1. Field of the Invention
The present invention relates to the field of optical devices and systems, and more particularly concerns optical assemblies for splitting and/or combining optical beams.
2. Description of Related Art
Optical beam splitters and combiners are useful devices for respectively splitting and combining optical beams of light having different optical characteristics (e.g. wavelengths, polarization states), which have been implemented into a wide array of optical systems and applications. For example, projectors generally form images by manipulating the relative intensities of three wavelength bands of relatively narrow bandwidth, typically in the red, green and blue regions of the electromagnetic spectrum (i.e. RGB arrangement), using three-channel beam combiners. Likewise, high-quality cameras rely on similar devices in a reverse way, that is, for splitting white light into three RGB spectral components which are subsequently directed to three different image sensors such as charge-coupled devices (CCDs).
In numerous illumination applications, beam combiners are used to combine light of various colors (i.e. wavelength bands) produced from light sources such as light-emitting diodes (LEDs) or lasers into a spectrally broader light output so as to re-create so-called “white light”. The concept of white light is linked with the perception and physiology of the human eye and is based on the premise that red, green and blue lights may be combined in order to make up light containing several wavelength bands inside the visible wavelengths, that is, white light. However, in several instances, the concept of white light may not be sufficient to cover wavelength bands lying outside the visible spectrum commonly used in modern photonics applications. For example, in fields such as life sciences, microscopy, spectroscopy, and laser processing of materials, there is a need for combining or splitting more than three spectral components, often over portions of the electromagnetic spectrum wider or outside the range of visible light or with higher spectral resolution than what is currently achievable in standard RGB applications. In particular, some imaging systems rely on thin-film interference coating technology to separate an optical beam into a plurality of spectrally narrower beams, or to combine the spectral content of a plurality of light beams into a spectrally broader beam. Yet, in the art, the term “white light” is still often understood as being limited to the portion of the electromagnetic spectrum that is visible to the human eye. The above-given interpretation is often restrictive because it does not encompass technologically relevant portions of the spectrum other than visible light.
In the context of the present disclosure, dichroic mirrors capable of separating light into different wavelength bands can be fabricated by depositing specific thin-film coatings on an optical surface substrate. Using such dichroic mirrors, combining light sources in different wavelength bands into a spectrally broader output or separating an input optical beam into a plurality of spectrally narrower light components may be achieved using various configurations of prism, glass plates, and structural mechanical elements. The problem of separating a broad light source into three distinct light beams is well known in the art and several complex and compact solutions have been proposed for the above-described purpose, for example the three-color prism described in U.S. Pat. No. 3,905,684 to Cook et al. and the dichroic pentaprism described in U.S. Pat. No. 5,828,497 to Neumann et al. These two examples illustrate a need to provide compact optical assemblies and to account for performance issues related to the influence of the polarization state and the angle incidence of light impinging on dichroic mirrors. In many optical applications, light is incident on dichroic mirrors or other selectively transmitting elements at an angle of incidence of 45 degrees, which may introduce undesirable polarization-related effects arising from the fact that the polarization state of light is affected at such a large angle of incidence. For example, the transmission and reflection coefficients of the P and S polarization states, the components of light polarized respectively in and out of the plane of incidence defined by the propagation direction of light and the normal to the interface exhibit different wavelength-dependent behaviors, which may be unacceptable in some applications.
Furthermore, existing methods for splitting an input optical beam into three spectral components are generally complex, bulky and costly, and many manufacturers are therefore intentionally avoiding their use. For example, only the most expensive present-day cameras are equipped with three-color beam-splitting prisms. Hence, with the ever increasing number of efficient narrow-wavelength-band LED and laser sources operable from the infrared to the ultraviolet range, optical devices capable of splitting and combining the spectral content of these light sources become highly desirable. In particular, the need for combining more than three wavelength bands of collimated LED or laser sources into a single optical beam is well established, as evidenced by the various products offering four-color mixing LED units launched on the market in recent years. However, these solutions come in relatively large and bulky packages, exhibit limited efficiency, and involve expensive dichroic filters used at 45-degree angles of incidence.
