Mounted Dove Prisms

Rotate, Invert, or Retroreflect an Image
Six Different Sizes Available
Available Uncoated or AR Coated for 350 - 700 nm or 650 - 1050 nm

PS991M

10 mm Wide Prism,
SM1-Threaded Mount

PS992M-A

15 mm Wide AR-Coated Prism,
SM1-Threaded Mount

PS990M

5 mm Wide Prism,
SM05-Threaded Mount

KS1RS Kinematic Rotation Mount
Allows 360º Rotation Control of
PS992M Mounted Dove Prism

Application Idea

Related Items

Unmounted Dove Prisms

Other Prisms

Kinematic Rotation Mounts

Slotted Ø1" Lens Tube

6-Axis Kinematic Mount

Lens Tube Systems

Optic Cleaning and Handling Tutorial

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Overview
Specs
Graphs
Lab Facts
Prism Guide
Feedback

Common Specifications^a
Material	N-BK7^b
Clear Aperture	>70% of Max Face Length and Width
Surface Quality of Polished Surfaces	40-20 Scratch-Dig
Surface Flatness	λ/5 at 632.8 nm

See the Specs tab for more information.
Click Link for Detailed Specifications on the Substrate Glass

Click to Enlarge
Dove Prism Cross-Sectional View (Left) and Side View (Right)
(See Specs Tab for Details)

Click to Enlarge
Mounted Dove Prism Inside a Slotted Lens Tube with Spanner Wrench
(All Sold Separately)

This animation shows how the image rotates as the prism is rotated.

Features

Rotate and Invert an Image or Retroreflect Light
Mounted Prisms Compatible with our Threaded Rotation Mounts
Uncoated Prisms Offered in Six Sizes (See Diagram to the Right)
- A = 5 mm, SM05-Threaded Mount
- A = 10 mm, SM1-Threaded Mount
- A = 15 mm, SM1-Threaded Mount
- A = 20 mm, SM2-Threaded Mount
- A = 25 mm, SM2-Threaded Mount
- A = 30 mm, SM2-Threaded Mount
15 mm Size Also Available with One of Two AR Coatings

350 - 700 nm
650 - 1050 nm

A Dove prism is used to rotate, invert, or retroreflect an image, depending upon the prism's rotation angle and the surface through which the light enters the prism. Thorlabs' mounted Dove prisms are fabricated from N-BK7 glass for high transmission from the visible to the near-infrared spectral range. Prisms of different sizes are available mounted inside externally SM05-threaded (0.535"-40), SM1-threaded (1.035"-40), or SM2-threaded (2.035"-40) housings. When combined with any of our selection of SM05, SM1, or SM2 rotation mounts, these housings allow an image incident on the angled face of the prism to be continuously rotated through a full 360°. The longest face is also left exposed, allowing the mounted prism to retroreflect light. Each prism has a square cross section. Our 15 mm mounted Dove prism is available either uncoated or with one of two AR coatings deposited on the two angled faces (see the Specs tab for more information on dimensions and AR coatings). We also offer these Dove prisms unmounted. For information on our full selection of prisms, please see the Prism Guide tab.

The anodized aluminum housings contain two slots designed to accept our SPW801 Adjustable Spanner Wrench. These slots enable the prism to be threaded into one of our Ø1/2", Ø1", or Ø2" Lens Tubes. The SPW908 and SPW909 Spanner Wrenches may also be used with SM05- and SM1-threaded mounted prisms, respectively. Shown to the right is a PS992M inserted into an SM1L30C Slotted Lens Tube. The SM1RR Retaining Ring included with the lens tube secures the mounted prism.

Dove prisms can be thought of as right-angle prisms with the triangular apex removed, which reduces the weight of the prism and stray internal reflections. They introduce astigmatism when used with converging light, so we recommend using them with collimated light. Additionally, these prisms affect the polarization state of light transmitted through them. See the Lab Facts tab for further details.

Image Rotation
Light is usually propagated along the longitudinal axis of a Dove prism. In this geometry, shown in the diagrams on the bottom left and middle, light reflects once from the bottom face, inverting the image on the other side. Rotation of the prism about the longitudinal axis rotates the image at twice the rate of the prism's rotation (see video to the right). For example, a 20° rotation of the prism results in a 40° rotated image. The AR-coated Dove prisms are designed specifically for the image rotation and inversion application.

