The present invention relates in general to optical devices and manufacturing processes therefore, and in particular to synthetic-image devices and manufacturing methods therefore.
The field of synthetic images has developed fast during the last years. Synthetic-image devices are today used for creating eye-catching visual effects for many different purposes, e.g. as security markings, tamper indications or simply as aesthetic images. Usually, the synthetic-image device is intended to be provided as a label or as an integrated part in another device. Many different optical effects have been discovered and used and often different optical effects are combined to give a certain requested visual appearance.
A typical realization of a synthetic-image device is a thin polymer foil, where focusing elements and image objects are created in different planes. The typical approach for a synthetic-image device is to provide an array of small focusing element. The focusing element may be different kinds of lenses, apertures or reflectors. An image layer is provided with image objects. The image layer is provided relative to the array of focusing elements such that when the device is viewed from different angles, different parts of the image objects are enlarged by the focusing elements and together form an integral image. Depending on the design of the image objects, the synthetic image can change in different ways when the viewing conditions, e.g. viewing angles, are changed. The actual perception of the synthetic image is performed by the user's eyes and brain. The ability of the human brain to combine different part information into a totality converts the fragmented part images from the individual focusing elements into an understandable synthetic image. This ability to create an understandable totality can also be used for creating “surprising effect”, which can be used as eye-catching features or for security and/or authentication purposes. However, the manner in which the brain correlates different fragments may in some cases result in unexpected difficulties to create an understandable totality.
A general object with the herein presented technology is to improve the ability for interpretation of synthetic images.
The above object is achieved by methods and devices according to the independent claims. Preferred embodiments are defined in dependent claims.
In general words, in a first aspect, a synthetic-image device comprises an image layer and a focusing element array. The image layer is arranged in a vicinity of a focal distance of focusing elements of the focusing element array. The image layer comprises composite image objects. The composite image objects of said image layer being a conditional merging of at least a first set of image objects, an envelope area associated with said first set of image objects and a second set of image object. The first set of image objects is arranged for giving rise to at least a first synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array. Likewise, said second set of image objects is arranged for giving rise to at least a second synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array. The envelope area of the first set of image objects is an area covering the first set of image objects and further comprises a margin area not covering the first set of image objects. The conditional merging is constitute by that the composite image objects are present only in points where the first set of image objects exists or in points where the second set of image objects exists but the envelope area associated with the first set of image objects does not exist.
In a second aspect, a method for producing a synthetic-image device, comprises creation of a numerical representation of a first set of image objects. The first set of image objects is arranged for giving rise to at least a first synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through that focusing element array. A numerical representation of a second set of image objects is created. The second set of image objects is arranged for giving rise to at least a second synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through that focusing element array. A numerical representation of an envelope area is created. The envelope area is associated with the first set of image objects. The envelope area of the first set of image objects is an area covering the first set of image objects and further comprising a margin area not covering the first set of image objects. The numerical representation of the first set of image objects and the numerical representation of the envelope area associated with the first set of image objects is merged with the numerical representation of the second set of image object according to a predetermined condition into a numerical representation of composite image objects. The conditional merging is such that the composite image objects are present only in points where the first set of image objects exists or in points where the second set of image objects exists but the envelope area associated with the first set of image objects does not exist. An image layer is formed according to the numerical representation of composite image objects. A focusing element array is formed. The image layer is arranged in a vicinity of a focal distance of focusing elements of the focusing element array.
One advantage with the proposed technology is that synthetic images are provided, which are experienced by the human eye in a clear and distinctive manner. Other advantages will be appreciated when reading the detailed description.
The invention, together with further objects and advantages thereof, may best be understood by making reference to the following description taken together with the accompanying drawings, in which:
Throughout the drawings, the same reference numbers are used for similar or corresponding elements.
For a better understanding of the proposed technology, it may be useful to begin with a brief overview of synthetic-image devices.
The synthetic-image device 1 further comprises an image layer 10 comprising image objects 12. The image objects 12 are objects that are optically distinguishable from parts 14 of the image layer 10 that are not covered by image objects 12. The image objects 12 may e.g. be constituted by printed product micro features 11 and/or embossed microstructures. The image layer is arranged in a vicinity of a focal distance d of the focusing elements 22 of the focusing element array 20. This means that a parallel beam 6 of light impinging on a focusing element 22 will be refracted 5 and focused at one point or small area 4 at the image layer 10. Likewise, light emanating from one point at the image layer 10 will give rise to a parallel beam 6 of light when passing the focusing elements 22. A point at an image object 12 will therefore appear to fill the entire surface of the focusing element 22 when viewed from a distance in the direction of the produced parallel beam 6 by a viewer, schematically illustrated by the eye 2. The material 9 between the image layer and the focusing element array 20 is at least partly transparent and is typically constituted by a thin polymer foil.
