Field of the art

The invention relates to a method of exposing light-sen¬ sitive materials as stated in the introductory portion of claim 1, and to an apparatus for performing the method as stated in the introductory portion of claim 15.

EP Patent Specification No. 0 572 507 discloses a laser scanner of the so-called internal drum type, wherein a film is exposed in an internal chamber, an optical rotat¬ ing element in the form of e.g. a mirror being moved per- pendicularly to the rotary movement across the film, thereby exposing the desired area of the film. This scan¬ ner type is capable of exposing films at a relatively great rate with a good quality.

However, it is difficult to increase the exposure or scanning rate additionally by the prior art, as, for many scanners, the necessary mechanical movement has been in¬ creased almost to the maximum point, which means that even comprehensive mechanical measures only result in small improvements in the scanning technique and the rate at which the scanning takes place.

The object of the invention is to provide a significant increase in the scanning rate in an image setter of the internal drum type.

Summary of the invention

When, as stated in claim 1, at least one additional light source generates an additional light beam with a wave¬ length λ _x which is different from λ _: , said additional

light beam with the wavelength λ _x being conducted via the input end of the optical system to the output end of the optical system so as to be geometrically coincident with the first light beam at the output end of the optical system, said additional light beam being conducted from there to an additional exposure point on the light-sensi¬ tive material inside the drum of the image setter in de¬ pendence on λ _x or the mutual difference between the wave¬ lengths Δλ, it is possible to optimize the exposure rate, as the necessary mechanical rotary movement may be re¬ duced to a minimum. It should moreover be noted that the method may be adapted to the nature and the rate of the mutual movement in a simple manner, thereby allowing the method to be performed on the same apparatus with a dif- ferent resolution, as the distance between the first ex¬ posure point and the additional exposure point or points may be adjusted e.g. by changing the wavelengths of the light sources. The method is thus extremely flexible and may be adapted for many applications without complicated mechanical or electronic measures.

Thus, the invention provides a greatly improved exposure rate by means which can actually be implemented under special physical conditions that apply to an internal drum scanner. Thus, according to the invention, it is possible to minimize the space occupied by the rotating mechanical system.

In this connection it is worth noting that the invention may thus be adapted to existing internal drum scanners without considerable constructional changes.

It will likewise be appreciated that, according to the invention, the precision may be maintained even at very high speeds of rotation.

Thus, by mixing the various light beams with correspond ^¬ ingly different wavelengths so that these are fed geomet ^¬ rically coincidently from the output end of the optical system, it is possible to carry out a relatively uniform and simple optical control via the rotating reflector to the exposure face.

Thus, by avoiding a spatial separation between the beams at the output end of the optical system, it is possible, in a simple manner, to avoid the complicated geometrical relations that exist between the output end and the axi¬ ally rotating reflector or mirror, thereby avoiding e.g. twisting on the exposure face in a simple manner.

The invention thus allows all light beams to be centered on the rotating reflector, thereby obtaining rotary sym¬ metry for the beams which are subsequently reflected by the exposure face, irrespective of the position of the reflector or the mirror in the path of rotation.

From two to several light sources may be used according to the invention.

The light sources used may be both of the same type or of different types.

The optical system comprises the necessary optical fea¬ tures to conduct light from source to exposure point. If the light sources are not modulated directly, the optical system may also comprise optical modulators.

According to the invention, a reflector is taken to mean e.g. a mirror, a pentaprism, or optical elements having a sufficiently deflecting effect.

When, as stated in claim 2, the light is conducted com¬ pletely or partly from the input end of the optical sys¬ tem via one or more light guides, preferably optical fibres, to the output end of the optical system, it is possible to conduct the light to the exposure points via a compact optical arrangement, as the optical system is hereby well-defined and easy to calibrate.

The use of optical fibres in this connection provides an additional advantage, as the spatial distribution of the complete light beam is improved considerably, since the light from the various light sources is coincident if the light from all light sources is conducted precisely to one optical fibre.

An additional advantage obtained by using optical fibres in this connection is that the precision is improved con¬ siderably, considering that the optical reflector per¬ forms very fast revolutions with consequent turbulent flows in the exposure chamber of the scanner. The use of optical fibres minimizes the optical temperature-sensi¬ tive distance, which is particularly important when using multi-beams whose mutual focusing distance on the expo¬ sure face is affected critically by temperature gradi- ents.

