Patent Description:
Generally, in times of an increasing number of applications comprising optical components such as image sensor, there is a growing need of an optical system and an optical method, which especially allow for an efficient magnification or demagnification, respectively, preferably in order to boost incoming light, and thus, in the case of such image sensors, increase image quality exemplarily due to an increased signal-to-noise ratio, which typically drops as the pixel size scales.

<CIT> relates to a transparent wearable data display having a source of collimated light, a deflector for deflecting the collimated light into a scanned beam, and a first of switchable grating elements sandwiched between first and second parallel transparent substrates, which together function as a first light guide. A first coupling is provided for directing the scanned beam into a first total internal reflection (TIR) light path of the first light guide along the first array column. The grating elements have diffracting and non-diffracting states, in their diffracting state deflecting light out of said light guide. The grating elements are switchable into their diffracting states one group of elements at a time. Disadvantageously, in accordance with the corresponding configuration and especially due to the lack of a confocal point, said transparent wearable data display does not allow for an efficient magnification or demagnification, respectively.

Furthermore, <CIT> discloses a waveguide display having an input image generator providing image light projected over a field of view, a waveguide having first and second external surfaces, and at least one grating optically coupled to the waveguide for extracting light towards a viewer. The waveguide has a lateral refractive index variation between said external surfaces that prevents any ray propagated within the waveguide from optically interacting with at least one of the external surfaces.

Moreover, <CIT> provides a multi-tiered computing hologram chromatic aberration elimination and vision correction waveguide display method and system. The method includes that components of object light emitted by a micro displayer are controlled to be irradiated to corresponding holograms at different angles through optical waveguide. Plane reference light and corresponding object light components interfere each other in the corresponding holograms, and an input coupling holographic grating is obtained. The micro displayer is controlled to be irradiated at a preset angle and then input to the input coupling holographic grating. Emergent parallel light is transmitted in a total reflection mode in the optical waveguide, so that the components of object light enter an output coupling holographic grating in the optical waveguide respectively. The output coupling holographic grating outputs an emergent hologram is used for chromatic aberration elimination and vision correction.

Additionally, <CIT> relates to a wide viewing angle waveguide lens, a manufacturing method and a head-mounted three-dimensional display device. By using a nano grating structure having a concentrated light field viewing angle amplifying function, namely a grating lens function, the viewing angle of three-dimensional virtual information is amplified and projected in front of human eyes. A virtual object is fused with a real scene via the wide viewing angle waveguide lens.

In further addition to this, <CIT> discloses an optical head and an optical data processing apparatus, wherein a planar waveguide is formed on a substrate for propagating the light emitted from a light source. A diffraction grating is concentrically formed around a specific point of the planar waveguide on the same planar waveguide. The light diffracted by the diffraction grating is irradiated on an optical disk, and the light reflected from the optical disk is received by an optical detector formed on the planar waveguide.

Accordingly, there is an object to provide an optical system and an optical method, which ensure a magnification or a demagnification, respectively, in a significantly efficient manner.

This object is solved by the features of claim <NUM> for an optical system and the features of claim <NUM> for an optical method. The dependent claims contain further developments.

According to a first aspect of the invention, an optical system is provided. Said system comprises an optical waveguide, and at least two coupling means forming one confocal point being located within the optical waveguide. In this context, a first coupling means of the at least two coupling means has a first focal length. In addition to this, a second coupling means of the at least two coupling means has a second focal length. Furthermore, the first coupling means is configured to couple and focus incident light to the optical waveguide, whereas the second coupling means is configured to emit and collimate light conveyed by the optical waveguide. Advantageously, magnification or demagnification can be achieved in a particularly efficient manner. Further advantageously, with respect to the optical waveguide, a folded waveguide may be used especially in order to limit aberration.

