High Damage Threshold Beamsplitter Cubes
    All of our polarizing beam splitter cubes are epoxy free, making them suitable for high power applications with energy densities exceeding 10 J/cm2 at 1064 nm.
    • Optical bonding for epoxy-free optical paths - no glue!
    • High-energy laser-line and broadband designs
    • Custom cubes for multiple wavelengths or wavelength regions available
    • RoHs Compliant
    In addition to the standard sizes and wavelengths, we can produce high-energy cube beamsplitters from 1×1 mm2 in size, and in a wide variety of materials including fused silica, BK7, YAG, and other optical glasses and crystals.

    High Damage Threshold Beamsplitter Cubes
    High Damage Threshold Beamsplitter Cubes

    Polarizing Beamsplitter Cubes
    All of our polarizing beam splitter cubes are epoxy free, making them suitable for high power applications with energy densities exceeding 10 J/cm2 at 1064 nm.
    These high-precision assemblies have been widely used in telecommunications, semi-conductor and biomedical applications where transmission efficiency, extinction ratio and wavefront quality are all critical specifications.

    In addition to the standard sizes and wavelengths, we can produce high-energy cube beamsplitters from 1×1 mm2 in size, and in a wide variety of materials including fused silica, BK7, YAG, and other optical glasses and crystals.

    Main Features:
    • Optical bonding for epoxy-free optical paths - no glue!
    • High-energy laser-line and broadband designs
    • Wavelength Range: 400-1100 nm /680-1080 nm
    • Damage Threshold up to >10 J/cm2 @ 1064 nm
    • Custom cubes for multiple wavelengths or wavelength regions available
    • RoHs Compliant


    Polarizing Beamsplitter Cubes
    Polarizing Beamsplitter Cubes

    Micro Optics
    These high-quality custom optics and optical assemblies combine our IBS coatings, ultraprecise fabrication capabilities and epoxy-free, which are widely used in the telecommunications, semi-conductor and biomedical industries.
    Because of their miniature size, they can be placed right at the objective lens or at the tip of optical fibers and light pipes.

    Applications:
    • Beam-delivery micro-systems
    • Fiber-optic
    • Endoscopic systems
    • Fluorescence spectroscopy
    • Raman spectroscopy
    • Optical-coherence tomography (OCT)
    • Multiphoton microscopy (MPM)
    • Confocal microscopy.
  • Main Features:
    • High precision laser optics and assemblies from 1 mm in size
    • Multi-element, micro-optic assemblies with epoxy-free optical paths
    • Custom dielectric HR, AR and polarizing coatings available
    • Operating Wavelength: UV, Visible, NIR, telecom bands, MWIR (250–5000 nm)
    Products include: Solid and air-spaced etalons,Polarization beam splitters,Waveplates,Beamsplitter cubes,Right angle turning prisms.

    Micro Optics
    Micro Optics

    Broadband Beamsplitters 458-1550nm - BBS
    BBS broadband beamsplitter plates can be used to either split or combine a laser beam with a broad bandwidth or multiple beams in the same optical path within a specified wavelength range.
    A durable all-dielectric multilayer coating design is used for neutral splitting of unpolarized visible or near-infrared light at a convient 90° angle.
    • Broadband dielectric 45° beamsplitter
    • Damage Threshold 100 mJ/cm2, 20 nsec, 20 Hz @ 1064 nm
    • 50/50 laser splitting
    • Low reflection BBAR coating on back surface (S2)
    • For CW and low energy pulsed laser applications
    • Wavelength Range: 458-529nm/488-694nm/650-1100nm/1200-1550nm
    • Other beamsplitting ratios are available
    • Other wavelengths and sizes are available


    Broadband Beamsplitters 458-1550nm - BBS
    Broadband Beamsplitters 458-1550nm - BBS

    Long Wave pass Dichroic Beamsplitters LWP
    LWP Long Wave Pass Dichroic Beamsplitters exhibit high transmission for a long wavelength band, high damage thresholds, and high reflectivity for a shorter band of wavelengths.

