This document provides information about waveplates produced by Photonchina. It describes what a waveplate is and how it modifies the polarization state of light. It then gives details on Photonchina's production process for various types of waveplates, including quarter waveplates, half waveplates, low order waveplates, zero order waveplates, and achromatic waveplates. Specifications are provided for each waveplate type as well as operating wavelengths and standards.
Power scaling 790nm-pumped Tm-doped devices from 1.91 to 2.13 µmnufchas
The aim of this presentation is to answer some common questions we receive about 790nm-pumped Tm-doped fibers. What are the wavelength limitations? What about single polarization? What is the fiber reliability?
50W single-mode linearly polarized high peak power pulsed fiber lasernufchas
We demonstrate 50W single-mode linearly polarized high peak power pulsed fiber laser with tunable ns–µs pulse durations and kHz–MHz repetition rates capable to address a wide range of applications: frequency conversion, LIDAR and others.
Power scaling 790nm-pumped Tm-doped devices from 1.91 to 2.13 µmnufchas
The aim of this presentation is to answer some common questions we receive about 790nm-pumped Tm-doped fibers. What are the wavelength limitations? What about single polarization? What is the fiber reliability?
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The attached narrated power point presentation describes the principle of working, various configurations, advantages, disadvantages and applications of Erbium Doped Fiber Amplifiers. The material will be useful to KTU final year B tech students who prepare for the subject EC 405, Optical Communications.
Optical fiber communication Part 1 Optical Fiber FundamentalsMadhumita Tamhane
Optical fiber systems grew from combination of semiconductor technology, which provided necessary light sources and photodetectors and optical waveguide technology. It has significant inherent advantages over conventional copper systems- low transmission loss, wide BW, light weight and size, immunity to interferences, signal security to name a few. One principle characteristic of optical fiber is its attenuation as a function of wavelength. Hence it is operated in two major low attenuation wavelength windows 800-900nm and 1100-1600nm . Light travels inside optical fiber waveguide on principle of total internal reflection. Fiber is available as single mode and multiple mode, step index and graded index depending on applications and expenditures. Principle of fiber can be understood by ray theory or mode theory. ...
Waveplate is an optic in which the polished faces contain the optical axis. All light incidents normal to the surface are composed of components polarized parallel and perpendicular to the axis. In such a device, light polarized parallel to the axis will propagate slower than light polarized perpendicular to the axis. As the light propagates through the optic, the phase shift between the two components with various thickness. The phase shift is called retardance. The most popular retarders in Photonchina are quarter and half wave.
With an appropriate choice of thickness, any degree of retardance may be achieved at any wavelength for which quartz is transparent. However, the minimum thickness necessary to achieve a mechanically strong part corresponds to several full waves of retardance.
A half waveplate rotates linearly polarized light to any desired orientation. The rotation angle is twice the angle between the incident polarized light and optical axis.
When linearly polarized light is input at 45deg to the axis of a quarter waveplate , the output is circularly polarized similarly, input circularly polarized light is transformed into linearly polarized light.
The thickness of the quarter waveplate is such that the phase difference is 1/4 wavelength ( λ /4, Zero order) or certain multiple of 1/4-wavelength [(2n+1)λ /4, multiple order].
LiNbO3 is widely used as electro-optic modulators and Q-switches for Nd:YAG, Nd:YLF and Ti:Sapphire lasers as well as modulators for fiber optics. The following table lists the specifications of a typical LiNbO3 crystal used as Q-switch with transverse E-O modulation. The light propagates in z-axis and electric field applies to x-axis. The electro-optic coefficients of LiNbO3 are: r33 = 32 pm/V, r31 = 10 pm/V, r22 = 6.8 pm/V at low frequency and r33 = 31 pm/V, r31= 8.6 pm/V, r22 = 3.4 pm/V at high electric frequency. The half–wave voltage: Vπ=λd/(2no3r22L), r c=(ne/no)3r33-r13.
The attached narrated power point presentation describes the principle of working, various configurations, advantages, disadvantages and applications of Erbium Doped Fiber Amplifiers. The material will be useful to KTU final year B tech students who prepare for the subject EC 405, Optical Communications.