In view of the above, there exists a need in the art for a cost-effective, high-spectral resolution and compact optical assembly capable of splitting/combining polarized and unpolarized optical beams over broad regions of the electromagnetic spectrum, while also alleviating at least some of the drawbacks of the prior art.
According to an aspect of the invention, there is provided a regular pentagon-arranged optical assembly for splitting an input optical beam into spectrally narrower output optical beams, or for combining input optical beams into a spectrally broader output optical beam. Between two and five can be split or combined in the above-described manner. The optical assembly includes five interfaces arranged with respect to one another so as to define a regular pentagonal arrangement. Some of these interfaces are selectively transmissive, while the others are transparent to the circulating light. The optical assembly according to embodiments of the present invention therefore splits or combines optical beams through multiple successive transmissions and internal reflections of optical beams impinging onto the selectively transmitting interfaces. The number of selectively transmissive interfaces corresponds to the number of optical beams to be split or combined, minus one; for example, in one embodiment, the optical assembly is used for splitting or combining five wavelength bands λ1, λ2, λ3, λ4 and λ5, and includes four selectively transmitting interfaces.
Embodiments of the present invention yield compact optical assemblies which may be used to combine or split optical beams for various optical applications and in numerous fields including, without being limited to, optogenetics, wavelength-division multiplexing (WDM), life sciences, microscopy, and LED color mixing.
Advantageously, the angle of incidence of any beam impinging on the selectively transmitting interfaces is preferably equal to 18 degrees and is preserved after each transmission and internal reflection involved in the splitting or the combining process. Also advantageously, such a relatively small angle of incidence contributes to mitigating the polarization sensitivity of the optical assembly according to embodiments of the invention, thereby making it more effective at splitting or combining than existing optical beam splitters and combiners.
In some embodiments, the selectively transmitting interfaces are embodied by coatings deposited on glass plates defining corresponding sides of a hollow regular pentagon. In other embodiments, the selectively transmitting interfaces are coated on corresponding sides of a regular glass pentagonal prism.
In some embodiments, the selectively transmitting interfaces are embodied by dichroic mirrors. Alternatively, in other embodiments, the selectively transmitting interfaces may be embodied by polarization-selective interfaces, wavelength-independent partially reflecting mirrors, or intensity beam splitters. In some of these latter embodiments, the optical assembly may be used as an intensity beam splitter. In further embodiments, the selectively transmitting interfaces may include combinations of dichroic mirrors and intensity filters.
In some embodiments, the optical assembly further includes glass wedges bonded to some of the sides of the regular glass pentagonal prism, so as to ensure that the input and output optical beams respectively enters and exits the optical assembly perpendicularly to an outer surface thereof, thereby advantageously minimizing undesirable polarization-dependent effects.
Other features and advantages of the present invention will be better understood upon reading of preferred embodiments thereof with reference to the appended drawings.
Referring to
One of ordinary skill in the art will understand that embodiments of the present invention may be useful to combine or split optical beams in various applications and in numerous fields including, without being limited to, optogenetics, wavelength-division multiplexing (WDM), life sciences, microscopy, and LED color mixing.
As used herein the term “optical beam” is meant to refer to any electromagnetic radiation of appropriate wavelength, preferably in covering a range encompassing the infrared, visible an ultraviolet portions of the electromagnetic spectrum. The optical beam may be produced by a laser source, a collimated LED source, a fiber-optic light source or any other appropriate light-emitting element.
The optical assembly 20 includes a transparent interface 26 and four selectively transmitting interfaces 28a and 28d. As illustrated in
In the illustrated embodiment, the transparent interface 26 is simply an open aperture (e.g. air), but those of ordinary skill in the art will recognize that it could alternatively be embodied by a layer of transparent material (e.g. a glass plate) that allows the input optical beam 22 to penetrate inside the hollow regular pentagon 30.