When, as stated in claim 3, the light is conducted from the individual light sources to a common optical fibre in the optical system via one or more couplers, a particu- larly advantageous structure of the optical system may be obtained, as an optical coupler causes relatively low op¬ tical losses in the mixing of two or more light waves from two or more optical fibres to one optical fibre.

Thus, in several applications, an optical T-coupler will exhibit very low optical losses in the actual mixing.

It should be mentioned that within the scope of the in ^¬ vention there are other possibilities of geometrically mixing light beams having several different wavelengths to a combined light beam which contains all these wave- lengths.

For example, it may be mentioned that a beam splitter may advantageously be used in several application types using linearly polarized light, as, in many cases, a beam splitter can better maintain the polarization than an op¬ tical coupler.

When, as stated in claim 4, the light is conducted from the individual light source to an exposure point via the optical system, an optical element with wavelength-split¬ ting properties reflecting or transmitting the light to the exposure point in dependence on the wavelength of the light, an advantageous and preferred embodiment of the invention is obtained, as the combined light signal may be split in a simple manner into a plurality of differ¬ ently oriented modulated light signals corresponding to the plurality of light sources with different wave¬ lengths, thereby providing a corresponding plurality of exposure points on the light-sensitive material. The op- tical element used may e.g. be produced holographically or lithographically according to the intended purpose. An element having wavelength-splitting properties may e.g. be a dispersive prism, a diffractive grating, a multi¬ layer beam splitter, a hologram, etc.

The optical element may thus be a mirror having an inte¬ grated optical grating or a grating which transmits the incident light to the exposure points.

It is thus possible to increase the exposure rate in in¬ ternal drum scanners considerably. As the requirements

with respect to the structure of the inner mechanical parts and the system as a whole are very critical for internal drum scanners, the invention is particularly advantageous in this connection, since the invention thus enables a very compact structure of the carriage of the scanner.

When, as stated in claim 5, the light beams are separated by means of a grating arranged at the output end of the optical system, thereby making the angle of incidence of the light to the rotating optical reflector and thus ex¬ posure point in the inner exposure chamber dependent on the wavelength of the incident light, an alternative em¬ bodiment of the invention is obtained, said embodiment being less exacting with respect to the dimensioning of the optical element.

When using a transmitting grating in this way a possibility of directing the grating perpendicularly to the incident light, thus gaining advantages regarding the dimensioning.

When, as stated in claim 6, the light is conducted from the individual light source to an internal exposure chamber via the optical system to an optical element in the form of a rotating reflector having a plurality of filter layers, said light being either transmitted to the next filter layer on the reflector or reflected toward an exposure point in dependence on the wavelength, a further and efficient embodiment of the invention is achieved, as a it is possible to manufacture a reflector comprising a plurality of coating layers each having given filter and reflection characteristics .

In this connection an advantage is also obtained with re¬ spect to the localization of the exposure points, as mi¬ nor inaccuracies in the wavelengths of the light sources do not displace the exposure point. This provides advan- tages in connection with light source dimensioning and light source dimensioning requirements.

The method allows a very well-defined orientation of the split modulated light toward the exposure points, as the split light is conducted in parallel from the reflector to the exposure points at a mutual distance. The distance between the exposure points may hereby be dimensioned uniquely and be determined on the basis of the thickness of the individual filter layers.

This, in principle, makes the localization of the expo¬ sure point independent of the distance between reflector and exposure point, thereby facilitating e.g. focusing optics .

When, as stated in claim 7, the light is focused toward the exposure points by means of a focus lens integrated in the optical element, it is possible to focus the modu¬ lated light on the light-sensitive material.

When, as stated in claim 8, the wavelength of the indi¬ vidual laser light source is measured currently and the wavelength of the laser source is adjusted in dependence on this measurement signal on the basis of a reference wavelength λ _re t given or desired for the laser light source, an effective control, necessary in several cases, of the wavelength of the light sources is ob¬ tained, as even relatively small deviations with respect to the reference wavelength may result in an undesired deviation in the localization of the exposure points.

