Halftone image recording device

Abstract: The invention makes it possible to drive a halftone image recording device and achieve high halftone reproduction by allowing at least one of the leading and trailing edges of a pulse width-modulated signal applied to a recording head, or forming amplitude- and width-modulated pulses, respectively, as driving pulses for placing one dot under halftone control, and changing a pulse width change of pulse width modulation in a stepwise manner, using the pulse width of the amplitude-modulated pulse as a unit pulse width. The invention intends to achieve high-voltage and high-speed pulse output and low power consumption by converting input data such as halftone image data to a voltage signal, superposing pulse voltages of opposite polarities and applying the resulting signal to a switching circuit constituting an output state in the form of a switching signal, and also makes it possible to achieve high speed and high-voltage driving by connecting at least one of equivalent two-terminal elements in series to at least one of the respective driving elements of a complementary FET driving circuit, said equivalent two-terminal elements are each put on with a current of a certain or higher value passing therethrough to show constant-voltage characteristics and put off with a current of a certain or lower value passing therethrough to become a constant resistance.

Description: The present invention relates to halftone image recording hardware for controlling a charge flow such as an ion flow for recording halftone images and to a high voltage-resistant circuit that enables such recording hardware to work at high speed. Some proposals have so far been made of a slit control type of image recorder harnessing corotron discharge in which ions generated by corotron discharge are introduced in a slit and the resulting ion flow is controlled by varying an electric field within the slit wall to form a charge pattern on a recording medium, an aperture control type of image recorder making use of corotron discharge in which ions generated by corotron are passed through apertures in two control electrodes while controlling an electric field between them, and the resulting ion flow that goes toward a recording medium is placed under on-off control to form a charge pattern on the recording medium, and an aperture control type of image recorder harnessing solid discharge in which high-frequency voltage is applied between electrodes with an insulator located between them to induce discharge and the resulting ions are selectively drawn by electric field control to form a charge pattern on a recording medium. In accordance with the image recorders harnessing such an ion flow, the ion flow is constricted by reducing the magnitude of the electric field between the ion flow-control electrodes, making the resulting dot diameter small and, at the same time, giving rise to dot density variations. On the other hand, as the magnitude of the electric field between the electrodes controlling the ion flow increases, there is an increase in the diameter of the ion flow, which concurs with dot density variations. In either case, it is possible to form halftone images by inter-electrode field control. Alternatively, when the application time of the electric field is varied while the magnitude of the electric field between the ion flow-controlling electrodes remains constant, the quantity of charges formed on the recording medium varies and so there is a change in the degree of distortion of the electric field by these charges. Consequently, the resulting latent image potential increases with a dot diameter increase. Here, too, it is possible to form halftone images. When forming halftone images with a controlled ion flow, it is structurally very difficult to control applied voltage, thereby varying the intensity of the electric field between the control electrodes, because the voltage applied to the electrode for ion flow control is as high as a few hundred volts. By contrast, it is structurally easy to control the voltage-applying time while the voltage applied to the control electrodes remains constant, because this is achieved by making use of pulse width modulation techniques. For this reason, a proposal has been made of image recording hardware making use of such halftone reproduction methods (see JP-A-60-175062 and 61-228771). Incidentally, when it is intended to carry out halftone reproduction by pulse width control modulation with an aperture control type of image recorder that harnesses solid discharge, the magnitude of latent image potential changes stepwise rather than linearly. This phenomenon will now be explained with reference to Figs. 1 to 3. Fig. 1 is a representation for illustrating an aperture control type of image recorder that makes use of solid discharge and is driven by alternating currents. A recording head shown generally at 1 is built up of a line electrode 1b and an insulator 1c stacked on an