Substrate for thermal recording head and thermal recording head using same

Abstract: The present invention concerns a thermal recording to be used for performing recording, preferably an ink jet thermal recording, a process for forming the same and a recording apparatus by use thereof, and accomplishes uniformized heat energy action of the heat acting surface (protective layer surface when there is protective layer) played primarily by the heat-generating resistors (102) of a plurality of electrothermal transducers (111). The present invention, for that purpose has uniformized the amount of heat energy generated during recording at the plurality of heat acting portions by positively changing the shape or the thickness of the resistors (102) concerned with the heat acing portions or/and the constitution itself of the protective layer depending on its existing position.

Description: This invention relates to a substrate for a liquid jet recording head, and to a liquid jet recording head comprising the aforesaid substrate. It also relates to a method of manufacturing a substrate for a liquid jet recording head. A particularly effective method of liquid jet recording works by bringing about a change of state in the recording liquid resulting in the formation of bubbles by applying heat energy to the liquid. On application of heat, the liquid is discharged through a discharge port as a result of the state change and forms droplets which fly to and attach onto the recording surface. This method of recording can be used to form letters, graphics images etc. The present invention provides a head for liquid jet recording using a novel substrate, and is particularly suitable for multi-integration type liquid jet recording heads. The invention is, however, generally applicable to thermal recording heads to be used in general purpose printers, copying machines, facsimile machines, computer output devices etc. Ink jet recording is a non-impact-method of producing images and has recently attracted attention and is being put into practical use. Amongst ink jet recording methods, those described in, for example, Japanese Laid Open Patent Application No. 54-51837, and German Laid Open Patent Application (DOLS) No. 2843064 differs from other liquid jet recording methods in that the power to bring about discharge of droplets is derived by applying thermal energy to the recording liquid. Application of thermal energy to the liquid brings about a change of state accompanied by an abrupt increase in volume. The force which is derived from this state change causes droplets to be discharged and projected from a discharge opening provided at the tip of the recording head so that they fly to and become attached to a recording medium so as to produce the required information record. The liquid recording method disclosed in DOLS No. 2843064 and US Patent Nos. 4723129 and 4740796 can not only be used effectively in so-called "drop-on-demand" recording, but also the necessary recording head can be produced easily with a multiplicity of discharge ports formed at high density to full line width. The method therefore has the advantage that high resolution images and high quality images can be obtained at high speed. An ink jet recording head that works on the above principles has a heat generation portion at which a voltage is applied and which is a resistor. The heat energy generated on application of the voltage brings about a change of state including the formation of bubbles, and the above mentioned patent specifications disclose a preferred form of recording head which works by "film boiling". The result is that the ink is projected through the discharge opening as a result of bubble formation or "foaming" due to the change of state. As the voltage is raised from a zero level, foaming starts at a particular voltage. This voltage is important and is hereinafter referred to as the foaming voltage. In order to bring about ink discharge, a voltage greater than the foaming voltage and referred to as the driving voltage has to be applied. From the standpoint of improving printing quality it is desirable to increase the voltage, whereas from the standpoint of improving pulse duration, it is desirable to reduce the driving voltage. The optimum value of these applied voltages has been standardised so as to correspond to a multiple of the foaming voltage. The method by which the foaming voltage which provides the reference standard is set is therefore a considerable factor in producing improvements in printing quality. More specifically, in order to obtain uniform printing characteristics and discharge characteristics within a recording head, and also to obtain durable discharging, it is desirable that the foaming voltage of the various discharge ports within the recording head should have the same value. In the production of thermal recordings, a plurality of heat-generating resistors, electrode pairs corresponding to them, and protective layers which provide insulation have to be formed by film forming techniques. The problem arises of variability in the constitution of the individual parts in mass production or from batch to batch. In practical devices it is necessary to ensure that the required heat energy to bring about ink discharge is present by adopting as the foaming voltage a value which may be significantly in excess of that for an individual heat generating resistor. However, variability in the electrothermal transducers including the resistors, electrodes and optional protective layers which form upper layers of these transducers are obstacles to the improvement in precision of the printing operation. One approach to the solution of this problem is disclosed in Japanese Patent Application No. 60-297217 (Japanese Laid Open Patent Application No. 62-152863) filed by Canon K.K. The specification of this patent draws attention to the fact that when film formation is by sputtering, the resistance layers, protective layers and electrodes all become thinner at the two end regions of the recording head than they are at the central region. It also explains that an electrothermal transducer of uniform thickness can be obtained at regions of concentric shape. In this patent, since the region with a relatively smaller range of variance is selected for film formation, it is impossible simply to obtain a higher density of transducers along the line, and also because the recording gaps relative to the recording medium differ from one another, further control has to be exercised on the whole recording. Also in this invention it is difficult to obtain a full line thermal head. US Patent No. 4740800 discloses that there is a distribution of the width of the heat