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Dual Wavelength Multi-Order Wave Plates


  • Operates as λ/2 @ λ1 & as λ/4 @ λ2
  • Dual Wavelength Operation: 532 nm and 1064 nm
  • Ø1/2" Waveplate Mounted in Ø1" Aluminum Mount

WPDM05M-1064H-532Q

WPDM05M-532H-1064Q

Wave Plate
Mounted in PRM1
Rotation Mount

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Features

  • Operates as a Quarter-Wave Plate at One Wavelength and a Half-Wave Plate at a Second Wavelength
  • Dual V AR Coating: Ravg <0.25% at 532 nm and 1064 nm (0° AOI)
  • Ø1/2" Waveplate Mounted in Ø1" Aluminum Mount
  • Clear Aperture: Ø10 mm (Ø0.39")
  • Custom Options Available, Please Contact Tech Support for More Information.

Thorlabs' dual wavelength, multi-order wave plates are made from high-quality crystalline quartz and are available at quarter-wave or half-wave retardance. The wave plates are designed to be used in dual wavelength setups (1064 nm and 532 nm) and operate as a quarter-wave plate at one wavelength and as a half-wave plate at the second wavelength. Two models are available: λ/4 @ 532 nm and λ/2 @ 1064 nm or a λ/4 @ 1064 nm and λ/2 @ 532 nm.

Unmounted Waveplate Polarization Axis

Multi-order refers to the fact that the retardance of a light path will undergo a certain number of full wavelength shifts (also referred to as the order, or m) in addition to the fractional design retardance. Compared to their zero-order counterparts, the retardance of multi-order wave plates are more sensitive to wavelength and temperature changes, however, they are less expensive and find use in many applications where the increased sensitivities is not an issue.

Our wave plates are mounted in a Ø1" housing with the fast axis of the wave plate clearly marked with a straight line on the housing's front panel. The wave plates are easily removed from their mounts for use in custom or OEM applications (see the Specs tab for the unmounted wave plate thickness). The unmounted waveplates have a small flat to indicate the fast axis (see image on the right). For further information on using and selecting a wave plate please visit our Wave Plate Selection Guide tab.

Thorlabs can also produce custom wave plates with no AR coating, a different AR coating, or a different design wavelength than those offered below. Please contact
Tech Support with inquiries.

Wave Plate Selection Guide
Achromatic Superachromatic Quartz Zero-Order
Half-Wave
Quartz Zero-Order
Quarter-Wave
Polymer Zero-Order
Half-Wave
Polymer Zero-Order
Quarter-Wave
Multi-Order Dual Wavelength Telecom Polarization Optics
General Specifications
Substrate Crystalline Quartz
Operating Wavelengths 532 nm & 1064 nm
Clear Aperture Ø10 mm (Ø0.39")
Diameter Unmounted: 12.7 mm ± 0.1 mm
Mounted: 25.4 mm
Retardance Accuracy (Typical) <λ/300 (Measured at 632.8 nm)
Reflectance Dual V AR Coating:
Ravg <0.25% at 532 nm and 1064 nm (0° AOI)
Transmitted Wavefront Error <λ/10
Beam Deviation <10 arcsec
Surface Quality 20-10 Scratch-Dig
Item # Unmounted Wave Plate Nominal Thickness
WPDM05M-532H-1064Q 1.1276532 mm
WPDM05M-1064H-532Q 0.3038145 mm

Operating Principle of Wave Plates

Optical wave plates are constructed from birefringent materials that have a difference in refractive index between two orthogonal axes. This birefringent property introduces a velocity difference between light polarized along the fast and slow principal axes of the wave plate. The fast principal axis of the wave plate has a lower refractive index, resulting in a faster velocity for light polarized in this direction. Conversely, the slow axis has a higher refractive index, resulting in a slower velocity for light with this polarization. When light passes through a wave plate, this velocity difference leads to a phase difference between the two orthogonal polarization components. The actual phase shift depends on the properties of the material, the thickness of the wave plate, and the wavelength of the signal, and can be described as:

Phase Shift

where n1 is the refractive index along the slow axis, n2 is the refractive index along the orthogonal fast axis, d is the thickness of the wave plate, and λ is the signal wavelength.