Due to the high incidence angle, the light reflecting from the bottom face undergoes total internal reflection, even if the light's propagation axis and the prism's longitudinal axis are not exactly parallel. Hence, in a Dove prism, the magnitude of the internal transmission is limited only by absorption.

Retroreflection
When light is incident on the longest face, the Dove prism acts as a retroreflector or a right-angle prism. The light exits parallel to the input light (independent of the incidence angle) and is inverted by 180°. This geometry is shown below and to the right. In situations with limited space or where more convenient mounting options are needed, the Dove prism can replace a retroreflector or right-angle prism.

Custom Coatings
Upon request, our uncoated prisms can be AR coated for the 290 - 370 nm (-UV), 350 - 700 nm (-A), 650 - 1050 nm (-B), or 1050 - 1700 nm (-C) spectral ranges. Please contact Technical Support for more information.

Light propagated along the longitudinal axis is inverted by 180°.

Rotation of the prism over some angle results
in a rotation of the image over twice that angle.

Light incident on the longest face of the prism is retroreflected and inverted by 180°.

Unmounted Prism Dimensions^a				Housing Specifications^a
Item # Prefix	A	B	L_P^b	D	L_H	Threading
PS990M	5 mm	7.1 mm	21.1 mm	Ø5 mm	26.3 mm	SM05 (0.535"-40)
PS991M	10 mm	14.1 mm	42.2 mm	Ø10 mm	49.9 mm	SM1 (1.035"-40)
PS992M	15 mm	21.2 mm	63.4 mm	Ø15 mm	70.6 mm	SM1 (1.035"-40)
PS994M	20 mm	28.3 mm	84.5 mm	Ø20 mm	94.8 mm	SM2 (2.035"-40)
PS995M	25 mm	35.4 mm	105.7 mm	Ø25 mm	115.9 mm
PS993M	30 mm	42.4 mm	126.3 mm	Ø30 mm	136.5 mm

Refer to the Diagram Below
Unbeveled Length

General Specifications
Material	N-BK7^a
Clear Aperture	>70% of Max Face Length and Width^b
Surface Quality of Polished Surfaces	40-20 Scratch-Dig
Surface Flatness	λ/5 at 632.8 nm
Optically Polished Surfaces^b	S1, S2, and S3
Fine Ground Surfaces^b	All Surfaces Except S1, S2, and S3
Dimensional Tolerance	±0.15 mm
Angular Tolerance	±3 arcmin

Click Link for Detailed Specifications on the Substrate Glass
Refer to the Diagram Below and to the Right

Click to Enlarge
Cross-Sectional View (Left) and Side View (Right)
of Unmounted Dove Prism and Housing

AR Coating Specifications
Item #	PS992M-A	PS992M-B
Wavelength Range (Click for Plot)	350 - 700 nm	650 - 1050 nm
Reflectance Over AR Coating Range (Avg., AOI = 45° with Respect to the Coated Surface)	<1%
AR-Coated Surfaces^a	S1 and S2

Refer to the Diagram to the Right

The transmission curve for N-BK7, a RoHS-compliant form of BK7, is shown below. The data was obtained for a 10 mm thick, uncoated sample and includes surface reflections. For an Excel file of the data, please click the link below the graph.

N-BK7 Transmission Curve
Click to Enlarge
Click Here for Raw Data

The graphs below give the measured reflectance of AR-coated Dove prisms at a 45° AOI with respect to the coated surface. The graph on the left corresponds to the PS992M-A Dove prism, while the graph on the right corresponds to the PS992M-B Dove prism. For Excel files of the reflectance data, please click the links below the graphs.

Click to Enlarge
Click Here for Raw Data
Please note that this is measured reflectance data. The shaded region indicates the range over which we guarantee the average reflectance will be <1% for a 45° AOI.