generating resistive layer in a recording head with the width at the end areas being smaller than that in the central area. As a result, recording density is not uniform and print density is lower towards the ends of the recording head then it is at the middle. The solution disclosed is to provide a set of electrothermal transducers or heaters each formed of a heat generating resistive layer and an electrode layer. The set of heaters has at each side thereof a number of dummy heaters which are used to make the areas of the heat generating resistive layers of the working heaters uniform but which do not participate in liquid discharge. As many dummy heaters as are necessary to prevent the appearance of an end effect are provided, and uniform and defect-free heads are obtained. However, this solution increases the size of the recording head. It can provide practical product in which the number of electrothermal transducers is less than 124 because the extent of enlargement is then not significant, and it is an invention that is actually available. However, although the central region in which there is relatively slight variance from transducer to transducer is used, secondary control means is required to take account of such variance. Furthermore, variance becomes more significant in the case of a full line recording head having 1000 or more electrothermal transducers. Therefore, in the prior art, the problem of variability of the individual heads of a multi jet recording head has been attacked by selecting electrothermal transducers in which the range of variance is reduced, without fundamental attack on the problem of variability itself. The present invention provides a substrate for a liquid jet recording head having the features of claim 1 having the characterising feature that the dimensions of the plurality of heat generating portions is varied so that the foaming voltage of the heat generating portions is kept substantially constant. Other features of the invention are defined in the accompanying claims to which attention is directed. How the invention may be carried out will now be described by way of example only and with reference to the accompanying drawings. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a plan view showing the substrate of an example of the present invention; Fig. 2 is a distribution diagram showing an example of the distribution of layer thicknesses and sheet resistances of the heat-generating resistance layer of an example of the present invention; Fig. 3 is a diagram showing an example of the heater design dimensions; Fig. 4A is a plan view showing the constitution of the substrate of an example of the present invention; Fig. 4B is a sectional view showing the constitution of the substrate of an example of the present invention; Fig. 5 is a partial perspective view of the recording head of an example of the present invention; Fig. 6 is a constitutional illustration of the recording head of another example of the present invention; Fig. 7 is an illustration of still another example of the present invention; Fig. 8 is an illustration of another heater design dimensions of the present invention; Fig. 9, Figs. 10A and 10B are each illustration of the recording apparatus of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENTS Figs. 4A and 4B show structural examples of typical head substrates of the prior art of the liquid jet recording heads according to the bubble jet recording system. Fig. 4A is a plan view of a substrate in which a heat-generating portion is arranged within a liquid path of ink (recording liquid) communicated to the discharge port, and Fig. 4B is a sectional view along the cut line of X′ - Y′ in Fig. 4A. Here, 101 is the whole substrate, 102 the heating portion positioned within the wall surface of liquid path communicated to the discharge port for discharging ink for generating bubbles by giving heat energy to the ink (called heater), 103, 104 and a pair of leader electrodes made of Aluminum connected to the heat-generating resistance layer 107 for applying a predetermined voltage on the heat-generating portion 102, 105 a support made of Si (silicon), and 107 a heat-generating resistance layer formed by lamination on the support 105. The heat-generating portion 102 is the portion positioned between a pair of electrodes 103, 104. 108 is a first upper protective layer (made of SiO₂) which protects the leader electrodes 103, 104, etc. by covering wholly thereover, 109 a third upper protective layer of the ink contact surface which further protects most of the first upper protective layer 108, and 110 a second upper protective layer which protects the portion where the heat-generating portion 102 exists. 111 is an electrothermal transducer comprising electrodes 103, 104 and heat-generating resistance layer 107. 112 is a foaming surface which is the surface of the upper protective layer 110 corresponding to the heat-generating portion 102, and bubbles are generated on this surface. The liquid jet recording head based on such principle is actuated by applying a voltage on the heating portion (heater) 102 of the heat-generating portion 111, generating bubbles on the foaming surface 112 of the second upper protective layer 110 by the heat energy generated thereby, and discharging the ink by extrusion through the discharge port by the force generated by such foaming. A. Basic principle of the invention Before explanation of specific examples of the present invention, the first basic principle of the present invention is to be described in detail. That is, the problems as described in the prior art example have been solved, because the recording head is prepared so that the pattern design with various dimensions of the heat-generating portion heater has been made so that the resistance values may be substantially the same corresponding to the distribution characteristic of sheet resistances (=specific resistance/layer thickness) of the heat-generating resistance layer. To describe in detail below, in the case when the sheet resistance at the both ends is 15 Ω, and the sheet resistance at the central portion 20 Ω in a full-multi integration type liquid jet recording head with A4 width, the dimensions of the heater (heat-generating portion) at the central portion are designed as 20 µm x 100 µm, and the dimensions of the heaters at both ends as 17 µm x 115 µm. When thus designed, the resistance values become: both becoming substantially the same. Here, the heater should be designed in view of the area of the heater. More specifically, in a recording head of the bubble jet recording system utilizing the bubbles expanded with abrupt gasification of ink by heat generation of the heater, the