Using a Wave Plate

Wave plates are typically available with a retardance of λ/4 or λ/2, meaning that a phase shift of a quarter wavelength or a half a wavelength (respectively) is created.

beam diagram
Half-Wave Plate Diagram

Half-Wave

As described above, a wave plate has two principal axes: fast and slow. Each axis has a different refractive index and, therefore, a different wave velocity. When a linearly polarized beam is incident on a half-wave plate, and the polarization of this beam does not coincide with one of these axes, the output polarization will be linear and rotated with respect to the polarization of the input beam (see image at right). When applying a circularly polarized beam, a clockwise (counterclockwise) circular polarization will transform into a counterclockwise (clockwise) circular polarization.

Half-wave (λ/2) plates are typically used as polarization rotators. Mounted on a rotation mount, a λ/2 wave plate can be used as a continuously adjustable polarization rotator, as shown below. Additionally, when used in conjunction with a Polarizing Beamsplitter a λ/2 wave plate can be used as a variable ratio beamsplitter.

The angle between the output polarization and the input polarization will be twice the angle between the input polarization and the wave plate’s axis (see diagram to the lower right). When the polarization of the input beam is directed along one of the axes of the wave plate, the polarization direction will remain unchanged.

Half-Wave Plate and Rotation Mount
Click to Enlarge

Half-Wave Plate Mounted in RSP1X15 Rotation Mount
beam diagram

Quarter-Wave

A quarter-wave plate is designed such that the phase shift created between the fast and slow axes is a quarter wavelength (λ/4). If the input beam is linearly polarized with the polarization plane aligned at 45° to the wave plate's fast or slow axis, then the output beam will be circularly polarized (see image at right). If the linearly polarized beam is aligned at an angle other than 45°, then the output will be elliptically polarized. Conversely, the application of a circularly polarized beam to a λ/4 wave plate results in a linearly polarized output beam. Quarter wave plates are used in Optical Isolators, optical pumps, and EO Modulators.

waveplate fast axis engraving
Click to Enlarge

Figure 1: Top Images (a,b): Engraving Reflects Updated Assembly Process as of October 2018; Bottom Images (c,d): Past Engraving

Fast and Slow Axis Identification

In October 2018, Thorlabs updated its wave plate assembly process and associated product engravings to be consistent with the IEEE/SPIE convention (see the Polarization Handedness Tutorial) for determining the fast and slow axes. By this convention, the current revisions of wave plates have the fast axis denoted by the “FAST AXIS” engraving visible in Figure 1 to the right. Although the location of the axes and the retardation value for each wave plate is easily determined, differentiating between the fast and slow axes is far more involved.

For most applications, the knowledge of whether an axis is fast or slow is not nearly as important as the retardation value. However, the fast/slow difference determines the left/right-hand circular polarization of light output from a quarter-wave plate, which can be important in applications such as atomic and solid state physics spectroscopy. To ensure the accuracy of our labeling moving forward, we have incorporated several redundant testing setups into our production processes, as described below.