Throughout the present description, the term “selectively transmitting interface” is understood to refer to an interface which selectively transmits electromagnetic radiation according to a given optical parameter thereof. It may include, without being limited to, wavelength-selective interfaces (e.g. dichroic mirrors and filters), polarization-selective interfaces (e.g. polarizers or polarization filters), wavelength-independent partially reflecting mirrors and intensity beam splitters.
In the illustrated embodiment, the four selectively transmitting interfaces 28a to 28d are four dichroic mirrors whose optical properties are relative orientation are selected so as to allow splitting and combining of the five optical beams 24a to 24e covering the different wavelength bands λ1, λ2, λ3, λ4 and λ5, respectively, as described hereinbelow. As used herein, the term “dichroic” refers to an optical property of a material or device which allows selective transmission (or reflection) of optical radiation whose wavelength is within a predetermined range, while reflecting (or transmitting) optical radiation whose wavelength lie outside the predetermined range. Accordingly, the terms “dichroic surface”, “dichroic mirror”, “dichroic filter”, “dichroic reflector”, “dichroic coating”, and the like refer to surfaces, mirrors, filters, reflectors, coatings, and the like that exhibit dichroic characteristics. In particular, the dichroic mirrors embodying the selectively transmitting interfaces 28a to 28d may consist of a transparent substrate (e.g. a glass plate) coated with a dielectric multilayer film including alternating layers of high and low refractive index materials.
It is to be noted that while the selectively transmitting interfaces 28a to 28d are embodied by dichroic mirrors with wavelength-dependent reflection and transmission coefficients in the embodiments described below, one of ordinary skill in the art will understand that in other embodiments, the optical assembly 20 may be also used as an intensity beam splitter, wherein the selectively transmitting interfaces 28a to 28d could be embodied by wavelength-independent partially reflecting mirrors or intensity beam splitters, as mentioned above. In such embodiments, the different separated output optical beams would not correspond to different wavelength bands as above but would be fractions of the input optical beam with the same spectral profile. It will be understood that the separated fractions of the input optical beam need not be all of the same intensity and that the intensity beam splitters could each extract a different proportion of the input optical beam. Furthermore, in other embodiments, the selectively transmitting interfaces 28a to 28d may include a combination of dichroic mirrors and intensity filters.
The optical assembly 20 may also include an appropriate support structure (not shown) for supporting the four selectively transmitting interfaces 28a to 28d deposited on their respective substrate (e.g. glass plate) and them as four sides of the hollow regular pentagon 30. It will be understood by one of ordinary skill in the art that the support structure is preferably lightweight, mechanically strong, and compact, while not obstructing the passage of light as it enters and exits the optical assembly 20. The support structure may be embodied, for example, by a metal housing having a regular pentagonal-shaped hole bored therethrough, thus defining the hollow regular pentagon 30. The metal housing could also be provided with additional holes along the five lateral faces thereof. In such an embodiment, the selectively transmitting interfaces 28a to 28d could be glued or otherwise affixed to the internal side of four of the five lateral faces of the metal housing, such that at least a portion of each of the selectively transmitting interfaces 28a to 28d is disposed in front of the holes, thereby allowing light to enter and exit the optical assembly 20.
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After passing through the transparent interface 26, the input optical beam 22 is incident on the first selectively transparent interface 28a, preferably at an angle of incidence of 18 degrees. The first selectively transmitting interface 28a is a dichroic mirror which may be selected so that the longest wavelength band λ1 is transmitted therethrough out of the optical assembly 20 as the first output optical beam 24a, while the shorter wavelength bands λ2, λ3, λ4 and λ5 are internally reflected toward the second selectively transmitting interface 28b. It will be understood by one of ordinary skill in the art that, in other embodiments, the first selectively transmitting interface 28a may be designed so as to transmit any one of the five wavelength bands λ1, λ2, λ3, λ4 and λ5 without departing from the scope of the present invention.