Click to Enlarge

Thorlabs Lab Fact: Dove Prisms Alter Polarization State and Image Orientation

We present laboratory measurements of the polarization and rotation state of a beam transmitted through Thorlabs’ PS992 and PS992M Dove Prisms. We also examine the influence of stress-induced birefringence on the final polarization state. In a polarization-dependent experiment, it is important to understand how the polarization and orientation of the input beam is altered by a Dove prism. While it is known that Dove prisms introduce changes in the polarization of the transmitted light [1], we also find that localized stress-induced birefringence can significantly alter the polarization state. Finally we compare theoretical predictions of induced polarization change to the measured polarization change for both our unmounted and mounted versions of Dove prism.

For our experiment we used the HL6320G Laser Diode (635 nm) as the light source. The laser beam was initially aligned using two crossed Glan-Taylor polarizers (GT10-A). The first polarizer set the polarization axis, and the rotation angle of the second crossed polarizer was recorded. The Dove prism was then placed in between the two polarizers, and the power of the beam was recorded after the second polarizer as a function of prism angle. Additionally, measurements were taken to determine the radii and orientation angle of the polarization ellipse. The polarization shift caused by the PS992 unmounted Dove prism and PS992M mounted Dove prism were measured. The unmounted prism was tested for polarization changes due to birefringence effects as well.

Click for Full Lab Facts Summary

The figure to the top right summarizes the measured results for image orientation as a function of prism angle. While it is well known that Dove prisms are used to invert images, it is interesting to note that the image rotation angle is twice that of the prism rotation angle. The figure to the bottom left summarizes the results of stress-induced birefringence on polarization state, while the figure to the bottom right summarizes the effects a Dove prism has on the polarization state and compares that to the theoretical values. Data is presented for both the unmounted and mounted Dove prisms with minimal stress. While Dove prisms do rotate the image, the polarization does not rotate with the image. Rather, the polarization is transformed from linear to various degrees of elliptical. For details on the experimental setup employed and the results summarized here, please click here.

Click to Enlarge

Click to Enlarge

[1] Miles J. Padgett & J. Paul Lesso, "Dove prisms and polarized light," J. Mod. Opt. 46, 175-179 (1999).

Selection Guide for Prisms

Thorlabs offers a wide variety of prisms, which can be used to reflect, invert, rotate, disperse, steer, and collimate light. For prisms and substrates not listed below, please contact Tech Support.

Beam Steering Prisms

Prism	Material	Deviation	Invert	Reverse or Rotate	Applications
Right Angle Prisms	N-BK7, UV Fused Silica, Calcium Fluoride, or Zinc Selenide	90°	90°	No	90° reflector used in optical systems such as telescopes and periscopes.
Right Angle Prisms	N-BK7, UV Fused Silica, Calcium Fluoride, or Zinc Selenide	180°	180°	No	180° reflector, independent of entrance beam angle. Acts as a non-reversing mirror and can be used in binocular configurations.
TIR Retroreflectors (Unmounted and Mounted) and Specular Retroreflectors (Unmounted and Mounted)	N-BK7	180°	180°	No	180° reflector, independent of entrance beam angle. Beam alignment and beam delivery. Substitute for mirror in applications where orientation is difficult to control.
Unmounted Penta Prisms and Mounted Penta Prisms	N-BK7	90°	No	No	90° reflector, without inversion or reversal of the beam profile. Can be used for alignment and optical tooling.
Roof Prisms	N-BK7	90°	90°	180^o Rotation	90° reflector, inverted and rotated (deflected left to right and top to bottom). Can be used for alignment and optical tooling.
Unmounted Dove Prisms and Mounted Dove Prisms	N-BK7	No	180°	2x Prism Rotation	Dove prisms may invert, reverse, or rotate an image based on which face the light is incident on. Prism in a beam rotator orientation.
Unmounted Dove Prisms and Mounted Dove Prisms	N-BK7	180°	180°	No	Prism acts as a non-reversing mirror. Same properties as a retroreflector or right angle (180° orientation) prism in an optical setup.
Wedge Prisms	N-BK7	Models Available from 2° to 10°	No	No	Beam steering applications. By rotating one wedged prism, light can be steered to trace the circle defined by 2 times the specified deviation angle.
Wedge Prisms	N-BK7	Models Available from 2° to 10°	No	No	Variable beam steering applications. When both wedges are rotated, the beam can be moved anywhere within the circle defined by 4 times the specified deviation angle.
Coupling Prisms	Rutile (TiO₂) or GGG	Variable^a	No	No	High index of refraction substrate used to couple light into films. Rutile used for n_film > 1.8 GGG used for n_film < 1.8