waveplate fast axis uncoated metal reflection test setup
Click to Enlarge

Figure 2: Uncoated Metal Reflection Wave Plate Test Setup
View Imperial Product List
Item #QtyDescription
HNL020LB1HeNe Laser, 632.8 nm, 2 mW, Polarized, 100 - 240 VAC Power Supply Included
HCM21XY Adjustable HeNe Mount for 60 mm Cage System (Imperial)
GTH10M-A2Mounted Glan-Thompson Calcite Polarizer, 10 mm x 10 mm Clear Aperture, 350 - 700 nm AR Coating
RSP13Rotation Mount for Ø1" (25.4 mm) Optics, 8-32 Tap
PM100D1Compact Power and Energy Meter Console, Digital 4" LCD
S120C1Standard Photodiode Power Sensor, Si, 400 - 1100 nm, 50 mW
SM1D12D1SM1 Ring-Actuated Iris Diaphragm (Ø0.8 - Ø12 mm)
KM100CP1Kinematic Mirror Mount for Ø1" Optics with Post-Centered Front Plate, 8-32 Taps
RP011Ø2" Manual Rotation Stage
SM1L203SM1 Lens Tube, 2.00" Thread Depth, One Retaining Ring Included
RS1.52Ø1" Pillar Post, 1/4"-20 Taps, L = 1.5", 8-32 Adapter Included
TR1.53Ø1/2" Optical Post, SS, 8-32 Setscrew, 1/4"-20 Tap, L = 1.5"
TR12Ø1/2" Optical Post, SS, 8-32 Setscrew, 1/4"-20 Tap, L = 1"
RSH1.52Ø1" Post Holder with Flexure Lock, Pedestal Base, L = 1.5"
PH15Ø1/2" Post Holder, Spring-Loaded Hex-Locking Thumbscrew, L = 1"
PF1752Clamping Fork for Ø1.5" Pedestal Post or Post Pedestal Base Adapter, Universal
RC14Dovetail Rail Carrier, 1.00" x 1.00" (25.4 mm x 25.4 mm), 1/4" (M6) Counterbore
RLA12001Dovetail Optical Rail, 12", Imperial
RLA06001Dovetail Optical Rail, 6", Imperial
View Metric Product List
Item #QtyDescription
HNL020LB1HeNe Laser, 632.8 nm, 2 mW, Polarized, 100 - 240 VAC Power Supply Included
HCM2/M1XY Adjustable HeNe Mount for 60 mm Cage System (Metric)
GTH10M-A2Mounted Glan-Thompson Calcite Polarizer, 10 mm x 10 mm Clear Aperture, 350 - 700 nm AR Coating
RSP1/M3Rotation Mount for Ø1" (25.4 mm) Optics, M4 Tap
PM100D1Compact Power and Energy Meter Console, Digital 4" LCD
S120C1Standard Photodiode Power Sensor, Si, 400 - 1100 nm, 50 mW
SM1D12D1SM1 Ring-Actuated Iris Diaphragm (Ø0.8 - Ø12 mm)
KM100CP/M1Kinematic Mirror Mount for Ø1" Optics with Post-Centered Front Plate, M4 Taps
RP01/M1Ø2" Manual Rotation Stage, Metric
SM1L203SM1 Lens Tube, 2.00" Thread Depth, One Retaining Ring Included
RS38/M2Ø25.0 mm Pillar Post, M6 Taps, L = 38 mm, M4 Adapter Included
TR40/M3Ø12.7 mm Optical Post, SS, M4 Setscrew, M6 Tap, L = 40 mm
TR30/M2Ø12.7 mm Optical Post, SS, M4 Setscrew, M6 Tap, L = 30 mm
RSH1.5/M2Ø25 mm Post Holder with Flexure Lock, Pedestal Base, L = 38 mm
PH30/M5Ø12.7 mm Post Holder, Spring-Loaded Hex-Locking Thumbscrew, L=30 mm
PF1752Clamping Fork for Ø1.5" Pedestal Post or Post Pedestal Base Adapter, Universal
RC14Dovetail Rail Carrier, 1.00" x 1.00" (25.4 mm x 25.4 mm), 1/4" (M6) Counterbore
RLA300/M1Dovetail Optical Rail, 300 mm, Metric
RLA150/M1Dovetail Optical Rail, 150 mm, Metric

Test Setup 1: Reflection Off Uncoated Metal with n > 1

This test setup is based on the method of Petre Logofatu1, which is also summarized well by Galgano and Henriques2. In this method, a light source passes through a generator, which is a linear polarizer oriented at 45° to the horizontal. Then, the light passes through the wave plate sample under test (SUT), is reflected off an uncoated metal surface (any metal with n > 1 will suffice), and passes through an analyzer (a second linear polarizer oriented at 90° to the generator). The light is then measured by a power sensor.

Our setup, shown in Figure 2 to the right, used a HeNe laser as the light source, two GTH10M-A Glan-Taylor polarizers as the generator and analyzer, a custom uncoated stainless steel reflective surface, an S120C power sensor, and a PM100D power meter console. A full parts list, except the custom metal surface and SUT, is provided below Figure 2.

As described by Logofatu, the power reflection coefficient, R in the equation below, can be derived from the Fresnel equations, showing that there will be a large difference in reflection off the metal depending on whether the fast or the slow axis of the SUT is horizontal.

power reflection equation

where Rp and Rs represent the p-polarized and s-polarized components of R, Δ is the retardance of the SUT, and φ is the phase difference between the p and s reflection coefficients of the metallic surface. From this, we can determine which axis we would expect a higher reflection value when horizontal, and compare expected values to experimental values. Using a large angle of incidence allows for a large separation between s and p coefficients. This correlates with high versus low measured reflection, enabling easy determination of fast versus slow axis. As in both papers, the test was performed at a variety of angles. The results were then fitted to a theoretical curve.

waveplate fast axis lci test setup
Click to Enlarge

Figure 3: Low Coherence Interferometry Wave Plate Testing Setup

Test Setup 2: Low Coherence Interferometry

This test setup uses low coherence interferometry to measure the optical path length (OPL) of the SUT as it is rotated, where the longest OPL corresponds with the slow axis, and the shortest OPL corresponds with the fast axis. This method is additionally verified by modifying the reference arm of the interferometer, adding a reference window and specular back surface to allow for calculation of the group index (ngSUT) along and normal to the crystal axis. These values can then be compared to known values, assuring the reliability of this test.