insulator 1a in this order. A central aperture is defined by a finger electrode 1d, an insulator 1e and a screen electrode 1f, and a high-frequency power source 5 is connected between the line and finger electrodes 1b and 1d. A signal source 6 is connected between the finger and screen electrodes 1d and 1f for the application of signal voltage. An insulating, recording member 2 provided with an electrode 3 is located in opposition to the recording head 1, and a direct-current power source E is connected between the recording head 1 and the recording member for ion flow acceleration. This image recorder works as follows. Ion generation is induced by intra-head discharge caused by the application of a high-frequency voltage of a few KV to a few MHz between the line and finger electrodes 1b and 1d. A flow of the resulting ions is controlled in dependence on signal voltage between the finger and screen electrodes 1d and 1f. This signal voltage or, in other words, a pulse width modulation signal is then varied in terms of width t in dependence on signal strength, as shown in Fig. 2 with TO representing the maximum signal width, whereby an electrostatic latent image having halftones is formed on the recording member. When such a signal of modulated pulse width is furnished to the recording head 1, the potential on the surface of the recording member varies with respect to a pulse width change in a stepwise form, as shown in Fig. 3; in other words, its variation is neither linear nor smooth. To see this, such a sine wave as shown in Fig. 4(a) was used as the high-frequency voltage to the recording head to measure the resulting ion flow. As a result, it was found that, as shown in Fig. 4(b), it is only at the peak of the high-frequency voltage that the ion flow can be detected or, to put it another way, the resulting ion flow is discrete. Even when there was a pulse width change between t1 and t2 that define the positions at which an ion flow is to occur, as shown in Fig. 4(c), there was neither any ion flow nor any change in the surface potential of the recording member. In addition, the moment the pulse width exceeded t2 slightly, there was an ion flow increase, making the surface potential variable in a stepwise form and so making it difficult to obtain variable or high contrast. So far, the formation of halftone images by use of an ion flow control type of image recorder has relied on voltage amplitude, pulse width or sawtooth wave modulation, but a problem with achieving high-speed driving and high contrast is how many halftones are attained for a certain time. That is to say, the determination of what driving speed is applied permits the determination of the time τ needed to print one dot. For instance, halftone control must be achieved at a time τ, when it is intended to reproduce 256 halftones. In this regard, low-speed driving offers no problem, but it is still very difficult to achieve high-contrast expression in the case of high-speed driving. For hardware such an ion printer that works at a few hundred volts, a voltage amplifier circuit of high input impedance and excellent in linearity is usually used so as to amplify halftone image data to a predetermined voltage, and a variety of D-A converters such as those of the resistance and integral types are used as well. However, use of an ordinary voltage amplifier circuit makes it difficult to obtain high voltage as high as a few hundred volts, resulting in some considerable expense. It is also difficult to obtain high-voltage and high-speed outputs having rectangular waves, because the through-rate of the voltage amplifier circuit is not very high. For instance, in the case of a transistor element allowed to have an amplification action, the degree of amplification may be increased by making loading resistance large and current consumption small, but there is a driving speed drop. On the other hand, higher driving speed may be achieved by decreasing loading resistance, but current consumption may be increased with a decrease in the degree of amplification. In short, no tradeoff is achieved between high-speed and low power consumption. In the case of capacitive loading, it is only at a waveform rise or fall time that the output current flows, but currents through loading resistance and transistor elements flow constantly at a high output level, incurring a power consumption increase. The D-A converters, when built up of ICs, unexceptionally produce only low-voltage output. In addition, when it is intended to set up discrete circuits, such problems as mentioned above arise, usually because of the need of using a voltage amplifier circuit. Conventional or ordinary D-A converters, because of being designed to obtain a continuos form of output, do not lend themselves well for ion printers, plasma displays, and so on, for which a discrete, high-voltage rectangular waveform of pulses must be produced. In addition, circuits for driving ion printers, plasma displays, and so on are