Depends on Angle of Incidence and Index of Refraction

Dispersive Prisms

Prism	Material	Deviation	Invert	Reverse or Rotate	Applications
Equilateral Prisms	F2, N-F2, N-SF11, Calcium Fluoride, or Zinc Selenide	Variable^a	No	No	Dispersion prisms are a substitute for diffraction gratings. Use to separate white light into visible spectrum.
Dispersion Compensating Prism Pairs	Fused Silica, Calcium Fluoride, SF10, or N-SF14	Variable Vertical Offset	No	No	Compensate for pulse broadening effects in ultrafast laser systems. Can be used as an optical filter, for wavelength tuning, or dispersion compensation.
Pellin Broca Prisms	N-BK7, UV Fused Silica, or Calcium Fluoride	90°	90°	No	Ideal for wavelength separation of a beam of light, output at 90°. Used to separate harmonics of a laser or compensate for group velocity dispersion.

Prism

Material

Deviation

Invert

Reverse or Rotate

Illustration

Applications

Equilateral Prisms

F2, N-F2,
N-SF11,
Calcium Fluoride,
or Zinc Selenide

Variable^a

Dispersion prisms are a substitute for diffraction gratings.

Use to separate white light into visible spectrum.

Dispersion Compensating Prism Pairs

Fused Silica, Calcium Fluoride, SF10, or N-SF14

Variable Vertical Offset

Compensate for pulse broadening effects in ultrafast laser systems.

Can be used as an optical filter, for wavelength tuning, or dispersion compensation.

Pellin Broca Prisms

N-BK7,
UV Fused Silica,
or Calcium Fluoride

90°

Ideal for wavelength separation of a beam of light, output at 90°.

Used to separate harmonics of a laser or compensate for group velocity dispersion.

Depends on Angle of Incidence and Index of Refraction

Beam Manipulating Prisms

Prism	Material	Deviation	Invert	Reverse or Rotate	Illustration	Applications
Anamorphic Prism Pairs	N-KZFS8 or N-SF11	Variable Vertical Offset	No	No		Variable magnification along one axis. Collimating elliptical beams (e.g., laser diodes) Converts an elliptical beam into a circular beam by magnifying or contracting the input beam in one axis.
Axicons (UVFS, ZnSe)	UV Fused Silica or Zinc Selenide	Variable^a	No	No		Creates a conical, non-diverging beam with a Bessel intensity profile from a collimated source.

Prism

Material

Deviation

Invert

Reverse or Rotate

Illustration

Applications

Anamorphic Prism Pairs

N-KZFS8 or
N-SF11

Variable Vertical Offset

Variable magnification along one axis.

Collimating elliptical beams (e.g., laser diodes)

Converts an elliptical beam into a circular beam by magnifying or contracting the input beam in one axis.

Axicons (UVFS, ZnSe)

UV Fused Silica
or Zinc Selenide

Variable^a

Creates a conical, non-diverging beam with a Bessel intensity profile from a collimated source.