Our setup, shown in Figure 3 to the right, used a modified Bristol 157 Series Optical Gauge. As can be seen in Figure 4 below, the majority of the low coherence interferometer is contained within the chassis of the optical gaugea. The measurement arm is then modified with Thorlabs components, such that the fiber output can be aligned with a low NA objective, passed through a LPNIR100 linear polarizer and partially reflected off a WG11010 reference window, all mounted on a 34 mm rail. The light then reflects off the SUT and a custom specular back surface to send the interferometric signal back to the optical gauge.

The additional reference surfaces and resulting physical thickness are used to double check the validity of the results. This is done with a quick calculation to determine the group index of both the fast and slow axes. Figure 5 shows a qualitative representation of the output produced by this setup. Peaks 1 and 2 are created by the reference window, Peaks 3 and 4 by the SUT wave plate, while Peak 5 is generated by the reference surface. Thickness data from peak to peak are calculated by the software and output into a table. By first taking the distance from Peak 2 to Peak 5 before the wave plate is inserted, the total physical thickness, Tair0, is obtainedb. When inserting the wave plate, we can then take the distance from Peak 2 to 3, Tair1, and Peak 4 to 5, Tair2. Using this information we can easily calculate the thickness of the wave plate, TSUT by subtracting Tair1 and Tair2 from Tair0. Measuring the distance from Peak 3 to Peak 4 would give us OPLSUT. Dividing OPLSUT by TSUT produces the group index of the SUT, ngSUT. Comparing this group index to that provided in literature for quartz3 or MgF24 both along and normal to the crystal axis, we are in good agreement.

  • Please note Figure 4 is a sample illustration and is not intended to accurately represent the internals of the Bristol optical gauge.
  • For the precision required in this case, it is sufficient to assume the OPL in air is equal to the physical thickness.
example LCI diagram
Click to Enlarge

Figure 4: Example Low Coherence Interferometry Diagram;
Numbered reflections in the measurement arm correspond with peak numbers in Figure 5.
lci output
Click to Enlarge

Figure 5: Representation of Output from Optical Gauge

  1. Galgano, G. D., and A. B. Henriques. "Determining the fast axis of a wave plate." Proceedings do ENFMC (2006).
  2. Logofatu, Petre-Catalin. "Simple method for determining the fast axis of a wave plate." Optical Engineering 41.12 (2002): 3316-3319.
  3. Ghosh, Gorachand. "Dispersion-equation coefficients for the refractive index and birefringence of calcite and quartz crystals." Optics communications 163.1-3 (1999): 95-102.
  4. Dodge, Marilyn J. "Refractive properties of magnesium fluoride." Applied Optics 23.12 (1984): 1980-1985.

Posted Comments:
srm37  (posted 2019-01-07 11:29:36.22)
Dear sir/madam, I was interested in these dual wavelength waveplates, but the system I'm using operates at 1050 nm and 515 nm. What performance quality would be expected using the waveplates as they are at those wavelengths? Cheers, Sam
YLohia  (posted 2019-01-09 04:02:07.0)
Hello Sam, thank you for contacting Thorlabs. As these are multi-order waveplates, unfortunately, the performance at non-design wavelengths is not optimal. I have reached out to you directly with data.
klee  (posted 2009-09-25 11:53:12.0)
A response from Ken at Thorlabs to olsonaj: We can do this as a special. We will send you a quotation by email.
olsonaj  (posted 2009-09-25 01:20:00.0)
This would be very useful if there was one that did 780nm and 1550 nm. (re: WPDM05M-1064H-532Q)

Choosing a Wave Plate

Thorlabs offers achromatic, superachromatic, zero-order (both unmounted wave plates and mounted wave plates), low-order, and multi-order wave plates (single wavelength and dual wavelength) with either λ/4 or λ/2 phase shift.