According to a first preferred implementation form of the first aspect of the invention, the first coupling means and the second coupling means are confocal. Additionally or alternatively, the second focal length is smaller than the first focal length. In further addition to this or as a further alternative, the optical system further comprises an optical sensor being configured to receive the light emitted and collimated by the second coupling means. Advantageously, light intensity at the pixel level can be increased. Further advantageously, the size of the optical sensor can be very small. As a further advantage, the size of the optical sensor is decoupled from the dimensions of the coupling means.

According to a second preferred implementation form of the first aspect of the invention, the optical sensor comprises or is a camera or an image sensor, preferably a complementary metal-oxide-semiconductor image sensor. Advantageously, more light can be brought to the camera or the image sensor, which leads to an increased light intensity at the pixel level.

According to a further preferred implementation form of the first aspect of the invention, the first coupling means comprises at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof. Additionally or alternatively, the second coupling means comprises at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof. In addition to this or as an alternative, if present, at least one further coupling means of the at least two coupling means comprises at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof. Further additionally or further alternatively, the optical waveguide comprises or is a slab-waveguide. Advantageously, at least one, preferably each, of the above-mentioned coupling means may additionally or alternatively comprise or be a fiber Bragg grating (FBG).

According to a further preferred implementation form of the first aspect of the invention, at least one, preferably each, of the optical waveguide, the first coupling means, and the second coupling means comprises at least one of liquid crystal, an electro-optic material, preferably barium titanate, geometrical variations, preferably a micro-electro-mechanical system, or any combination thereof. Additionally, if present, at least one further coupling means of the at least two coupling means comprises at least one of liquid crystal, an electro-optic material, preferably barium titanate, geometrical variations, preferably a micro-electro-mechanical system, or any combination thereof. Advantageously, for instance, this allows for tunability or makes the respective portions of the optical system modulatable, respectively.

According to a further preferred implementation form of the first aspect of the invention, at least one, preferably each, of the optical waveguide, the first coupling means, and the second coupling means is configured to be thermally and/or electrically tunable. In addition to this or as an alternative, if present, at least one further coupling means of the at least two coupling means is configured to be thermally and/or electrically tunable. Advantageously, each of the above-mentioned liquid crystal, the electro-optic material, preferably barium titanate, the geometrical variations, preferably the micro-electro-mechanical system, may allow for said tunability. Further advantageously, especially in the case of the above-mentioned fiber Bragg grating (FBG), it noted that tuning may be understood as modulating the corresponding positions of the reflective portions of said FBG.

As further advantages, especially in the case that at least the optical waveguide is tunable, an optical zoom can be implemented preferably in a single-camera system exemplarily for mobile phones, no moving element is necessary for zooming, and a very compact form factor is ensured.

Further advantageously, especially in the case that at least one, preferably the first and the second, coupling means is tunable, autofocusing and/or image stabilization can be achieved in a highly efficient manner exemplarily without any moving element.

According to a further preferred implementation form of the first aspect of the invention, the optical system further comprises adjusting means. In this context, the adjusting means is configured to adjust or tune at least one optical parameter of the optical waveguide and/or the first coupling means and/or the second coupling means and/or, if present, at least one further coupling means of the at least two coupling means, preferably to adjust or tune at least one optical parameter of the optical waveguide especially at least in the region between the first coupling means and the second coupling means. Advantageously, for instance, tuning or modulating, respectively, can be performed in a particularly accurate and efficient manner.

According to a further preferred implementation form of the first aspect of the invention, the at least one optical parameter comprises or is a refractive index. Advantageously, for example, complexity can be reduced, which leads to an increased efficiency.

According to a further preferred implementation form of the first aspect of the invention, with respect to the optical waveguide, the adjusting means is configured to tune an optical path distance between the first coupling means and the second coupling means especially in order to tune an effective magnification factor of the optical system. Advantageously, for instance, inefficiencies can be decreased by further reducing complexity.