heater area becomes an important factor in bubble generation. Depending on the size of the heater area, the foaming volume is determined, and therefore if the heater area is made smaller, the foaming volume becomes smaller, while if it is made larger, the foaming volume becomes larger. On the other hand, since the discharge volume of ink depends greatly on the foaming volume, the discharge volume will vary depending on variation of the heater area. Accordingly, printing characteristic (quality) is concerned greatly with uniformity of discharge volume, and therefore it is important to make the heater area uniform as a whole. By making thus the heater area the same, the heaters at the central portion and the both ends become to have the same resistance values, whereby the foaming voltage becomes the same in all the segments. Thus, if the heat-generating portions of the central portion and the both ends have the same area and the same foaming voltage, by setting adequate driving voltage values with good pulse durability as well as good printing characteristic, all the segments from the central portion to the both ends can be driven under the same conditions. By doing so, it is possible to prepare a recording head with all the segments having the whole (total) performance as the recording head, particularly the balance of printing characteristic/durability. While the sheet resistance of the central portion and the both ends is described above, it is practically necessary to vary the design pattern of the heater according to the distribution of the whole sheet resistance. Next, heater resistance and design of dimensions of the heater are to be described. However, for brevity of explanation, the heater is made rectangular. First, the sheet resistance distribution can be shown as a function f(x) of the distance x from either one end of the sheet. Now, if the dimension in the longer direction of the heater is defined as ℓ, and the dimension in the shorter direction as m, the heater resistance h is given by the following formula (1): If the area of the heater is defined as s, since the heater area s is constant and therefore represented by the following formula: s = ℓ x m ℓ = s/m (2). From the above formula (2) and the above formula (1), the following formula (3) is derived m² = f(x) x s h (3) Hence, m = √ s/h x f(x) (4). Therefore, if the heater resistance h, the heater area s and the distribution date f(x) of the sheet resistance are given, the pattern design of the heater becomes possible according to the above formulae (4) and (2). Specific examples are clarified in the Examples described below. B. First example Fig. 1 to Fig. 5 show an example of the present invention. First, as shown in Fig. 4A, 4B, on a support of Si (silicon) (also called glass substrate) is formed a heat-generating resistance layer 107 of HfB₂ by RF (high frequency) sputtering method. The layer thickness distribution of the heat-generating layer 107, as shown by curve of the chain line in Fig. 2, exhibited a tendency that the both ends were thick, and the central portion was thin with A4 size width. It has been found that the layer thickness (film thickness) distribution of the film forming device has constantly the same tendency. Therefore, it is possible that the layer may have the layer thickness distribution characteristic opposite to this if the film forming device is changed. When the sheet resistance distribution of the heat-generating resistance layer 107 of HfB₂ is practically measured, it has become as shown by the solid line in Fig. 2. When calculation was performed by substituting the values of s=2000 µm², h=100Ω in the above formula (4) of m=√ s/h x f(x) for the heat-generating resistance layer 107 having such sheet resistance distribution, the values of m and ℓ became the relationship as shown in Fig 3. Accordingly, a photomask was prepared by pattern designing of the heater so as to satisfy the relationship in Fig. 3. On the heat-generating resistance layer 107 as described above was vapor deposited Aℓ (aluminum ) to a thickness of 5000 Å as electrode materials 103, 104, and then a rectangular heater (heat-generating portion) 102 was formed according to the photolithographic technique by use of the photomask as described above (see Fig. 1). When the dimensions of the heater 102 were practically measured, the dimensional relationship as shown in Fig. 3 was obtained. Next, as the first upper protective layer 108, SiO₂ (silicon oxide) was prepared with a thickness of 1 µm according to the RF sputtering method. Further, as the second protective layer 110, Ta (tantalum) film was formed with a thickness of 0.5 µm, and then Ta 110 was subjected to patterning by the photolithographic technique only around the heater 102, and SiO₂ 108 was subjectd to patterning by opening thru-holes only on the common leader electrode 103 and the individual leader electrodes 104. Next, Photonies (trade name of Toray K.K.) was coated, a window was opened on the heater 102, and thru-holes were opened at similar places as in the layer 108 of SiO₂ (see Figs. 4A and 4B). Next, as the electrode of the second layer (not shown), Aℓ was deposited and patterning was effected so as to leave only the common electrode portion. Next, discharge ports were formed as shown in Fig. 5 to complete the recording head. In Fig. 5, 401 is liquid path, 402 discharge port, 403 ink path wall which is the wall of the path 401, 404 common liquid chamber, 405 ceiling, and 406 ink feeding inlet. C. Experimental results When the foaming voltage and the resistance value of the heater 102 of the recording head obtained by manufacturing by use of the photomask of which the mask design was performed as shown in Fig. 3 were practically measured, the results as shown in the following Table 1 were obtained. Distance from A4 end surface (mm) Total resistance (Ω) Foaming voltage (V) 0 106 10.4 50 106 10.3 100 105 10.5 150 106 10.3 200 105 10.4 As can be seen from Table 1, both resistance values and foaming voltages became substantially constant. In contrast, as Comparative example with the present Example, in the heater 102 of which the mask was designed by the fixed dimensions of the heater 102 of 20 µm x 100 µm, without the mask design as shown in Fig. 3, the results of its foaming voltages and resistance values became as shown in the following Table 2. Distance from A4 end surface (mm) Total resistance (Ω) Foaming voltage (V) 0 80 9.8 50 97 10.3 100 105 10.5 150 97 10.3 200 80 9.7 Thus, in Comparative example by use of the prior art, foaming voltages were varied from 9.7 to 10.5 V. When the recording head of the present Example obtained by designing as shown in Fig. 3 was driven with a driving voltage of 10.4 