Achromatic Wave Plates provide phase retardance that is relatively independent of wavelength over a wide spectral range, and Superachromatic Wave Plates provide phase retardance almost entirely independent of wavelength over a much wider range than achromatic wave plates. In contrast, zero-order and multi-order wave plates provide a phase shift that is strongly wavelength dependent. Our achromatic wave plates are available with four operating ranges: 260 - 410 nm, 350 - 850 nm, 400 - 800 nm, 690 - 1200 nm, and 1100 - 2000 nm. Additionally, we offer superachromatic wave plates for the 310 - 1100 nm and 600 - 2700 nm ranges.

Round Zero-Order Wave Plate Comparison
Material Quartz LCP
Sizes Ø1/2" and Ø1" Ø1/2", Ø1", and Ø2"
Mounted Versions Available Yes Yes
Retardances Available 1/4 λ and 1/2 λ 1/4 λ and 1/2 λ
Retardance Accuracy <λ/300 <λ/100
Surface Quality 20-10 Scratch-Dig 60-40 Scratch-Dig
Coating V Coat Broadband AR
Coating Reflectance
(per Surface)
0.25% 0.5% Average Over Specified Coating Range

Zero-order wave plates are designed such that the phase shift created is exactly one quarter or one half of a wave. They offer substantially lower dependence on temperature and wavelength than multi-order wave plates. Our Zero-Order Quartz Half-Wave and Quarter-Wave Plates are composed of two wave plates stacked together with the fast axis of one aligned to the slow axis of the other to achieve zero-order performance. Thorlabs' zero-order wave plates are available for a number of discrete wavelengths ranging from 266 nm to 2020 nm. Our Polymer Zero-Order Half-Wave and Quarter-Wave Plates consist of a thin layer of liquid crystal polymer retarding material sandwiched between two glass plates and are available at discrete wavelengths between 405 nm and 1550 nm. Our quartz zero-order wave plates provide better retardance accuracy and lower reflectance (see table), while our LCP zero-order wave plates produce a smaller decrease in retardance at larger AOIs. In addition, Thorlabs also offers unmounted true Zero-Order Telecom Wave Plates for WDM applications.

MIR Wave Plates are made from a single piece of high-quality magnesium fluoride and provide either quarter-wave or half-wave retardance at 2.5 µm, 3.5 µm, 4.0 µm, 4.5 µm, or 5.3 µm. Light passing through these MIR wave plates will undergo a low number of full or partial wavelength shifts (also referred to as the order, or m) in addition to the fractional design retardance. This differs from true zero-order and multi-order wave plates which undergo no shift or a high number of shifts, respectively. The low-order design maintains near to true zero-order performance, making it a good alternative to true zero-order wave plates. The single magnesium fluoride substrate is also thinner compared to a zero-order design, which combines two multi-order wave plates, making our low-order retarders well suited for applications that are sensitive to dispersion.

Multi-Order Wave Plates are made such that the retardance of a light path will undergo a certain number of full wavelength shifts (also referred to as the order, or m) in addition to the fractional design retardance. Compared to their zero-order counterparts, the retardance of multi-order wave plates is more sensitive to wavelength and temperature changes. Multi-order wave plates are, however, a more economical solution for many applications where increased sensitivities are not an issue. Our multi-order wave plates are available for a number of discrete wavelengths ranging from 405 nm to 1550 nm. Thorlabs also offers Dual-Wavelength Multi-Order Wave Plates designed for use at both 532 nm and 1064 nm.

In addition to these options, Thorlabs also has the ability to design and manufacture custom wave plates for both OEM sales and individual low quantity orders. Our technical staff is able to help with all phases of your request: quoting, sales, and planning and manufacturing support. If you have a custom request or a question about our capabilities, please contact Tech Support to start a discussion.

Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Universal Price Available
WPDM05M-1064H-532Q Support Documentation
WPDM05M-1064H-532QØ1/2" Mounted Multi-Order Dual Wavelength Wave Plate 1/2-wave @ 1064 nm & 1/4-wave @ 532 nm, Ø1" Mount
$363.59
5-8 Days
WPDM05M-532H-1064Q Support Documentation
WPDM05M-532H-1064QØ1/2" Mounted Multi-Order Dual Wavelength Wave Plate 1/2-wave @ 532 nm & 1/4-wave @ 1064 nm, Ø1" Mount
$363.59
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