According to a further preferred implementation form of the first aspect of the invention, with respect to the optical waveguide, the adjusting means is configured to bias an optical path between the first coupling means and the second coupling means in a biasing direction. Advantageously, for example, efficiency can further be increased.

According to a further preferred implementation form of the first aspect of the invention, the optical path and the biasing direction enclose an angle between <NUM> and <NUM> degrees, preferably between <NUM> and <NUM> degrees, more preferably between <NUM> and <NUM> degrees, most preferably <NUM> degrees. Advantageously, for instance, not only accuracy but also efficiency can further be increased.

According to a further preferred implementation form of the first aspect of the invention, for biasing the optical path between the first coupling means and the second coupling means, the adjusting means is configured to generate an electrical field especially being parallel to the biasing direction. Advantageously, for example, inefficiencies can further be reduced.

According to a further preferred implementation form of the first aspect of the invention, the adjusting means comprises or is a modulator and/or a capacitance. Advantageously, for instance, complexity, and thus costs, can further be reduced, which leads to an increased efficiency.

According to a further preferred implementation form of the first aspect of the invention, the optical system is used in the context of at least one of an imager application, a display application, an X-ray application, a beyond magnification application, an endoscopy application, preferably a medical endoscopy application, or any combination thereof. Advantageously, for example, a high flexibility can be ensured.

Before the second aspect of the invention and its preferred implementation forms are described in the following, it is noted that all the advantages mentioned above analogously apply for the inventive optical method explained below.

According to a second aspect of the invention, an optical method is provided as specified in appended claim <NUM>. Said method comprises the steps of providing an optical waveguide and at least two coupling means, forming one confocal point being located within the optical waveguide with the aid of the at least two coupling means, coupling and focusing incident light to the optical waveguide with the aid of a first coupling means, having a first focal length, of the at least two coupling means, and emitting and collimating light conveyed by the optical waveguide with the aid of a second coupling means, having a second focal length, of the at least two coupling means. According to a first preferred implementation form of the second aspect of the invention, the first coupling means and the second coupling means are confocal. Additionally or alternatively, the second focal length is smaller than the first focal length. In further addition to this or as a further alternative, the optical method further comprises the step of receiving the light emitted and collimated by the second coupling means with the aid of an optical sensor. According to a second preferred implementation form of the second aspect of the invention, the optical sensor comprises or is a camera or an image sensor, preferably a complementary metal-oxide-semiconductor image sensor.

According to a further preferred implementation form of the second aspect of the invention, the first coupling means comprises at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof. Additionally or alternatively, the second coupling means comprises at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof. In addition to this or as an alternative, if present, at least one further coupling means of the at least two coupling means comprises at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof. Further additionally or further alternatively, the optical waveguide comprises or is a slab-waveguide.

According to a further preferred implementation form of the second aspect of the invention, at least one, preferably each, of the optical waveguide, the first coupling means, and the second coupling means comprises at least one of liquid crystal, an electro-optic material, preferably barium titanate, geometrical variations, preferably a micro-electro-mechanical system, or any combination thereof. Additionally, if present, at least one further coupling means of the at least two coupling means comprises at least one of liquid crystal, an electro-optic material, preferably barium titanate, geometrical variations, preferably a micro-electro-mechanical system, or any combination thereof.

According to a further preferred implementation form of the second aspect of the invention, the method comprises the step of configuring at least one, preferably each, of the optical waveguide, the first coupling means, and the second coupling means to be thermally and/or electrically tunable. In addition to this or as an alternative, the optical method comprises the step of configuring, if present, at least one further coupling means of the at least two coupling means to be thermally and/or electrically tunable.

According to a further preferred implementation form of the second aspect of the invention, the optical method further comprises the step of with the aid of adjusting means, adjusting or tuning at least one optical parameter of the optical waveguide and/or the first coupling means and/or the second coupling means and/or, if present, at least one further coupling means of the at least two coupling means, preferably adjusting or tuning at least one optical parameter of the optical waveguide especially at least in the region between the first coupling means and the second coupling means.

