My ExportersIndia

For Buyer

For Seller

For Help

Our Products

  1. Optical & Laser Instruments 11 Products available
  2. Spectrometers 6 Products available
  3. Industrial Coupler 3 Products available
  4. Rope

    2 Products available
  5. Surgical Light Source

    2 Products available
  6. Sunglasses

    2 Products available
  7. Metal & Metal Products

    2 Products available
  8. Measuring Instruments & Equipment

    2 Products available
  9. Lenses

    2 Products available
  10. Eye Care & Surgery Equipment

    2 Products available
  11. Others Products 38 Products available

Our Products

We are leaders in the market for providing best range of Lithium Niobate Crystal, Single Crystals Oxide, Substrates Single Crystals, Potassium Titanyl Phosphate Crystal and Potassium Titanyle Arsenate Crystal

Lithium Niobate Crystal

  • Used as frequency doublers for wavelength >1m and OPOs pumped at 1064nm and quasi-phase-matched (QPM) devices
  • Most commonly used material for Pockel Cells Q-switches and phase nodulators, waveguide substrate, and surface acoustic wave (SAW) wafers, etc.

Single Crystals Oxide

  • BaTiO, CoO, Cr2O3, FeO, Fe2O3, Gd3Ga5O12, MnO, NiO, SiO2, etc.
  • Polishing ofsurfaces with an orientation accuracy from 2 to

Metal And Alloy Sputtering Targets

  • Shape: Ingot, Plate, Foil, Sheet, Disc, Ring, Rod, Wire, Tube, Granule, Pellet, Shots etc.
  • Aluminum (Al) Target, Antimony (Sb) Target, Silver (Ag) Target
  • Gold (Au) Target, Cerium (Ce) Target, Cobalt (Co) Target
  • Carbon (C) Target, Chromium (Cr) Target, Copper (Cu) Target
  • Cadmium (Cd) Target, Dysprosium (Dy) Target, Erbium(Er) Target
  • Gadolinium (Gd) Target, Germanium (Ge) Target, Holmium (Ho) Target
  • Hafnium (Hf) Target, Indium (In) Target, Iridium (Ir) Target
  • Iron (Fe) Target, Lanthanum (La) Target, Lutetium (Lu) Target
  • Lead (Pb) Target, Magnesium (Mg) Target, Molybdenum (Mo) Target
  • Niobium (Nb) Target, Neodymium (Nd) Target, Nickel (Ni) Target
  • Praseodymium (Pr) Target, Platinum (Pt) Target, Rhenium (Re) Target
  • Ruthenium (Ru) Target, Scandium (Sc) Target, Silicon (Si) Target
  • Samarium(Sm) Target, Tantalum (Ta) Target, Terbium (Tb) Target
  • Titanium (Ti) Target, Thulium(Tm) Target, Tin (Sn) Target
  • Vanadium (V) Target, Tungsten (W) Target, Ytterbium (Yb) Target
  • Yttrium (Y) Target, Zirconium (Zr) Target, Zinc (Zn) Target
View Complete Details

Substrates Single Crystals

  • For Superconductivity: Al2O3, LaAlO3, MgO, NdGaO3, SrLaGaO4, SrTiO3, Nb:SrTiO3, YAlO3, ZrO2(Y), etc.
  • Bicrystals: AlO3, MgO, SrTiO3, Nb:SrTiO3, ZrO2(Y), etc.
  • For III-V nitrides: Al2O3, LiAlO2, LiGaO2, MgAl2O4, MgO, NiAl, SiC, ZnO, etc.
  • Epi-ready polishing of surfaces with an orientation accuracy of