presumed to work in the form of a parallel array of many identical circuits. To achieve this, however, lower power and lower cost are needed. Besides, driving circuits with built-in FETs are available for driving ion printers, etc. Fig. 5 is an illustration of a typical driving circuit using a complementary FET. As illustrated, an N-channel FET 11 and a P-channel FET 12 are connected in series, and 0 V and 15 V, for instance, are added to this series circuit as gate input. Connected to the gate of P-channel FET 12 is a level shifter 13 for converting 0 or 15 V to the on-off control signal level of P-channel FET 12. Then, 0 V and 15 V are alternately fed to the gates of N-channel FET 11 and P-channel FET 12 to put them on and off to achieve low and high-level outputs. Fig. 6 is an illustration of a typical driving circuit using resistance loading. As illustrated in Fig. 6(a), a resistance R is connected to the drain side of an N-channel FET 14. At a gate input of 15 V, FET 14 is put on to produce nothing, whereas at a gate input of 0 V, FET 14 is put off to produce low- and high-level outputs. Fig. 7 is a typical representation of a totem pole combination of N-channel FETs, in which a buffer is provided to a resistance load type of circuit shown by a broken line in Fig. 7(a). With this circuit, it is possible to obtain a large output current by a buffer 18 and to achieve a sharp rise as well. Fig. 8 is an illustration of a typical high voltage-resistant driving circuit built up of a series combination of low voltage-resistant P-channel FETs 20 and 21. This circuit is designed to work such that putting P-channel FET 21 off causes P-channel FET 20 to be off, and putting P-channel FET 21 on gives rise to putting P-channel FET 20 on. This circuit is allowed to withstand high voltage because of a series combination of P-channel FETs 20 and 21. Illustrated in Fig. 5 is a basic driving circuit, but this is unsuitable for a high-voltage driving circuit, because much difficulty is now involved in procuring P-channel FETs having a voltage resistance of 300 V or higher. The circuit of Fig. 6 can work at high speed and at a short output waveform fall time, but its rise characteristics are generally not well, because it depends on the value of resistance R and output load, as shown in Fig. 6(b). When the value of R is reduced so as to improve its rise characteristics, there is a current increase when N-channel FET 14 is put on, resulting in a power consumption increase. The circuit of Fig. 7 is favorable for large capacity loading, but a similar problem as in the resistance loading type circuit of Fig. 6 arises under a capacitive load almost similar to the gate input capacity of an FET. In short, the value of resistance R must be reduced so as to allow N-channel FET 17 to work at high speed, but this results in a power consumption increase. The circuit of Fig. 8 may be made high-resistant to voltage, because of being built up of a series combination of P-channel FETs, but it cannot work at high speed due to a time constant ascribable to resistance R and the capacities of the FETs. When the value of R is reduced so as to achieve high-speed performance, there is a current increase when N-channel FET 19 is put on, as in the circuit of Fig. 6, only to give rise to a power consumption increase. US-A-4,679,057 discloses an electrophotographic apparatus, in which a laser beam modulated by an image signal is irradiated to a photosensitive member to form an electrostatic latent image and a toner image is obtained. Gradation is provided by simultaneously performing pulse width-modulation and amplitude-modulation. EP-A-0,451,770 discloses an electrophotographic apparatus, in which a laser beam modulated by an image signal is irradiated on a photosensitive member to form an electrostatic latent image, and a toner image is obtained. The amplitude-modulation is performed on a triangular wave with a density signal, and a semiconductor laser is driven by a modulation signal; the photosensitive member is irradiated. An electrostatic latent image is formed by attenuating the potential on the photosensitive member by the intensity of the irradiated light. JP-60-219,071 shows the waveform of an ion current generated from the corona wire. By gate control using ON and OFF signals applied on a gate terminal, the width and size of the signal to be applied to the recording electrode are changed and the charge flow is controlled to perform gradation recording. Thus, the recording diameter is controlled by pulse width modulation. An object of the invention is to provide a halftone image recorder apparatus that makes good-quality halftone reproduction feasible. Another object of the invention is to provide an aperture control type of image recorder apparatus by alternating-current driven solid discharge, which can be used to smooth a surface potential change in a recording member with respect to pulse width, thereby achieving good-quality halftone reproduction. These objects are solved with the features of the claims. