RESISTIVE RIBBON FOR USE IN RESISTIVE RIBBON THERMAL TRANSFER PRINTING

Abstract: The invention relates to a resistive ribbon (10) for use in a resistive ribbon thermal transfer printing process, of the type comprising a resistive layer (12) which produces localised heating to effect printing when an electric current is passed therethrough and which has a non-linear current-voltage characteristic occurring at a knee voltage, an ink layer (16) comprising an ink which is transferable when heated by the localised heating, and a metal layer (14) located between between the resistive layer (12) and the ink layer (16) and along which the electrical current passes. A ribbon according to the invention is characterised by the inclusion of an electrical interface layer (18) located between the resistive layer (12) and the metal layer (14) and serving to increase the interface resistance between the resistive layer (12) and the metal layer (14) and to increase the knee voltage of the current-voltage characteristic.

Description: This invention relates to a resistive ribbon for use in a printing process involving the resistive ribbon thermal transfer of ink from a ribbon to a print medium. The art of non-impact printing is becoming increasingly popular for producing high quality written material, where such characteristics are desirable. Among the non-impact printing techniques, thermal transfer printing has proved particularly desirable where high quality, low volume printing is necessary, such as in computer terminals and typewriters. In thermal transfer printing, ink is printed on the surface of a receiving material (such as paper) whenever a fusible ink layer brought into contact with the receiving surface is softened by a source of thermal energy. The thermal energy can be supplied from a source of electricity, the electrical energy being converted to thermal energy. In one type of thermal transfer printing, termed resistive ribbon thermal transfer, a thin ribbon is used. The ribbon generally comprises either three or four layers, including a support layer, a layer of fusible ink that is brought into contact with the receiving material, and a layer of electrically resistive material. In a variation, the resistive layer is thick enough to be the support layer, so that a separate support layer is not needed. A thin electrically conductive layer is also optionally provided to serve as a current return. In order to transfer ink from the fusible ink layer to the receiving material, the layer of ink is brought into contact with the receiving surface. The ribbon is also contacted by an electrical power supply and selectively contacted by a thin printing stylus at those points opposite the points on the receiving material where it is desired to print. When current is applied to the thin printing stylus, it travels through the resistive layer and causes local resistive heating, which melts a small volume of ink in the fusible ink layer. This melted ink is then transferred to the receiving medium to effect printing. Resistive ribbon thermal transfer printing is described by way of example in US-A-3,744,611; A-4,309,117; A-4,400,100; A-4,491,431; and A-4,491,432. In resistive ribbon thermal transfer printing, it is often the situation that the points of contact of the support layer with the printing head become unduly heated and debris accumulates on the printhead. This increases contact resistance and develops heat in the printhead. To overcome the accumulation of debris and the increasing contact resistance, the amplitude of the applied current has to be increased. This is disadvantageous, however, because it can produce adverse fumes and ruin the support layer. A technique for reducing the amount of power required to be supplied by the printhead in a resistive ribbon thermal transfer process is described in IBM Technical Disclosure Bulletin, Vol. 23, No. 9, Feb. 1981, at page 4302. In this approach, a bias current is provided through a roller into the resistive layer located in the printing ribbon. The bias current produces some heating so that not all of the energy required to melt the ink has to be applied through the printhead. US-A-4,470,714 describes an improved resistive ribbon for use in thermal transfer printing. As noted in this specification, prior art attempts to provide resistive ribbons for thermal transfer printing typically encountered significant limitations. For example, the material selected to support both the fusible ink layer and the resistive layer has been difficult to adhere to other layers of the ribbon. Another problem arises because the same supporting layer may act as a thermal barrier to the transfer of heat from the resistive layer to the ink layer, thereby impeding the printing process. Additionally, the resistive layers of prior art ribbons have typically comprised graphite dispersed in a binder. Since these resistive layers require a great deal of energy for heating, it has sometimes been the situation that the resistive layer would burn through before printing