Ceramic Sputtering Targets

  • Boride CeramicSputter Targets:Cr2B, CrB, CrB2, Cr5B3, FeB, HfB2, LaB6, Mo2B, Mo2B5, NbB, NbB2, TaB, TaB2, TiB2, W2B, WB, VB, VB2, ZrB2
  • Carbide CeramicSputter Targets:B4C, Cr3C2, HfC, Mo2C, NbC, SiC, TaC, TiC, WC, W2C, VC, ZrC
  • Fluoride CeramicSputter Targets:AlF3, BaF3, CdF2, CaF2, CeF3, DyF3, ErF3, HfF4, KF, LaF3, PbF2, LiF, PrF3, MgF2, NdF3, ReF3, SmF3, NaF, Cryolite, Na3AlF6 , SrF2, ThF4, YF3, YbF3
  • Nitrides CeramicSputter Targets:AlN, BN, GaN, HfN, NbN, Si3N4, TaN, TiN, VN, ZrN
  • Oxide Ceramic Sputter Ttargets:Al2O3, Sb2O3, ATO , BaTiO3, Bi2O3, CeO2, ZnO, WO3, Nb2O5, , Cu2O, ITO, CuO, Cr2O3 , Dy2O3 , Er2O3, Eu2O3, Gd2O3, Ga2O3, GeO2, HfO2, Ho2O3, In2O3, ITO, Fe2O3, Fe3O4, La2O3, PbTiO3, PbZrO3, LiNbO3, Lu3Fe5O12, Lu2O3, MgO, MoO3, Nd2O3, Pr6O11, Pr(TiO2)2, Pr2O3, Sm2O3, Sc2O3, SiO2, SiO, SrTiO3, SrZrO3, Ta2O5, Tb4O7, TeO2, ThO2, Tm2O3, TiO2, TiO, Ti3O5, Ti2O3, SnO2, SnO, WO3, V2O5, YAG, Y3Al5O12, Yb2O3, Y2O3, ZnO, ZnO:Al, ZrO2(unstabilized), ZrO2-5-15wt%CaO)
  • Selenides Ceramic Sputter Targets:Bi2Se3, CdSe, CuSe, Ga2Se3, In2Se3, PbSe, MoSe2, NbSe2, TaSe2, WSe2, ZnSe
  • Silicides Ceramic Sputter Targets:Cr3Si, CrSi2, CoSi2, HfSi2, MoSi2, NbSi2, TaSi2, Ta5Si3, TiSi2, Ti5Si3, WSi2, V3Si, VSi2, ZrSi2
  • Sulfides Ceramic Sputter Targets:AgS, Ag2S, CuS, Cu2S, Sb2S3, As2S3, CdS, FeS, GaS, GeS, PbS, SnS, In2S3, MoS2, NbS1.75, TaS2, WS2, ZnS
  • Tellurides Ceramic Sputter Targets:Al2Te3, Bi2Te3, CdTe, CuTe, Ga2Te3, GeTe, PbTe, MoTe2, NbTe2, TaTe2, TmTe, WTe2, ZnTe
  • Others:AZO, Cr-SiO, CIGS, ITO, TiZrO3, PbZrTiO3, LaSrMnO3, SrRuO3, IGZO, GaAs, Ga-P, GaSb, In-Sb, InAs, InP, InSn, LSMO, Na3AlF6 , YBCO, LCMO, YSZ
View Complete Details

Laser Safety Devices

Our aim is to make the application oflaser safetyas easy as possible for all of our customers. We offer an extremely wide range oflaser safety products laser goggles, laser safety cabins, laser castle, laser blocking curtains, screens and roller blinds.

Potassium Titanyl Phosphate Crystal

  • Large nonlinear optical coefficient
  • Wide angular bandwidth and small walk-off angle
  • Broad temperature and spectral bandwidth
  • High electro-optic coefficient and low dielectric constant
  • Large figure of merit
  • Nonhydroscopic, chemically and mechanically stable

Semiconductor Wafers

  • Silicon (Si) Wafers, Sapphire Wafer, Germanium (Ge) Wafers
  • Gallium Arsenide (GaAs) Wafers, Gallium Antimonide (GaSb) Wafers
  • Indium Arsenide (InAs) Wafers, Thermal Oxide Wafers
  • Silicon-On-Insulator (SOI) Wafers, Silicon Carbide (SiC) Wafers
  • Zinc Oxide (ZnO) Wafers, Magnesium Oxide (MgO) Wafers
  • Strontium Titanate Oxide (SrTiO3) Wafers, Single Crystal Wafers
  • Quartz Wafers, Glass Wafers, Ceramic Wafers

Potassium Titanyle Arsenate Crystal

  • Crystal length from 0.1mm to 30mm and size up to 15 x 15 x 30mm
  • AR-coating from visible to 3300nm
  • Re-polishing, re-coating service

BIBO Crystal

  • Large crystal size up to 10x10x15mm3
  • AR-coating, mounts and repolishing services

Optical Components

Optics usually describes the behavior ofvisible, ultraviolet, andinfraredlight. Because light is anelectromagnetic wave. Other forms ofelectromagnetic radiationsuch asX-rays, microwaves, andradio wavesexhibit similar properties.