The distance d does not have to be exactly equal to the focusing distance of the focusing elements 22. First, there is always a certain degree of aberrations, which anyway broadens the area from which the optical information in a parallel beam 6 is collected. This appears more at shallower angles and in order to have a more even general resolution level, a distance in a vicinity, but not exactly equal to the focal distance may be beneficially selected. Furthermore, since the focusing element surface has a certain two-dimensional extension, also this surface could be used to produce fine objects of the total synthetic image. In such cases, fine objects of a small area on the image layer 10 may be beneficial to enlarge to cover the surface of the focusing element, which means that also in such a case, the actual selected distance d is selected to be in a vicinity, but not exactly equal to the focal distance. Such circumstances are well known in the art of synthetic images.
By arranging the image objects 12 of the image layer 10 in a suitable manner, the part images produced at each individual focusing element 22 surface will collectively be perceived by a viewer 2 as a synthetic image. Different images may be displayed for the viewer when the synthetic-image device 1 is viewed in different directions, which opens up for creating different kinds of optical effects, as will be described further below.
When viewing the synthetic-image device 1 at another angle, as e.g. illustrated in the right part of the figure, the area 4 on which the focusing element 22 focuses is shifted at the side. In the illustrated situation, the area 4 overlaps with at least a part of an image object 12 and an enlarged version can be seen at the surface of the synthetic-image device 1. In this way, the images presented at the surface of the synthetic-image device 1 may change for different viewing angles, which can be used for achieving different kinds of optical effects of the synthetic images.
One type of synthetic image is a so-called moiré image. The moiré effect is well known since many years and is based on the cooperation of two slightly mismatching arrays.
An area 4 is also marked, which corresponds to the focusing area of each focusing element 22. In the illustrated case, the area 4 corresponds to a view direction straight from the front. The parts of the image objects 12 that are present within each of the areas 4 will thereby be presented in an enlarged version over the surface of the corresponding focusing element 22, here denoted as a projected image 25. In the lower part of
The viewer will interpret such a motion as a result of a position of the large “K” at a certain imaginary depth below the surface of the synthetic-image device 1. In other words, a depth feeling is achieved. Both the magnification and the experienced depth depends on the relation between the focusing element array 20 and the repetitive pattern 15 of image objects 12. It has in prior art been shown that the obtained magnification M is determined as:
where Po is the period of the repetitive pattern 15 of image objects 12 and Pl is the period of the focusing element array 20. For Po<Pl, the magnification is positive, for Po>Pl, the magnification becomes negative, i.e. the synthetic image 100 becomes inverted compared to the image objects 12.
The apparent image depth di of the moiré image can also be determined as:
d
i=(d−Rl)/(1−F)+Rl (2)
where d is the thickness of the synthetic-image device and Rl is the radius of the curvature of the spherical microlenses. One can here notice that for Po<Pl, the apparent depth is typically positive, while for Po>Pl, the apparent depth becomes negative, i.e. the moiré image 105 seems to float above the surface of the synthetic-image device 1.
It should be noted that the differences in periods illustrated in
The moiré images have, however, certain limitations. First of all, they can only result in repetitive images. Furthermore, the size of the image objects 12 is limited to the size of the focusing elements. In
A solution is presented in
As long as the focusing area of the associated focusing element is kept within the cell 16 a synthetic image similar to a moiré image will be produced. However, when the focusing area of the associated focusing element enters into a neighbouring cell 16, the synthetic image will suddenly disappear and will instead appear at another position; a flip in the synthetic image occurs.
Such flipping effects may be somewhat extenuated by introducing an image object-free zone between each cell at the image layer.
The ideas of having cells with different image objects can be driven further. The moiré synthetic images can be given an apparent depth, but is in principle restricted to one depth only. A true three-dimensional appearance is difficult to achieve. However, when considering integral synthetic images, the freedom of changing the image objects from one cell to another can also be used e.g. to provide a more realistic three-dimensionality of the produced images.