When, as stated in claim 9, the light is modulated in the optical system, it is possible to control the wavelength of the individual light sources in an effective manner, as a non-modulated light source, in the form of e.g. a laser diode, can be maintained more easily on the desired wavelength in the event that the light is modulated out¬ side the laser diode.

When, as stated in claim 10, the distance travelled by the optical element during one rotation is a multiple of the distance between the first exposure and the addi¬ tional exposure point or points in the axial travelling direction of the optical element and the number of light sources with different wavelengths, it is possible to adapt the speed of rotation and the exposure rate of the optical element to the desired resolution on the exposed films or light-sensitive materials.

When, as stated in claim 11, the light is conducted from the individual light source to an internal exposure cham¬ ber via the optical system, a rotating optical element reflecting or transmitting the light to the exposure point, the light path between light source and exposure point extending through at least one optical element placed in the light path and having focus-changing prop¬ erties, it is possible to perform splitting or compensa¬ tion for e.g. the direction and the focusing of the light, which may e.g. be successive.

When an optical compensating element is used, it is also possible to compensate completely or partly for varia¬ tions in the illumination wavelengths caused by inaccura¬ cies in the illumination sources. Thus, the compensating optical element makes it possible to maintain the focus and the illumination direction geometrically before

and/or after splitting of the light, and thereby the mu ^¬ tual distance between the exposure points.

When, as stated in claim 12, the light is conducted to the exposure points via at least one compensating optical element with focus-changing properties positioned between light sources and exposure points, said compensating op¬ tical element rotating with the rotating optical element, it is possible to obtain a precise focusing of all expo- sures points on the film, as the compensating optical element compensates for the mutual change in the focusing between the exposure points which is provided by the splitting of the light.

When the compensating optical element rotates with the optical reflecting element, it is ensured that the expo¬ sure points do not get twisted, and the mutual position is maintained on the film.

When, as stated in claim 13, the light is conducted to the exposure point via at least one optical element with refractive properties positioned between the rotating optical element and the exposure point, said optical ele¬ ment with refractive properties rotating with the rotat- ing optical element, an advantageous embodiment of the invention is achieved.

When, as stated in claim 14, the light is conducted from the individual light sources to a common optical fibre in the optical system via a beam splitter, a particularly advantageous embodiment of the invention is achieved, which is particularly pronounced when it is desired to maintain the linear polarized light, as a beam splitter advantageously maintains the polarization during this mixing.

When, as stated in claim 15, the apparatus comprises at least one optical element arranged to split incident light in dependence on the wavelength of the light, the optical diffractive element being adapted to rotate at the same speed of rotation as the rotating optical ele¬ ment to maintain a fixed mutual position between the op¬ tical rotating element and the optical diffractive ele¬ ment or elements, it is possible to perform multi-beam illumination in an internal drum scanner without complex rotation mechanisms.

An element to split light in dependence on wavelength is taken to mean e.g. a dispersive prism, a diffraction grating, a multi-layer beam splitter, a hologram, etc.

When, as stated in claim 16, the optical diffractive ele¬ ment or elements are formed by optical gratings, a simple embodiment of the invention is achieved.

When, as stated in claim 17, the output end of the opti¬ cal system is formed by a light guide, a particularly ad¬ vantageous embodiment of the invention is achieved, as the light guide can "contain" or, more particularly, con¬ duct light beams with different wavelengths and modula- tion in a simple manner in one geometrically coincident transmission.

Light guide is preferably taken to mean an optical fibre, a selfoc guide or the like.

When, as stated in claim 18, at least one optical compen¬ sation element is arranged between the output end of the optical system and at least one exposure point, so that all light beams with different wavelengths are focused mutually spaced on the exposure face, a special and im¬ portant embodiment of the invention is achieved, as, ac-

cording to the invention, said splitting may have as a result that the focus of the individual light beams is not sufficiently close to or coincident with the exposure face, unless simple focus compensation is performed for the light beams concerned.

It should be stressed that the above-mentioned embodiment may also be implemented as a pre-focusing of the light beams, so that these are suitably conducted to the re- flector and from there for focusing on the exposure plane.