According to a further preferred implementation form of the second aspect of the invention, the at least one optical parameter comprises or is a refractive index.

According to a further preferred implementation form of the second aspect of the invention, with respect to the optical waveguide, with the aid of the adjusting means, the method comprises the step of tuning an optical path distance between the first coupling means and the second coupling means especially in order to tune a respective effective magnification factor.

According to a further preferred implementation form of the second aspect of the invention, with respect to the optical waveguide, with the aid of the adjusting means, the optical method further comprises the step of biasing an optical path between the first coupling means and the second coupling means in a biasing direction.

According to a further preferred implementation form of the second aspect of the invention, the optical path and the biasing direction enclose an angle between <NUM> and <NUM> degrees, preferably between <NUM> and <NUM> degrees, more preferably between <NUM> and <NUM> degrees, most preferably <NUM> degrees.

According to a further preferred implementation form of the second aspect of the invention, for biasing the optical path between the first coupling means and the second coupling means, with the aid of the adjusting means, the method comprises the step of generating an electrical field especially being parallel to the biasing direction.

According to a further preferred implementation form of the second aspect of the invention, the adjusting means comprises or is a modulator and/or a capacitance.

According to a further preferred implementation form of the second aspect of the invention, the optical method is used in the context of at least one of an imager application, a display application, an X-ray application, a beyond magnification application, an endoscopy application, preferably a medical endoscopy application, or any combination thereof.

Firstly, before exemplary embodiments of the invention will be discussed in greater detail, some general and introductive aspects, especially in the form of advantages, are explained in the following.

For instance, to overcome limitations with scaled pixel size, the invention can be used for separating focal plane to pixel array. In this context, focal plane especially means where incoming light is focused exemplarily using a lens, and pixel array especially means where incoming light is converted to electron.

Then, the light signals illuminated on focal plane are delivered to the pixel array (for example, image sensor) using wave guide. During this delivery, the size of the image can be scaled. For example, in case of scaling down, disadvantages of the small size pixel can be overcome. Also, by changing the degree of the scaling, zooming operation can also be included.

Generally, separating the focal plane from the imaging plane in the sense of the invention enables several advantages such as sensitivity boosting, zoom operation especially in horizontal domain (low lens module thickness), color (light wavelength) separation, and enhancing signal-to-noise ratio and/or resolution. In addition to this, especially by changing properties of the materials in between focal plane and imaging plane, optical zoom is possible. For instance, in this way, compactness of a corresponding camera hardware can be achieved.

Now, with respect to <FIG>, a block diagram of an exemplary embodiment of an inventive optical system <NUM> is shown. According to <FIG>, said optical system <NUM> comprises an optical waveguide <NUM>, first coupling means <NUM> having a first focal length (f<NUM>) and being optically connected to a first terminal of the optical waveguide <NUM>, and second coupling means <NUM> having a second focal length (f<NUM>) and being optically connected to a second terminal of the optical waveguide <NUM>.

In this context, the first coupling means <NUM> is configured to couple and focus incident light 16a to the optical waveguide <NUM>. In addition to this, the second coupling means <NUM> is configured to emit and collimate light 16b conveyed by the optical waveguide <NUM>.

It is noted that with respect to the above-mentioned incident light 16a and the above-mentioned conveyed light 16b, said kinds of light are analogously marked with the aid of the same reference signs in the context of <FIG>, <FIG>, <FIG>, <FIG>, and <FIG>.

It is further noted that the first coupling means <NUM> and the second coupling means <NUM> are confocal, wherein the second focal length (f<NUM>) is smaller than the first focal length (f<NUM>). In this context, it should be mentioned that the respective focal point is located within the optical waveguide <NUM>. Such an optical system <NUM> can also be called confocal system.