V x 1.2≈12.5 V, all good printing results were obtained with A4 width. Also, since the driving voltage becomes 1.2-fold of the foaming voltage for any segment, good printing characteristics were obtained, and also discharging durability was also good. As compared with this, in the above Comparative example, when the recording head is driven with a driving voltage of 12.6 V which is 1.2-fold of the maximum value 10.5 V of the foaming voltage (see Table 2), a segment with poor discharging durability appeared with the voltage becoming 1.3-fold of the minimum value 9.7 V of the foaming voltage. In the case of a driving voltage which is 1.3-fold of the foaming voltage, the pulse number was worsened by one cipher or more as compared with the 1.2-fold driving voltage. Thus, although the pulse durability of the central segment is good to be persistent for a long time, the segments on both ends became worse by one cipher or more than the central segment. When driven with 11.6 V which is 1.2-fold of the minimum value 9.7V of the foaming voltage (see Table 2), the central portion of the maximum value of the foaming voltage became 1.1-fold, whereby printing characteristic (printing quality) was lowered to give no good printing. This is because, for the segment at the central portion, 11.6 V of the driving voltage is 1.1-fold of the foaming voltage, whereby the foaming stability was worsened. Thus, in Comparative example of the prior art, wherein the foaming voltage has a distribution, printing characteristic and discharging durability are varied and a tendency appears that the characteristics of a part of the segment group are worsened. In the first place, determination of at what fold voltage of the foaming voltage should be the head driven depends on printing characteristic and durability, and the optimum values of printing characteristics, etc. are within the permissible ranges of about 0.05-fold of the standard values. Therefore, if the foaming voltage is varied by 10 % or more, adverse effects will appear in the printing characteristic and durability of the recording head. Particularly, in the full-multi integration type liquid jet recording head of A4 width or A3 width size, due to the restriction of the thin film forming device, layer thickness distribution, namely the sheet resistance distribution (variation) is generated, whereby the foaming voltage is distributed (varied) within the recording head. Accordingly, it becomes necessary to make the foaming voltage constant by varying the design dimensions of the heater corresponding to the change in the sheet resistance distribution as in the present Example. D. Other examples In the present Example as described above, the case of having two layers 108, 110 of upper protective layers on the heater was shown, but the present invention is of course applicable to a liquid jet recording head having no upper protective layer. Also, the shape of the heater need not be rectangular, but the pattern may be designed so that the resistance of the heater, the heater area may be the same. In the present Example as described above, the discharge direction of the recording liquid was in the plane direction of the heater (see Fig. 5), but the present invention is also applicable to the liquid jet recording head of the type which discharges recording liquid in the vertical direction to the heater as shown in Fig. 6. As described above, according to the present invention, since the heat-generating portions have been formed by varying the dimensions of a plurality of heat-generating portions so that the resistance values may be substantially equal to each other corresponding to the sheet resistances of the heat-generating portions of the heat-generating resistance layer, a full-multi integration type liquid jet recording head of A4 width, A3 width, etc. having good pulse durability as well as good printing quality can be prepared by use of an inexpensive film forming device, whereby quality improvement along with reduction in production cost of the recording head can be effected. A1. The second basic principle of the invention Before explanation of specific examples of the present invention, the basic principle of the present invention is to be described in detail. The problems as described in the prior art example can be solved, if the recording head is prepared by pattern designing with various dimensions of the heat-generating portion (heater) has been made so that the foaming voltages may be substantially equal to each other corresponding to the distribution characteristic of the layer thickness (layer thickness data) of the upper protective layer (hereinafter abbreviated as upper layer). To describe in detail below, in a full-multi integration type liquid jet recording head, when the film thickness of the upper layer at both ends and the central portion are different, for example, with required power for foaming (heat-generating energy) of 0.8 at the central portion relative to 1 at both ends, the resistance values of the heat-generating portion (heater) may be designed at 0.8 : 1 of both ends : central portion corresponding to the change in layer thickness. However, the point of care in designing of the heat-generating portion is the area of the heat-generating portion. More specifically, in a recording head of the bubble jet recording system which discharges ink by generation of bubbles with heat, the area of the heat-generating portion becomes an important factor in bubble generation. Depending on the size of the area, the foaming volume is determined, and therefore if the area is made smaller, the foaming volume becomes smaller, while if it is made larger, the foaming volume becomes larger. On the other hand, since the discharge volume of ink depends greatly on the foaming volume, the discharge volume will vary depending on variation of the area of the heat-generating portion. Accordingly, printing characteristic (quality) is concerned greatly with uniformity of discharge volume, and therefore it is important to make the area of the heat-generating portion uniform as a whole. By designing the heat-generating portion as described above, the heaters at the central portion and the both ends become to have the same foaming voltages. Thus, because the heat-generating portions of the central portion and the both ends have the same area and the same foaming voltage, by setting adequate driving voltage values with good pulse durability as well as good printing characteristic, all the segments from the central portion to the both ends can be driven under the same conditions. Thus, it is possible to prepare a recording head with all the segments having the whole performance as the recording head, particularly