EP1333976A1

EP1333976A1 - Method for the production of screen cavities in a rotogravure form and base body applicable in said method

Info

Publication number: EP1333976A1
Application number: EP01980111A
Authority: EP
Inventors: Jakob Frauchiger
Original assignee: MDC Max Daetwyler AG
Current assignee: Daetwyler Global Tec Holding AG
Priority date: 2000-11-15
Filing date: 2001-11-15
Publication date: 2003-08-13
Anticipated expiration: 2021-11-15
Also published as: JP2004512997A; EP1333976B1; DE50110828D1; US20040029048A1; WO2002040272A1

Abstract

The invention relates to the production of a rotogravure form, preferably comprising a rotationally symmetrical base body (1) and with screen cavities (5) as print information, by means of time-modulated, particularly pulsed laser radiation (9), whereby an erosion support layer (13) is applied to the surface regions (8), provided for information engraving on the base body (1), through which the screen cavities (5) are produced in said surface regions (8) with the laser radiation (9), by means of material ablation. Said erosion support layer (13) is subsequently removed to give burr-free screen cavities (5).

Description

Process for the production of halftone cells in a gravure printing form and base body which can be used in the process

The invention relates to a method according to the preamble of patent claim 1 and a base body of a gravure printing plate according to the preamble of patent claim 8.

PRIOR ART DE-A 2 218 393 describes a non-generic method for the production of

Gravure forms with electron beams are known. In the production of gravure printing forms using electron beams, difficulties arose in the production of scanning cells with a depth of less than 10 μm. DE-A 2 218 393 has therefore proposed coating the surfaces to be engraved with electron beams with a separating layer made of silver or copper sulfide with a layer thickness of only 0.1 μm. A second layer of copper with a layer thickness of 15 μm was then applied to the separating layer. The separating layer and the second layer only served to reduce the depth of removal. After engraving with electron beams, where Cups with a depth of up to 20 μm were produced, when the separation and copper layers were subsequently removed, only cups with a depth of 5 μm remained; ie below 10 microns as desired.

The process described in DE-A 2 218 393 was a complicated process due to the production of two layers with different materials and working in a vacuum.

DE-A 30 35 714 discloses a further method for producing pressure cups for an intaglio printing plate. Here, the still "raw" gravure form was coated with an etchant-resistant varnish. The varnish was then removed with an electronic engraving device at the points where grid pits should later be available. A stylus, a laser beam or an electron beam was used as the electronic engraving device. After the targeted removal of the lacquer, an etching process was carried out to produce the grid cells. The manufacturing process described here was complicated and time consuming. A method analogous to this is described in DE-A 2 344 233.

In EP-B 0 473 973 it is now proposed to use laser radiation to carry out a direct engraving of the scanning cups for the intaglio printing form, it being pointed out here that laser processing of intaglio printing forms with an outer layer of copper was associated with the following difficulties: 1 Very strong reflection of the copper layer;

2. High melting or vaporization temperature of copper;

3. High melting or evaporation heat of copper;

4. Good thermal conductivity of copper and thus strong heat transfer to the surroundings of the cell. In the laser engraving of copper layers, there was also a protruding one

Ejection crater rim on the bowl. This edge then had to be removed with difficulty.

For this reason, EP-B 0473 973 proposes to produce the cells no longer in copper but in zinc. Although the method described in EP-B 0 473 973 can be used, it is disadvantageous in the case of the gravure printing forms produced thereby that the entire gravure Printing technology is now geared towards copper as the material in which the grid cells are located.

Object of the invention

The object of the invention is to present a method and to create a base body in which or on the screen cup of a gravure printing form directly by means of laser radiation, preferably in copper, but also in other materials without an ejection crater rim, i.e. burr-free grid cups can be produced.

Solution of the task

The object is achieved in that a, preferably only a single ablation support layer is applied to the base body over the upper layer areas provided for the information embossing, through which scanning pits with the laser radiation by material ablation (evaporation and / or ejection of molten material) into the jacket areas are introduced and then this support layer is removed, whereupon burr-free rest cases are obtained. The laser radiation is radiation that is modulated in terms of its intensity over time. As a rule, pulsed radiation will be used, but this is not mandatory. Laser spikes, Q-switches, mode-locking etc. are also possible. When the support layer is removed, there is no change in the grid cells in the upper layer areas. The quality of the grid cells produced in this way without burr is so good that a hard layer, in particular a chrome layer, can be applied without aftertreatment. The chromium layer in gravure forms of this type is preferably applied with a layer thickness between 4 μm and 30 μm, in particular between 8 μm and 10 μm.