Optical fiber communication Part 1 Optical Fiber FundamentalsMadhumita Tamhane
Optical fiber systems grew from combination of semiconductor technology, which provided necessary light sources and photodetectors and optical waveguide technology. It has significant inherent advantages over conventional copper systems- low transmission loss, wide BW, light weight and size, immunity to interferences, signal security to name a few. One principle characteristic of optical fiber is its attenuation as a function of wavelength. Hence it is operated in two major low attenuation wavelength windows 800-900nm and 1100-1600nm . Light travels inside optical fiber waveguide on principle of total internal reflection. Fiber is available as single mode and multiple mode, step index and graded index depending on applications and expenditures. Principle of fiber can be understood by ray theory or mode theory. ...
Waveplate is an optic in which the polished faces contain the optical axis. All light incidents normal to the surface are composed of components polarized parallel and perpendicular to the axis. In such a device, light polarized parallel to the axis will propagate slower than light polarized perpendicular to the axis. As the light propagates through the optic, the phase shift between the two components with various thickness. The phase shift is called retardance. The most popular retarders in Photonchina are quarter and half wave.
With an appropriate choice of thickness, any degree of retardance may be achieved at any wavelength for which quartz is transparent. However, the minimum thickness necessary to achieve a mechanically strong part corresponds to several full waves of retardance.
A half waveplate rotates linearly polarized light to any desired orientation. The rotation angle is twice the angle between the incident polarized light and optical axis.
When linearly polarized light is input at 45deg to the axis of a quarter waveplate , the output is circularly polarized similarly, input circularly polarized light is transformed into linearly polarized light.
The thickness of the quarter waveplate is such that the phase difference is 1/4 wavelength ( λ /4, Zero order) or certain multiple of 1/4-wavelength [(2n+1)λ /4, multiple order].
LiNbO3 is widely used as electro-optic modulators and Q-switches for Nd:YAG, Nd:YLF and Ti:Sapphire lasers as well as modulators for fiber optics. The following table lists the specifications of a typical LiNbO3 crystal used as Q-switch with transverse E-O modulation. The light propagates in z-axis and electric field applies to x-axis. The electro-optic coefficients of LiNbO3 are: r33 = 32 pm/V, r31 = 10 pm/V, r22 = 6.8 pm/V at low frequency and r33 = 31 pm/V, r31= 8.6 pm/V, r22 = 3.4 pm/V at high electric frequency. The half–wave voltage: Vπ=λd/(2no3r22L), r c=(ne/no)3r33-r13.
This presentation include the detailed explanation of various parts of a UV-Visible spectrophotometer and two types of UV-Visible spectrophotometers-Single beam and Doube beam. It also include the comparison between single beam and double beam spectrophotometers.
Photonchina’s wollaston polarizer can separate an incident beam into two rays: extraordinary and ordinary ray with a deviation angle which is dependent on wavelength. Both rays are transmitted through the other surface.
HIGH TRANSMSSION POLARIZER
High Transmission Glan Laser Polarizers is a special type of Glan Laser Polarizers. Its incidence angle is brewster angle cut which can greatly improve the transmission ray up to 98% in a wide range of wavelength without coating. The polarizer can be made from Calcite or YVO4 crystals. In order to get transmission of a wide range of wavelength, the polarizers are not recommended to use for large acceptance angle. It is typically used at the angle within+/-5°.
Photonchina is the leading manufacturer of high transmission polarizer in the world
Glan Taylor polarizer is made of two birefringent prisms that are assembled with an air space.
The polarizer with no side escape windows is suitable for low to medium power application where the side rejected beams are not required.
Photonchina provides a wide range of polarizers including glan taylor polarizer.
Photonchina’s Glan-Thompson Polarizer is made of two cemented calcite (or a-BBO) prisms that are at the highest optical level. When the unpolarized light enters Glan-Thmopson Polarizer, it will separate at the intersection of the two calcite crystals. S-polarized light (e-ray) then goes on and P-polarized light (o-ray) will be reflected.