Depends on Prism Physical Angle

Polarization Altering Prisms

Prism	Material	Deviation	Invert	Reverse or Rotate	Applications
Glan-Taylor, Glan-Laser, and α-BBO Glan-Laser Polarizers	Glan-Taylor: Calcite Glan-Laser: α-BBO or Calcite	p-pol. - 0° s-pol. - 112°^a	No	No	Double prism configuration and birefringent calcite produce extremely pure linearly polarized light. Total Internal Reflection of s-pol. at the gap between the prism while p-pol. is transmitted.
Rutile Polarizers	Rutile (TiO₂)	s-pol. - 0° p-pol. absorbed by housing	No	No	Double prism configuration and birefringent rutile (TiO₂) produce extremely pure linearly polarized light. Total Internal Reflection of p-pol. at the gap between the prisms while s-pol. is transmitted.
Double Glan-Taylor Polarizers	Calcite	p-pol. - 0° s-pol. absorbed by housing	No	No	Triple prism configuration and birefringent calcite produce maximum polarized field over a large half angle. Total Internal Reflection of s-pol. at the gap between the prism while p-pol. is transmitted.
Glan Thompson Polarizers	Calcite	p-pol. - 0° s-pol. absorbed by housing	No	No	Double prism configuration and birefringent calcite produce a polarizer with the widest field of view while maintaining a high extinction ratio. Total Internal Reflection of s-pol. at the gap between the prism while p-pol. is transmitted.
Wollaston Prisms and Wollaston Polarizers	Quartz, Magnesium Fluoride, α-BBO, Calcite, Yttrium Orthovanadate	Symmetric p-pol. and s-pol. deviation angle	No	No	Double prism configuration and birefringent calcite produce the widest deviation angle of beam displacing polarizers. s-pol. and p-pol. deviate symmetrically from the prism. Wollaston prisms are used in spectrometers and polarization analyzers.
Rochon Prisms	Magnesium Fluoride or Yttrium Orthovanadate	Ordinary Ray: 0° Extraordinary Ray: deviation angle	No	No	Double prism configuration and birefringent MgF₂ or YVO₄ produce a small deviation angle with a high extinction ratio. Extraordinary ray deviates from the input beam's optical axis, while ordinary ray does not deviate.
Beam Displacing Prisms	Calcite	2.7 or 4.0 mm Beam Displacement	No	No	Single prism configuration and birefringent calcite separate an input beam into two orthogonally polarized output beams. s-pol. and p-pol. are displaced by 2.7 or 4.0 mm. Beam displacing prisms can be used as polarizing beamsplitters where 90^o separation is not possible.
Fresnel Rhomb Retarders	N-BK7	Linear to circular polarization Vertical Offset	No	No	λ/4 Fresnel Rhomb Retarder turns a linear input into circularly polarized output. Uniform λ/4 retardance over a wider wavelength range compared to birefringent wave plates.
Fresnel Rhomb Retarders	N-BK7	Rotates linearly polarized light 90°	No	No	λ/2 Fresnel Rhomb Retarder rotates linearly polarized light 90°. Uniform λ/2 retardance over a wider wavelength range compared to birefringent wave plates.

S-polarized light is not pure and contains some P-polarized reflections.

Beamsplitter Prisms

Prism	Material	Deviation	Invert	Reverse or Rotate	Illustration	Applications
Beamsplitter Cubes	N-BK7	50:50 splitting ratio, 0° and 90° s- and p- pol. within 10% of each other	No	No		Double prism configuration and dielectric coating provide 50:50 beamsplitting nearly independent of polarization. Non-polarizing beamsplitter over the specified wavelength range.
Polarizing Beamsplitter Cubes	N-BK7, UV Fused Silica, or N-SF1	p-pol. - 0° s-pol. - 90°	No	No		Double prism configuration and dielectric coating transmit p-pol. light and reflect s-pol. light. For highest polarization use the transmitted beam.

Prism

Material

Deviation

Invert

Reverse or Rotate

Illustration

Applications

Beamsplitter Cubes

N-BK7

50:50 splitting ratio, 0° and 90°

s- and p- pol. within 10% of each other

Double prism configuration and dielectric coating provide 50:50 beamsplitting nearly independent of polarization.

Non-polarizing beamsplitter over the specified wavelength range.

Polarizing Beamsplitter Cubes

N-BK7, UV Fused Silica, or N-SF1

p-pol. - 0°

s-pol. - 90°

Double prism configuration and dielectric coating transmit p-pol. light and reflect s-pol. light.

For highest polarization use the transmitted beam.

Posted Comments:

Timothy Lee (posted 2023-07-20 10:10:51.077)

Hello, I am interested in ordering a custom mounted dove prism. Would you be able to produce a 7.5 mm x 7.5 mm dove prism (height and width) mounted in an sm05-thread mount? Length can be as necessary. Transmission should be optimized for 920 nm wavelength. Let me know if you need any additional information. Thanks, Tim

jdelia (posted 2023-07-20 01:37:52.0)

Thank you for contacting Thorlabs. In the future, you can direct custom requests to your local tech support team. We are reaching out to you directly regarding the feasibility of your custom request.