the balance of printing characteristic/durability. Having described above about the layer thicknesses of the upper layer at the central portion and the both ends, it is practically necessary to vary the design pattern of the heat-generating portion according to the distribution of the whole distribution (change) of the layer thickness. Next, layer thickness distribution of the upper layer and design of dimensions of the heat-generating portion (hereinafter called heater) are to be described. However, for brevity of explanation, the heater is made rectangular. First, the layer thickness distribution of the upper layer can be expressed as a function f(x) of the distance x from either one end of the sheet as the original point. Now, if the dimension in the longer direction of the heater is defined as ℓ, the dimension in the shorter direction as m, and the sheet resistance of the heater as R, the heater resistance h is expressed by the following formula (1): If the area of the heater is defined as s, s is represented by the following formula: s = ℓ x m (2) If the layer thickness dependency of the upper layer on the foaming initiation power (W B ) is defined as g(t), g(t) is represented by the following formula (3). However, t is defined as the layer thickness (film thickness). W B = g(t) (3) g(t) is determined previously by experiments. When the foaming voltage is defined as V B , the following formula (4) is valid: From the formulae (1), (3) and (4), the following formula (5) is obtained. Since ℓ=s/m from the above formula (2), the following formula (6) is obtained from the above formula (5): To rewrite the above formula (6) with respect to V B , the following formula (7) is obtained. (where S, R are constant) Therefore, it can be understood from the formula (7) that g(t)/m² may be made constant for making the foaming voltage V B constant. In other words, since there is the relationship of m=K x√ g(t) (where K is a constant value), the lateral dimension m of the heater can be designed from the experimental data of the layer thickness dependency g(t) of the foaming initiation power. Specific examples are clarified in the Examples described below. E. Third example Description is made by referring to the constitution shown in in Fig. 4A, 4B. On a support 101 of Si (silicon) (also called glass substrate) is formed a heat-generating resistance layer 107 of HfB₂ by RF (high frequency) sputtering method. In this case, the layer thickness of the heat-generating layer 107 is made 1000 Å, the sheet resistance 20Ω. On the heat-generating resistance layer 107 were vapor deposited Aℓ (aluminum) to a thickness of 5000 Å as the electrode materials 103, 104. Next, according to the photolithographic technique by use of a photomask, a rectangular heater (heat-generating portion) 102 is formed (see Fig. 1). However, designing of the photomask used at this time is described below. Next, as the first upper protective layer 108, SiO₂ (silicon oxide) was prepared according to the RF sputtering method. When the layer thickness distribution of the SiO₂ 108 was practically measured, as shown in Fig. 2, a tendency was exhibited that both ends are thin (7000 Å) and the central portion is thick (11000 Å) with A4 width. Further, as the second protective layer 110, Ta (tantalum) film was formed with a thickness of 5000 Å, and then Ta 110 was subjected to patterning by the photolithographic technique only around the heater 102, and SiO₂ 108 was subjected to patterning by opening thru-holes only on the common leader electrode 103 and the individual leader electrodes 104. Next, Photonies (trade name of Toray K.K.) was coated, a window was opened on the heater 102, and thru-holes were opened at similar places as in the layer 108 of SiO₂ (see Fig. 4). Next, as the electrode of the second layer (not shown), Aℓ was deposited and patterning was effected so as to leave only the common electrode portion. Next, discharge ports were formed as shown in Fig 5 to complete the recording head. In Fig. 5, 401 is liquid path, 402 discharge port, 403 ink path wall which is the wall of the path 401, 404 common liquid chamber, 405 ceiling, and 406 ink feeding inlet. Next, description is made about practical designing of the photomask for forming the heater 102. The layer thickness dependency of the foaming power per unit area of the upper layer 108 of SiO₂, the foaming power Δp per unit area and the layer thickness t were found to be proportional to each other, having the relationship of the following formula (8): Whereas, when the thickness of the upper layer 108 of SiO₂ was 9000 Å, and the area of the heater 102 was 20 µm x 100 µm, the foaming initiation power was confirmed to be 0.8 W (watt). By substituting the numerical values of the layer thickness in the above formula (8), it can be understood that bubble initiation power of 0.88 W is obtained when the thickness of the upper layer 108 of SiO₂ is 11000 Å, 1nd the foaming initiation power is 0.72 W when the thickness of the layer 108 is 7000 Å. From the above results, when calculation is performed with the voltage applied on the heater 102 being constant, the heater resistance of the heater 102 becomes 90Ω, when the thickness of the upper layer 108 of SiO₂ is 11000 Å, while the heater resistance of the heater 102 becomes 110Ω, when the thickness of the upper layer 108 of SiO₂ is 7000 Å. By calculation with the area of the heater 102 being constant, the area of the heater 102 becomes 21 µm x 95 µm when the thickness of the upper layer 108 of SiO₂ is 11000 Å, while the area of the heater 102 becomes 19 µm x 105 µm when the thickness of the upper layer 108 of SiO₂ is 7000 Å. The results thus calculated are shown in Fig. 3. F. Experimental results When the foaming voltage and the resistance value of the heater 102 including the protective layer obtained by manufacturing by use of the photomask of which the mask design was performed as shown in Fig. 8 were practically measured, the results as shown in the following Table 3 were obtained. Distance from A4 end surface (mm) Total resistance (Ω) Foaming voltage (V) 0 115 9.4V 50 100 9.5V 100 95 9.4V 150 100 9.4V 200 115 9.5V As can be seen from Table 3, foaming voltages became substantially constant. In contrast, as Comparative example with the present Example, in the heater 102 including the protective layer of which the mask was designed by the fixed dimensions of the heater 102 of 20 µm x 100 µm, without the mask design as shown in Fig. 8, the results of its foaming voltages and resistance values became as shown in the following Table 4. Distance from A4 end surface (mm) Total resistance (Ω) Foaming voltage (V) 0 105 9.0V 50 106 9.7V 100 105 9.9V 150 105 9.6V 200 106 9.1V