As it can further be seen from <FIG>, the optical system <NUM> or confocal system, respectively, additionally comprises an optical sensor <NUM>, wherein the optical sensor <NUM> is configured to receive the light 16b emitted and collimated by the second coupling means <NUM>.

In this context, it is noted that it might be particularly advantageous if the optical sensor <NUM> comprises or is a camera or an image sensor, preferably a complementary metal-oxide-semiconductor (CMOS) image sensor. Such a CMOS image sensor may especially called CIS in the following.

With respect to the first coupling means <NUM>, it is noted that the first coupling means <NUM> may comprise at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof.

Additionally or alternatively, the second coupling means <NUM> may comprise at least one of a lens, preferably a Fresnel lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof. With respect to the optical waveguide <NUM>, it is noted that it might be particularly advantageous if the optical waveguide <NUM> comprises or is a slab-waveguide.

Furthermore, it might be also particularly advantageous if at least one, preferably each, of the optical waveguide <NUM>, the first coupling means <NUM>, and the second coupling means <NUM> comprises at least one of liquid crystal, an electro-optic material, preferably barium titanate, geometrical variations, preferably a micro-electro-mechanical system, or any combination thereof.

Moreover, at least one, preferably each, of the optical waveguide <NUM>, the first coupling means <NUM>, and the second coupling means <NUM> may especially be configured to be thermally and/or electrically tunable. In this context, it is noted that each of the above-mentioned liquid crystal, the electro-optic material, preferably barium titanate, the geometrical variations, preferably the micro-electro-mechanical system, may exemplarily allow for said tunability.

In further accordance with <FIG>, the confocal system <NUM> additionally comprises adjusting means <NUM>, wherein the adjusting means <NUM> is generally configured to adjust or tune at least one optical parameter of the optical waveguide <NUM> and/or the first coupling means <NUM> and/or the second coupling means <NUM>, preferably of the optical waveguide <NUM> especially at least in the region between the first coupling means <NUM> and the second coupling means <NUM>.

In this exemplary embodiment, said preferred alternative is implemented. Accordingly, the adjusting means <NUM> adjusts or tunes the at least one optical parameter of the optical waveguide <NUM>. With respect to the at least one optical parameter, it is noted that it might be particularly advantageous if the at least one optical parameter comprises or is a refractive index.

In addition to this or as an alternative, with respect to the optical waveguide <NUM>, the adjusting means <NUM> may preferably be configured to tune an optical path distance between the first coupling means <NUM> and the second coupling means <NUM> especially in order to tune an effective magnification factor of the optical system <NUM>.

Further additionally or further alternatively, also with respect to the optical waveguide <NUM>, the adjusting means <NUM> may preferably be configured to bias an optical path between the first coupling means <NUM> and the second coupling means <NUM> in a biasing direction. In this context, it might be particularly advantageous if the optical path and the biasing direction enclose an angle between <NUM> and <NUM> degrees, preferably between <NUM> and <NUM> degrees, more preferably between <NUM> and <NUM> degrees, most preferably <NUM> degrees.

Furthermore, for biasing the optical path between the first coupling means <NUM> and the second coupling means <NUM>, the adjusting means <NUM> is configured to generate an electrical field especially being parallel to the biasing direction. Exemplarily, as it can be seen from <FIG>, the adjusting means <NUM> especially is a capacitance or a capacitor, respectively, which generates said electrical field. As an alternative, it is noted that the adjusting means <NUM> may comprise or be a modulator and/or a capacitance.

Fundamentally, it is noted that it might be particularly advantageous if the optical system <NUM> is used in the context of at least one of a mobile phone application such as a smartphone application, an imager application, a display application, an X-ray application such as application <NUM> according to <FIG>, a beyond magnification application such as application <NUM> according to <FIG>, an endoscopy application, preferably a medical endoscopy application, a time-of-flight system especially for at least one of a mobile application, an augmented reality application, an automotive and/or machine vision application, or any combination thereof.