occurred, with the release of adverse fumes. In order to overcome these obstacles, the resistive ribbon described in the aforementioned US-A-4,470,714 includes the use of an inorganic resistive layer, preferably comprising a binary alloy. One example of such a resistive layer is a metal silicide layer. These resistive materials were used to induce resistive heating at very low energy inputs and to avoid the need for a polymeric binder in the resistive layer. This was to eliminate the burn-through problem described above, and also to avoid the possibility of toxic fumes, which may occur when polymeric binders are used. In resistive ribbons of the prior art, and especially as typified by US-A-4,470,714, a particular characteristic often appeared which could be troublesome. This characteristic was a switching behaviour in which the impedance level of the resistive layer changed at a certain voltage. At initial non-printing voltages, the materials of the prior art would exhibit high impedance. However, when a certain voltage was reached (termed the knee voltage), the resistive material would switch to a low impedance state. As a result, a "holding" voltage (i.e., the voltage associated with the low impedance state) was obtained wherein the current through the resistive layer sharply increased. The holding voltage in these materials (such as the binary alloys) is typically about 1.5 volts. The presence of this switching behaviour means that constant current power sources can be used only with difficulty, and therefore constant voltage power sources have been preferred. Since resistive layers commonly require a certain level of power in order to induce sufficient resistive heating to adequately melt the fusible ink layer, it is preferable that the voltage of the low impedance state (in which printing occurs) should be as high as possible. For a constant power, this means that the magnitude of the required current can be brought into the range available from the power supply. In the prior art, it has not been possible to increase interface resistance between the resistive layer and the electrically conductive layer and the knee voltage beyond approximately 6 volts. Further, it has not been possible to provide resistive ribbons having enhanced interface resistance and knee voltage while still providing ribbon flexibility and durability, as well as good adhesion between the various layers of the ribbon. Still further, in previous resistive ribbons using aluminium having a coating of aluminium oxide thereon, other difficulties arose. While these films would exhibit an impedance switching behaviour, it was very difficult to enhance the knee voltage and interface resistance to desired levels. Further, the aluminium oxide films cannot be produced as continuous, pinhole-free films having reproducible and controllable properties. The object of the present invention is to provide an improved resistive ribbon for use in a resistive ribbon thermal transfer printing process. The invention relates to a resistive ribbon, for use in a resistive ribbon thermal transfer printing process, as defined in claim 1. The additional electrically resisting interface layer is used to provide enhanced electrical properties of the ribbon. In a preferred embodiment of the invention the additional layer has a thickness of less than about 100 nm (1000 angstroms) and is used to impart a non-linearity in the current-voltage characteristic of the ribbon. This non-linearity occurs at a knee voltage of greater than 6 volts. The onset of non-linearity is not reversible even over short time intervals. Thus, once the non-linearity is reached and the current-voltage characteristic changes to a low impedance state, a reduction in current will not cause the same curve to be followed. Thus, an essentially constant voltage can be used, where the voltage is in excess of 6 volts. The additional layer in the resistive ribbon, termed the electrical interface layer, is continuous and pinhole free, and can be made with constant thickness by well known techniques. Generally, the electrical interface layer comprises a polymer so that solvent casting, plasma polymerization, etc. can be used to deposit the layer. A suitable class of materials for the electrical layer is alkylalkoxy silanes having the general formula: (RO) m - Si - (R') 4-m where m = 1,3 (non-symmetrical materials) m = 2,4 (symmetrical materials) R = -CH₃, (CH₂) p - CH₃ p = 0,1,2,3 R'= (CH₂) n - CH₃ n = 0,1,2,...,21, and branched isomers thereof. if m = 1 or 3, these materials are non-symmetrical, and will enhance both interface resistance and knee voltage. However, if m = 2 or 4, the materials will be symmetrical and the primary effect of the electrically resisting layer will be an enhancement of the interface (if the knee voltage is enhanced, it is only by a very small amount when symmetrical alkylalkoxy silanes are used). The improved resistive printing ribbon described above provides printing at lower currents and with higher speed, without requiring techniques such as chemical heat