In
In a similar fashion, by modifying the image content in each cell separately, different kinds of optical phenomena can be achieved. By adapting each part of the cell according to the requested image appearance in a corresponding viewing direction, the integral synthetic image can be caused to have almost any appearances. The so achieved image properties can be simulations of “real” optical properties, e.g. a true three-dimensional image, but the image properties may also show optical effects which are not present in “real” systems.
An example of a part of an image layer 10 of an integral synthetic-image device giving rise to an image of the figure “5” is illustrated in
One effect that is possible to achieve by both moiré synthetic images and integral synthetic images is that two synthetic images can be imaged at the same time. These synthetic images may have different apparent depth or height. When tiling such an optical device, the two synthetic images moves relative each according to the ordinary parallax effect. In certain viewing angles, the synthetic images may come in line of sight of each other, i.e. one object covers at least a part of the other object.
When preparing the image layer for such a synthetic optical device, different principles can be followed. If e.g. the different synthetic images are created by image objects in different colours, a simple overlay of the two image objects results in that both synthetic images are visible, but with a mix of the colours. An impression of a partially transparent front synthetic image becomes the result. However, if the front synthetic image is to be perceived as a non-transparent object, an overlap between the synthetic images should give an impression of that the back synthetic image disappear behind the front synthetic image. Thus, the image object associated with the back synthetic image has to be modified.
Note that, typically, there are no image layers produced with the separate image objects 31 and 32 of the left and middle cells. They are presented here only for simplify the discussion. Typically, an image layer with the composite image object 33 is created directly.
When viewing the synthetic-image device from a direction close to the normal direction of the synthetic-image device, the first synthetic image comes in front of the second synthetic image. If both the synthetic images are based on a same or at least similar colour, it becomes difficult for the viewer to distinguish which part belongs to which object. The correlation made by the human brain between the part images provided by each focusing element is not totally obvious. The result may be that the viewer experiences a blurred image or that the depth feeling, at least partly, disappears. In particular in cases where narrow structures, as the tongues of the first set 31 of image objects, are involved, the composite image often becomes deteriorated.
In one embodiment, a synthetic-image device, comprises an image layer and a focusing element array. The image layer is, as was described earlier, arranged in a vicinity of a focal distance of focusing elements of the focusing element array. The image layer comprises composite image objects. These composite image objects of the image layer array are a conditional merging of at least a first set of image objects, an envelope area associated with the first set of image objects and a second set of image objects. The first set of image objects is arranged for giving rise to at least a first synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array. Likewise, the second set of image objects is arranged for giving rise to at least a second synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array. The envelope area of the first set of image objects is an area covering the first set of image objects and further comprises a margin area not covering the first set of image objects. The conditional merging being that the composite image objects are present only in points where the first set of image objects exists or in points where the second set of image objects exists but the envelope area associated with the first set of image objects does not exist.
The idea is to introduce a margin when deciding which parts of the first set of image objects that are going to be cut away. Instead of only cutting such parts that are directly overlapping, also some parts outside the first set of image objects may be removed. The envelope area thereby operates as a mask to decide which parts of the first set of image objects that are to be removed.
In
By combining the first set 31 of image objects with a second set 32 of image objects, in this particular embodiment similar to the second set 32 of image objects of
When such composite image objects 36 are created for a portion of the image layer, the synthetic-image device gives rise to a combined synthetic image composed by the first synthetic image based on the first set of image objects and the second synthetic image based on the second set of image objects. When the parallax effect brings the first synthetic image to cover at least a part of the second synthetic image, the use of the envelope area 35 as a masking facilitates the interpretation made by the human brain about which parts that belongs to which structure. A more clear combined synthetic image is thus produced.
The width of the narrow rim 34A is selected to be large enough to assist the eye to separate the different synthetic images. At the same time, it is preferred that the narrow rim 34A is narrow enough not to constitute a synthetic image at its own. The actual sizes depends on different parameters, such as magnification, focusing element aberration, focusing element strength etc. and could be adapted for different applications. Anyone skilled in the art knows how large a feature in the image objects has to be to be seen and how small a feature in the image objects has to be not to be seen. If there are doubts, a simple test with a range of different margins areas can be performed and a preferred size can be determined by just observing the produced synthetic images. Such tests of different design features are commonly used in the art. In a particular embodiment, an average width of objects of the margin area is within the range of 0.1% to 10% of a diameter of the focusing elements.
