, short decay time, excellent timing and energy resolution. These properties make LYSO(Ce) becoming the most popular scintillators in Nuclear medicine (Positron Emission Tomography, PET/CT, and SPECT scan system), high energy physics, security scanners, and other applications. OST Photonics has a complete set of crystal processing and assembly line, we can process all kinds of lyso scintillation crystal and LYSO(Ce) arrays according to customer's requirements. We have our own laboratory to test the product performance to ensure that the product performance meets the requirements of our customers. We provide professional solutions for lyso crystal growth, surface treatment and array assembly. Application of LYSO Ce Scintillators (LYSO:Ce Scintillators) Positron emission tomography-computed tomography (PET-CT) Nuclear magnetic resonance imaging (NMRI) Single photon emission computed tomography (SPECT) High energy physics Advantages of LYSO scintillator (LYSO:Ce Scintillators) High light output High density Short decay time Stable chemical and physical lyso scintillator properties The Ability of OST Photonics Maximum Size: 105mm x 200mm Available items: monolithic crystal, scintillation screen, pixellated array
LYSO crystal is an ideal generation scintillator crystal. LYSO stand for Cerium doped Lutetium Yttrium Orthosilicate. LYSO crystal has the advantages of high light output, high density, fast decay time, good energy resolution and low cost. These properties mean that LYSO is an ideal candidate for a range of ray detection applications in nuclear physics and nuclear medicine, which require higher though improved timing resolution and superior energy revolution. Growth Method: Czochralski method Max. Blank Size: Dia65mmxLength200mm Shapes: cylinder, rectangular solid, disk The thinnest thickness: 0.05mm Content of (Ce): 0.5%mol Physical Properties Of our LYSO: Density(g/cm3) 7.1 light output to NaI(Tl)(%) 75 Decay time(ns) 41 Energy Resolution(%) 10 Fluorescence wavelength(nm) 420 Hardness(Mohs) 5.8
OST Photonics CdWO4 Scintillators(Cadmium Tungstate Scintillators) CdWO4 Cadmium tungstate crystal is a high density, high atomic number scintillator with a relatively high light yield. The emission maximum is at 475nm and the total light output is 12 to 15 photons/keV. The light yield relative to NaI(Tl) on a bialkali PMT is 30 to 50%. In addition, CdWO4 Scintillator cadmium tungstate scintillator also has the advantages of strong radiation resistance and no radioactive background. The high light output and low afterglow make it ideal for use with silicon photodiodes in detectors for medical and industrial Computed Tomography (CT) scanners. OST Photonics is able to supply CdWO4 crystals cadmium tungstate scintillator and CdWO4 linear or 2-D array upon your requests.
CdWO4 Cadmium tungstate crystal is a high density, high atomic number scintillator with a relatively high light yield. The emission maximum is at 475nm and the total light output is 12 to 15 photons/keV. The light yield relative to NaI(Tl) on a bialkali PMT is 30 to 50%. In addition, CdWO4 Scintillator cadmium tungstate scintillator also has the advantages of strong radiation resistance and no radioactive background. The high light output and low afterglow make it ideal for use with silicon photodiodes in detectors for medical and industrial Computed Tomography (CT) scanners. Ost Photonics is able to supply CdWO4 crystals cadmium tungstate scintillator and CdWO4 linear or 2-D array upon your requests. Application of CdWO4 Scintillators (Cadmium Tungstate Scintillators) Industrial computed tomography (CT) scanners Medical computed tomography (CT) scanners Security inspection High energy physics Advantages of CdWO4 Scintillator (Cadmium Tungstate Scintillator) Low afterglow Relatively high light yield Strong radiation resistance High density high atomic number No radioactive background The Ability of OST Photonics CdWO4 Scintillators(Cadmium Tungstate Scintillators) Maximum Size: �¸80mm x 200mm Available items: monolithic crystal, linear or 2-D array
Properties of LYSO: Density(g.cm-3): 7.2 Radiation length(cm): 1.16 Decay constant(ns): 40 Emission peak(nm): 420 Light output(Photons/Mev): 20,000 Anti-radiation(rad): 108 Melting point(C): 2047 Hardness(Mho): 5.8 Refractive Index: 1.82 Hygroscopicity: none Cleavage: none.