    Reflectivity bandwidth is limited by coating design, incidence angle and polarization.
    • Fluorescence microscopy
    • Optical parametric generation
    • Customer-specified reflected and transmitted wavelengths
    • Custom substrate diameters and thicknesses
    • Damage Threshold:
      • cw:1 MW/cm2 @ 1064 nm
      • Pulsed: 10 J/cm2, 20 nsec, 20 Hz @ 1064 nm


    Long Wave pass Dichroic Beamsplitters  LWP
    Long Wave pass Dichroic Beamsplitters  LWP

    Broadband Dielectric Cube Beamsplitters BSD

    • Wavelength Range: UV 250-440nm/ 450-650nm/650-900nm/1300-1600nm
    • UV Transmission:
      • 50%±5% for 280–400 nm wavelength range
      • 45%±5% for 250–280 nm wavelength range
    • VIS & NIR Transmission: 50%±5% for average polarization
    • Material: UV-grade synthetic fused silica/ BK7 for VIS & NIR


    UV- VIS- NIR Broadband Dielectric Cube Beamsplitters BSD
    UV- VIS- NIR Broadband Dielectric Cube Beamsplitters BSD

    Fixed Ratio Polarizing Cube Beamsplitters - PCBS
    PCBS Fixed Ratio Cube Beamsplitters provide a choice of split ratios at a variety of narrowband wavelengths for specific polarization states.
    A durable all-dielectric partial reflection coating is used at the internal interface, and all external surfaces are anti-reflection coated for the wavelength specified.
    For best spectral performance and transmitted wavefront, fixed ratio cube beamsplitters should be used with collimated or near-collimated input light.

    The PCBS and other cemented beamsplitter cubes are easy to mount.
    • Damage Threshold: 1 J/cm2, 20 nsec, 20 Hz @ 1064 nm
    • Optical Material: BK7 glass
    • Fewer ghost images than plate beamsplitter
    • Choice of wavelength and split ratios
    • Easy to handle and mount
    • Equal optical path lengths


    Fixed Ratio Polarizing Cube Beamsplitters - PCBS
    Fixed Ratio Polarizing Cube Beamsplitters - PCBS

    Broadband Hybrid Cube Beamsplitters-BSC
    BSC - Broadband Hybrid Cube Beamsplitters, Ultraviolet , Visible and Near infrared.
    • UV Transmission:
      • 43%±6% for 280–400 nm wavelength range
      • 38%±6% for 250–280 nm wavelength range
      • s- and p-components matched to within 5% for both ranges
    • Visible & IR Transmission:
      • 45%±6%
      • Coating HEBBAR™ antireflection coating (entrance and exit faces)


    UV, VIS NIR Broadband Hybrid Cube Beamsplitters-BSC
    UV, VIS NIR Broadband Hybrid Cube Beamsplitters-BSC

    High Energy Plate Beamsplitter 193-2100nm - BS1
    BS1 high energy beamsplitters are plate windows coated with an all-dielectric coating to separate laser light into your choice of R/T split ratios.
    The BS1 high energy plate beamsplitters exhibit almost no absorption and are designed specifically for 45° at the wavelength and polarization of interest.
    Ultrahard, high-damage-threshold coatings are available for all wavelengths from 193 nm to 2100 nm. Internally reflected ghost images are minimized by an antireflection coating on the rear surface.
    • Each face is polished to flatness of λ/10 or better.
    • Beamsplitters are ideal for beam separation or combination
    • Damage Threshold:
      • cw: 1 MW/cm2 @ 1064 nm
      • Pulsed: 10 J/cm2, 20 nsec, 20 Hz @ 1064 nm
      • Wavelength Range: 193nm to 2100nm


    High Energy  Plate Beamsplitter 193-2100nm - BS1
    High Energy  Plate Beamsplitter 193-2100nm - BS1

    Broadband Polarizing Cube Beamsplitters -PBSH
    Serie PBSH: These broadband polarizing beamsplitter cubes are made from N-SF2 glass to improve broadband performance. For high-energy applications, CVI Melles Griot recommends other materials such as fused silica or N-BK7 glass, although they may not work as well over a wide wavelength range.
    • Improved 500:1 extinction ration
    • Broadband polarizer optimized for visible and near infrared wavelength
    • Damage Threshold:
      • cw: 100 W/cm2 @ 515 nm
      • Pulsed: 500 mJ/cm2, 20 nsec, 20 Hz @ 515 nm
    • Polarizing Bandwidth: 250nm at 515nm
    • Optical Material: N-SF2 glass
    • Reflected and transmitted beams separated by 90°


    Broadband Polarizing Cube Beamsplitters -PBSH
    Broadband Polarizing Cube Beamsplitters -PBSH