Each of the first synthetic image and the second synthetic image can be a moiré image or an integral synthetic image.
In a particular embodiment, at least one of the first synthetic image and the second synthetic image is an integral synthetic image. In a further particular embodiment, the first synthetic image is an integral synthetic image. In yet a further particular embodiment, both the first synthetic image and the second synthetic image are integral synthetic images.
In
However, also sets of image objects giving rise to moiré images can be used for creating the composite image objects. In a particular embodiment, at least one of the first synthetic image and the second synthetic image is a moiré image. In a further particular embodiment, the second synthetic image is a moiré image. In yet a further particular embodiment, both the first synthetic image and the second synthetic image are moiré images.
When using a first set 31 of image objects intended to give rise to an integral synthetic image as first synthetic image, the image objects of the first set 31 of image objects are limited to a certain area of cell 16. The second set of image objects can be intended to give rise to a moiré image, and its image objects are therefore not limited by the area of the cell 16 of the first set 31 of image objects. Likewise, if the second set of image objects is intended to give rise to an integral synthetic image but with a different cell size and/or cell geometry, the image objects of the second set of image objects may be controlled to appear in other areas.
It has been found that since the first synthetic image, if being an integral synthetic image, disappears when the viewing direction moves the projected area over the border of the associated cell, the sensitivity for misinterpretation of different synthetic images more or less vanishes. It is therefore not of interest to add any margin area in such a case, or at least not a too wide margin area. This situation can be illustrated by
In other words, the first set of image objects 31 are provided within a set of first cells 16, wherein each said first cell 16 is associated with a respective focusing element of the focusing element array. The margin area 34 encloses edges of first images objects not coinciding with borders of the first cells.
The above described combining can be understood as a masking or cutting of the second set of image objects. These principles can be extrapolated also to additional sets of image objects. A first set of image objects and its associated envelope area may thereby mask or cut more than one other set of image objects.
In an alternative view, the second set of image objects may be considered as a combined set of image objects, composed by two or more sets of image objects. Such a composed set of image objects may itself comprise a cutting or masking by use of envelope areas.
In other words, several different part images can be produced, which are provided at different heights/depths and which at certain angles may cover each other in different relations. Margin areas may then be used in the different images to increase the viewability at such covering relationships.
The effects above are achieved by applying logics between different “layers” of image objects. Conditional merging of sets of image objects into composite image objects may also be performed in other ways.
The result is that when the first synthetic image and the second synthetic image overlap, both images disappear leaving an “empty” space. Such an optical effect does not directly correspond to a traditional three-dimensional physical behaviour, but gives still information of the existence of overlap regions that is relatively easy to understand and interpret.
Another example of such an exclusive “OR” conditional merging is illustrated in
In further other embodiments, exclusive “OR” conditional merging between one set of image objects associated with a moiré image and one set of image objects associated with an integral synthetic image can be used.
Composite image objects associated with different sets of image objects can be configured in many other configurations. One approach is to let an appearance of a first set of image objects be dependent on any existence of a second set of image objects at the same position.
This gives rise to an eclipse-like behaviour. In
The second set of image objects 32 does never give rise to any directly perceivable synthetic image 120. However, since the second set of image objects 32 is used as a condition for the appearance of the first synthetic image, parts of the shape of the intended synthetic image associated with the second set of image objects 32 may be seen as the borders of the appearing eclipses.
Also other conditional rules can be applied.
This gives rise to a developer-like behaviour. In
The first set of image objects 31 does never give rise to any directly perceivable synthetic image 120 if not overlapping with the second set of image objects 32. Likewise, the second set of image objects 32 does never give rise to any directly perceivable synthetic image 120 if not overlapping with the first set of image objects 31. One of the sets of image objects is thus needed to “develop” the other set of image objects.
In one embodiment, a synthetic-image device comprises an image layer and a focusing element array. The image layer is arranged in a vicinity of a focal distance of focusing elements of the focusing element array. The image layer comprises composite image objects. The composite image objects of the image layer array are a conditional appearance of a first set of image objects dependent on a second set of image objects. The first set of image objects gives rise to a first synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array. Likewise, the second set of image objects gives rise to a second synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array.