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a view that illustrates an alternating-current driven, aperture control type of image recorder operated by solid discharge, Figure 2 represents a rectangular pulse width-modulated signal, Figure 3 represents the relation between pulse width and surface potential, Figure 4 illustrates the phase relation between high-frequency voltage and rectangular pulse width-modulated signal, Figure 5 is a view showing a conventional complementary driving circuit diagram, Figure 6 represents a resistance loading type of driving circuit, Figure 7 is a totem pole-connected type of driving circuit diagram, Figure 8 is a conventional high voltage-resistant driving circuit diagram, Figure 9 represents a pulse width-modulated signal waveform with a time constant imparted to the trailing edge, Figure 10 represents a pulse width-modulated signal waveform with a time constant imparted to the leading edge, Figure 11 a pulse width-modulated signal wave form with time constants imparted to the leading and trailing edges, Figure 12 illustrates an embodiment of a waveform conversion circuit, Figure 13 illustrates another embodiment of the waveform conversion circuit, Figure 14 illustrates the principle of halftone expression according to the invention, Figure 15 represents a waveform with time constants imparted to the leading and trailing edges and surface potential obtained when this waveform is used, Figure 16 represents another waveform with time constants imparted to the leading and trailing edges and surface potential obtained when this waveform is used, Figure 17 represents the relation between pulse width and surface potential when triangular and square waves are used, Figure 18 represents a triangular wave with time constants imparted to the leading and trailing edges, Figure 19 illustrates one embodiment of a pulse width- and amplitude-modulated signal, Figure 20 illustrates another embodiment of the pulse width- and amplitude-modulated signal, Figure 21 is a rough representation of one embodiment of a driving circuit, Figure 22 is a rough representation of how the driving circuit works, Figure 23 is a rough representation of how ion generation occurs, Figure 24 is a conceptional illustration of a corotron type of ion printer, DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the halftone image recorder according to the invention will now be explained with reference to Figs. 9-18. This embodiment is characterized by imparting a time constant to at least one of the leading and trailing edges of a pulse width-modulated signal applied to a recording head. For instance, signals 30 and 31 that are pulse-widthwise modulated in correspondence to image signals are converted to signals 32 and 33 of a waveform with a time constant imparted to the trailing edge through a waveform conversion circuit to be described later, as illustrated in Fig. 9. In Fig. 10 signals 30 and 31 that are pulse-widthwise modulated in correspondence to image signals are converted to signals 34 and 35 of a waveform with a time constant imparted to the leading edge, and in Fig. 11, signals 30 and 31 that are pulse-widthwise modulated in correspondence to image signals are converted to signals 36 and 37 of a waveform with time constants imparted to the trailing and leading edges. Signals 32 and 33 having the waveform of Fig. 9 are obtained by subjecting the output of a signal power source 43 that generates a pulse width-modulated signal to waveform conversion through a waveform conversion circuit 40, as shown in Fig. 12(a). Waveform conversion circuit 40 is built up of switches S1 and S2, a resistance R1 and a capacitor C, and is designed such that switches S1 and S2 are respectively closed and opened at a pulse rise time to apply a pulse voltage to capacitor C, and switches S1 and S2 are respectively opened and closed at a pulse fall time for discharge by a time constant circuit defined by capacitor C and resistance R1. It is noted that this may be achieved by the mere application of the point of contact of switch S1 with resistance R1 to the electrode of the recording head. Waveform signals of Fig. 10 are obtained by a waveform conversion circuit 41 shown in Fig. 12(b). In waveform conversion circuit 41, switches S1 and S2 are respectively closed and opened at a pulse rise time, so that a time constant can be obtained by a time constant circuit comprising resistance R1 and capacitor C. At a pulse fall time, on the other hand, switches S1 and S2 are respectively opened and closed, so that capacitor C can be short-circuited and so is instantaneously discharged and then drops to ground potential. Waveform signals 36 and 37 of Fig. 11 are obtained by a waveform conversion circuit 42. In waveform conversion circuit 42, switches S1 and S2 are respectively closed and opened at a pulse rise time, so that a time constant can be provided by a charging curve due to a time constant