Rochon polarizer is made of two birefringent material prisms cemented or optical contacted together. Photonchina's Rochon prism was invented by and is named after Abbé Alexis Marie Rochon. It is in many ways similar to the Wollaston prism, but the ordinary ray passes through the prism undeviated. Any separation angle can be designed according to request of customers.
Glan Laser polarizer is made of two same birefringent material prisms that are assembled with an air space. Photonchina’s polarizer is a modification of the Glan Taylor type and is designed to have less reflection loss at the prism junction. The polarizer with two escape windows allow the rejected beam to escape out of the polarizer, which makes it more desirable for high energy lasers. The surface quality of these faces is relatively poor as compared to that of entrance and exit faces. No scratch dig surface quality specifications are assigned to these faces.
The yttrium orthovanadate (YVO4) is a positive uniaxial crystal grown with Czochralski method. It has good mechanical and physical properties and is ideal for optical polarizing components because of its wide transparency range and large birefringence. Photonchina YVO4 has an excellent synthetic substitute for Calcite (CaCO3) and Rutile (TiO2) crystals in many applications including fiber optic isolators and circulators, beam displacers, Glan polarizers and other polarizing optics, etc.
Dove prism is a type of reflective prism which is used to invert an image. Photonchina dove prisms are shaped from a truncated right-angle prism. A beam of light entering one of the sloped faces of the prism undergoes total internal reflection from the inside of the longest (bottom) face and emerges from the opposite sloped face. Images passing through the prism are flipped, and because only one reflection takes place, the image's handedness is changed to the opposite sense.
Right Angle Prisms
Right angle prisms (RAP) are widely used for rotating image and redirecting the input light. They serve as a mirror to deviate light through 90 degrees and also as a retro-reflector to deflect light through 180 degrees by total internal reflection. They are the main components for polarizing and non-polarizing cube beamsplitters.
The total internal reflection (TIR) in the right angle prisms with specific anti-reflection (AR) coatings on the two leg sides make themselves the perfect alternatives of 45 degree mirrors.
Photonchina Laser Grade Right-Angle Prisms are fabricated by special selection optical materials with low scatter and absorption. Standard size laser grade right angle prisms, with better surface finish, flatness as high as l/10 and high accuracy are available in Photonchina.
Penta Prism is a five-sided prism containing two reflecting surfaces at 45deg to each other, and two refracting faces perpendicular to the entering and emerging beams. The deviation angle of 90deg is thus independent of the orientation of the prism, making it especially important in applications in which the prism orientation cannot be precisely controlled. Due to the geometry that total internal reflection cannot be used, the reflecting surfaces must be coated with a metallic or dielectric coating. Photonchina standard Pentagonal Prism reflecting surfaces are coated with aluminum or enhanced aluminum. The coated surfaces can be painted black
Photonchina’s pentagonal prism reflects light rays through a 90° angle by two reflections and does invert or revert the image. The reflecting surfaces are aluminized. Slight movement of the prism does not affect the true right angle at which light rays are reflected. It also shortens the optical path length of an instrument.
Dove prism is a type of reflective prism which is used to invert an image. Photonchina dove prisms are shaped from a truncated right-angle prism. A beam of light entering one of the sloped faces of the prism undergoes total internal reflection from the inside of the longest (bottom) face and emerges from the opposite sloped face. Images passing through the prism are flipped, and because only one reflection takes place, the image's handedness is changed to the opposite sense.
The Double Convex Lenses are made of BK7 material, which are manufactured with an identical convex surface on both sides of the lens. The Double Convex lenses have positive focal lengths and form both real and virtual images. Photonchina also provides precision grade Double Convex lenses with tighter manufacturing tolerances
Cylindrical lens, also called a cylinder, is an optical lens which focuses light on to a line instead of on to a point, as a spherical lens would. The curved face or faces of a cylindrical lens are sections of a cylinder, and focus the image passing through it onto a line parallel to the intersection of the surface of the lens and a plane tangent to it. The lens compresses the image in the direction perpendicular to this line, and leaves it unaltered in the direction parallel to it (in the tangent plane).