Metal Single Crystals

  • Aluminium (Al), Antimony (Sb), Bismut (Bi), Cadmium (Cd)
  • Chromium (Cr), Cobalt (Co), Copper (Cu), Dysprosium (Dy)
  • Gadolinium (Gd), Germanium (Ge), Gold (Au), Hafnium (Hf)
  • Holmium ( Ho), Indium (In), Iridium (Ir), Iron (Fe), Lead (Pb)
  • Lithium (Li), Magnesium (Mg), Molybdenum (Mo), Nickel (Ni)
  • Niobium (Nb), Palladium (Pd), Platinum (Pt), Rhenium (Re)
  • Rhodium (Rh), Ruthenium (Ru), Silicon (Si), Silver(Ag), Tantalum (Ta)
  • Tellurium (Te), Tin (Sn), Titanium (Ti), Tungsten (W), Vanadium (V)
  • Yttrium (Y), Zinc (Zn), Zirconium (Zr)

Diffusion Bonded Crystals

  • Consist of one laser crystal and one or two undoped material.
  • Combined by optical contact method and further bonded under high temperature
  • Helps to decrease thermal lensing effect considerably

Lithium Iodate Crystal

  • Used for frequency-doubling, -tripling and mixing of low and medium power lasers
  • Provides large size of LiIO3Crystals with high optical homogeneity

Laser Power Meter

  • Thermal Laser Sensors with High Sensitivity for very low powers: 10W to 2W.Low noise and low drift thermal sensors that accurately measure low laser powers over a broadwavelengthrange. They can also be used to measure low single shot laser energies down to 200J.
  • Low Power Thermal Sensors: 10mW to 40W (200W short term): A selection of measurement sensors for low average laser powers, for continuous or pulsed sources having beam sizes up to 60mm. Sensors are so robust that a version of the 40W model can be safely used up to 200W.
  • Laser Thermal for Pulsed and High Energy Density Lasers: Includes very high damage threshold sensorsspecially designed for use with very high energy/high peak power lasers. They have been optimized for laserslike Ruby, Nd:YAG and its Harmonics, Erbium and Ho: YAG.
  • Thermal Sensors for Excimer Lasers: Designed for a power range up to 600W and the 190nm to 400nmwavelength range. Their uniqueExcimer Absorberprovides increased damage threshold and high repetition rate operation under long term UV exposure. Excimer Laser Sensors feature high accuracy and large active areas (up to 50mm)
  • Low-Medium Range Thermal Sensors: Up to 200W, apertures from 25 to 60mm.
  • Laser Power Sensors for Low-MediumCW or Pulsed Lasers Powers:Intermittent use up to 300W.
  • Medium Power Thermal Sensors: 300 and 500W, apertures 60mm and 70mm
  • Medium-High Power Fan and Water Cooled Thermal Sensors: 600W, apertures 30mm, 40mm and 60mm
  • Laser Thermal Sensors for High Powers: Includes water cooled, high power thermal laser measurement sensors up to 6KW, and apertures to 55mm.
  • Photodiode BasedLaser Sensors:Can measure powers between 100nW and 500mW and cover a spectral range between 200nm to 1800nm.
View Complete Details

Titanium Doped Sapphire Crystal

  • Used for widely tunable and ultrashort pulsed lasers with high gain and high power outputs
  • Growth method of Temperature Gradient Technique (TGT)

Collimators And Focusers

  • We offer a complete line of fiber collimators and focusers with lowback reflection, designed to collimate or focus light exiting a fiber to a desired beam diameter or spot size.