Li-6 lithium glass scintillator is a kind of inorganic scintillator which can be used for thermal neutron detection. It has the advantages of short decay time, high efficiency of slow neutron detection and good temperature performance. In addition, the Li-6 glass scintillator is easy to process and form, non-hygroscopic, acid and alkali resistant, can withstand the high and low temperature rapid change. Therefore, in the harsh situation that contains corrosive liquid and vapor, the lithium glass (Ce) can still work, but other scintillators cannot be suitable. Li-6 glass scintillator are widely used in neutron time-of-flight experiments, oil and natural gas exploration, moisture content measurement, nondestructive testing and neutron photography. OST Photonics can provide different specifications of Li-6 glass scintillators according to your requirements. Neutron time-of-flight experiments Oil and natural gas exploration Moisture content measurement Nondestructive testing(NDT) Neutron photography Advantages of Li-6 Glass Scintillators Fast decay time High efficiency of slow neutron detection Good temperature performance Non-hygroscopic The Ability of OST Photonics Maximum Size: �¸50mm x 50mm Available items: monolithic glass
OST Photonics KDP Crystals/DKDP Laser Nonlinear Crystals Potassium Dihydrogen Phosphate (KDP) and Potassium Dideuterium Phosphate (DKDP, KD*P) are among the most widely-used commercial NLO materials. KDP crystals and DKDP crystals are commonly used for doubling, tripling and quadrupling of Nd:YAG laser at the room temperature. In addition, KDP crystals and DKDP crystals are also excellent electro-optic crystals with high electro-optic coefficients, widely used as electro-optical modulators, Q-switches, and Pockels Cells, etc. If you would like to know more about KDP crystals and DKDP crystals prices, please do not hesitate to contact Ost Photonics.
OST Photonics GSGG Substrates GGG (12.373) has a similar lattice constant of YIG (12.376), it is widely used as the substrate material of YIG magneto-optical thin film. However, in order to improve the magneto-optical optimum value of magneto-optical thin film, sometimes it is necessary to select a single crystal substrate with a larger lattice constant. GSGG (12.554) is that the 2 Ga of the octahedron in the GGG crystal are replaced by Sc with a larger ionic radius, thus having a larger lattice constant.
OST Photonics Cylindrical Lenses Cylindrical lenses are utilized for astigmatism correction in the eye and rangefinders, inducing astigmatism by elongating a point of light into a line. They find extensive application in barcode scanning, projection optics systems, laser measurement systems, and holography. Ost Photonics offers cylindrical concave lens in plano-concave or plano-convex configurations. Basics about Cylindrical Lenses LENSES MATERIALS ILLUSTRATION PROPERTIES AND APPLICATIONS CYLINDRICAL LENS BK7/ Fused Silica/CaF2 /other optical glass Used to provide focusing power in one section only. For illumination or detection of light from line sources. Also used for the anamorphic compression of beams and images. Specifications of Cylindrical Lenses Material Schott N-BK7, CDGM H-K9L, Fused silica, CaF2, Sapphire Design wavelength 546.07nm Design index (bk7) 1.51680 for BK7, 1.45846 for Fused Silica Diameter tolerance +0.0, 0.15mm +0.0, 0.05mm Paraxial focal length �±2% �±0.5% Centration Clear aperture 80% 90% Surface quality 60-40 scratch and dig 10-5 Scratch and dig Surface irregularity Protective bevel 0.25 + 0.25, -0.0mm 0.2 �± 0.1mm Coating Uncoating, AR or Single layer MgF2 coating upon request What Is a Cylindrical Lens Used For? Cylindrical lenses are specialized optical components used primarily to correct astigmatism, a common refractive error in the eye. Unlike spherical lenses, which have the same curvature in all directions, cylindrical lenses have curvature in only one direction. This unique property allows them to focus light into a line rather than a point, making them ideal for applications requiring precise control over light direction and focus. OST Photonics, a leader in cylindrical optics, offers high-quality cylindrical lenses designed to meet various optical needs.
Crystals such as sodium chloride (NaCl), potassium bromide (KBr) and potassium chloride (KCl) are uniform, bright and high transmittance within 0.250-20 �¼m when thickness less than 10mm, and no impurity absorption. These single crystals are ideal materials for making optical elements for prisms, lenses, filters, and various windows in infrared devices and optical instruments. OST Photonics offers high quality KBr substrates for researchers and industries. Crystal orientation, size and thickness can be customized according to your requirements. Application of KBr Substrates Infrared devices optical instruments Advantages of KBr Substrate Uniform, bright and high transmittance within 0.250-20 �¼m when thickness less than 10 mm No impurity absorption Ability of KBr Substrates Orientation:,,, etc. Dimension: 1, 2, 10x10mm, 20x20mm, etc. Thickness: 0.5mm, 1.0mm, 2mm, 5mm, etc. Available items: windows, substrates, blanks and customized optics
OST Photonics LiTaO3 Crystal Substrates The chemical formula of lithium tantalate is LiTaO3, lithium tantalate crystal is colorless or yellowish crystal. LiTaO3 crystal is a ferroelectric crystal with excellent electro-optical, piezoelectric, electrical and pyroelectric properties. Use the pulling method to grow. The lithium tantalate crystal is used as a Q-switch in laser technology, as a pyroelectric detector in infrared technology, and can also be used to make filters and resonators.