With respect to the above-mentioned imager application, it is noted that such an imager application may exemplarily comprise an imager with a fixed magnification for a small CIS especially at low cost but large magnification, an imager with a zoom lens in a mobile phone especially at an ultimate small form factor, or an imager for lens-free imaging especially with large pixels.

Furthermore, with respect to the above-mentioned display application, such a display application may exemplarily comprise an eye tracking sensor especially for an augmented reality and/or virtual reality application, preferably an augmented reality and/or virtual reality glass application. Moreover, with respect to the above-mentioned endoscopy application, preferably the medical endoscopy application, it is noted that a small camera system can advantageously be integrated in disposable endoscopes.

In addition to this, regarding the eye tracking sensor mentioned above and/or with respect to the above-mentioned time-of-flight system especially for at least one of a mobile application, an augmented reality application, an automotive and/or machine vision application, it is noted that the intensity of a respective infrared source can advantageously be limited especially in order to fulfill eye safety requirements.

Now, on the basis of <FIG> and <FIG> showing an exemplary confocal system <NUM> in the sense of a free-space optics setup, the invention is further explained in the following.

As it can be seen from <FIG>, said confocal system, which specifically is a confocal magnification or demagnification, respectively, lens system, comprises a first lens <NUM> having a first focal length f<NUM>, and a second lens <NUM> having a second focal length f<NUM>. Said lenses <NUM> and <NUM> are arranged in free-space in a confocal manner, wherein the second focal length is smaller than the first focal length (f<NUM> < f<NUM>). In other words, the two confocal lenses <NUM>, <NUM> with different focal lengths as depicted in <FIG> form the exemplary (de)magnification system <NUM> especially for a free-space optics setup.

In this context, <FIG> illustrates an exemplary use case <NUM>' of the system according to <FIG>. As it can be seen, a large window <NUM> to the respective scene is converted or demagnified, respectively, to a small chip imager <NUM> especially with dense small pixels.

Furthermore, with respect to <FIG>, a further exemplary embodiment <NUM> of the inventive optical system is illustrated. Said exemplary embodiment <NUM> especially is an integrated optical magnification or demagnification, respectively, system. In this context, it is noted that the inventive system <NUM> according to <FIG> may also be an integrated optical (or confocal) system, especially an integrated optical (de)magnification system.

In this exemplary case according to <FIG>, coupling structures <NUM>, <NUM> such as focusing grating couplers or complex diffractive components, are used to convert three-dimensional (3D) free-space propagation to a two-dimensional (2D) free-space propagation in a slab-waveguide <NUM> especially with only z-direction confinement.

It might be particularly advantageous if the first coupling structure <NUM> is configured to couple light into the waveguide <NUM>, whereas the second coupling structure <NUM> is configured to couple light out of the waveguide <NUM>. In this context, the first coupling structure <NUM> may preferably be configured to convert 3D to 2D propagation, whereas the second coupling structure <NUM> may preferably be configured to convert 2D to 3D propagation. It is noted that the above-mentioned coupling structures <NUM> and <NUM> especially are examples for the first and second coupling means <NUM> and <NUM> according to <FIG>, whereas the slab-waveguide <NUM> is an example of the optical waveguide <NUM> of <FIG>.

Moreover, <FIG> and <FIG> sketch the usage of the above-mentioned system <NUM> according to <FIG> for magnification (<FIG>) and demagnification (<FIG>), especially demonstrating the reciprocity of such passive confocal systems, whereas <FIG> being especially based on the system <NUM> of <FIG> exemplarily depicts an implementation <NUM> especially for increasing the effective area of a small CIS.

In the context of <FIG>, it is noted that the coupling structure converting 3D to 2D propagation might have to be modified especially in order to handle the proximity, and eventually bear-field mounting, of the CIS or the CIS chip, respectively.