Optical Fiber Fusion Splicer

  • Our Fiber Fusion Splicer is a reliable single fiber fusion splicer. It has automatic or manual splicing mode, fast splicing (8 second), large color LCD display, large internal battery, communication port, and multiple display language option.
    • Fiber Type: SM, MM, DS, NZ-DS, EDF
    • Cladding Diameter: 100-150um
    • Coating Diameter: 100-1000um
    • Fiber Cleave Length: 8-22mm

Wdm Coupler

  • We provide WDM couplers or multiplexers for special wavelengths. These optical couplers are manufactured using fused fiber technique. They combine and split signals at 1064nm and 1550nm, or 1550nm and 1625nm, with low insertion loss, polarization insensitive, high reliability and high isolation. Other available wavelengths include 980/1310nm, 1064/1310nm WDM couplers.

Femtoline Optics

  • Femtoline Components including: mirrors, lens kits, laser dispersing prisms, polarizing optics, laser and nonlinear crystals for fundamental wavelengths of Ti:Sapphire and Yb:KGW/KYW lasers and their doubled, tripled or quadrupled frequencies.

Beam Expander

  • Galilean type, compact or zoom beam expanders for 1064 nm, 532 nm and 355 nm wavelengths. F-Theta lens for scanning and engraving applications for 1064 nm, 532 nm wavelengths. Special form lens used to distribute energy of Gaussian beam to Top Hat profile - Gauss-to-Top Hat Beam Shaping Lens.
  • Zoom Beam Expanders: Compact Galilean type zoom beam expanders for Nd:YAG lasers fundamental and its harmonics wavelength: 1064nm, 532nm and 355nm.
  • Compact Beam Expanders: A laser beam expander is designed to increase the diameter of a collimated input beam to a larger collimated output beam.

Laser Beam Dump

  • Air-Cooled Beam Dump can be used on beams of up to 50Watts in the wavelength range from 0.1-30m.
  • Water-Cooled Beam Dump can be used for beams up to 1 kW in the wavelength range from 0.1-30m.

Laser Windows

Wide selection of Laser Windows made from high quality UV FS, BK7 optical material. Round (Dia from 12.5-76.5mm, Thickness from 2-6mm) and Rectangular (from 15x20 to 50, 8x50x8mm, Thickness from 3-156mm) Laser Windows can be found in product catalogue, other custom sizes are available under request.

  • Round/Rectangualr windows
  • Precision Thin Round Windows
  • Precision Round/Rectangular Windows
  • Optical Flats

Polarizing Optics

Complete selection of components that modify the state of polarization of optical radiation. Polarizing optics includes: brewster windows, polarization plane rotators, round or rectangular thin film laser polarizers that are coated for particular laser application. Cube polarizing beam splitters, glan-taylor polarizing prisms, wollaston and rochon polarizing prisms are available. Wide selection of quartz retardation plates, including: zero order optically contacted and air-spaced wave plates, achromatic air-space wave plate, zero order dual wavelength wave plate, low order and multiple order wave plates.

  • Brewster windows
  • Round thin film laser polarizers
  • Rectangular thin film laser polarizers
  • Cube polarizing beam splitters
  • Natural calcite glan laser polarizing prisms
  • -BBO glan laser polarizing prisms
  • Wollaston prisms, rochon polarizing prisms
  • Zero order optically contacted wave plates
  • Zero order air-sapced wave plates
  • Achromatic air-sapced wave plates
  • Zero order dual wavelength wave plates
  • Low order wave plates
  • Multiple order wave plates
  • Multiple order dual wavelength wave plates
  • Polarization plane rotators
  • Frensel rhombs
View Complete Details

Photomultiplier Detection System

  • Provides a complete detection system for SP's Digikrom monochromators
  • Easy USB2.0 interface
  • Wide selection of PMTs
  • Range 185-900nm, 185-650nm, 400-1100nm, 185-850nm, 185-930nm

Helium Neon Laser Sources

  • Ideal for Raman spectroscopy, holography, fast scanning, and test and measurement applications.
  • Wavelength 632.8nm, Upto Power 35mW, TEM00
  • Available either in randomly or linearly polarized
  • Stabilized He-Ne Lasers are also available

Plano Concave Lens

Plano-convex, Plano-concave, Bi-convex, Bi-concave, Plano-convex cylindrical, Plano-concave cylindrical lenses made of BK7, UVFS or CaF2 optical material. Focal lengths vary from 1000 to 5000mm.