When, as stated in claim 19, the output end of the opti¬ cal system in the form of an optical fibre is arranged on a carriage, which carries the rotating optical element as well as associated movement and control means, at a sub¬ stantially fixed distance between the optical rotating element and the output end, said carriage being adapted to perform a movement along the axis of rotation of the optical rotating element inside a scanner cavity, a par¬ ticularly advantageous embodiment of the invention is achieved, as the output end may thus be moved inside the drum while maintaining setting and precision.

Drawings

The invention will now be explained more fully below with reference to the drawing, in which

fig. 1 shows an embodiment of the invention,

fig. 2 shows a detail of the embodiment shown in fig. 1, and

figs. 3-8 show additional embodiments of the invention.

Example

Fig. 1 shows a sketch of a preferred embodiment of the invention.

The principle of the present invention is that light beams from at least two light sources having their re¬ spective wavelengths are gathered by means of one or more optical couplers and/or beam splitters.

According to the preferred embodiment, the overall opti¬ cal system consists of an optical system which collimates and optionally cuts the light, as well as a rotating op¬ tical system capable of rotating at e.g. 24,000 rpm.

A light source 1 in the form of a laser diode with a wavelength λi is connected to a first modulator 3, which is in turn connected to an optical coupler 20 formed by a so-called T-coupler.

Correspondingly, a light source 11 in the form of a laser diode with a wavelength λ ₂ is connected to a first modu¬ lator 13, which is in turn connected to the above- mentioned T-coupler 20.

The light sources used may e.g. be external cavity lasers with the wavelengths 634.785 nm and 634.355 nm.

The optical coupler 20 is connected via an optical fibre 21 to an optical system consisting of a collimator lens 22 and a focusing lens 23. A rotating mirror 24 is ar¬ ranged at the output end of the optical system, said mir¬ ror being oriented with an axis of rotation that has a uniform spacing from a surrounding light-sensitive mate- rial, in this case formed by a film 30. The mirror 24 has

an integrated grating structure in the form of a litho ^¬ graphically produced grating.

An alternative to the above-mentioned lithographic pro- duction of the grating may be a holographic production.

According to the present embodiment, the light sources 1 and 11 are each formed by a laser diode of the same type. It is preferred in connection with laser diodes of the same type that they emit light with a wavelength which is mutually close.

According to the present embodiment, λi and λ ₂ are both in the range 620-670 nm, which means that the light sources 1 and 11 are to be driven at different current and temperature conditions.

The laser light sources 1 and 11 thus emit light with different wavelengths modulated by the modulators 3 and 13. The light is conducted from the modulators 3 and 13 via the optical coupler and the optical fibre 21 to the optical system in the actual scanner, the modulated light with the wavelengths λi and λ ₂ being mixed in the optical coupler 20 to a gathered light signal in the optical fibre 21.

The light is collimated in the lens 22 and is focused on the rotating mirror 24 by the focus lens 23.

The optical grating in the mirror 24 is designed with a surface or grating structure so that the incident light is refracted in dependence on the wavelength λ. As the light incident on the mirror comprises two different wavelengths λi and λ _? according to the present invention, the light will be refracted and reflected in two light signals directed toward two different exposure points on

the film 30, as, in the case shown, λi is focused on the exposure point 7 and λ ₂ is focused on the exposure point 17.

If the laser light sources used are of different types, it is preferred according to the invention that Δλ be¬ tween the laser sources is relatively great, e.g. 30 nm, as the laser light sources can hereby be driven at the same temperature and current conditions.

Fig. 1 additionally shows two couplers 2 and 12 connected to the light sources 1 and 11, each of said couplers be¬ ing connected to a measuring unit 5 and 15 in the form of so-called wave power meters.

The measuring units 5 and 15 are moreover connected to control units 4 and 14, which are coupled back to the light sources 1 and 11.

The function of the feedback circuit described above is as follows:

The measuring units 5 and 15 register the wavelength and power of each light source 1 and 11, and this registra- tion subsequently causes the control units 4 and 14 to iteratively apply control signals to the light sources 1 and 11.

The registration of the wavelengths λi and λ ₂ is compared in the control unit with a desired preset reference value λ _r efi and λ _re f ₂ , and then the wavelengths λi and λ ₂ of the light sources are adjusted in response to this compari¬ son. Control algorithms and control parameters are se¬ lected on the basis of knowledge of the laser sources used, the actual control of the laser sources being pri-

marily performed thermoelectrially and/or by means of the diode current according to the preferred embodiment.