It is further noted that each component of such optical systems in the sense of the invention can be made variable by, for example, introducing liquid crystal, electro-optic materials such as barium titanate (BTO), thermal tuning, geometrical variations such as micro-electro-mechanical systems (MEMS), etc. Tuning, for instance, the optical path distance between the respective coupling structures such as the coupling structures <NUM> and <NUM>, tunes the corresponding effective magnification factor.

Said tuning of the magnification factor may be implemented in camera objectives by mechanically moving lenses or lens groups, but in accordance with the invention, this can efficiently be done especially be vertically biasing the horizontal optical path. In this context, it is noted that only modifying one optical path may result in optical aberrations which should eventually be compensated by modifying various optical lengths and/or by tuning the focus strengths of the respective coupling structures.

Again, with respect to <FIG>, it is noted that for the implementation case of increasing the effective area of the CIS, pixel with super high full well capacity might be essential, while especially keeping the noise level low preferably to cope with increased illumination level. It is further noted that the foregoing explanations, especially regarding image sensor systems, can analogously be applied to projection systems and to alternative applications, wherein fixed or tunable magnifications are required.

With respect to <FIG>, the inventive tunable (de)magnification having already been described above, which is especially obtained through optical propagation path tuning, is illustrated. As it can be seen from <FIG>, the first coupling means of the inventive system is implemented in the form of a first varifocal lens <NUM> being especially embodied as a structure of the optical waveguide <NUM>. Furthermore, the second coupling means is implemented in the form of a second varifocal lens <NUM> being especially embodied as a structure of the optical waveguide <NUM>. Moreover, the respective optical length between said lenses <NUM> and <NUM> is preferably variable.

Now, with respect to <FIG>, an exemplary usage, especially in the form of a system <NUM>, of the invention in the context of an X-ray image sensor is depicted. Said system <NUM> comprises a scintillator <NUM>, an optical waveguide <NUM> (with coupling means) such as the waveguides <NUM>, <NUM>, <NUM> above, an optical sensor such as the optical sensor <NUM>, exemplarily a CIS or a CIS chip <NUM>, respectively, and a shielded box <NUM>.

It is particularly advantageous that the optical sensor can be fully protected with a shielding structure, exemplarily with the aid of the shielded box <NUM>, which makes the design of the optical sensor or the CIS chip <NUM>, respectively, significantly easier.

Further advantageously, the respective X-ray dose can be reduced while the corresponding signal-to-noise ratio is at least maintained or even increased, whereby low costs are ensured. In this context, the optical waveguide <NUM> preferably connects the scintillator <NUM> of the system <NUM> to the optical sensor or the CIS chip <NUM>, respectively.

<FIG> shows a further exemplary usage of the invention in the context of beyond magnification, which may preferably be employed for ultra compact form factor image handling such as a color direction from one RGB scene to three (or more) wavelength-dedicated imagers, or a multi-function system with 3D sent to an ID NIR imager and 2D high res sent to 2D imager, or a Fourier domain imaging in an equivalent 4F system.

Finally, <FIG> shows a flow chart of an embodiment of an optical method. In a first step <NUM>, incident light is coupled and/or focused to an optical waveguide with the aid of first coupling means having a first focal length and being optically connected to a first terminal of the optical waveguide. Then, in a second step <NUM>, light conveyed by the optical waveguide is emitted and/or collimated with the aid of second coupling means having a second focal length and being optically connected to a second terminal of the optical waveguide. In this context, the first coupling means and the second coupling means are confocal, wherein the second focal length is smaller than the first focal length. It is noted that such an optical method can also be called confocal method.

It might be particularly advantageous if the method further comprises the step of receiving the light emitted and/or collimated by the second coupling means with the aid of an optical sensor. In this context, the optical sensor may especially comprise or be a camera or an image sensor, preferably a complementary metal-oxide-semiconductor image sensor.

With respect to the first coupling means, it is noted that the first coupling means may especially comprise at least one of a lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof.