  • Plano-Convex Lens (Materials BK7/UVFS/CaF2)
  • Bi-Convex Lens (BK7/UFVS)
  • Plano Concave Lens
  • Biconcave Lens
  • Conical Lenses (Axicones)
  • Plano Conave/ConvecCylindrical Lenses
  • BK7/UVFS Series Lens Kit

High Power Laser To Fiber Couplers

  • Available Wavelengths: 180 - 2000nm
  • Power Handling: Up to 5 Watts CW for SM applications
  • Over 100 Watts CW for MM Applications

High Power Pulsed Fiber Laser Source

Pulsed Fiber Sources (PFS) are a series of compact turnkeysystems or OEM modules based on a highly reliable master oscillator/power amplifier (MOPA) design, to deliver multi-kilowatt level peak powers with average output powers of up to 1W.

  • Peak powers up to 10 kW
  • Average output power from 20 mW to 1W
  • Output wavelengths of 1064, 1085, or 1550nm
  • Adjustable pulse durations, repetition rates
  • Gaussian beam profiles

Optical Coupler

  • Multimode optical fiber couplers are widely used in optical local networks or FTTx networks that use multimode fibers. These couplers can be fabricated using 50/125 or 62.5/125 micron fibers and at central wavelengths of 850nm or 1310n.
  • Single mode wideband couplers have 80nm bandwidth, compared to 40nm of standard single mode couplers. This product has very low excess loss and high temperature stability.

Hand Held Optical Power Meter

  • A high-resolution optical power meter with a wide dynamic range covering a broad spectrum of wavelengths.
    • Hand held optical power meter with InGaAs Detector & battery for wavelength range 800-1650nm. Measurement range -75-10dBm. Measures in watt/dBm/dB.
    • Hand held optical power meter with Silicon Detector & rechargeable battery for wavelength range 440-900nm. Measurement range -65dBm. Measures in watt/dBm/dB.

Compact Meter Monochromator

  • Czerny-Turner, dual-grating turrets
  • Focal Length 110mm
  • Double grating turret allows for broad spectral range coverage
  • Maximum Resolution

CCD Camera

  • Cooled CCD cameras are available for your specific application and budgetary needs
  • Accessories such as fibers/fiber couplers, special probes, and light sources are also available to help complete your system
  • We offering the best value in CCD spectroscopy, you can select high resolution spectrographs for use with cameras operating from 200nm to 1100nm
  • Multiple input imaging is also supported by the larger 1/4 meter and 1/2 meter spectrograph systems

IR Viewer

  • Wavelength Range: 350-2000nm.
  • Magnification: 1X/1.8X/2X.
  • Field Of View: 40deg/25deg/20deg.
  • Infrared (IR) radiation is non-visible to human eye, so there is a need for a device toobserve the radiation. Usually IR Laser Beam Visualizers are used for align infrared laser beam & calibrate Laser system.

Optical Circulators

  • Optical circulators typically have three ports: an input, a common port and an output. The light from input port is guided out at the common port, while the light fed in from the common port can only emit from the output port. Optical circulators can be used to separate the light transmitted in opposite directions inside a single optical fiber.

Calibration Light Source

  • Depending on the gas filled in a lamp, discrete spectral lines of defined wavelength, spectral width and relative intensity can be obtained
  • Five Elemental Emitters Hg, Ne, Xe, Ar, and Kr

Fiber Pigtailed Isolators

Isolators are optical devices that allow light to be transmitted in one direction only. They are most often used to prevent any reflected light from entering the source, thus preventing any feedback problems, such as frequency instability, relaxation oscillations, amplified stimulated emissions, or optical damage from occurring.

  • Wavelength Range: 1050 -1080nm
  • Reliable high power handling: As much as 80Watts
  • High Isolation, up to 50dB isolation possible from a single stage

Deuterium Light Source

  • Application: The most useful source of UV for analyticalinstruments
  • Wavelength Range: 180 to 400nm(Maximum 160- 400nm)
  • Power Output Available: 30W, Continuous, Collimated Output
  • Optional Accessories: Optical fiber with termination SMA, FC, ST

Digital Tunable Attenuator

  • We offer a compact, rugged and low cost digital attenuator with high resolution, high speed, high attenuation range and high power handling (blocking technique only).

Metallic Laser Mirrors

Dielectric and Metallic Laser Mirrorsfor Fixed, Narrowband or Broadband wavelength applications covering UV-IR. Wide range of Round, Customized Shapes as well as Plano, Spherical, Cylindrical Surfaces Mirrors and Substrates are available.