In a particular further embodiment, the composite image objects of the image layer array are a conditional merging of at least the first set of image objects and the second set of image objects. The conditional merging is that the composite image objects are present only in points where the first set of image objects exists but the second set of image objects does not exist and/or the composite image objects are present only in points where both the first set of image objects and the second set of image objects exist.
In a particular further embodiment, the conditional merging is that the composite image objects are present only in points where the first set of image objects exists but the second set of image objects does not exist.
In another particular further embodiment, the conditional merging is that the composite image objects are present only in points where both the first set of image objects and the second set of image objects exist.
In
In an alternative interpretation of the synthetic-image device 1 of
The different embodiments and examples of applying logics between different “layers” of image objects can be combined in different configurations. For instance, if three sets of image layers are considered to be combined, a first kind of logics can be applied between two of the layers, whereas a different kind of logics can be applied relative the third image layer. The person skilled in the art realizes that the different embodiments and examples can be combined in any configurations and numbers.
As mentioned above, using one or more integral synthetic images, different kinds of optical effects can be achieved, both effects that resembles optical effects of the three-dimensional physical world and effects that behaves in “strange” manners.
In one embodiment at least one of the first synthetic image and the second synthetic image is a three-dimensional image. This gives the possibility to combine typical three-dimensional view effects with parallax-caused effects.
In a moiré image, the magnification depends on the relation between the periodicity of the focusing elements and the periodicity of the image objects. A small difference gives rise to a high magnification. Thus, when the difference comes extremely close to zero, i.e. when the ratio of periodicities becomes very close to 1, the magnification approaches infinity. This means at the same time that the synthetic image no longer is perceivable by a viewer, since the same optical information is presented by each of the focusing elements. However, such types of synthetic images, of moiré image type or integral synthetic image type, may anyway be useful. By watching or registering the synthetic-image device from a very small distance, the viewing angles becomes slightly different for the different focusing elements, and the “infinite” magnification becomes revoked. This can easily be utilized e.g. for security markings. Such synthetic images may also advantageously be used in combination with the above described composite image object aspects.
In one embodiment, the first set of image objects gives rise to the first synthetic image when viewed through said focusing element array from a distance less than 15 cm and/or the second set of image objects giving rise to the second synthetic image when viewed through the focusing element array from the distance less than 15 cm.
Another design alternative is to create a synthetic image with an infinite magnification in one direction, but a finite magnification in a perpendicular direction. Also such a synthetic image will be un-perceivable when presented for a viewer in a flat form. However, by bending the synthetic-image device around an axis transversal to the axis of the infinite magnification, the relations between the periods of the focusing elements and the periods of the image objects change, giving rise to a finite magnification in both directions. The synthetic image then becomes perceivable.
In one embodiment, the first set of image objects gives rise to the first synthetic image when viewed through a bent focusing element array and/or the second set of image objects giving rise to the second synthetic image when viewed through a bent focusing element array.
This effect can be achieved by moiré images, where the pitch of the repeated image objects is modified. However, integral synthetic images may also be designed to give a similar effect.
The combination of sets of image objects can be developed further by using additional sets of image objects on which composite image objects are dependent. The additional sets of image objects may overlap with the first and/or second sets of image objects, and all sets of image objects may then be involved in the conditional merging in at least some areas of the image layer. The additional sets of image objects may in other alternatives only be provided as non-overlapping with the first and/or second sets of image objects and the conditional merging may then be different for different part areas of the image layer.
In one embodiment, composite image objects of the image layer array is further dependent on at least one additional set of image objects. This additional set of image object gives rise to an additional synthetic image when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array.
In
As anyone skilled in the art understands, combinations of different sets of image objects can be performed in almost unlimited number of variations. It becomes possible to give properties to dynamic surfaces of synthetic images.
When producing synthetic image devices according the above described ideas, the actual combination of the different sets of image objects is preferable made before the image layer is created. In other words, instead of modifying physical sets of image objects, numerical representations of the sets of image objects are instead created. In the case an envelope area is used for creating the composite image objects, also this is expressed by a numerical representation. The combination into a composite image object is then performed on these numerical representations. When a numerical representation of final composite image objects is achieved, the image layer is created according to that numerical representation. The transfer of the numerical representation into a physical image layer is performed according to well-known manufacturing principles, using e.g. different kinds of printing or embossing.
The steps 240 and 250 can be performed in either order or at least partially simultaneously.
The steps 240 and 250 can be performed in either order or at least partially simultaneously.
