公司简介
Innovation Photonics于2009年12月由Don Wilson发起,专业应用包括中红外和量子级联激光器应用;聚焦发射到光纤中的目标;中红外偏振,方解石偏振片限制在1.9μm,YVO4限制在4.8μm;以及覆盖2μm至12μm的宽带偏振器。是世界一流的精密光学元件设计师和制造商,也是支持量子级联激光器应用的中红外元件和其他波长元件的领先供应商。
产品列表
Products
。Mid-IR Isolators
。4.5 μm ISOLATORS
。WideBand IR POLARIZER 2 μm – 12 μm
。ShortCell IR POLARIZER 3 μm – 11 μm
。Infrared Polarization Rotator
。Flat-Top Beam Expander
。Fiber-Optic Coupling Lenses
。Mid-IR Focusing Objectives 2 μm to 12 μm
。Fiber-Optic Collimators
。Mid-IR Fiber Collimators
。IR Fiber Cables
Mid-IR Isolators
Our Mid-IR Optical Isolators eliminate the annoying effects of feedback in quantum cascade laser applications and systems, operating at specific wavelengths from 4 μm to beyond 14 μm.
Standard wavelengths in stock are:
4.5 μm, 8.0 μm, 10.6 μm
These can be tuned more than ± 10% of center λ
Other wavelengths available. Please inquire.
It’s the IR that makes IR isolators difficult. The critical component in any isolator is the magneto-optic material that performs the rotation of the plane of polarization in the magnetic field. Whereas in the VIS and NIR there are many candidate magneto-optic materials, in the infrared the choices are greatly reduced. In our Mid-IR Isolators we utilize a very small family of highly specialized materials that demonstrate low absorption and acceptable Verdet Constant at the wavelength of operation.
The other critical component is the polarizer, and again, there are few choices in the infrared. See POLARIZERS in our Flat-Top Beam Expander and Fiber-Optic Coupling Lenses pages for descriptions of our IR Polarizers.
Escape Window option allows monitoring of feedback that is rejected by the Isolator. When ordering, specify Escape Window on Input or Out-put Polarizer.
Catalog Number | Aperture | Transmittance | Isolation | Total Length | Power Rating |
FIO-5-λ | 4.5 mm | 75-86% | >> 1000:1 | ∼ 6″ | inquire |
λ: When ordering, specify wavelength between 4 μm and 14 μm.
4.5 μm ISOLATORS
4 mm aperture
Temporarily Not Available
This high performance, utility-sized isolator economizes on space requirement while utilizing novel design features that greatly reduce production costs, thus enabling a selling price that is far below competing products.
Our Mid-IR Optical Isolators eliminate the annoying effects of feedback in laser applications and systems, operating at specific wavelengths from 4 μm to beyond 14 μm.
FEATURES
Wavelength Tunable +/-10%
Transmission 75% to 86%
Isolation 10,000:1 (40 dB)
Other wavelengths available in utility-sized package.
The high transmission, high extinction polarizer is a size-reduced version of our PGC-5 WideBand IR Polarizer (see page 6). This Polarizer is characterized by extremely low insertion loss and extremely high extinction ratio.
Catalog Number | Aperture | Transmittance | Isolation | Total Length | Power Rating |
FIO-4-4.5 | 4.0 mm | 75-86% | > 10,000:1 | ∼ 2″ | Discuss |
WideBand IR POLARIZER 2 μm – 12 μm
InnPho’s unique Wideband IR Polarizer utilizes two precision polished Germanium plates at Brewster’s angle in “chevron” orientation. Low deviation, <10 seconds, with very high extinction and transmittance.
Cell length, 2.2”. See also ShortCell IR Polarizer below.
Catalog Number | Aperture | Transmittance of P-Ray | Power Rating | Extinction of Crossed Pair |
PGC-4 PGC-5 | 4 mm 5 mm | ≥98% ≥98% | 100 MW/cm2 100 MW/cm2 | 2×105 2×105 |
PGC-4: 15 mm Diameter x 36 mm long
PGC-5: 1-inch long x 2.2 inches long
ShortCell IR POLARIZER 3 μm – 11 μm
InnPho’s ShortCell IR Polarizer is used when short package length is important. Because of the delicacy of wire-grid polarizers, we have improved the mounting cell so that the hyper-delicate grid coating is protected from external contact. Cell is 12 mm thick.