OST Photonics BaF2 IR Windows Crystals BaF2 window crystals or Barium Fluoride window crystals, with their extremely broad transmission range from the deep UV to LWIR spectrum, are prevalent for Infrared applications requiring additional transmission in the Ultraviolet region. BaF2 window crystals are excellent when being used for IR spectroscopes and as viewport windows for thermal imaging inspection in electric power facilities and petroleum industries. A low refractive index of 1.48 implies BaF2 crystal windows have high transmission rates without anti-reflection coating. BaF2 window crystals has similar properties to CaF2, the difference mainly lies in that barium fluoride window is more resistant to highly energetic radiation, and with an equivalent thickness, the transmission range of BaF2 window extends approximately 1 micron further into the long-wave IR region than calcium fluoride. BaF2 window crystals could also accommodate high-temperature environments up to 800 â??. However, exposure to moisture will increase its sensitivity to temperature and reduce its transmission rate to UV lights. If you would like to know more about BaF2 IR windows, BaF2 window crystals prices, please do not hesitate to contact Ost Photonics.
BaF2 window crystals or Barium Fluoride window crystals, with their extremely broad transmission range from the deep UV to LWIR spectrum, are prevalent for Infrared applications requiring additional transmission in the Ultraviolet region. BaF2 window crystals are excellent when being used for IR spectroscopes and as viewport windows for thermal imaging inspection in electric power facilities and petroleum industries. A low refractive index of 1.48 implies BaF2 windows have high transmission rates without anti-reflection coating. BaF2 window crystals has similar properties to CaF2, the difference mainly lies in that barium fluoride window is more resistant to highly energetic radiation, and with an equivalent thickness, the transmission range of BaF2 window extends approximately 1 micron further into the long-wave IR region than calcium fluoride. BaF2 window crystals could also accommodate high-temperature environments up to 800 â??. However, exposure to moisture will increase its sensitivity to temperature and reduce its transmission rate to UV lights. If you would like to know more about BaF2 IR windows, BaF2 window crystals prices, please do not hesitate to contact Ost Photonics. Infrared and ultraviolet windows/prism High energy physics Nuclear physics Nuclear medicine Advantages of BaF2 Window (Barium Fluoride Window)Crystals Excellent Transmission from 200nm 12m Resistant to High-Energy Radiation Provide High Transmission without AR Coatings
±-BBO (±-BaB2O4) is a negative uniaxial crystal which has large birefringence over a broad transparent range of 190nm to 3500nm. ±-BBO is an excellent crystal especially in UV and high power applications. The physical, chemical, thermal, and optical properties of alpha-BBO crystal are similar to those of Beta-BBO. However, there is no second order nonlinear effect in alpha-BBO crystal due to the centrosymmetry in its crystal structure and thus it has no use for second order nonlinear optical processes. Instead, alpha BBO is widely used for fabrication of polarizers, polarizing beam displacers, phase retarders, birefringent plates, and time delay compensators especially those for UV and high power lasers. Applications of ±-BBO Crystals High power Beam displacers for isolators. High power Polarizer Time delay compensators Advantages of ±-BBO Crystals High UV transmittance Large birefringence High damage threshold Here at OST Photonics, we value integrity, accountability, and punctuality. Our vision is to be the most professional and reliable supplier of crystal products in the world.
Scintillator crystal including CsI(Tl) scintillator, NaI(Tl) scintillator, BGO, LYSO, LaBr3,Ce scintillator, CWO, PWO, plastic scintillator.