circuit comprising resistance R2 and capacitor C At a pulse fall time, on the other hand, switches S1 and S2 are respectively opened and closed, so that a time constant can be provided by a charging curve due to a time constant circuit comprising capacitor C and resistances R1 and R2. As regards Fig. 10(b) and 11(b) wherein the time constants are imparted to the leading edges, the pulse peak value has been described as being approximately reached for a given time. Strictly speaking, however, some considerable time is needed until a constant voltage is reached. Therefore, in order to achieve a constant voltage for a given time, as shown, it is required to open switch S1 at that time - in which case switch S2 is held open, thereby holding that peak by capacitor C. It is noted that these switches S1 and S2 may be placed under preprogrammed control by making use of a microcomputer, etc. It is understood that the driving waveforms of the instant embodiment are not limited to those having such time constants as shown in Figs. 9-11; in other words, they may go up or down linearly. For instance, if the resistance in the conversion circuit shown in Fig. 12 is replaced with a constant-current circuit, it is then possible to obtain such a trapezoidal waveform as shown in Fig. 13. Fig. 13(a) represents an arrangement in which a constant-current circuit I1 is built in the discharge circuit, thereby obtaining a linearly going-down waveform such as on shown in Fig. 13(b). Fig. 13(c) represents an arrangement wherein a constant-current circuit I2 is incorporated in the charging circuit, thereby obtaining a linearly going-up waveform such as one shown in Fig. 13(d). Fig. 13(e) illustrates an arrangement wherein constant-current circuits are built in the charging and discharging circuits, thereby obtaining a waveform that goes up linearly and, after a constant voltage is reached, goes down linearly, such as one shown in Fig. 13(f). Then, reference will be made to the case where, for instance, a signal that is pulse-widthwise modulated in correspondence to an image signal is subjected to waveform conversion to give a time constant to the trailing edge. Even when there are discrete ion flows, as shown in Fig. 14(b), that are generated by a high-frequency voltage such as one shown in Fig. 14(a), the presence of the time constant shown in Fig. 14(c) permits the discretely generated ion flow to be accepted at a time period T1 or T2. Because this gives rise to a change in an ion current that makes some contribution, even when there is a pulse width change between t1 and t2, surface potential changes approximately linearly (smoothly) in dependence on pulse width but without undergoing a stepwise change. For instance, this will be explained with reference to the results of simulation shown in Fig.s 15 and 16. In this simulation, varying time constant values were imparted to the leading edge of a rectangular wave, as shown in Fig. 15(a), to detect surface potentials. Such results as shown in Fig. 15(b) were obtained. In Fig. 15(a), as the time constant of the leading edge increases, the surface potential obtained in Fig. 15(b) changes from a stepwise curve to a smoothly changing curve. It is thus understood that the suitable choice of a suitable time constant value enables good-quality halftone reproduction to be achieved, because a change of surface potential with respect to pulse width is made smooth. Fig. 16(a) represents the case where time constants are imparted to the leading and trailing edges of a rectangular wave. In the case of a waveform P, there is obtained a triangular wave that has an increased time constant but is free from any constant-voltage part. As can be seen from Fig. 16(b), there is a stepwise change of surface potential with respect to pulse width as long as the time constant is small, but that surface potential changes smoothly, as the wave approximates to a triangular waveform with increases in the time constants imparted to the leading and trailing edges. The changes in surface potential with respect to pulse width were measured using a triangular wave (characteristic A) and a square wave (characteristic B). The results are shown in Fig. 17. It is here noted that a wave form comprising charging and discharging curves, as shown in Fig. 18, was used as the triangular wave. As can be understood from Fig. 17, the surface potential change with respect to the pulse width change is smoother in the triangular wave than in the square wave. According to this embodiment mentioned above, it is possible to obtain high halftone output, because there is no influence by the generation of discrete ion flows that are corresponding to the alternating-current frequency applied to the recording head, and so the change of the surface potential formed on the recording member becomes smooth in correspondence to pulse with. In the following description, another embodiment of the halftone image recorder according to the invention will be explained. Fig. 