Cylindrical lenses are used to correct the output from diode lasers, to produce a round beam from the diode’s elliptical output. They are also applied in optical systems to correct the shape of laser beams, change image aspect ratios, and illuminate in the shape of line source.
Photonchina’s cylindrical lens is among top-level in terms of surface quality, irregularity and dimension tolerance. It also provides the high precision, special shapes and specifications designed by customers.
BBO is very good for tunable laser sources, such as ultrafast Ti:Sapphire or dye lasers. And it is also widely used for SHG, 3HG, 4HG, and autocorrelation of femtosecond and picosecond Ti:Sapphire lasers; SHG, 3HG, 4HG, 5HG of YAG lasers at 1064 nm and 1320 nm to yield output of 212-660nm; SHG of tunable dye or solid-state laser sources from 410-750 nm to yield output of 205-375 nm, SFM of dye laser and YAG harmonics to yield output of 189-400 nm; DFM (difference-frequency mixing) from the Visible to the IR range up to over 3000 nm; OPO pumped with SHG or 3HG of YAG or Ti:Sapphire with an output range of 400-3000 ; Intracavity SHG of Argon ion lasers (488, 514 nm) or Copper vapor lasers (510 nm, 578 nm).
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Quartz waveplate
1. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
Waveplate is an optic in which the polished faces contain the optical axis. All light
incidents normal to the surface are composed of components polarized parallel and
perpendicular to the axis. In such a device, light polarized parallel to the axis will propagate
slower than light polarized perpendicular to the axis. As the light propagates through the optic,
the phase shift between the two components with various thickness. The phase shift is called
retardance. The most popular retarders in Photonchina are quarter and half wave.
With an appropriate choice of thickness, any degree of retardance may be achieved at any
wavelength for which quartz is transparent. However, the minimum thickness necessary to
achieve a mechanically strong part corresponds to several full waves of retardance.
Photonchina’s waveplate can transmit light and modify its polarization state without
attenuating, deviating, or displacing the beam.It is ideal for applications requiring high damage
thresholds and retardation stability over temperature change, such as for use with lasers or
infrared light sources.
Production
Photonchina’s waveplates fabrication starts from quartz materials cutting with their axes
oriented within a few arcminutes before being polished to a laser-quality finish, arcsecond
parallelism, and <λ/10 wavefront. Their thickness tolerance is a only small fraction of a micron.
To verify retardation tolerances, specially-trained optical technicians use purpose-built test
gear. After anti-reflective coating, zero order and achromatic waveplates are matched in pairs
and accurately aligned to each other within their cell mounts.
2. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
Wavepalte Types:
Half waveplate
A half waveplate rotates linearly polarized light to any desired orientation. The rotation angle is
twice the angle between the incident polarized light and optical axis.
Quarter Waveplate
When linearly polarized light is input at 45deg to the axis of a quarter waveplate , the output is
circularly polarized similarly, input circularly polarized light is transformed into linearly
polarized light.
The thickness of the quarter waveplate is such that the phase difference is 1/4 wavelength ( λ
/4, Zero order) or certain multiple of 1/4-wavelength [(2n+1)λ /4, multiple order].
Photonchina provides standard waveplate wavelengths (nm) listed as below:
355 532 632.8 808 850 980 1064 1310 1480 1550 1590
Other wavelengths within the ranger of 200-2300nm are also available.
4. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
Low Order Waveplate
Low(multiple) order waveplate is designed to give a retardance of several full waves,
plus the desired fraction. This result in a single, physically robust component with
desired performance. However, even small changed in wavelength or temperature will
result in significant changes in the desired fractional retardance. They are less
expensive and find use in many applicatios where the increased sensitivities are not
an important.