The burr-free grid cells, preferably in copper, can be achieved in particular by selecting the support layer in such a way that it enables good energy coupling for the laser radiation with good initiation of material ablation (ablation) to the underlying material with minimized directed radiation backscattering. Minimized radiation backscatter is important so that no radiation gets back into the laser resonator. This would be intensified there and could cause damage to the optical components. A good energy coupling of the laser radiation is important, since then only a small portion of the radiation remains, which is still necessary for a back reflection could come into question. On the other hand, a good energy coupling causes a strong heating of the material of the support layer. Once the support layer has changed to the liquid state, there is practically no longer any need to worry about radiation absorption. If one now selects this material of the support layer in such a way that the melting point of its essential material portion is low, the high radiation absorption also occurs quickly. However, the melting point should in any case be lower than that of the underlying upper layer material, in which the grid cells are then located. If the grid cells are to be in copper, the melting point should be below 1083 ° C. Merely from the melting point, the metals would be silver with 961 ° C, aluminum with 660 ° C, gold with 1063 ° C (which, however, immediately falls out of the cost), gallium and germanium with 937 ° C, indium with 927 ° C, lead at 327 ° C, tin at 232 ° C, zinc at 419 ° C, etc. However, only materials whose vapors are not harmful to health can be used sensibly, since otherwise great expenditure would have to be made for steam extraction. An essential material fraction of the layer material is understood to mean a percentage which causes the property mentioned above. Depending on the material, a substantial proportion of the material should be between 80% and close to 100%. The material of the support layer is said to be a material removal in which the

Cause print information carrying underlying material. That is, the local thermal energy introduced with the laser radiation should cause the material underneath to melt as quickly as possible. As experiments have shown, this reproducible melting is only possible if the layer thickness of the ablation support layer is the same everywhere. If this is the case, the well volume to be generated can be precisely specified via the radiated maximum pulse intensity and the pulse shape. The easiest way to determine the well volume is by experiment. Good results have resulted in copper as information-bearing layer and zinc as erosion support layer with the layer thickness of between 1 micron to 15 microns, preferably microns between 5 and 10 microns is less than 10 with a layer thickness tolerance of ^"3, preferably better than 5 ^■ 10 ^{of" 5} , A zinc layer with such accuracy is best applied galvanically. Tests have also shown that the material of the ablation support layer should have the highest possible vapor pressure. "Background material" ejected by the laser pulse from the information-carrying layer, which still falls fluidly onto the support layer, causes it to melt and evaporate and is then thrown away by the steam with a further loss of heat. The vapor pressure of the "background material" should be at least five times lower than that of the material lying on it. If the example above remains, zinc has a vapor pressure that is about 100 times higher than that of copper.

The material of the ablation support layer should be able to be removed well, in particular chemically, without attacking the information-carrying jacket regions.

The wavelength of the laser radiation used is to be adapted to the absorption of the material of the ablation support layer. The wavelength must also be adapted to the dimensions of the grid cells to be produced in accordance with the optical imaging laws. A CO ₂ laser (wavelength 10.6 μm) can be used for scanning cells with a diameter larger than 10 μm. For small diameters, an Nd: YAG laser (1.06 μm) is preferred. Pulse shaping and an optical structure for the beam guidance of the laser will preferably be carried out as described in EP 00 810 552.0. If an Nd: YAG laser is used, zinc has also proven itself in this case as the material of the ablation support layer.

The ablation support layer not only initiates material removal in the underlying material, it also causes a switch-on delay for the drilling process in the underlying layer. The laser pulse has therefore already risen to a higher intensity value than its initial pulse value, which results in an increase in the drilling intensity. This results in a good, i.e. a hemispherical shape.

Further advantages of the invention and of the design variants also result from the text below.

An exemplary embodiment is given below, which, however, can also be varied in material in a wide range according to the above statements.

From the following detailed description and the entirety of the claims, further advantageous embodiments and combinations of features result. tion of the invention.

Brief description of the drawings

The drawings used to explain the exemplary embodiments show:

1 shows a cross section through the base body according to the invention in an enlarged view with a pulsed laser beam generating a scanning cell,

FIG. 2 shows a cross section analogous to FIG. 1, the removal support layer being removed here

3 shows a cross section analogous to FIGS. 1 and 2, a hard layer being applied here.

In principle, the same parts are provided with the same reference symbols in the figures.

Ways of Carrying Out the Invention

Metallic rotogravure forms are usually made up of several functional elements. A steel cylinder is usually used as the base body 1. A copper layer 3 with a thickness of a few millimeters is applied to the steel cylinder. The copper layer 3 is the information-bearing gravure form. The information consists of an arrangement of a multiplicity of grid cells 5 which receive the color required for printing. To increase the resistance, a chromium coating 7 with a typical thickness of approximately 10 μm is applied as the top layer. The print information is now introduced directly into the copper layer 3 in its upper layer area 8 with a beam 9 of a pulsed Nd: YAG by material removal. In order to achieve this direct material removal with burr-free raster cups 5, the copper surface 11 is galvanically provided with a zinc layer 13 as a removal support layer with a small thickness tolerance (less than 5 ^· 10 ^"5 ). The absence of burrs is a prerequisite for perfect quality in the printing process ,

The laser pulse 9 for generating a grid 5 each pierces the zinc layer 13 while melting. Solid zinc has an absorption for the radiation 9 of the Nd: YAG laser of approximately 50%. In addition, solid zinc shows almost no directional reflection. Does the zinc go due to its relatively low melting and its low thermal conductivity compared to copper into the liquid state, there is almost 100 percent radiation absorption. There is a strong local heating of the zinc, which continues to pass it on to the underlying copper in the absorbing state, whereupon this also changes into the liquid state. Copper is now of an almost 100 percent reflection for the radiation 9 of the Nd: YAG laser (although the reflection does not come into effect because the copper is still covered by zinc) in the solid state, now liquid in an approximately 100 percent absorption passed.