SPECIFICATIONS
Catalog Number: PSP-5
Aperture: 5 mm
Transmittance: 70%
Extinction of Crossed Pair: 100:1
Power Rating: Discuss
Infrared Polarization Rotator
Broadband Achromatic, VIS to 9 μm*
*10.6 μm under development
Continuous Rotation Manual Control
Rotary Scale Readout 0º- 360º
Rotates POP (Plane of Polarization) to any angle.
Continuous Transmission VIS to 9 μm
Coaxial Input-Output beams
Number | Description |
RF-4 | Infrared Polarization Rotator |
RF-1/2 | ½-Wave, Double Fresnel Rhomb, mounted |
RF-1/4 | ¼-Wave Fresnel Rhomb, mounted |
Flat-Top Beam Expander
InnPho’s Flat-Top Beam Expanders convert a Gaussian laser beam input into an output that has a flat-top profile. The conversion is caused by an Engineered Diffuser™, manufactured by RPC Photonics, Inc.
Spectral Range: 350 nm to 2 μm
Cross section uniformity: ±5-10% (neglecting speckle)
Laser damage threshold: 20 J/cm2, 1054 nm, 1 ns pulse
Optimum performance of the apodizing element (Engineered Diffuser™) is achieved when the input beam diameter is 3-4 mm, using our GCE-9.
Click Here to Download PDF Poster
Part Number | Description |
ELG-10-λ | Flat-Top Beam Expander, 10 mm dia collimated output |
ELG-20-λ | Flat-Top Beam Expander, 20 mm dia collimated output |
ELG-45-λ | Flat-Top Beam Expander, 45 mm dia collimated output |
GCE-9 | Flat-Top Converter element, mounted |
λ: When ordering, specify wavelength for AR coatings.
GAUSSIAN COMPENSATING PLATE
Catalog Number | Dimensions |
WCG-25 | 1” dia x 1⁄4” thick |
WCG-51 | 2” dia x 1⁄4” thick |
Fiber-Optic Coupling Lenses
Coupling Lenses for VIS-NIR
InnPho’s Fiber-Optic Coupling Lenses are mounted in the industry standard RMS Threaded Mount favored in most laboratories. Transmittance of these AR-AR coated lenses exceeds 96% at the peak wavelength. Performance is diffraction limited when Maximum Beam Diameter is not exceeded; see below.
Catalog Number | Focal Length | Working Distance | Numerical Aperture | Maximum Beam Dia | Magnification |
LFO-2-4-λ | 4.0 mm | 3.6 mm | 0.19 | 1.5 mm | 40X |
LFO-2-6-λ | 6.0 mm | 5.2 mm | 0.17 | 2.0 mm | 27X |
LFO-2-9-λ | 9.0 mm | 8.1 mm | 0.50 | 2.0 mm | 18X |
LFO-3-12-λ | 12.0 mm | 10.9 mm | 0.30 | 2.5 mm | 13X |
LFO-3-15-λ | 15.0 mm | 13.4 mm | 0.53 | 2.5 mm | 11X |
Antireflection Coatings
Max T Spectrum | Order as |
380 – 640 nm | – VIS |
600 – 990 nm | – NIR |
970 – 1100 nm | – YAG |
1100 – 1550 nm | – IR |
1.9 – 2.15 um | – HoYAG |
Mid-IR Focusing Objectives 2 μm to 12 μm
InnPho’s Mid-IR Focusing Objectives are designed for maximum efficiency in coupling the output from a mid-IR source into single-mode or multimode IR transmitting bers.
ZnSe MicroLens
AR-AR in Mid-IR
Diffraction limited
Easy alignment using HeNe
Mounting RMS thread
2 μm to 12 μm
Catalog Number | Clear Aperture | Numerical Aperture | Working Distance | Focal Length |
LFO-5-6 | 5 mm | 0.25 | 5.3 mm | 6 mm |
LFO-5-12 | 5 mm | 0.13 | 11.5 mm | 12 mm |
LFO-5-18 | 5 mm | 0.08 | 17.5 mm | 18 mm |
– – FOCAL SPOT DIAMETER (μm) – – | |||||||||||
Beam Dia (mm) | Focal Length (6, 12, 18 mm) | ||||||||||
6 | 12 | 18 | 6 | 12 | 18 | 6 | 12 | 18 | |||
2.0 mm | 15 | 30 | 46 | 23 | 46 | 69 | 30 | 61 | 91 | ||
3.0 mm | 14 | 20 | 30 | 15 | 30 | 46 | 20 | 41 | 61 | ||
4.0 mm | 32 | 15 | 23 | 32 | 23 | 34 | 32 | 30 | 46 | ||
λ = 4 μm | λ = 6 μm | λ = 8 μm |
TRANSMISSION
The ZnSe lens in LFO-Series Objectives is Broadband AR (BBAR) coat- ed on both sides. Transmission from 2 μm to 12 μm is 90% to 96%.