Specifications:
Material: Quartz
Wavelength Range: 200~2300 nm,
Dimension Tolerance: +0.0, -0.1mm
Surface Quality: 20 / 10
Parallelism: <1 arc Sec
Wavefront Distortion: < λ/8@633nm
Retardation Tolerance: < λ/300
Clear Aperture: >90%
Damage Threshold: >500 MW/cm2
AR Coating: R<0.2%@wavelength
Mount: Black Anodized Aluminium
5. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
Zero Order Waveplate
The zero order waveplate is designed to give a retardance of zero full waves, plus the
desired fraction. Zero order waveplate shows better performance than low/multiple order
waveplates. It has broad bandwidth and a lower sensitivity to temperature and wavelength
changes. It should be considered for more critical applications。
It is constructed of two low order waveplates with their axes crossed. Thus,the effect
of the first plate is canceled by the second,except for the residual difference between
them. There are normally three different structures as follows,
Optical Contact
Cemented by Epoxy
Air spaced
Specifications:
Material: Quartz
Wavelength Range: 200~2300 nm,
Dimension Tolerance: +0.0, -0.1mm
Surface Quality: 20 / 10
Parallelism: <1 arc Sec
Wavefront Distortion: < λ/8@633nm
Retardation Tolerance: < λ/500
Clear Aperture: >90%
10. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
3. Cemented
This type of zero order waveplate is constructed of one true zero order waveplate and
one BK7/K9 substrate.
As the waveplate is very thin and easy to be damaged,the BK7 plate’s function is to
strengthen the waveplate.
Standard Thickness:1.1±0.2mm
Cemented by Epoxy
Wide Angle Acceptance
Better Temperature Bandwidth
Wide Wavelength Bandwidth
Standard wavelength:
532nm, 632.8nm, 780nm, 808nm,980nm, 1064nm,1310nm, 1480nm, 1550nm
11. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
Achromatic Waveplate
Achromatic waveplate is made from two different substrate materials such as crystal
quartz and magnesium fluoride. For the single material,waveplate’s working wavelength
is very limited because of the dispersion of the material. But Achromatic Waveplate uses
two different kinds of materials,with the different dispersion, such waveplate is not
sensitive to the wavelength change.
Specifications:
Material: Quartz and MgF2
Dimension Tolerance: +0.0, -0.1mm
Surface Quality: 40 / 20
Parallelism: <1 arc Sec
Wavefront Distortion: < λ/8@633nm
Retardation Tolerance: < λ/100
Clear Aperture: >90%
Damage Threshold: >10MW/cm2;
AR Coating: Ravg<1.5%@wavelength
Structure: Optical contact or Air contacted
Standard wavelength:
460-650nm, 550-750nm, 650-1000nm, 900-2100nm.
12. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
Dual Wavelength Waveplate
Dual wavelength waveplate is a special type of multiple waveplate that provides a
specific retardance at two different wavelengths, it’s particularly useful when used
in conjunction with other polarization sensitive components to separate coaxial laser
beams of different wavelength. It is widely used to improve conversion efficiency in
solid double frequency laser device.
Specifications:
Material: Quartz
Wavelength Range: 350~2100 nm,
Dimension Tolerance: +0.0, -0.1mm
Surface Quality: 20 / 10
Parallelism: <1 arc Sec
Wavefront Distortion: < λ/8@633nm
Retardation Tolerance: < λ/100
Clear Aperture: >90%
Damage Threshold: >1GW/cm2
AR Coating: R<0.2%@wavelength
Mount: Black Anodized Aluminium
Standard wavelength:
λ@1064nm+λ/2@532nm, λ/2@1064nm+λ@532nm;
λ@532nm+λ/2@355nm, λ/2@532nm+λ@355nm
13. PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
PPHHOOTTOONNCCHHIINNAA
www.photonchinaa.com
Polarization Rotator
Due to the rotation activity of natural quartz crystal, it also can be used as
polarization rotators so that the plane of input linearly polarized beam will be rotated
at special angle which is determined by the thickness of quartz crystal.
Made of quartz, 200-2500nm
Up to 50.8mm diameter
Custom rotation angle available
RoHS Compliant
Specifications:
Material: Crystal Quartz 200-2500nm
Dimension Tolerance: +/-0.2mm
Surface Quality: 20 / 10
Parallelism: <10 arc Sec
Wavefront Distortion: < λ/4@632.8nm
Rotation accuracy: < 5 arc Min
Rotation: clockwise or counter-clockwise
Damage Threshold: >1GW/cm2
AR Coating: R<0.25%@wavelength