In the embodiments of methods for producing a synthetic-image device ion the present disclosure, numerical representations of sets of image objects are created. This is, as such, well-known in prior art, and will just be described briefly here below.
In a first approach of numerical representations, the numerical representations of the image objects are vector representations of areas. The objects are described by polygons which can be rendered smoothly at any desired display size. However, the polygons smoothness is generally adjusted to match the resolution of step 240, in order to avoid too large amount of data. This kind of representations of areas is well-known e.g. in the fields of mechanical design or integrated circuit design.
In another approach, of numerical representations, the numerical representations of the image objects are pixel-based. The total area is then divided into a number of pixels. Each pixel is then defined as either belonging to the image object or belonging to a surrounding. The different logic operations are in such an approach performed essentially pixel by pixel.
Also other types of numerical representations may be used.
In a particular embodiment, the merging 231 is that the composite image objects are present only in points where the first set of image objects exists but the second set of image objects does not exist and/or the composite image objects are present only in points where both the first set of image objects and the second set of image objects exist.
In the examples and embodiments above, cells used for integral synthetic images have been illustrated as regular hexagonal cells.
The cells may also be smaller than the maximum allowed size, e.g. for making image flips less pronounced, as discussed further above. However, the density of the cells 16 equals the density of focusing element 22. In other words, each cell 16 can be associated to a unique focusing element 22.
However, other configurations of cells are also possible and, depending on the application, may even be preferred.
This shape of the cells 16 may be preferred in different applications. In the illustrated case, the cells 16 comprise image objects 12 creating a phrase “PHRASE” in each cell 16. The length of the phrase is larger than the focusing element diameter and in order not to induce any flip of the integral synthetic image when a viewer tries to read the entire phrase, the dimension of the cell 16 in the direction of the phrase is allowed to be larger than the diameter of the focusing element 22. Instead, the cell 16 is made narrower in a perpendicular direction. This means that the synthetic-image device 1 can be tilted to a larger angle in the horizontal direction, as illustrated, than in the vertical direction, without causing any flip of the integral synthetic image. If the integral synthetic image, as in this case, is a text, flips in the horizontal direction, i.e. the reading direction, is generally more disturbing than a flip in the vertical direction. The selection of the geometry and size of the cell 16 solves such problems.
Another use of extending the cell range may be in connection with lenses with high F numbers. In such applications, the angle necessary for reaching the border of a hexagonal cell is then relatively low, and flips between integral synthetic images therefore occurs more frequently when tilting such devices. However, these effects can be mitigated in one direction by instead extend the cell in that direction. The disadvantage is, however, that the angle range before a flip occurs in a transverse direction becomes smaller.
Further examples of cell shapes are illustrated schematically in
In real synthetic-image devices, the focussing elements typically present different kinds of optical aberrations. This means that the focusing that is achieved is not totally perfect. Also some light emanating from areas slightly outside the intended area, for a certain viewing direction, is thereby refracted by the focussing elements in that viewing direction. The result is a diffuse shadowing in the colour of the object to be seen. The shape of this shadowing depends on both the shape of the object intended to be imaged and the shape of the cell, and is in principle some sort of convolution of the shapes.
In some applications, the appearance of such a shadow may be disturbing. This may be even more accentuated if the shadow presents distinct geometrical features, e.g. caused by a cell having such distinct geometrical features. In such cases, it is might be wise to select a cell that has a relatively neutral shape. Circular cells 16, such as illustrated in
The shadowing effect also depends on the magnification of the synthetic-image device.
For applications where the shadowing is unwanted, neutral cell shapes as well as lower magnification factors are to prefer.
However, such shadowing effects may also be utilized on purpose. In
In one embodiment, a synthetic-image device comprises a focusing element array and an image layer. The focusing element array is a two-dimensional periodic array having a geometrical symmetry. The image layer is arranged in a vicinity of a focal distance of focusing elements of the focusing element array. The image layer has sets of image objects arranged in cells of a cell array, wherein each cell is associated with a respective one of the focusing elements. The set of image objects is arranged for giving rise to at least a first synthetic image when being placed in a vicinity of a focal distance of the focusing elements and viewed through the focusing element array. Each of the cells has a shape with a geometrical symmetry that is different from the geometrical symmetry of the two-dimensional periodic array.
In a particular embodiment, the area of the cells is less than the area of the focusing element array divided by the number of focusing elements of the focusing element array.