The second selectively transmitting interface 28b is adapted to receive the input optical beam 22 with remaining wavelength bands λ2, λ3, λ4 and λ5 at the same 18-degree angle of incidence. In the illustrated embodiment, the dichroic mirror of the second selectively transmitting interface 28b is selected so that the longest remaining wavelength band λ2 is transmitted therethrough out of the optical assembly 20 as the second output optical beam 24b, while the shorter remaining wavelength bands λ3, λ4 and λ5 are internally reflected toward the third selectively transmitting interface 28c.
The input optical beam 22 with remaining wavelength bands λ3, λ4 and λ5 is subsequently incident on the third selectively transmitting interface 28c of the optical assembly 20, again at an angle of incidence of 18 degrees. The dichroic mirror defining the third selectively transmitting interface 28c transmits therethrough the longest remaining wavelength band λ3, which exits the optical assembly 20 as the third output optical beam 24c, while the shorter remaining wavelength bands λ4 and λ5 are internally reflected toward the fourth selectively transmitting interface 28d.
Finally, the fourth selectively transmitting interface 28d receives thereonto the input optical beam 22 with remaining wavelength bands λ4 and λ5. The dichroic mirror embodying the fourth selectively transmitting interface 28d transmits the wavelength band λ4 out of the optical assembly 20 as the fourth output optical beam 24d and internally reflects the last wavelength band λ5 toward the transparent interface 26, where it exits the optical assembly as the fifth output optical beam 24e. The exit of optical beam 24e completes the splitting of the input optical beam 22 into output optical beams 24a to 24e. It will be understood that the fully transmitting side of the hollow regular pentagon 30 defined by the transparent interface 26 is crossed by both the input optical beam 22 and the fifth output optical beam 24e, at an angle of 36 degrees from each other.
In summary, the embodiment of
It should be noted that, while the splitting of the input optical beam 22 into five spectrally narrower output optical beams 24a to 24e has been described above as being performed in decreasing order of wavelength, that is, from λ1 to λ5, in other embodiments the wavelength bands λ1, λ2, λ3, λ4 and λ5 may be removed from the input optical beam 22 according to any appropriate order or sequence without departing from the scope of the present invention.
From the above considerations, it will also be apparent to one of ordinary skill in the art that the optical assembly 20 illustrated in
As illustrated in
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Furthermore, in the illustrated embodiment, 18-degree glass wedges 38a to 38d are preferably bonded (e.g. glued together using epoxy) or otherwise affixed to the selectively transmitting interfaces 28a to 28d. Likewise, a glass biprism 40 with an apex angle of 144 degrees may be bonded or otherwise affixed to the transparent interface 26 defining the remaining side of the regular glass pentagonal prism 36. It will be understood by one of ordinary skill in the art that the 18-degree glass wedges 38a to 38d and the 144-degree glass biprism 40 allow the input optical beam 22 to enter and the spectrally narrower output optical beams 24a to 24e to exit the optical assembly 20 perpendicularly to an outer surface thereof, thereby advantageously minimizing undesirable polarization-dependent effects on the beams 22 and 24a to 24e. It will be understood that the glass wedges 38a to 38d and the glass biprism 40 are preferably made of the same material as the regular glass pentagonal prism 36. However, in embodiments where the material is not the same, one of ordinary skill in the art will understand that the respective angle defining the glass wedges 38a to 38d and the glass biprism 40 would have to be recalculated to account for the difference in refractive index between the regular glass pentagonal prism 36 and each of the glass wedges 38a to 38d and the glass biprism 40.
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While the invention has been particularly shown and described with reference to the preferred embodiments thereof, it will be understood by those skilled in the art that the foregoing and other changes in form, and details may be made therein without departing from the spirit and scope of the invention.
This U.S. Patent Application claims priority under 35 U.S.C. 119 to U.S. Provisional Patent Application Ser. No. 61/678,822 filed on Aug. 2, 2012.
Number | Date | Country | |
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61678822 | Aug 2012 | US |