amplification. Lower printing currents are also provided in a controllable manner without causing electrode fouling. Still further, both the interface resistance and the knee voltage are simultaneously enhanced by the use of the electrically resisting layer. While the interface resistance and the knee voltage are enhanced, the possibility of switching and bi-stability is not a problem, and very high knee voltages can be obtained. As additional advantages, the electrical interface layer provides a very stable and inert interface which is not subject to environment or humidity problems. Also, the metal current-return layer can comprise metals other than Al including, for example, Au, Ni, Cu, stainless steel, etc. Different silanes have been used as bonding layers in resistive ribbons, as noted in the aforementioned US-A-4,400,100. In that patent, a thin organic adhesion promoter is used between the resistive layer and the aluminium current-return layer. The adhesion promoter is an alkoxysilane compound including an amine for bonding the polycarbonate resistive layer and a siloxane for bonding with the aluminium. No mention is made of the electrical properties of the adhesion promotion layer. Further, adhesion promotion layers can be very thin, for example, one monolayer, which would be too thin to affect the electrical properties of the ribbon. In addition to these differences, where the electrical interface layer of a ribbon in accordance with the present invention is an alkylalkoxy silane, no amine group is used. This contrasts with the adhesion layer of US-A-4,400,100, where an amine group is required for adhesion to the polycarbonate resistive layer. In order that the invention may be more readily understood an embodiment will now be described with reference to the accompanying drawings, in which: FIG. 1 is a schematic illustration of a resistive ribbon in accordance with the present invention, which can be used for printing applications when current is passed through the electrodes illustrated, FIG. 2 is a current-voltage (I-V) characteristic for the ribbon of FIG. 1, for different thicknesses of an electrical interface layer comprising of plasma polymerized octadecyltriethoxy silane, FIG. 3 is a plot of knee voltage V K versus thickness of the electrical layers in the ribbons having the I-V characteristics of FIG. 2, FIG. 4 is a plot of initial resistance, which is proportional to interface resistance, versus thickness of the electrical interface layer, where this interface layer comprises plasma polymerized octadecyltriethoxy silane, FIG. 5 is a plot of the current-voltage characteristics of a resistive ribbon in accordance with the present invention, where the electrical interface layer comprises a symmetrical alkylalkoxy silane, being in this example tetrabutoxy silane, FIG. 6 is a plot of the current-voltage characteristics for the resistive ribbon of FIG. 1, where the electrical interface layer comprises different thicknesses of the alkylalkoxy silane, which in this example is plasma polymerized butyltrimethoxy silane, FIG. 7 is a plot of current-voltage characteristics for another resistive ribbon in accordance with the present invention, where the characteristics were developed for different thicknesses of an electrical interface layer comprising butyltrimethoxy silane which was produced by plasma polymerizing a vapour of the silane introduced into a plasma chamber, FIG. 8 is a plot of current versus voltage for the resistive ribbon of FIG. 1, including an electrical interface layer comprising octadecyltriethoxy silane, where the I-V curves result from application of electrical pulses having different rise times, FIG. 9 is a plot of current versus voltage for the ribbon of FIG. 1, in which the electrical interface layer is plasma polymerized octadecyltriethoxy silane and the thin conductive layer is Au, and FIG. 10 shows examples of branched isomers which can be used in the electrical interface layer illustrated in FIG. 1. In the embodiment to be described the electrical characteristics of a resistive printing ribbon are improved by the inclusion of an additional layer between the resistive layer and the metal current-return layer. As will be noted, advantages in addition to the enhancement of electrical properties also result, since the electrical interface layer allows the use of metals other than aluminum as the metal current-return layer. As will become more apparent later, the enhanced electrical properties can include both an increase in the interface resistance between the resistive layer and the metal current-return layer and in the knee voltage, where both of these increases are dependent upon the thickness of this additional layer. Further, the onset of the non-linearity leading to the knee voltage is not reversible, even over very short time intervals (i.e., short electrical pulses and rapid pulse repetition times). The provision of this additional layer does not impair the flexibility of the resistive ribbon, and in many ways enhances its durability and mechanical