In a particular embodiment, the focusing element array has a hexagonal geometrical symmetry.
Despite the flow character of
In many applications, repetitive patterns are requested. The moiré images are always of this kind, but also integral synthetic images may be designed to give a repetitive pattern. The most common type of focusing element array is a regular hexagonal array. This means that the achieved synthetic image in most cases also presents a regular hexagonal patterns repetition.
When designing integral-image devices, pattern size, magnification, apparent depth/height etc. can be selected according to what is most appropriate for each application. In certain applications based on repetitive patterns, it might even be of interest to provide more than one item associated with each focusing element. This may e.g. be useful if a small apparent image size and a large apparent depth are requested at the same time.
In
In
It may be noted that if the part image objects 12A-C are perfectly aligned to each other over the entire device, some of the depth feeling may be difficult to achieve. This may be dependent on that the eye becomes confused by competitive image object parts and thereby cannot obtain an apparent depth correctly. However, such artifacts may easily be corrected for by on purpose misalign the part image objects 12A-C a very small distance, typically less than 1% of the cell diameter. The eye will now be assisted in the correct correlation at the same time as the parts of the synthetic image are displaced such a small distance that the misalignment is not perceived.
In
In
In the applications where different magnifications are used in different directions, the icons can be stretched or compressed in one direction to get the right icon shape when applying different magnification horizontally and vertically.
Other alternatives are also possible. Table 1 summarizes some different combinations of multiple objects per cell with different horizontal and vertical magnifications to achieve different packings. The magnification ratio is given as the magnification in a direction parallel to a closed-packed direction of the hexagonal focusing element array divided by the magnification in a direction perpendicular to the closed-packed direction of the hexagonal focusing element array.
Similar possibilities of combining multiple objects and packing geometries are of course possible with other geometrical symmetries of the focusing element array, e.g. a square symmetry or a rectangular symmetry.
In one embodiment, a synthetic-image device comprises a focusing element array and an image layer. The focusing element array is a two-dimensional periodic array having a geometrical symmetry. The image layer is arranged in a vicinity of a focal distance of focusing elements of the focusing element array. The image layer has sets of image objects arranged in cells of a cell array, wherein each cell is associated with a respective one of the focusing elements. The set of image objects is arranged for giving rise to at least a first synthetic image when being placed in a vicinity of a focal distance of the focusing elements and viewed through the focusing element array. The image objects being arranged to present different magnifications in two perpendicular directions within the plane of the synthetic-image device.
In a particular embodiment, each of the cells has a shape with a geometrical symmetry that is different from the geometrical symmetry of the two-dimensional periodic array.
In a particular embodiment, the image objects of each cell comprises at least two displaced copies of a set of image objects.
In a particular embodiment, the focusing element array has a hexagonal geometrical symmetry.
Despite the flow character of
In one embodiment, a synthetic-image device comprises a focusing element array and an image layer. The image layer is arranged in a vicinity of a focal distance of focusing elements of the focusing element array. The image layer comprises composite image objects. The composite image objects of the image layer array are a conditional appearance of a first set of image objects dependent on a second set of image objects. The first set of image objects gives rise to a first synthetic image at a non-zero height or depth when being placed in a vicinity of a focal distance of focusing elements and viewed through the focusing element array. The second set of image objects is arranged at a same periodicity as the focusing elements of the focusing element array.
The different configurations of cells and image objects as presented above can be applied as such in synthetic-image devices. However, the different configurations can also by advantage be combined with e.g. the application of logics between different “layers” of image objects. The different aspects can thereby be combined depending on the nature of the synthetic image that is intended to be presented.
As mentioned further above, viewing a synthetic-image device from a close distance may change the perceived image. It is also possible to achieve a related effect by instead providing a light source positioned at a very short distance from the synthetic-image device.
A point light source 50, or at least a light source emitting essentially diverging rays, is then placed on a distance d from a synthetic-image device 1. Note that some dimensions in the figure are extremely exaggerated in order to better visualize the optical effects. The light impinging at a right angle on the synthetic-image device 1, as illustrated in the middle of the figure, is refracted into one focus spot positioned at the image object 12. That spot on the image object 12 therefore becomes intensively illuminated. Light emitted from this spot will be emitted in all directions. A main part of that re-emitted light will reach the lenses 24 at the lens straight above the emitting spot. Some of this light will be scattered and the lens surface 52 will be experienced as having the same colour as the image object 12.