19 represents one embodiment of a pulse width- and amplitude-modulated signal. It is noted that this embodiment is applicable to every ion flow control type of image recorder. As shown in Fig. 19(a), the amplitude of a pulse having a unit time duration t 0 in correspondence to the input signal voltage is now changed to an amplitude V at a unit amplitude step v. When the input signal voltage is large, a pulse having a time duration t 0 and an amplitude V is shifted in phase by unit time duration t 0 , as shown in Fig. 19(b). Then, the pulse having unit time duration t 0 is likewise changed to amplitude V. When the input signal voltage is larger, a pulse having a time duration 2t 0 and amplitude V is shifted in phase by unit time duration t 0 , as shown in Fig. 19(c). Then, the pulse having unit time duration t 0 is similarly changed to amplitude V. When the signal voltage is much larger, phase shift is done by unit time duration t 0 . Then, the pulse having unit time duration t 0 is similarly changed to amplitude V at unit amplitude step v. Thus, amplitude modulation is done with a pulse having unit time duration t 0 at step v, while pulse width modulation is carried out using time duration t 0 as the unit; amplitude and pulse width modulations are done independently from each other. Now let us call amplitude modulation N halftone control and pulse width modulation M halftone control. We can then define the total halftone in terms of N x M halftones. In this case, the driving speed is determined by either N or M, although the chosen N or M must be larger than the other. Now, if M < N, it is then possible to make the driving speed M times as large. For instance, if N = 64 and M = 4 in the case of 256-halftone expression, it is then possible to apply the driving speed for 64-halftone expression even to the 256-halftone expression or, in other words, the driving speed can be increased to 4 times as large. If N = M = 16 , it is then possible to apply the driving speed for 16-halftone expression even to 256-halftone expression or, in other words, the driving speed can be increased to 16 times as large. It is noted that, in Fig. 19, the amplitude-modulated part of the driving pulse waveform is gradually shifted in phase by t 0 , as it goes from Fig. 19(a) through Fig. 19(b) to Fig. 19(c). For actual ready control, however, it is preferable to fix the phase of the amplitude-modulated part. For this reason, it is desired to perform such waveform control as shown in Fig. 20. In other words, it is desired that, as shown in Fig. 20(a), the amplitude of the pulse having unit time duration t 0 be changed to amplitude V at unit amplitude step v, corresponding to the input signal voltage. When the input signal voltage is larger, a pulse having time duration t 0 and amplitude V is shifted in phase by time duration t 0 , as shown in Fig. 20(b). Then, the pulse having unit time period t 0 is likewise changed in the same phase to amplitude V at unit amplitude step v. When the input signal voltage is larger, a pulse having a time duration 2t 0 and amplitude V is shifted in phase by time duration t 0 , as shown in Fig. 20(c). Then, the pulse is changed in the same phase to amplitude V at unit amplitude step v. These pulse width- and amplitude-modulations are also true when the input signal voltage is much larger. With such a pulse waveform, amplitude modulation control is easy to perform, because the phase of the amplitude-modulated part is fixed. Fig. 21 illustrates the waveform conversion circuit for generating the pulse waveform shown in Fig. 20, and Fig. 22 is a representation of how the waveform conversion circuit works. In Fig. 21, reference numeral 45 stands for a voltage setting block, 46 a pulse width setting block, 47 an input terminal, and S1-S3 switches. As already explained in connection with Figs. 19 and 20, the voltage setting block produces at a given unit step a plurality of varying voltages that correspond to the number of halftones. The pulse width setting block produces a plurality of pulses having varying widths at a given unit time duration step. When switch S1 is first put on, output terminal 47 acquires a power source +B level. When switch S1 is put off followed by putting switch S2 on, output terminal 47 acquires the output level of voltage setting block 45, and when switch S3 is put on, output terminal 47 becomes zero. Hence, it is possible to generate the modulated pulse that has been explained with reference to Fig. 20 by placing switches S2 and S3 under switching control at the unit time duration and at the unit time duration or a time duration that is an integral multiple thereof. It is then possible to achieve high-speed driving and high-contrast expression by applying such a modulated pulse through output terminal 47 to an ion head. It is here noted that, when such a sine wave as shown in Fig. 23(a) is used as the high-frequency voltage for an aperture control type of halftone image recorder operated by solid