stability by providing an interface which is inert to the environment. Referring now to FIG. 1, a schematic illustration of a resistive ribbon 10 and a structure required for resistive ribbon thermal transfer printing are shown. Ribbon 10 comprises a resistive layer 12, a thin metal current-return layer 14, an ink layer 16, and an electrical interface layer 18 located between the resistive layer 12 and the metal layer 14. An optional ink release layer (not shown) can be used between the metal layer 14 and the ink layer 16. A print electrode 20 and a portion of a large ground electrode 22 are also shown. The operation of the resistive ribbon printing technique is well known in the art, and will not be described in detail. When a current is provided through electrode 20, it will travel through the resistive layer 12, the electrical interface layer 18 and the metal layer 14, before returning to ground through the large ground electrode 22. This passage of electrical current causes heat to be developed in the resistive layer 12 and in the electrical layer 18 , particularly due to the increased interface resistnace between the resistive layer 12 and the metal layer 14 provided by the electrical interface layer 18. This localised heat is transmitted to the ink layer 16, causing it to be melted locally and transferred to a receiving medium, such as paper (not shown). The components which can be used for the resistive layer 12, the metal layer 14, the optional ink release layer, and the ink layer 16 are well known in the art. In the embodiment being described the materials forming these layers can be selected from any of the well known materials used for these layers. Resistive layer 12 can be comprise polycarbonate filled with graphite. For example, resistive combinations can be prepared from about 75%-65% polycarbonate, by weight, and from about 20%-35% of carbon, by weight. Other suitable materials for resistive layer 12 include polyimide containing about 20-35% carbon, polyester containing about 20-32% carbon, and polyurethane containing about 20-30% carbon. Of course, other polymeric materials may be used and the amount of carbon is selected to obtain the appropriate resistance. A representative thickness of the resistive layer 12 is approximately 17 micrometers, in a printing system using current pulses of 20-30mA. The thermally transferable ink layer 16 usually comprises a polymeric material which has a melting point of about 100°C, and a colour former. An example of a suitable ink is one which contains a polyamide and carbon black. These inks are also well known in the art (see, for example, Macromelt 6203 prepared by Henkel Corp. and containing carbon black). Ink layer 16 is typically about 5 micrometers thick. Metal layer 14 is used as a current-return layer, and is preferrably Al. However, in the embodiment being described other metals can be used including stainless steel, Cu, Mg, and Au. One advantage of the embodiment being described is that high quality printing will be obtained regardless of the metal which is used in layer 14, in contrast with prior art ribbons which often require a particular metal in order to provide good print quality. The thickness of layer 14 is typically about 100 nm (1000 angstroms). The electrical interface layer 18 is about 50-100 nm (500-1000 angstroms) in thickness, and is a uniform continuous, pinhole-free layer which can be easily formed on the resistive layer 12. In a preferred embodiment, layer 18 is a polymer comprised of alkylalkoxy silanes having the general formula: (RO) m - Si - (R') 4-m where m = 1,3 (non-symmetrical materials m = 2,4 (symmetrical materials) R = CH₃, (CH₂) p -CH₃ p = 0,1,2,3 R' = (CH₂) n -CH₃ n = 0,1,2,...,21 and branched isomers thereof. Examples of suitable branched isomers for the group R' are illustrated in Figure 10. The electrical interface layer 18 is chosen to be one which will increase the interface resistance between the resistive layer 12 and the metal layer 14 close to the ink transfer layer 16, and also one in which the knee voltage of the current-voltage characteristic of the ribbon is enhanced (i.e., increased). Specifically, the material of layer 18 is one which makes the knee voltage in excess of 6 volts. The resistivity of layer 18 can be varied depending upon its composition, and expedients such as doping can be used to adjust the interface resistance and knee voltage. As an example, thin layers of polymerized octadecyltriethoxy silane, 50-100 nm (500-1000 angstroms) thick, were coated on the resistive layers in three separate ribbons. In the first ribbon, the knee voltage of the ribbon without the electrical interface layer was about 7 volts. The presence of the electrical interface layer moved the knee voltage to a value between 9 and 12 volts. In the second ribbon, the initial knee voltage (i.e., without the electrical interface layer) was approximately 0 volts. The presence of an electrical interface layer comprising octadecyltriethoxy silane moved the knee voltage to 8 volts. In the third ribbon, the