Thus, in Comparative example by use of the prior art, foaming voltages were varied from 9.0 to 9.9 V. When the recording head of the present Example obtained by designing as shown in Fig. 8 was driven with a driving voltage of 9.5 V x 1.2≈11.4 V, all good printing results were obtained with A4 width. Also, since the driving voltage can be made 1.2-fold of the foaming voltage for any segment, bubble formation by film boiling can be stabilized. Therefore, according to the present Example, good printing characteristics were obtained, and also discharging durability was good. As compared with this, in the above Comparative example, when the recording head is driven with a driving voltage of 11.9 V which is 1.2-fold of the maximum value 9.9 V of the foaming voltage (see Table 4), a segment with poor discharging durability appeared. Such segment with poor discharging durability appeared at the both ends with low foaming voltages. That is, since the driving voltage 11.9 V for those poor segments becomes 1.3-fold or more of the foaming voltage, it can be understood the durability is worsened. On the other hand, when driven at 10.8 V which is 1.2-fold of the minimum value 9.0 V of the foaming voltage (see Table 4), the printing characteristic (printing quality) at the central portion was lowered. Since 10.8 V of the driving voltage is 1.1-fold or lower of the foaming voltage of the segment of the central portion, it can be understood to be no good printing region. Thus, in Comparative example according to the prior art, since the foaming voltage has a distribution, printing characteristic and discharging durability are varied, whereby a part of the segment group tends to become worsened. In the first place, determination of at what fold voltage of the foaming voltage should be the head driven depends on printing characteristic and durability, and the optimum values of printing characteristics, etc. are within the permissible ranges of about 0.05-fold of the standard values. Therefore, if the foaming voltage is varied by 10 % or more, adverse effects will appear in the printing characteristic and durability of the recording head. Particularly, in the full-multi integration type liquid jet recording head of A4 width or A3 width size, due to the restriction of the thin film forming device, layer thickness distribution, namely the sheet resistance distribution (variation) is generated, whereby the foaming voltage is distributed (varied) within the recording head. Accordingly, it becomes necessary to make the foaming voltage constant by varying the design dimensions of the heater corresponding to the change in the sheet resistance distribution as in the present Example. G. Other examples In the present Example as described above, the case of having two layers 108, 110 of upper protective layers on the heater was shown, but the present invention is of course applicable wherein the upper protective layer has further some layers. In that case, the characteristics of the respective films for the foaming power may be determined, and the heater mask may be designed by determining the foaming power at that place by the addition calculation method. In the present Example as described above, the discharge direction of the recording liquid was in the plane direction of the heater (see Fig. 5), but the present invention is also applicable to the liquid jet recording head of the type which discharges recording liquid in the vertical direction to the heater as shown in Fig. 6. As described above, according to the present invention, since the heat-generating portions have been formed by varying their dimensions so that the foaming voltages may be substantially equal to each other in every segment corresponding to the layer thickness distribution (layer thickness change) of the upper layer formed on the electrothermal transducer, a full-multi integration type liquid jet recording head of A4 width, A3 width, etc. having good pulse durability as well as good printing quality can be prepared by use of an inexpensive film forming device, whereby quality improvement along with reduction in production cost of the recording head can be effected. Fig. 3 is a diagram showing an example of the heater design dimensions, Fig. 9 is a constitutional diagram of pertinent portions of a serial color printer to which the recording head of the present invention is applied. The arrowhead A is the deliver direction of the conveying means 25, 25 which convey the cut sheet 24 or the roll sheet 30 as the recording medium, and this Example moves the recording head 5 with the pulley 2A which synchronizes the carriage 205 for mounting four of cyan C, magenta M, yellow Y, black BK with the pulse motor 2B, the driving belt 2D wound therearound and the pulley 2C at the other end region. Also, the carriage 200 having ink tanks for supplying the respective inks to these recording heads 5 mounted thereon is moved by the belt 204 wound over the pulleys 201, 202 and the motor 203 for driving the pulley 201. These constitutions are burdened on the motor 203 exhibiting sufficient driving force, which is not of high precision because of great weight of the ink carriage weight 200, while on the other hand recording head carriage 205 which is based on a premise of high precision is made lightweight and driven by the pulse motor 2B, and the carriage 200 moves following the carriage 205 at a distance not so greatly apart therefrom but without contact therewith. 207 is an absorbing member (paper or sponge) for ink of blank discharge, and held as fixed on a predetermined position together with the head cleaning blade 208. 209 is a known recording head cap, which prevents evaporation of ink by capping the recording head during non-recording period, and a negative pressure is given thereto, if necessary, by a suction pump not shown. R is a color printing region, and since the 4 recording heads are stabilized with the above-mentioned recording heads, sufficient densities can be obtained also at the boundaries between the regions R, and therefore the density balance of full color becomes highly precise, whereby pitch irregularity can be prevented. This Example is color mode, but also good printing can be performed in monochromatic mode as a matter of course. Fig. 10A shows application of the full-line head 1 of the recording head of the present invention to a recording apparatus, and 3 is a paper delivery means as the conveying means of the recording medium, and paper delivery is performed by the control means 4 corresponding to recording with the recording head 1. Ordinarily, paper delivery is performed continuously. By doing so, good printing without recording irregularity over the entire width can be