discharge, shown in Fig. 1, ion flows are detectable only at the peak of the high-frequency voltage, as already explained in connection with Fig. 4 and as illustrated in Fig. 23(b). To put it another way, they are discretely generated at a certain period and so there is a variation in the quantity of the ions generated. Hence, if the unit time duration t 0 explained with reference to Figs. 19 and 20 corresponds to one ion-generation cycle or cycles that are an integral multiple thereof, it is then possible to generate ion flows in association with a pulse width change. The instant embodiment, because of making high halftone control easy even when it is driven at high speed, enables printing speed to be increased and good-quality halftone reproduction to be carried out. While the embodiment mentioned above has been described with respect to the alternating-current drive mode, it is noted that the invention may be carried out on a direct-current ion generation mode. A corotron type of ion printer, shown in Fig. 24 as an example, can be placed under halftone control only by pulse width modulation, because of the constant emission of ions. Figs. 24(a) and (b) provide a conceptional representation of such a corotron type of ion printer, wherein reference numeral 51 stands for a corona ion-generation source, 52 an ion head, 52a an upper aperture electrode, 52b an insulating layer, 52c a lower aperture electrode, 53 a hole, 54 a recording medium, 54a an insulator, 54b an electrically conductive layer, 55 a corona ion-generating power source, 56 and 57 control signal power sources, and 58 a bias electrode. Corona ion-generating power source 51, for instance, may be built up of a casing electrode 51a and a corona wire 51b laid on in it.. A direct-current high voltage is applied by corona ion-generating power source 55 between casing electrode 51a and corona wire 51b to generate corona ions. Upper and lower aperture electrodes 52a and 52c formed on both sides of insulating layer 52b are provided with a through-aperture that corresponds to hole 53 provided through insulating layer 52b to define a unit recording element, and serves to place an ion flow under on/off control in dependence on the polarity of the control signal voltage applied through control signal power sources 56 and 57. The corona ions that have passed through the hole in the insulating layer are guided by an electric field made between the insulating layer and conductive layer 5 of recording medium 4b by bias power source 58, thereby forming a latent image on the insulator 54a of recording medium 54. In such an arrangement, signal voltage is furnished to lower electrode 52, as shown in Fig. 24(a), to make upper aperture electrode 52a so positive that a corona ion flow can go onto recording medium 54 along an electric field formed in the electrode aperture to form a latent image on insulator 54a. On the other hand, when signal voltage is applied such that the polarity of the signal power source is reversed, as shown in Fig. 24(b), an electric field is formed within the electrode aperture in the direction that prevents any ion flow, and so the ions cannot pass through the aperture. On insulator 54a) there is thus formed a latent image that corresponds to a control signal.

Claims: A halftone image recording device which includes a recording head (1) for forming a charge pattern by a charge flow on a recording medium and a waveform conversion circuit (40-42) for modulating the pulse width of a signal voltage applied to the recording head in dependence on the density level of the image to be recorded and in which the dot diameter of the charge pattern formed is controlled by modulating the pulse width of the signal voltage applied to the recording head, characterized in that said waveform conversion circuit (40 to 42) is designed to convert the signal voltage to a waveform with at least one of the leading and trailing edges of the pulse width-modulated signal having an unsharp characteristic by including a charge and discharge circuit for imparting time-constant for the leading and/or trailing edges of the pulses A device as recited in Claim 1, comprising means adapted for stepwise varying the pulse width of the pulse width-modulated signal by using a unit pulse width. A device as recited in Claim 2, characterized in that said unit pulse width is equal to an integral multiple of one ion-generation cycle. A device as recited in any one of claims 1 to 3, characterized by being an ion printer.

Inventors: IIJIMA MASAYUKI, KADOWAKI HIROYUKI, SHIBUYA AKIRA, SHINBO TOMOHIRO, IIJIMA, MASAYUKI, KADOWAKI, HIROYUKI, SHIBUYA, AKIRA, SHINBO, TOMOHIRO, Iijima, Masayuki, c/o DAI NIPPON PRINTING CO., LTD, Kadowaki, Hiroyuki, c/o DAI NIPPON PRINTING CO.LTD, Shibuya, Akira, c/o DAI NIPPON PRINTING CO., LTD., Shinbo, Tomohiro, c/o DAI NIPPON PRINTING CO., LTD
Applicants: DAINIPPON PRINTING CO LTD, DAI NIPPON PRINTING CO., LTD.
Application year: 1993
Main classification: H04N1
IPC codes: H04N1