    High Energy Harmonic Separators - BSR
    BSR Serie: High energy harmonic separators are used to reflect a lasers primary or harmonic wavelength while transmitting another. Our standard High Energy Harmonic Separators are designed for the Nd:YAG and Ti:Sapphire laser systems.
    • Isolate Nd:YAG and Nd:YLF harmonics
    • 2nd, 3rd, 4th, and 5th harmonic separation
    • Characterization of collagen orientation in human dermis by two-dimensional second-harmonic-generation polarimetry
    • High energy all dielectric coating design, AR coated on side 2
    • 45° dichroic beamsplitters
    • Damage Threshold:
      • cw: 1 MW/cm2 @ 1064 nm and 532 nm
      • Pulsed: 10 J/cm2, 20 nsec, 20 Hz for reflection @ 1064 nm
      • 4 J/cm2, 20 nsec, 20 Hz; for reflection @ 532 nm
      • 4 J/cm2, 20 nsec, 20 Hz for transmission @ 1064 nm
    • Transmitted Wavelength Range: 266-1064nm/ 488-515nm/ 532-1064nm


    High Energy Harmonic Separators - BSR
    High Energy Harmonic Separators - BSR

    Continously Variable Beamsplitters - ABS
    Continuously variable attenuation of linearly polarized light is achieved with a multiorder rotatable half-waveplate followed by a polarizing beamsplitter cube. The s-polarized light is reflected at 90° while p-polarized light is transmitted straight through the assembly.
      Applications include:
    • Variable laser sampling
    • Holography
    • Interferometry
    • Light entanglement
    • Variable ratio beamsplitting
    • Available Wavelengths: 266-355-515-535-633-780-830-850-1030-1064-1550nm
    • ABS standard cubes are cemented
    • ABSO high powered cubes are optically contacted
    • Damage Threshold:
      • ABS: 1 J/cm2, 20 nsec, 20 Hz @ 1064 nm
      • ABSO: 5 J/cm2, 20 nsec, 20 Hz @ 1064 nm
    • Optical Material:
      • ABS: Crystal quartz and BK7 glass
      • ABSO: Crystal Quartz and Fused Silica


    Continously Variable Laser Beamsplitters - ABS
    Continously Variable Laser Beamsplitters - ABS

    High Energy Ultra Thin Beamsplitters - UT
    The UT ultra thin plate beamsplitters is an all-dielectric, non-absorbing plate beamsplitter on a fused silica substrate for high energy beamsplitting.
    Use this beamsplitter when you need to minimize beam displacement
    With greater than 10J/cm2 damage threshold, CVI's ultra thin plate beamsplitters are especially useful for high energy applications where cemented beamsplitter cubes may fail.
    Plate beamsplitters are thinner and lighter than cube beamsplitters.
    This may be required in some applications where there is not enough room for a cube.
    • Minimizes displacement of transmitted beam
    • Damage Threshold:
    • cw: 1 MW/cm2 @ 1064 nm
    • Pulsed: 10 J/cm2, 20 nsec, 20 Hz @ 1064 nm
    • User specified reflectance from 1 percent to 99.5 percent
    • User specified CWL from 244nm to 1550nm
    • Standard 1.25" OD ring mount prevents breakage and fits easily into 1.25" lens or ring mount


    High Energy Ultra Thin Beamsplitters - UT 244 nm to 2100 nm
    High Energy Ultra Thin Beamsplitters - UT 244 nm to 2100 nm

    Laser Line Non-polarizing Plate Beamsplitter -BSNP
    The BSNP all dielectric 45 degree non-polarizing plate beamsplitters divide laser energy while preserving input polarization in reflected and transmitted beams. Choose from three aperture dimensions and a variety of laser wavelengths.
    With 3J/cm2 damage threshold, CVI's nonpolarizing plate beamsplitters are especially useful for high energy applications where cemented beamsplitter cubes may fail.