Fig. 2 shows how the two exposure points 7 and 17 have a mutual spacing d. Since the rotating mirror is mounted on a carriage (not shown) which moves in an axial direction relative to the rotation of the mirror, it is important that the mutual spacing between the exposure points 7 and 17 is adapted to the travelling speed of the carriage and the rotation of the mirror.

It is intended according to the present embodiment that the spacing d between the exposure points is approxi¬ mately half the distance travelled by the carriage during precisely one rotation in an axial direction. If several light sources are used, this ratio is correspondingly different. In principle, the mutual spacing d may be var¬ ied according to the desired resolution and carriage speed corresponding thereto by dynamically changing one of the laser source wavelengths or both of them.

It should be noted in this connection that this facility imparts flexibility to the overall system, as the poss¬ ible resolutions in this multi-beam system may be ob- tained by control-technical features, without changing mechanical or hardware properties or set-up.

In practice, the mutual spacing d may e.g. be 320 μm with a suitable corresponding spot diameter.

Fig. 3 shows a further embodiment of the invention, where the rotating mirror in the embodiment shown in fig. 1 is replaced by a rotating beam splitter comprising two fil¬ ter layers 25 and 26 which each reflect part of the total light amount to the film 30.

The filter layer 25 in the present embodiment thus has a reflecting effect for the light signal with one wavelength, for which reason the light signal is reflected to the exposure point 7, while the light signal with the other wavelength is transmitted further on to the reflecting surface 26, from which it is reflected to the exposure point 17.

If more than the two light sources with different wave- lengths used in this case are employed, the number of filter layers must be increased correspondingly, as this splitting by means of filter layers can define a large number of exposure points in a simple manner, the spacing between the exposure points being defined by the mutual spacing between the filter layers in the axial direction.

Fig. 4 shows a further embodiment where two light sources (not shown) generate light with two different wavelengths to an optical fibre 21, which conducts light via a collimation lens 22 through a compensating optical element 40, from which the light is conducted via a ro¬ tating optical reflecting element 50 to exposure points 7 and 17 on a film 30.

The compensating optical element 40 rotates with the op¬ tical reflecting element 50, so that the exposure points 7 and 17 are not twisted and the mutual position is main¬ tained on the film 30.

The inserted holographic optical element 40 serves to en¬ sure that both exposure points 7 and 17 are focused cor¬ rectly on the film 30 after splitting from the optical reflecting element 50.

Fig. 5 shows a further embodiment where an optical ele¬ ment 40 splits the incident light, and where an optical

reflecting element 50 focuses the light correctly on the film, said element 50 compensating for the movement or distortion of the focus on the exposure points 7 and 17 which the optical element 40 provides by said splitting.

Fig. 6 shows a further embodiment of the invention, which has the same overall functionality as the embodiments shown in figs. 4 and 5.

According to this embodiment, however, the optical ele¬ ment 50 is formed by a transmitting holographic element which splits and conducts incident light toward two expo¬ sure points 7 and 17 in dependence on the wavelength of the light. A compensating transmitting optical element 40 is interposed between the optical fibre 21 and the opti ^¬ cal element 50, ensuring that the light is conducted toward the optical element 50 at an angle which provides a correct focusing of both exposure points 7 and 17.

The optical compensating element 40 thus compensates for the change in focusing points provided by the optical element 50.

Fig. 7 shows a further embodiment of the invention, where an optical element 50 in this case is formed by a re¬ flecting mirror having an integrated grating structure, which ensures splitting of the incident light in depend¬ ence on wavelength.

Since the focusing of the exposure points 7 and 17 do not coincide with the surface of the film 30, a compensating optical element 40 is likewise inserted, ensuring that the focusing coincides with the film 30.

Although a method comprising two light sources is used in the embodiment shown, it is possible to select more light

sources within the scope of the invention, thereby achieving an additionally improved resolution, as each rotation of the optical element or the reflector mirror thereby sweeps a larger area on the film or the light- sensitive material.