presence of the electrical interface layer provided an increase in knee voltage of approximately 4 volts. The polymer electrical interface layer 18 can easily be deposited by known techniques including plasma polymerization, vapour deposition, and solvent casting. Well known coating techniques such as blading, dipping, spraying, silk screening and the like can be used. In the case of plasma polymerization, either a liquid or a vapour can be introduced into the plasma chamber. For example, a resistive polycarbonate layer can be placed in a plasma chamber which contains vapours of alkylalkoxy silanes. Following a few minutes exposure, the thin electric interface layer 18 will be formed. As further examples, the following materials were coated as thin layers between a conductive polycarbonate layer (resistive layer) and an Al ground return layer, in order to form the electrical interface layer. These materials were: 1. Octadecyltriethoxy silane dissolved in alcohol; 2. Polydimethyl siloxane acetoxy terminated dissolved in kerosene or petroleum ether; and 3. Polyimide dissolved in 1 methyl 2 pyrrolidone. Each of these materials was coated on the surface of the polycarbonate by a roller and then dried in air or in a heated oven to form the electrical interface layer. Al was then deposited on the interface layer, and Current-Voltage measurements were undertaken. The improvements due to the electrical interface layers are illustrated in the following table. For the alkylalkoxy silane described above, it has been observed that the non-symmetrical silane compounds (when m=1, 3) exhibit both enhanced interfacial resistance and enhanced knee voltage. In contrast with this, symmetrical alkylalkoxy silanes (where m=2, 4) exhibit enhanced interface resistance, but do not significantly enhance the knee voltage. The reason for this difference is not fully known, but it is indicative of the unexpected uniqueness of this class of materials. Electrical Characteristics FIGS. 2-9 show the electrical characteristics of various ribbon samples, and illustrate the effects of the addition of the electrical interface layer to a ribbon. For example. FIG. 2 is a current-voltage (I-V) PLOT for a ribbon comprising a resistive layer of polycarbonate and a 1000 angstrom thick Al metal layer. Samples of this type of ribbon were made with different thicknesses of an electrical interface layer located between the resistive layer and the Al metal layer. The resulting I-V curves are shown in FIG. 2 for a ribbon with no electrical interface layer, and for ribbons with various thicknesses of the interface layer. These thicknesses were about 30, 50, 100, and 200-300 nm (300, 500, 1000 and 2000-3000 angstroms). Thus, curve A illustrates the ribbon where no electrical interface layer is present, while curves B-E show the I-V characteristics as the thickness of the interface layer increases from about 30 nm (300 angstroms) to about 200-300 nm (2000-3000 angstroms). In the ribbons used for the measurements in FIG. 2, the electrical interface was plasma polymerized octadecyltriethoxy silane. The presence of this layer enhanced the initial resistance and also enhanced the knee voltage V K of the ribbon, where V K is defined in the inset in FIG. 2. In order to eliminate the effect of contact reistance, 127 micrometers (5 mil) Au dots were deposited on the resistance layer. During the measurements 50 microsecond continuous voltage pulses were applied. This technique was also used to obtain the electrical characteristics illustrated in FIGS. 3-9. The electrical interface layer gives the ribbon a non-linear I-V characteristic in which the initial slope of each I-V curve is a measure of the interface resistance between the resistive layer 12 and the metal layer 14. As the thickness of the interface layer increases, this interface resistance increases. Thus, a resistance close to the ink layer is produced in order to have a sizeable quantity of heat produced in the region closest to the ink layer. These more favourable I-V curves allow printing at lower currents. FIG. 3 plots the knee voltage V K against the thickness of the electrical interface layer 18 (FIG. 1). This plot was obtained in the same manner, using sample ribbons having the I-V characteristics of FIG. 2. As is apparent from FIG. 3, the knee voltage V K increases with the thickness of the electrical interface layer in a manner which is non-linear with thickness. FIG. 4 is a plot of the initial resistance of a resistive ribbon as a function of the thickness of the electrical interface layer 18. This ribbon comprised a polycarbonate resistive layer and a 100 nm (1000 angstrom) thick Al layer. Various thicknesses of the electrical interface layer used between the resistive layer and the Al metal layer were used. In the samples used to plot FIG. 4, the electrical interface layers were plasma polymerized octadecyltriethoxy silane compound. Their thicknesses were between 0 and 100 nm (0 and 1000 angstroms). In FIG. 4, the initial resistance increases substantially linearly with the