See graph above.
Fiber-Optic Collimators
Twist-On Collimators for VIS-NIR (425 nm – 1550 nm)
Twist-On Collimators connect quickly to FC or SMA connectorized fiber cables to produce a collimated beam.
Twist-On Collimators contain a micro lens that is designed for diffraction-limited performance. Both surfaces of the lens are antireflection coated, with >98% transmission at the peak wavelength.
Focal compensation for different wavelengths is achieved by a simple hand adjustment of the ne-threaded spring loaded focusing barrel.
Catalog Number | Focal Length | Output Beam Diameter | Clear Aperture | Numerical Aperture |
FCC-2-λ | 2 mm | 0.5 mm | 1.5 mm | 0.30 |
FCC-5-λ | 5 mm | 1.0 mm | 2.3 mm | 0.25 |
FCC-8-λ | 8 mm | 1.6 mm | 3.3 mm | 0.22 |
λ: When ordering, specify wavelength for AR coatings
Twist-On Collimators are available with a choice of different focal length Lenses as follows:
Connector | Focal Length | Fiber Type | Best Collimation Distance at |
FC | 2 mm | SM | 2 cm to 50 cm |
FC | 5 & 8 mm | SM | 5 cm to 1 m |
SMA | 5 & 8 mm | MM | 1 cm to 2 m |
Mid-IR Fiber Collimators
MID-IR Collimators for SMA Connectors (2 μm to 12 μm)
The same AR-AR coated ZnSe micro-lens used in our Mid-IR Focusing Objectives is used in our Mid-IR Collimators. These are designed to connect to SMA connectorized IR ber cables.
Our Mid-IR Collimators are focusable so as to compensate for different wavelengths. These are available “as is” or mounted in the 1-inch diameter Cell, which in turn mounts into our HTP Tilt Plate Positioner or any 1-inch laboratory X-Y stage.
Catalog Number | Focal Length | Clear Aperture | Numerical Aperture |
FCR-6-λ | 6 mm | 0.5 mm | 0.25 |
FCR-12-λ | 12 mm | 1.0 mm | 0.13 |
FCR-18-λ | 18 mm | 1.6 mm | 0.08 |
λ: When ordering, specify wavelength for AR coatings.
A comment on Numerical Aperture… think of the NA of the fiber as a cone or a funnel… if the light rays are at an angle that is smaller than the cone angle, the light will get through the fiber.
2NA = d/f
d = laser beam diameter
f = focal length of lens
IR Fiber Cables
InnPho IR Fiber Cables are complete from laser in to collimator out. On the input end of an IR Fiber is a fully adjustable and stable InnPho Laser Port that can attach to a laser or mount remotely to provide stable coupling of the laser output into the IR Fiber Cable. On the output end is a focusable InnPho Collimator that contains an AR coated ZnSe micro-lens.
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Core Diameters (μm) | Spectral Range | Standard Lengths (m) |
Chalcogenide: 100 μm | 1.5 – 6.0 μm | 0.5, 1.0, 1.5, 2.0 meter |
Hollow Core: 300, 1000 μm | 2.5 –12.0 μm | 0.5, 1.0, 1.5, 2.0 meter |
IR FIBER CABLES, complete from input to output, SMA
Catalog Number | Description | Core Diameter (μm) |
FCM-C-100-l | IR Fiber Cable, chalcogenide | 100 μm |
FCM-H-300-l | IR Fiber Cable, hollow core | 300 μm |
FCM-H-1000-l | IR Fiber Cable, hollow core | 1000 μm |
l : When ordering, specify Length (meters),
for example, FCM-H-1000-1.5.
IR Fiber Cables, characteristics
InnPho IR Fiber Cables are available in chalcogenide core or hollow core, depending upon the wavelength of operation. See below.