    Plate beamsplitters are thinner and lighter than cube beamsplitters.
    This may be required in some applications where there is not enough room for a cube.
    • 50% reflectance
    • |Rs-RP|< 5%
    • Damage threshold > 3 J/cm2
    • Cement free
    • Laser Line Wavelengths: 532nm-633nm-1064nm-1550nm


    Laser Line Non-polarizing Plate Beamsplitter -BSNP
    Laser Line Non-polarizing Plate Beamsplitter -BSNP

    Laser Line Non-Polarizing Cube Beamsplitter -NCBS
    Non-polarizing cube beamsplitters divide a single wavelength into nearly equal reflected and transmitted beams. The NCBS serie nonpolarizing coating reduces |Rs-Rp| and |Ts-Tp| from 35% to less than 5% for popular visible and near infrared laser wavelengths.
    • 3-axis control prism mount available
    • Designed for low power applications
    • Optical Material: BK7 glass
    • Transmitted Wavefront Error: λ/4 at 633 nm
    • Laser Line Wavelengths: 488-515nm/532nm/633nm/780nm/830nm/1064nm


    Laser Line Non-Polarizing Cube Beamsplitter -NCBS
    Laser Line Non-Polarizing Cube Beamsplitter -NCBS

    Optical Isolators 248nm-1550nm - OI
    The OIO high energy optical isolator utilizes a multiple order waveplate (QWPM) and an optically contacted cube beamsplitter (PBSO), while the standard OI isolator uses a cemented beamsplitter cube (PBS).
    This alternative to a Faraday isolator achieves passive isolation of linearly polarized light by combining a cube polarizer and a 1/4-waveplate.
    • Passive isolation of linearly polarized light
    • Custom isolators available for other wavelengths UV to NIR
    • Isolation: 20dB or 35dB
    • Clear Aperture: 6.35 and 12.7mm
    • Damage Threshold:
      • 20 dB OI: 1 J/cm2, 20 nsec, 20 Hz @ 1064 nm
      • 20 dB OIO: 5 J/cm2, 20 nsec, 20 Hz @ 1064 nm
      • 35 dB: 100 mJ/cm2, 20 nsec, 20 Hz @ 1064 nm
    • Optical Material:
      • OI: Crystal quartz and BK7
      • OIO: Crystal quartz and Fused Silica


    Optical Isolators 248nm-1550nm - OI
    Optical Isolators 248nm-1550nm - OI

    High-Energy Laser Polarizing CubeBeamsplitter PBSO
    PBSO - High-Energy Laser-Line Polarizing Cube Beamsplitters coatings are designed for maximum extinction ratio (T p/T s). Those applications requiring maximum transmission efficiency, Tp > 98.0% can be achieved by slightly reducing the extinction ratio.
    • Optically contacted
    • Reflected and transmitted beams separated by 90°
    • Contact us for other wavelengths from UV to near IR
    • Extinction Ratio: λ=532 nm or 1064 nm: T p/T s>500:1/λ < 500 nm: T p/T s>250:1
    • Damage Threshold:
      • cw: 1 MW/cm2 @ 1064 nm
      • Pulsed: 5 J/cm2, 20 nsec, 20 Hz @ 1064 nm


    High-Energy Laser Polarizing CubeBeamsplitter PBSO
    High-Energy Laser Polarizing CubeBeamsplitter PBSO

    Pellicle Beamsplitters - PLB
    PLB Pellicle beamsplitters is a high tensile strength elastic membrane, stretched like a drumhead over a black anodized flat metal frame, and bonded to the precision lapped edge.
    • There is virtually no ghosting.
    • Chromatic and spherical aberration are negligible in converging beams.
    • Low absorption is exhibited across the visible spectrum. Nitrocellulose material does exhibit some absorption in the ultraviolet and in the infrared beyond 2 μm.
    • There is no change in the optical path.
    • Available uncoated or coated
    • Pellicle Thickness: ≤2 μm
    • Wavelength range: 400-700nm & 633nm


    Pellicle Beamsplitters - PLB 400-700nm or Uncoated
    Pellicle Beamsplitters - PLB 400-700nm or Uncoated

    Laser Line Polarizing Cube Beamsplitters PBS
    Serie PBS: Polarizing beamsplitter cubes are used to split a laser beam into two orthogonally polarized components; p-polarization is transmitted straight through while s-polarization is reflected at 90°. PBS polarizer cubes utilize a durable all-dielectric coating at the internal cemented interface, and all external surfaces are antireflection coated for the wavelength specified.
    • Improved 1000:1 extinction ration
    • Damage Threshold:
      • cw: 100 W/cm2 @ 515 nm
      • Pulsed: 1 J/cm2, 20 ns, 20 Hz @ 1064 nm
    • Projection systems, signal monitoring, color separation and recombination, optical coupling
    • Fewer ghost images than plate beamsplitters
    • Optical isolation (in combination with waveplate)
    • Continuously variable beamsplitter (In combination with waveplate)