The copper material ejection or that of the zinc 15 lie on the zinc layer 13 and can be easily removed by chemically detaching it in a subsequent cleaning process. The exposed engraving (small cup 5) in copper 3 is burr-free and can be chrome-plated without any problems.

With the thinly applied zinc layer 13, an economical, direct, burr-free laser engraving in copper 3 has now become possible. Zinc in particular prevents the melts from sticking, reduces the initial reflection for the laser radiation 9 and therefore allows an efficient drilling process in copper 3.

The method just described is of course not limited to zinc 13 as a copper coating. As stated at the beginning, a number of other materials are possible. The removal support layer to be applied to copper 3 does not necessarily have to be a metal layer either. Non-metals are also suitable, provided they have the required properties with regard to absorption, directed reflection and melting point.

Instead of only a single ablation support layer 13, several layers can also be applied one above the other. However, the only zinc layer 13 has proven itself for reasons of cost and simple handling.

The base body 1 of a gravure printing plate does not necessarily have to be cylindrical; it can also be semi-cylindrical, flat or shaped differently.

Claims

claims

1. A method for producing a scanning cup (5) as a printing information bearing, preferably having a rotationally symmetrical base body (1), gravure printing plate by means of time-modulated, in particular pulsed laser radiation (9), characterized in that on the base body (1), a removal support layer (13) is applied for the upper layer areas (8) provided for information imprinting, through which raster cells (5) with the laser radiation (9) are introduced into the layer areas (3, 8; 13) by material ablation and then this removal support layer ( 13) is removed, whereupon burr-free cups (5) are obtained.

2. The method according to claim 1, characterized in that only a single ablation support layer (13) is applied, and after its removal a hard layer (7), in particular a chrome layer (7), preferably with a layer thickness between 4 μm and 30 μm, in particular between 8 μm and 10 μm, is applied and the layer areas (8) provided for the information embossing are preferably made of copper.

3. The method according to claim 1 or 2, characterized in that the support layer (13) is selected such that it has a good energy coupling for the laser radiation (9) with a good material removal initiation to the underlying material (3, 8) with a minimized directed beam - Backscattering made possible.

Method according to one of claims 1 to 3, characterized in that the support layer (13) with a thickness which is constant up to a tolerance is applied in order to be able to generate the depth of the scanning cup via an adjustable energy or a time-modulated intensity profile of the laser radiation (9) with a predeterminable, reproducible form factor, and the support layer (13) with a thickness between 1 μm and 15 μm, in particular between 5 μm and 10 μm, especially galvanically, with special attention to a layer thickness tolerance of less than 10 ^"3 , preferably less than 5-10 ^{" 5} .

5. The method according to any one of claims 1 to 4, characterized in that a material with a high vapor pressure, preferably with at least one higher than copper by a factor of five is selected for the support layer (13) and in particular the support layer (13) is good, in particular chemically, can be removed without attacking the information-carrying layer regions (8).

6. The method according to any one of claims 1 to 5, characterized in that a substantial proportion of the material of the support layer (13) is selected such that it has a low melting point, preferably below that of copper, in particular below 500 ° C and especially a metal , especially zinc.

7. The method according to any one of claims 1 to 6, characterized in that a laser radiation (9) with a preferred wavelength between 0.8 microns and 11 microns, preferably the radiation of a CO ₂ laser, especially in the micrometer range, the radiation of a Nd: YAG laser is used.

8. Main body (1) of a gravure printing plate, in the upper layer area or areas (8) of which there are raster cups (5) as print information with time-modulated, in particular Pulsed laser radiation (9) can be introduced using a method according to claims 1 to 7, characterized in that each top layer area (8) is covered with a removable, preferably single, ablation support layer (13) through which the scanning cups (5) with the laser radiation pass (9) can be introduced and the support layer (13) enables good energy coupling for the laser radiation (9) with a good material removal initiation to the underlying material (3) with a minimized directional radiation backscattering.

9. Base body (1) according to claim 8, characterized in that the layer regions (8) provided for the information embossing are made of copper and the support layer (13) has a thickness between 1 μm and 15 μm, in particular

-3 between 5 μm and 10 μm, with a layer thickness tolerance of less than 10, in particular

-5 especially less than 5 ^■ 10, the support layer (13) being a material with a high vapor pressure, preferably with at least one higher than copper by a factor of five, and in particular the support layer (13) being good, in particular chemically, without attacking the information-bearing layer areas (8) can be removed.

10. Base body (1) according to claim 8 or 9, characterized in that a substantial proportion of the material of the support layer (13) has a low melting point, preferably below that of copper, in particular below 500 ° C and is above all a metal, in particular zinc.