effected. Fig. 10B shows a resistor shape as the heat-generating portion of the heater. In this Fig. 10A, along the standard L on the discharge port side, the length is varied toward the ink supplying side, with the lengths at the both ends E, the both end sides N, the intermediate portion M, the central region C1, the center C being reduced in this order (C, C1 are the same, M, N are the same). Their widths are greater in the order of E, N, M, C1, C, with the respective resistance values indicating the tendency for becoming constant. This Example shows an example with stepwise variations instead of the continuous variation in the above Figure, which is also included within the present invention. The present invention brings about excellent effects particularly in a recording head, a recording apparatus of the bubble jet system among the ink jet recording systems. As for its representative constitution and principle, for example, those by use of the basic principles disclosed in U.S. Patents 4,723,129 and 4,740,796 are preferred. This system is applicable to either of the so called on-demand type and the continuous type. However, particularly in the case of the on-demand type, by applying at least one driving signal which gives quick temperature elevation in excess of nuclear boiling corresponding to the recording information to an electrothermal transducer arranged corresponding to the sheet or the liquid path where a liquid (ink) is held, heat energy is generated at the electrothermal transducer to effect film boiling at the heat acting surface of the recording head, thereby consequently effectively forming bubbles within the liquid (ink) corresponding one by one to the driving signal. By growth and shrinkage of such bubbles, the liquid (ink) is discharged through openings for discharge, to form at least one droplet. When the driving signal is made in pulse shape, growth and shrinkage can be effected instantly and adequately, whereby discharging of liquid (ink) particularly excellent in response characteristic can be more preferably accomplished. As the driving signal shaped in such pulse shape, those described in U.S. Patents 4,463,359 and 4,345,262 are suitable. Further excellent recording can be effected by employment of the conditions described in U.S. Patent 4,313,124 which is the invention concerning the temperature elevation rate of the above heat acting surface. As the constitution of the recording head, in addition to the combined constitution of discharge port, liquid path, electrothermal transducer (linear liquid path or right angle liquid path), the constitutions by use of U.S. Patents 4,558,333 and 4,459,600 disclosing the constitution wherein the heat acting portion is arranged in flexed region are also included in the present invention. Additionally, the present invention is also effective if the constitution may be made on the basis of Japanese Laid-open Patent Application No. 59-123670 disclosing the constitution with a slit common to a plurality of electrothermal transducers as the discharge portion of the electrothermal transducers or Japanese Laid-open Patent Application No. 59-138461 disclosing the constitution in which openings absorbing pressure wave heat energy are made correspondent to the discharge portion. Further, as the recording head of the full-line type having a length corresponding to the maximum width of the recording medium which can be recorded with the recoding device, either a constitution satisfying its length or a constitution formed integrally as one recording head according to the combination of the plurality of recording heads as disclosed in the above-mentioned specification, but the present invention can exhibit the effects as described above further effectively. In addition, the present invention is also effective for a recording head of the freely interchangeable chip type, which enables electrical connection to the main device and supply of ink from the main device by being mounted on the main device, or the case by use of a recording head of the cartridge type integrally provided on the recording head itself. Also, addition of a restoration means, a preliminary auxiliary means of the recording head provided as the constitution of the recording apparatus of the present invention is preferable, because the effects of the present invention can be further stabilized thereby. To mention these in more detail, capping means, cleaning means, pressurization or suction means, pre-heating means with an electrothermal transducer, another heating element different from this or a combination of these, and practice of preliminary discharge mode which performs discharge separately from recording are also effective for performing stable recording. Further, as the recording mode of the recording apparatus, the present invention is effective for not only the recording mode of the main color alone such as black, etc., but also for the device equipped with plural colors of different colors or at least one of full-color by color mixing, either by way of integrated constitution of recording heads or a combination of plural recording heads. In the Examples of the present invention as described above, ink is described as liquid, but even an ink which is solidified at room temperature or lower may be employed, provided that it is liquid when used for recording, since it is generally practiced to control the viscosity of the ink by temperature control under stable discharge range, which is softened or liquid at room temperature, or by temperature control of the ink itself within the range of 30 o C to 70 o C in the ink jet as described above. In addition, use of an ink having the property which is for the first time liquefied by heat energy is also applicable to the present invention, such as one in which temperature elevation of heat energy is positively prevented by using it as the energy for the state change from the solid state to the liquid state, or which is solidified under the state left to stand for the purpose of preventing evaporation of ink, anyway one which is discharged as ink liquid by liquefaction of ink by imparting heat energy corresponding to signals or one which already begins to be solidified when reaching the recording medium, etc. In such case, the ink may be made the state held as the liquid or solid product in concavities or thru-holes of a porous sheet, and in the form opposed to the electrothermal transducer, as described in Japanese Laid-open Patent Application No. 54-56847 or Japanese Laid-open Patent Application No. 60-71260. In the present invention, the most effective for the respective inks as described is one which implements the film boiling system as described above.