thickness of the electrical interface layer. The initial resistance comprises the interface resistance and a small series resistance, and is substantially proportional to the interface resistance. The results of FIG. 4 are consistent with those in FIG. 2, where the initial portions of the I-V curves showed increasing resistance as the thickness of the electrical interface layer increased. FIG. 5 is an I-V plot for some sample ribbons, which comprised a graphite-filled polycarbonate layer as the resistive layer and a 100 nm (1000 angstrom) Al layer. Located between the resistive layer and the Al layer was a plasma polymerized alkylalkoxy silane. For this set of data, a symmetrical alkylalkoxy silane, tetrabutoxy silane, was used. Curve A illustrates the ribbon characteristic when no interface layer is present, while curves B-D indicate the presence of increasing thicknesses of the electrical interface layer. For example, the ribbon used to provide curve D had a thicker electrical interface layer than the ribbon of curve C, which in turn had a thicker electrical interface layer than the ribbon used to obtain curve B. The interface resistance was enhanced using this symmetrical alkylalkoxy silane, but the knee voltage was not significantly enhanced. Although some improvement in knee voltage is obtained, the amount of increase in V K is not as great as when nonsymmetrical alkylalkoxy silanes are used. FIG. 6 shows the I-V characteristics of 3 ribbons, as presented by curves A, B, and C. Curve A is for a ribbon which did not include an electrical interface layer, but which included layers of resistive material and a metal current-return conductor. In this case, the resistive layer was graphite-filled polycarbonate, while the metal layer was 100 nm (1000 angstroms) of Al. Curves B and C show the I-V characteristics of the same ribbon, but in which an electrical interface layer comprising plasma polymerized butyltrimethoxy silane was used between the resistive layer and the Al layer. The thickness of the electrical interface layer is greater in the ribbon used to derive curve C than that in the ribbon used to derive curve B. Butyltrimethoxy silane is a non-symmetrical alkylalkoxy silane, and therefore both the interface resistance and the knee voltage of the ribbon are increased by incorporation of this electrical interface layer. The increases in interface resistance and the knee voltage are greater as the thickness of the electrical interface layer is increased. FIG. 7 shows three I-V curves for resistive ribbons in which the presence of the electrical interface layer shifts the I-V characteristic. Curve A is that for a ribbon which does not contain an electrical interface layer, the ribbon comprising a graphite-filled polycarbonate resistive layer and a thin layer of Al. Curves B and C are for the same ribbon, except that an electrical interface layer is included between the resistive layer and the Al layer. The electrical interface layer is the same as that used to obtain the curves of FIG. 6, butyltrimethoxy silane, but in this case this silane was produced by introducing a vapour rather than a liquid into a plasma chamber. Further, the thicknesses of the electric interface layers used in the ribbons of FIG. 7 are greater than the thicknesses of the electrical interface layers used in the ribbons of FIG. 6. This is the primary reason why the ribbons of FIG. 7 exhibit greater interface resistances and knee voltages than the ribbons of FIG. 6. FIG. 8 is an I-V plot for a resistive ribbon including an electrical interface layer comprising octadecyltriethoxy silane located between a graphite-filled polycarbonate resistive layer and an Al metal layer, where the curves are generated for different rise times t of an applied ramp pulse having a peak voltage of 14.5V. The thicknesses of the electrical interface layers were 50-100 nm (500-1000 angstroms). From these curves, it is apparent that the amount of energy delivered to the ribbon has an effect on the electrical properties of the ribbon, there being a type of non-linear breakdown when the pulse width (rise time) becomes suffiently great that a large quantity of energy is supplied to the electrical layer. FIG. 9 shows the I-V characteristics of a ribbon without an electrical interface layer (curve A) and 3 ribbons of identical structures, except that they each include an electrical interface layer (curves B, C, D). All of these ribbons comprised a resistive layer of graphite filled polycarbonate, and a thin metal current return layer of 100 nm (1000 angstroms) thickness. The interface layers were plasma polymerized octadecyltriethoxy silane of thicknesses of about 50 nm (500 angstroms) (curve B), 100 nm (1000 angstroms) (curve C), and 200-300 nm (2000-3000 angstroms) (curve D). For these ribbons, the metal current return layer was Au, in contrast to the Al metal layer of, for example, the ribbons of FIG. 2. The presence of the Au layer in contrast to an Al layer changes the I-V characteristics somewhat, as can be seen by comparing FIGS. 2 and 