Fig. 8 shows a further embodiment of the invention where two external cavity lasers 101 and 111 with the wave¬ lengths 634.785 nm and 634.355 nm conduct light to an op- tical coupler 120, which may advantageously be formed by a beam splitter in several cases in spite of the inherent higher optical loss of such a splitter, and then the light is conducted via an optical coupler 120 to an opti¬ cal fibre 121, which forms the output end of the optical system.

According to a preferred embodiment of the invention, the laser sources used must be capable of being varied in the wavelength range 634-636 nm, just as the line width should be narrower than 0.01 nm for an 8 μm spot to be made on the film.

The laser sources must likewise be capable of maintaining a given wavelength within +/- 0.0003 nm (223 MHz), since the spacing between the two spots on the film is to be kept within +/- 0.5 μm.

The laser sources are additionally coupled to a polariza¬ tion-maintaining fibre so that the fibre output is line- arly polarized at the output end.

The output end of the optical system, or in this case the fibre 121, subsequently conducts both light beams geomet¬ rically coincidently to collimation optics 122 and an iris 123 and from there to a rotating optical system 124.

The iris 123 is used for spot size adjustment.

A quarter-wave plate 123' which converts the linearly po¬ larized light emerging from the output end of the optical fibre into circularly polarized light, is provided after the iris 123.

The rotating optical system 124 is rotated at a speed of rotation of 24,000 by means not shown.

According to the invention, the rotating optical system comprises a rotating window 125 whose function is to pro ^¬ tect the rotating diffractive optical element against turbulent destruction and dusting. The window may e.g. be formed in BK7 with a thickness of 1.626 mm.

The heart of the rotating optical system 124 is subse¬ quently formed by a rotating diffractive optical element 126, which comprises a grating substrate and a grating positioned on the rear side of the grating substrate. The grating substrate may e.g. be made of a plane piece of silica glass which is 3 mm thick.

The concretely used grating consists of 2184 grooves/lines which are etched in the grating surface by means of photolithography.

Subsequently, the rotating optical system comprises an achromat 127 whose function is to focus the two separated beams, which have their separate wavelengths, down on the exposure face 130. The achromat e.g. has a focal length of 238.9 mm and must be as thin as possible.

The collimation optics may e.g. be formed by a collima- tion achromat of the type S&H f200 achromat. This achro¬ mat is movable so that it may be moved closer to/further

away from the output end of the optical fibre 121, thereby permitting the focal length to be adjusted, which in turn makes it possible to allow for the various thick¬ nesses of the light-sensitive materials to be exposed.

The rotating optical system and collimation optics are arranged on a carriage (not shown) , which may in turn be moved under the control of a control unit capable of per¬ forming a movement in the direction of the arrow A. The output end of the optical system, i.e. the optical fibre 121, is mounted on the carriage at a substantially fixed distance between the output end and the rotating optical system, while light sources and associated control units are stationary.

Thus, the optical system 124 may be reciprocated inside the internal cavity 125 under control and conduct illumi¬ nation beams to the internal exposure face 130 of the im¬ age setter on the exposure points 107 and 117.

The mutual spacing between the exposure points may e.g. be 320 μm.

Also, as shown in fig. 8, the optical system 124 may be moved to an initiation position where the exposure points 107, 117 are passed to a so-called PSD 115 (Position Sensing Device) capable of registering the optical power of the two spots and their positions and transmitting these registered data to a control unit 104.

The control unit 104, which is also connected to the light sources 101 and 111, can thus modulate image data suitably on the basis of introduced control algorithms, added image data and the registration of the PSD 115, so that one or more runs of the carriage (not shown) provide a total image on the exposure face.

Part of this data processing takes place according to known principles via an RIP (Raster Image Processor not shown) , which generates the necessary data sequences which are subsequently fed via a buffer to the laser sources 101, 111 which are thus modulated in dependence on these. Another ready alternative may of course be to feed these data sequences to a separate modulator if the laser sources are not modulated directly.

If the illustrated system e.g. was to be built with four light sources, each of which has its own wavelength, and consequently four simultaneous separate exposure points on the exposure face, the wavelengths may e.g. have a mu- tual difference of 0.43 nm: 634 nm, 355 nm, 634.785 nm, 635.215 nm and 635.645 nm.

These four wavelengths can give four spots on the film, each of which is separated by 320 μm.