  • Substrate for Laser Mirrors
  • Elliptical Substrate for Laser Mirrors
  • Laser Line Mirrors
  • Dual Laser Line Mirrors
  • Broadband Laser Mirrors
  • Dichroic Mirrors
  • Metal Coated Flat Round/Rectangular/Spherical Mirrors
  • Aluminum/Silver/Gold Protected Mirrors
  • BK7/UVFS/IRFS/Infrasil/Calcium/Magnesium Fluoride Dichroic Mirrors

UV And IR Optics

Substrates and finished optical components such as windows, lenses, mirrors manufactured from lithium fluoride (LiF), magnesium fluoride (MgF2), calcium fluoride (CaF2), barium fluoride (BaF2), sapphire (Al2O3), zinc selenide (ZnSe), germanium (Ge) for UV and IR applications.

  • LiF/ MgF2/CaF2 components
  • BaF2 lneses
  • BaF2 windows
  • Sapphire (Al2O3) components
  • ZnSe lenses/windows
  • Germanium components
  • Copper mirrors
  • Silicon mirrors

DPSS Lasers And Diode Lasers

  • 04-01 Series: Compact & Low Noise SLM CW DPSS Lasers, Wavelength Range: 457-1064nm, CW power up to 400mW
  • 05-01 Series:Single Frequency & High Power Ultra-Low Noise DPSS Lasers, Wavelength Range:355-1064nm, CW power up to 3W
  • 06-01 Series:Ultra-compact diode & DPSS lasers, Wavelength Range:405-660nm up to 250mW
  • Cobolt Odin Series:Wavelength selectable 2-5m, Up to 80mW at 10 kHz, Compact & tunable Mid-IROPOs, Tunable up to 50nm
  • Cobolt Tor Series: Up to 1W average power, 7 kHz pulse repetition rate
  • Cobolt Optogenetics Solutions: Wavelength 473, 532, 561, 594, 638, 660nm, >100mW output power
  • Options & Accessories:Heatsinks, Fiber coupling solutions, Dual combiners, Modulated dual combiners

Photon Counters

Photon counting is a technique in which individual photons are counted using some single-photon detector (SPD). The counting efficiency is determined by the quantum efficiency and any electronic losses that are present in the system.

Laser Barrier And Curtains

  • Portable or Stand-alone.
  • Wall Attached/Floor Attached.
  • Window Coverings.
  • Ceiling Attached.
  • Custom.
  • Ideal for containing high powered laser to a specific area. We supply standard or custom configurations to meet your requirements.

Polarizer Maintaining Patchcords

  • Polarization Maintaining (PM) patchcords are based on a high precision butt-style connection technique. The PM axis orientation is maintained by using male connectors with a positioning key and a bulkhead female receptacle with a tightly tolerance keyway, ensuring good repeatability in extinction ratios and insertion losses.

Photon Detector

ID100 VIS Best Dark Count Rate

  • Silicon Avalanche Photodiode, Free-Running
  • 40ps Timing Resolution, Low Dark Count Rate

Xenon Light Source

  • Application: Xenon is most suitable for UV, Visible and NIR range spectroscopic Application
  • Wavelength Range:185-2200nm
  • 320-2200nm Ozone Free
  • Power Output Available: 100W- 1000W
  • Optional Accessories: Monochromator for tuning the wavelength range

Optical Filters

Include Color Glass filters, Neutral Density absorption type filters, Crystalline Materials for UV Bandpass Filters.

  • Crystallline material for optical UV band pass filters
  • ND Reflective type filters at 400-2000nm
  • ND Absorption type filters at 450-650nm
  • Color Glass Filters

Halogen Light Source

  • Application: QTH Light is suitable visible and NIR range spectroscopic Application
  • Wavelength Range: 300nm to 2.6m
  • Power Output Available:5W 30W fiber coupling QTH Light Source
  • 50W- 150W collimated output

F Theta Lenses

  • The F-Theta Lens is designed to provide a flat field on the image plane for scanning and engraving applications where a high power laser and set of rotating mirrors are used to scan across a given field.
Tell Us What are you looking for? Will call you back

Contact Us