Haozhe Kang (posted 2021-08-31 20:26:24.02)

The product display diagram of ps992m-a-sm1 is inconsistent with the sldprt file in the provided document. The lens sleeve and threaded mounting base in the display drawing and PDF document are round, while the sldprt file is non-circular. I want to know the real shape of lens sleeve and threaded mount and get the real sldprt file.

cdolbashian (posted 2021-10-29 11:07:31.0)

Thank you for reaching out to us at Thorlabs! We are in the process of updating this part's drawing and will reach out to you as soon as it is updated!

voronov.alexander (posted 2014-02-19 09:37:18.18)

Could you make a mounted Dove prism with UV fused silica and with AR coating on 355nm? I would like to have a few units of prisms. If yes, could you send me a quotation?

jlow (posted 2014-02-27 02:23:59.0)

Response from Jeremy at Thorlabs: We will contact you directly on quoting this.

Mounted Dove Prisms, Uncoated

Zoom

Click to Enlarge
Cross-Sectional View (Left) and
Side View (Right) of a Dove Prism

Item #	A^a	L^a	Threading^b
PS990M	5 mm	21.1 mm	SM05 (0.535"-40)
PS991M	10 mm	42.2 mm	SM1 (1.035"-40)
PS992M	15 mm	63.4 mm	SM1 (1.035"-40)
PS994M	20 mm	84.5 mm	SM2 (2.035"-40)
PS995M	25 mm	105.7 mm
PS993M	30 mm	126.3 mm

As Specified in the Diagram to the Right
Please See the Specs Tab for Housing Details

Uncoated N-BK7 for the 350 nm to 2.0 µm Wavelength Range
Available in Six Sizes (See Table and Diagram to the Right)
Rotate, Invert, or Retroreflect an Image
Compatible with SM05-, SM1-, or SM2-Threaded Optomechanics

These mounted, uncoated Dove prisms are offered with square cross sections in six different sizes (please see the table and diagram to the right). As described in the Overview tab above, the two angled faces are typically used together to rotate an image, while the longest face can be used to retroreflect an image. The angled faces and longest face of our Dove prisms are optically polished surfaces. All other surfaces are fine ground and inaccessible due to the mount.

Mounted Dove Prism, AR Coated: 350 - 700 nm

Zoom

Click to Enlarge
Cross-Sectional View (Left) and Side View (Right) of a Dove Prism

AR Coated for the 350 nm to 700 nm Wavelength Range
Available in One Size: A = 15 mm, L = 63.4 mm (See Diagram to the Right)
Rotate or Invert an Image
Compatible with SM1-Threaded Optomechanics

This SM1-mounted Dove prism has a 15 mm square cross section and an AR coating for 350 to 700 nm deposited on the two angled faces (shown in the diagram to the right, please see the Specs tab for details). This coating provides an average reflectance of <1% (AOI = 45°) over the specified wavelength range. For a plot of the reflectance versus wavelength, please see the Graphs tab.

As described in the Overview tab above, the two angled faces of a Dove prism are typically used together to rotate an image. With an AR coating on both angled faces, this prism is specifically designed for image inversion and rotation. Please note that the AR coating makes these prisms unsuitable for use as retroreflectors. For retroreflecting applications, please use our uncoated Dove prisms. The angled faces and longest face of this Dove prism are optically polished surfaces. All other surfaces are fine ground and inaccessible due to the mount.

Mounted Dove Prism, AR Coated: 650 - 1050 nm

Zoom

Click to Enlarge
Cross-Sectional View (Left) and Side View (Right) of a Dove Prism

AR Coated for the 650 nm to 1050 nm Wavelength Range
Available in One Size: A = 15 mm, L = 63.4 mm (See Diagram to the Right)
Rotate or Invert an Image
Compatible with SM1-Threaded Optomechanics

This SM1-mounted Dove prism has a 15 mm square cross section and an AR coating for 650 nm to 1050 nm deposited on the two angled faces (shown in the diagram to the right, please see the Specs tab for details). This coating provides an average reflectance of <1% (AOI = 45°) over the specified wavelength range. For a plot of the reflectance versus wavelength, please see the Graphs tab.