Claims: A substrate for a liquid jet recording head, comprising: a support member (105); and a plurality of electrothermal transducers (111) provided on said support member, said transducers (111) each having a heat generating resistance layer (107), a pair of electrodes (103, 104) connected to said heat generating resistance layer (107) and a heat generating portion (102) formed by a portion of said heat generating resistance layer between said pair of electrodes (103, 104), said heat generating portion (102) generating thermal energy utilized for discharging a liquid droplet, the electrical resistance of the heat generating layer of the several transducers (111) differing depending upon the position of each transducer on the support member, characterized in that the dimensions of the heat generating portions (102) of the several transducers (111) are varied depending upon the electrical resistance of the resistance layer (107) at each transducer so that the transducers (111) each have a foaming voltage which is substantially the same as that of the others. A substrate as claimed in Claim 1 in which the transducers have a protective layer (108) on them to protect them from the ink, the thickness of the upper layer (108) of the several transducers (111) differs depending upon the position of each transducer on the support member, and the dimensions of the heat generating portions (102) of the several transducers are varied depending upon the thickness of the upper layer (108) at each transducer so that the transducers each have a foaming voltage which is the same as that of the others. A substrate for liquid jet recording head according to Claim 1 or 2, wherein the heat generating portions (102) of the transducers are all rectangular, the areas of said heat generating portions are substantially equal to each other, and said dimensions are varied by varying the ratio of the lengths of the sides of said heat generating portions. A liquid jet recording head comprising a substrate according to any previous claim, a liquid chamber (404), means defining liquid paths (401) leading from the liquid chamber (404) with a heat generating portion (102) of each transducer (111) being located in each liquid path and with each liquid path (401) terminating in a discharge port (402). A full line type liquid jet recording head comprising a recording head according to claim 4 having a length corresponding to the width of the medium to be recorded or a plurality of recording heads as claimed in claim 4 together having a length corresponding to the width of the medium to be recorded. A method of manufacturing a substrate for a liquid jet recording head, as claimed in any of claims 1-5, comprising: providing a support member (105); forming a plurality of electrothermal transducers on said support member, said transducers each having a heat generating resistance layer (107), a pair of electrodes (103, 104) connected to said heat generating resistance layer (107) and a heat generating portion (102) formed by a portion of said heat generating resistance layer between said pair of electrodes (103, 104), said heat generating portion generating thermal energy utilized for discharging a liquid droplet, the electrical resistance of the heat generating layer of the several transducers (111) differing depending upon the position of each transducer on the support member, characterized by the step of varying the dimensions of the plurality of heat generating portions (102) of the several transducers (111) depending upon the electrical resistance of the resistance layer (107) at each transducer so that the transducers (111) each have a foaming voltage which is substantially the same as that of the others. A method as claimed in Claim 6, comprising the further steps of forming a protective layer (108) on the transducers (111), the thickness of the protective layer (108) differing depending upon the position of each transducer on the support member, and the dimensions of the heat generating portions (102) being varied depending upon the thickness of the upper layer (108) at each transducer so that the transducers each have a foaming voltage which is the same as that of the others. A method according to Claim 6 or 7, wherein the plurality of heat generating portions (102) of the transducers are all rectangular, the areas of said heat generating portions are substantially equal to each other, and said dimensions are varied by varying the ratio of the lengths of the sides of said heat generating portions. A method as claimed in Claim 6, 7 or 8, comprising the steps of: measuring previously the respective sheet resistances of the plurality of heat-generating portions comprising the portions of said heat-generating layer positioned between said pair of electrodes, forming said heat-generating portions with varied dimensions of said plurality of heat-generating portions so that the resistance values may be substantially equal to each other corresponding to the respective sheet resistances measured in said step. A method as claimed in Claim 6, 7 or 8, comprising the steps of: measuring previously the change in layer thickness of said upper layer; and forming the heat-generating portions with respective varied dimensions so that the foaming voltages within the recording head may become substantially constant with each other corresponding to the layer thickness data of said upper layer measured in said step. A method of manufacturing a liquid jet recording head includes the step of incorporating a substrate manufactured by the method of any one of claims 6 to 10.

Inventors: KOMURO HIROKAZU, KOMURO, HIROKAZU
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1990
Main classification: B41J2
IPC codes: B41J2