    Laser Line Polarizing Cube Beamsplitters  PBS
    Laser Line Polarizing Cube Beamsplitters  PBS

    Sampling Beamsplitter Cubes - SBC
    Known as a leaky polarizing beamsplitter, the SBC Sampling Beamsplitter Cube is both a fixed ratio beamsplitter while also maintaining a controlled amount of P polarization to "leak through" into the reflected beam
    • Optical disk testing
    • Polarization sensitive beamsplitter cubes
    • Four standard beamsplitting ratios available


    SBC.pdf

    Low-Dispersion Polarizers 400-800nm TFPK
    The TFPK serie is low-dispersion polarizing beamsplitters to satisfy requirements for very-high-power, short-pulse lasers. These optics are ideal for intracavity use in femtosecond regenerative amplifiers. The main emphasis is on linear phase characteristics.
    • Ideal for intracavity use in femtosecond regenerative amplifiers
    • Low group-velocity dispersion for ultrashort femtosecond applications
    • Custom wavelengths from 250–1550
    • Substrate material: UV grade fused silica or BK7 glass
    • High reflector, metal and partial reflector coatings available


    Low-Dispersion Polarizers  400-800nm TFPK
    Low-Dispersion Polarizers  400-800nm TFPK

    Ultrafast Isosceles Brewster prisms IB
    Isosceles Brewster angle prisms are designed specifically for intracavity laser applications, usually for specific wavelengths or wavelength ranges. The dispersion of these prisms is less than that of an equilaterial prism, but the beam enters and exits the prism near Brewster's angle, minimizing intracavity losses.
    • GVD correction prisms for femtosecond systems
    • Two sides (AB) optically polished
    • Extremely small loss for p-polarized beam
    • Damage Threshold:
      • Suprasil 1: 15 J/cm2, 20 nsec, 20 Hz @ 1064 nm
      • Fused Silica: 15 J/cm2, 20 nsec, 20 Hz @ 1064 nm
    • Optical Material: Suprasil 1, UV-grade fused silica or N-SF10 glass


    Isosceles Brewster prisms  IB
    Isosceles Brewster prisms  IB

    UV Laser-Line Polarizing Cube Beamsplitters UPBS
    Serie UPBS: UV polarizing cube beamsplitters are made from UV grade fused silica to improve UV performance.
    • Fused-silica cube polarizers for doubled argon, tripled Nd:YAG, quadrupled Nd:YAG, and UV excimer lasers
    • 100:1 extinction ratio
    • Transmission efficiency > 90%
    • For use with fluences less than 10 mJ/cm2
    • Contact us for 193 nm polarizers
    • Damage Threshold:
      • cw: 10 W/cm2 @ 266 nm
      • Pulsed: 10 mJ/cm2, 20 nsec, 20 Hz @ 266 nm
    • Wavelengths: 248-257-266-308-351-355nm


    UV Laser-Line Polarizing Cube Beamsplitters UPBS
    UV Laser-Line Polarizing Cube Beamsplitters UPBS

    Short Wave Pass Dichroic Beamsplitters SWP
    Short wave pass dichroic beamsplitters exhibit high transmission for a short wavelength band, high damage thresholds, and high reflectivity for a longer band of wavelengths.
    • Fluorescence microscopy
    • Optical parametric generation
    • Custome-specified reflected and transmitted wavelengths
    • To maximize efficiency, reflect 45° s-polarization and transmit 45° p-polarization
    • Damage Threshold:
      • cw; 1 MW/cm2 @ 1064 nm
      • Pulsed: 10 J/cm2, 20 nsec, 20 Hz @ 1064 nm


    Short Wave Pass Dichroic Beamsplitters SWP
    Short Wave Pass Dichroic Beamsplitters SWP

    Standard Plate Beamsplitters UV-VIS-NIR
    Standard plate beamsplitter are an economical option for separating a beam into two orthogonal paths. Standard plate beamsplitter are offered in ultra-Violet, Visible and near-Infrared wavelengths.
    • Angle of Incidence: 45°
    • round and square shape
    • Material: Optical crown glass or Optical quality synthetic fused silica


    Standard Plate Beamsplitters UV-VIS-NIR
    Standard Plate Beamsplitters UV BTQ serie Standard Plate Beamsplitters Visible & NIR BTF serie

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