9, in which the ribbons used differed only in the metal forming the current return layer. When the current return layer is Au, the interface resistance and knee voltage are less than when the current return layer is Al. This is most likely due to the fact that when Al is used, a thin Al₂O₃ layer forms that increases interface resistance and knee voltage. An oxide layer will not be formed on a Au layer. For all metals, however, there is a significant increase in interface resistance and knee voltage when the ribbon includes an electrical interface layer of the type described. As noted previously, it is possible to alter the electrical characteristics of the electrical interface layer by changing its resistivity, etc., as for instance, by doping the electrical interface layer. For example, an electrical interface layer comprising polyimide can be doped with carbon to change the electrical resistivity of that layer. The doping will also affect the interface resistance and the knee voltage of the ribbon. In the embodiment described, a thin electrical interface layer is placed between the resistive layer and the metal current-return layer in a resistive printing ribbon, for the purpose of altering the electrical characteristics of the ribbon. The electrical interface layer can be used in any type of resistive ribbon, such as those with organic resistive layers and those with inorganic resistive layers. The electrical interface layer is chosen to make the knee voltage of the I-V characteristic of the ribbon greater than about 6 volts, and to increase the interface resistance. The electrical interface layer must be a continuous, pinhole-free layer whose presence does not alter the flexibility, stability, and durability of the ribbon. In order to achieve these characteristics, the electrical interface layer must be very thin and for this reason is less than approximately 100 nm (1000 angstroms) in thickness. At this thickness, it must provide the required electrical properties and, therefore, polymer films are preferred. Such films can be applied in a variety of conventional processes to provide uniform thickness and substantially uniform composition in order to have the electrical properties of this layer be substantially uniform throughout the length of the ribbon. In this regard, it is known that metal oxides, such as Al₂O₃, cannot be made pinhole-free at such small thicknesses, and do not exhibit the required electrical properties, especially in a uniform manner throughout the length of the ribbon. It is envisaged that polymer films other than those described can be provided which will produce the required electrical results described above, while at the same time not adversely affecting the mechanical and chemical properties of the ribbon.

Claims: A resistive ribbon (10), for use in a resistive ribbon thermal transfer printing process, comprising a resistive layer (12) which produces localised heating to effect printing when an electric current is passed therethrough, and which has a non-linear current-voltage characteristic occurring at a knee voltage, which is dependent on the rise time of a saw tooth pulse in the electrical current, an ink layer (16) comprising an ink which is transferable when heated by said localised heating, and a metal layer (14) located between said resistive layer (12) and said ink layer (16) and along which said electrical current passes, characterised by the inclusion of a continuous, substantially pin-hole free, electrically resisting interface layer (18) located between said resistive layer (12) and said metal layer (14) having a thickness of at least 50 nm (500 angstroms) and serving to increase the electrical interface resistance between said resistive layer (12) and said metal layer (14) and to increase the knee voltage of said current-voltage characteristic. A ribbon as claimed in claim 1, characterised in that said electrically resisting interface layer is less than about 100 nm (1000 angstroms) thick. A ribbon as claimed in either of the preceding claims, characterised in that said electrically resisting interface layer is formed from a monomer. A ribbon as claimed in claim 3, characterised in that said monomer is selected from the group consisting of the alkylalkoxy silanes having the formula: (RO) m - Si(R') 4-m where m = 1,3 (non-symmetrical materials) m = 2,4 (symmetrical materials) R = - CH₃ , (CH₂) p - CH₃ p = 0, 1, 2, 3 R' = (CH₂) n - CH₃ n = 0, 1, 2, .......,21, and branched isomers thereof. A ribbon as claimed in claim 4, characterised in that m = 2, 4. A ribbon as claimed in claim 4, characterised in that m = 1,3. A ribbon as claimed in claim 1, characterised in that said resistive layer is formed from a polymer and said metal layer is chosen from the group consisting of Al, Ni, Cu, stainless steel and Au. A ribbon as claimed in claim 7, characterised in that said polymer is polycarbonate.

Inventors: AVIRAM, ARI, SHIH, KWANG KUO
Applicants: LEXMARK INTERNATIONAL, INC.
Application year: 1986
Main classification: B41J31
IPC codes: B41M5, B41J31