When considering lenses 24 that are not situated directly beneath the point light source 50, the impinging angle α is different. This means that the spot at which the light is focused will be displaced somewhat sideward. This is seen at the lenses at the sides of the figure. The focus spot here is positioned outside the image object 12 and no, or at least much less, light will be re-emitted. Consequently, the surface of the associated lens is not experienced as coloured.
The total effect will be that a synthetic image will be experienced by a viewer. This synthetic image corresponds essentially to a synthetic image created by an image layer having the image object periodicity of Po, but with a lens array with a larger efficient periodicity Pleff. By simple geometrical considerations, it can be concluded that the efficient lens periodicity becomes:
From this, it can be concluded that the effect will only be noticeable when the distance between the light source and the synthetic-image device is not too large compared to the lens radius and device thickness.
For typical dimensions of lens radii in common types of synthetic-image devices the distance between the light source emitting divergent rays and the surface of the synthetic-image devices is preferably less than 10 cm, more preferably less than 5 cm and most preferably less than 3 cm.
As a non-exclusive example to illustrate the order of magnitudes of the changes in effective lens periods; assume a 70 μm thick synthetic-image device having a lens radius of 45 μm. By placing a point light source at a distance of 5 cm from the surface, would give an efficient lens period that is 0.05% larger than the physical one. If the image object period and the physical lens period are the same, such a change in efficient lens period would give rise to a magnified image with a magnification of 2 000. An image object of a real size of 10 μm would thus appear as a synthetic image of a size of 20 mm. The impression that the image is provided at a certain depth is however, not present.
It should be noted that some of the re-emitted light from the image objects 12 that are hit by the focus points also are spread to the neighbouring lenses, which means that lenses that covers focus spots that do not re-emit any light anyway may be slightly illuminated by its neighbours. However, this effect is rapidly reduced with increasing angle. The overall result is that the experienced synthetic image will be slightly blurred.
In the examples above, a synthetic-image device based on lenses has been discussed. However, corresponding behaviour is also present in e.g. synthetic-image device based on concave mirrors.
The irradiating described above is performed from the front side of the synthetic-image device, i.e. from the side where a synthetic image is supposed to be seen.
However, by selecting other relations between Pl and Po, other effects can be achieved. By having a Pl just slightly larger than Po will give a synthetic image having a large magnification. By irradiating the synthetic-image device by a point light source from a short distance, an additional synthetic image, congruent with the original one, will appear without depth and with a smaller magnification. By instead having Pl just slightly smaller than Po will give a synthetic image having a large magnification but with an apparent height above the surface of the device. By irradiating the synthetic-image device by a point light source from a short distance, an additional synthetic image, congruent with the original one, will, when the distance is short enough, appear without depth and with a mirror magnification.
This effect can be utilized as an authentication or safety marking. One embodiment of a method for authentication of a synthetic-image device and thereby an item on which synthetic-image device may be attached can be described by the following. The synthetic-image device comprises a focusing element array and an image layer. The image layer is arranged in a vicinity of a focal distance of focusing elements of the focusing element array. The image layer comprises image objects. The method comprises illumination of the synthetic-image device by a light source emitting divergent rays, e.g. a point light source. The illumination is performed from a short distance. The short distance is preferably less than 10 cm, more preferably less than 5 cm and most preferably less than 3 cm. During that illumination, any appearance of a synthetic image not being present without the illumination, is observed as sign of authenticity.
In one further embodiment, the image objects are arranged not to give any perceivable synthetic image when not being illuminated by the point light source. The image objects are thus arranged to give an apparent infinite magnification.
In another further embodiment, the image objects are arranged to give a perceivable synthetic image also when not being illuminated by the point light source. When the point light source is caused to illuminate the synthetic-image device, another copy of that synthetic image appears.
The examples of
The embodiments described above are to be understood as a few illustrative examples of the present invention. It will be understood by those skilled in the art that various modifications, combinations and changes may be made to the embodiments without departing from the scope of the present invention. In particular, different part solutions in the different embodiments can be combined in other configurations, where technically possible. The scope of the present invention is, however, defined by the appended claims.
Number | Date | Country | Kind |
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1650830-1 | Jun 2016 | SE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/SE2017/050598 | 6/7/2017 | WO | 00 |