Additionally or alternatively, the second coupling means may especially comprise at least one of a lens, a grating structure, preferably a focusing grating coupler, a diffractive element, preferably a complex diffractive component, or any combination thereof.

With respect to the optical waveguide, it is noted that it might be particularly advantageous if the optical waveguide comprises or is a slab-waveguide.

It is further noted that it might be also particularly advantageous if at least one, preferably each, of the optical waveguide, the first coupling means, and the second coupling means comprises at least one of liquid crystal, an electro-optic material, preferably barium titanate, geometrical variations, preferably a micro-electro-mechanical system, or any combination thereof.

Moreover, the optical method or the confocal method, respectively, may further comprise the step of configuring at least one, preferably each, of the optical waveguide, the first coupling means, and the second coupling means to be thermally and/or electrically tunable.

In this context, it is noted that each of the above-mentioned liquid crystal, the electro-optic material, preferably barium titanate, the geometrical variations, preferably the micro-electro-mechanical system, may exemplarily allow for said tunability.

In addition to this or as an alternative, the method may comprise the step of adjusting or tuning at least one optical parameter of the optical waveguide and/or the first coupling means and/or the second coupling means, preferably of the optical waveguide especially at least in the region between the first coupling means and the second coupling means, with the aid of adjusting means.

With respect to the above-mentioned at least one optical parameter, it might be particularly advantageous if the at least one optical parameter comprises or is a refractive index. Moreover, with respect to the optical waveguide, the method may additionally or alternatively comprise the step of tuning an optical path distance between the first coupling means and the second coupling means especially in order to tune an effective magnification factor of the confocal system with the aid of the adjusting means.

In further addition to this or as a further alternative, with respect to the optical waveguide, the optical method may comprise the step of biasing an optical path between the first coupling means and the second coupling means in a biasing direction with the aid of the adjusting means.

In this context, it might be particularly advantageous if the optical path and the biasing direction enclose an angle between <NUM> and <NUM> degrees, preferably between <NUM> and <NUM> degrees, more preferably between <NUM> and <NUM> degrees, most preferably <NUM> degrees.

Furthermore, for biasing the optical path between the first coupling means and the second coupling means, the optical method may additionally or alternatively comprise the step of generating an electrical field especially being parallel to the biasing direction with the aid of the adjusting means.

With respect to the adjusting means, it is noted that it might be particularly advantageous if the adjusting means comprises or is a modulator and/or a capacitance.

Fundamentally, it is noted that it might be particularly advantageous if the optical method is used in the context of at least one of an imager application, a display application, an X-ray application such as the above-mentioned application <NUM> according to <FIG>, a beyond magnification application such as the application <NUM> described above according to <FIG>, or any combination thereof.

Furthermore, with respect to the above-mentioned display application, such a display application may exemplarily comprise an eye tracking sensor especially for an augmented reality and/or virtual reality application, preferably an augmented reality and/or virtual reality glass application.

While various embodiments of the present invention have been described above, it should be understood that they have been presented by way of example only, and not limitation. Numerous changes to the disclosed embodiments can be made in accordance with the disclosure herein without departing from the scope of the invention as specified in the appended claims. Thus, the breadth and scope of the present invention should not be limited by any of the above described embodiments. Rather, the scope of the invention should be defined in accordance with the following claims and their equivalents.

Claim 1:
An optical system (<NUM>) comprising:
an optical waveguide (<NUM>),
at least a first coupling means (<NUM>) having a first focal length (f<NUM>), and
at least a second coupling means (<NUM>) having a second focal length (f<NUM>),
wherein the first coupling means (<NUM>) is configured to couple and focus incident light (16a) to the optical waveguide (<NUM>),
wherein the second coupling means (<NUM>) is configured to emit and collimate light (16b) conveyed by the optical waveguide (<NUM>),
characterized in that
the at least first and second coupling means (<NUM>, <NUM>) have one confocal point being located at the first and second focal lengths within the optical waveguide (<NUM>).