Array form 16x1, 8x8, 16x16, 21x21, and customization Minimum singe pixel: 0.2x0.2x0.5mm Available Crystal material: LYSO(Ce), BGO and CsI(Tl Reflective Materials BaSO4, 3M ESR for BGO and LYSO array TiO2 main for CsI(Tl) array Thickness of BaSO4 and TiO2 0.1mm Thickness of ESR 0.065mm Type: single-layer array, double-layer array and Linear array Application: LYSO and BGO array: Nuclear medicine such as PET and SPECT CsI(Tl) array: Security scanner and Container scanner
Bismuth germinate Bi4Ge3O12 commonly abbreviated as BGO, is the crystalline form of an inorganic oxide with cubic eulytine structure, colorless, transparent and insoluble in water. When exposed to radiation of high energy particles or other sources, such as gamma-rays, x-rays, it emits a green fluorescent light with a peak wavelength of 480nm, with its high stopping power, high scintillation efficiency, good energy resolution and non-hygroscopes, Our BGO is a good scintillation material and has found a wide range of applications in high energy physics, nuclear physics, space physics, nuclear medicine, geological prospecting and other industries. Growth Method: Bridgman method Max. Blank Size: 40mmx80mmx200mm Dia65mmxLength200mm Standard size: Dia1.0â??xLength1.0â??,Dialength 2.0â??xLength2.0â?? Shapes: cylinder, rectangular solid, disk The thinnest thickness: 0.05mm The Property of Our BGO Crystal: Density(g/cm3) 7.13 Emission center wavelength(nm): 480 light output To NaI(Tl)(%) 20 energy resolution(%) 12 Decay time(ns) 300 Hardness(Mohs) 5
1. DESCRIPTION The Model YE2730 d33 meter is a special instrument directly to measure piezoelectric constant d33 values of piezoelectric ceramics, polymers, and single crystals. This meter can also measure d33 value in various single crystal materials, such as lithium niobate, quartz, and tourmaline. This meter is capable of measuring d33 value over a very large range, at high resolution, and with a high degree of reliability. The measurement is quickly, and easily made with a minimum of training required. Specimens of a variety of sizes and shapes can easily be accommodated and measured. For example: d33 value of disks, blocks, rings, tubes and semispherical shells can be easily measured and displayed on the Model YE2730 d33 meter. Measuring d33 value is displayed on a 3 1/2 inch digital meter. This instrument is invaluable as a tool for quality assurance of piezoelectric materials, production in-line inspection, or for research applications. 2. SPECIFICATIONS D33 Range: x 1 range: 10 to 2000 PC/N x 0.1 range: 1 to 200 PC/N Accuracy: x 1 range: ±2% of d33 value in 100 to 2000 PC/N ±5% of d33 value in 10 to 200 PC/N x 0.1 range:.±2% of d33 value in 10 to 200 PC/N ±5% of d33 value in 1 to 20 PC/N Resolution:. x 1 range: 1 PC/N . x 0.1 range: 0.1 PC/N Force: Frequency: 110Hz Amplitude: 0.25N Polarity Indication: indicates polarity on upper face of test element in compression. (â??-â??sign means negative, no sign positive) Shunt Capacitance: 1 pF (for x 1 range) 0.1 pF (for x 0.1 range) Dimensions: .Force Head: 110x140mm, Chassis: 280x200x90mm Weight: Force Head: 3 kgs, Chassis: 2 kgs Power: 110/220V, 50/60Hz, 20W (In the instrument panel on the back of the switch are switch selectable.)
Tl-doped sodium iodide NaI(Tl)ï¼?It is most widely used in all the scintillation materials especially used in Environmental monitoringï¼?radiation monitoringï¼?oil exploration and nuclear medicine. It has the maximum light output in all the scintillation crystals. Typesï¼?Blank and Aluminum encapsulation stock size: Dia:1.0â??xL1.0â??, Dia: 2.0â??xL2.0â?? Max size for cylinder: Dia:150mmxL400mm Max size for rectangular solid: 100x100x400mm Property of our NaI(Tl) crystal: Density (g/cm3) 3.67 Light output(%NaI:Tl) 100 Hygroscopicity Deliquescent Energy Resolution (%) 7.3 Emission wavelength(nm) 415 Hardness (Mohs) 2
The luminescence efficiency of CsI(Na) is similar to that of NaI(Tl) crystals. The emission spectrum peaked at 420nm can match well with PMT. Its temperature dependence is small and can be mainly applied in the well logging. Regular size: Dia 50mmx Length300mm Customized sizeï¼?Dia 39mmxLength 49mm Typesï¼?Blank and aluminum encapsulation Property of our CsI(Na) Density (g/cm3) 4.51 Light Yield NaI(Tl) (%) 85 Radiation length 1.86 Emission peak(nm) 420 Hygroscopicity deliquescent Hardness (Mohs) 2 Melting point(â??) 621
