COUPLED SAWTOOTH OSCILLATOR

Abstract: Relaxation oscillator comprising a chain of coupled sawtooth generator stages. Each stage has a capacitor which is charged and discharged. The charging of a capacitor begins when the voltage (C>c1<) of a previous stage reaches a threshold voltage (V>H<). To avoid sampling of noise on the threshold voltage (V>H<) each new voltage ramp is started gradually.

Description: Coupled sawtooth oscillator. The invention relates to a relaxation oscillator including stages each having a capacitor and means for charging the capacitor as soon as the voltage of the capacitor of another stage passes a first threshold voltage. Such a relaxation oscillator is known inter alia from an article published in IEEE Journal of Solid State Circuits, Vol. 27, No. 7, July, 1992, pp. 982-987, particularly from Figure 4 of this article. This article describes a two-stage relaxation oscillator in which the charging of the one stage is started when the voltage of the other stage passes a threshold voltage. Once the one capacitor is charged the other capacitor is discharged. Charging is effected with a constant current whose magnitude is adjustable. Discharging is effected by means of a discharge switch in such a short time that the period of one cycle and, consequently, the frequency of the relaxation oscillator is determined solely by the sum of the charging times of the two capacitors. By making the charging currents adjustable by means of a control signal, for example a control current or a control voltage, the frequency of the oscillator can be varied. This makes such an oscillator suitable for use as a voltage-controlled oscillator (VCO) or current-controlled oscillator (CCO) in phase-locked loops (PLL) and as a frequency modulator or demodulator. These applications require a high linearity and a low phase jitter. The linearity defines the relationship between the oscillation frequency and the magnitude of the control signal. Detection whether the threshold voltage is reached is effected by means of a decision circuit, usually a comparator or a Schmitt trigger, which compares the instantaneous voltage on the capacitor to be charged with a threshold voltage. Such a decision circuit has an internal inertia, as a result of which a certain delay T d occurs until the threshold voltage detection takes effect. The effect of this delay increases comparatively as the oscillation frequency increases. The result is that the oscillation frequency no longer increases proportionally as the control signal increases. For high frequencies the linearity deteriorates. Reducing the delay T < j, i.e. choosing a faster decision circuit, improves the high-frequency linearity but at the same time it causes the noise bandwidth of the equivalent input noise of the decision circuit to increase. The equivalent input noise of the decision circuit may be assumed to be superimposed on the threshold voltage. As a consequence, the threshold voltage fluctuates and charging of the capacitors each time starts at another instant. As the decision circuit is faster the bandwidth of its equivalent input noise becomes larger and the input noise is also sampled with a larger bandwidth by the decision circuit. This results in an increasing phase noise or jitter as the delay of the decision circuit decreases. Therefore, it is difficult to construct a relaxation oscillator having a high linearity as well as a low phase noise. It is an object of the invention to provide relaxation oscillators having improved characteristics as regards the linearity and/or the phase noise. To this end, the relaxation oscillator of the type defined in the opening paragraph is characterized in that the means for charging are adapted to gradually cause the charging of the capacitor to be started. Gradually causing the charging of the capacitor to be started reduces the influence of the equivalent input noise because the decision instant is spread in time. As a result of this, the noise on the reference level is sampled with a substantially smaller bandwidth, which considerably reduces the amplitude of the phase noise or jitter. Gradually increasing the charging current can be achieved in various manners, for example by means of a voltage-controlled or current-controlled current source which is gradually turned on by a comparator. Very suitable for this purpose is a differential transistor pair whose tail current is fed to the capacitor to be charged via one of the transistors of the transistor pair. The one transistor of the transistor pair has its control electrode connected to the threshold voltage and the other transistor has its control electrode connected to the capacitor whose voltage is monitored. The advantage of the use of a transistor pair as a decision element is not only the simplicity but also the linearity. To enable the oscillation frequency to be varied the tail current is made variable. Owing to the symmetry properties of the differential transistor pair the current range in which the deciding differential pair raises the charging current for the capacitor from zero to its maximum value is always situated symmetrically with respect to the instant at which the voltage of the capacitor being monitored passes the threshold voltage, regardless of the magnitude of the tail current. Configurations having two or more stages are possible for the relaxation oscillator in accordance with the invention. In configurations having only a few stages comparatively little time may be available to discharge a capacitor before this capacitor can be recharged. In such cases special provisions are necessary in order to achieve a correct timing of the charging and discharging operations of the capacitors in the various stages. Measures by means of which this is possible are defined in the subsidiary Claims. When the relaxation oscillator is started the charge conditions of the various capacitors in the mutually coupled stages are indeterminate. In order to ensure a correct starting of the various conditions the invention proposes measures which are defined in the subsidiary Claims. The structure and the timing of the relaxation oscillator according to the invention allows the off-switching of currents in a stage during time periods in which the capacitor of that stage is not being charged. This directly results in a reduction of current consumption of the relaxation oscillator, which is particularly interesting for configurations having two or more stages. This off-switching of currents may also contribute to a reduced effect of the 1/f noise component in the charging current, particularly in CMOS implementations of the stages. Implementations of this off-switching are defined in the subsidiary Claims. These and other aspects of the invention will be described in more detail with reference to the accompanying drawings, in which: Figure 1 is a functional diagram of a first prior-art relaxation oscillator; Figure 2 is a diagram which represents the voltage waveform across the capacitor of the relaxation oscillator of Figure 1 ; Figure 3 shows a detail of the voltage waveform shown in Figure 2; Figure 4 is a graph which illustrates the relationship between the oscillation frequency and the control current of the relaxation oscillator of Figure 1; Figure 5 is a diagram which represents the voltage waveform across the capacitor of the relaxation oscillator of Figure 1, illustrating the effect of noise on a decision level; Figure 6 is a diagram of a second prior-art relaxation oscillator; Figure 7 is a diagram which represents the voltage waveform across the capacitors of the relaxation oscillator of Figure 6; Figure 8 is a diagram which represents the waveforms of the capacitor voltages in a relaxation oscillator in accordance with the invention; Figure 9 is a diagram showing the construction of a stage in a relaxation oscillator in accordance with the invention; Figure 10 is a diagram which represents the transfer characteristic of a differential transistor pair for different values of the tail current; Figure 11 shows a diagram of a circuit in which a stage as shown in Figure 9 is driven by the capacitor voltage of a stage elsewhere in the relaxation oscillator in accordance with the invention; Figure 12 is a diagram which represents the linearized transfer characteristic of a differential transistor pair; Figure 13 is a diagram which represents the variation of the capacitor voltage as a function of time around the instant of turning on of the charging current of a capacitor in a stage of the relaxation oscillator in accordance with the invention; Figure 14 is an electrical circuit diagram of the first stage of a four-stage relaxation oscillator in accordance with the invention; Figure 15 is an electrical circuit diagram of the second, the third and the fourth stage of a four-stage relaxation oscillator in accordance with the invention ; Figure 16 is an electrical circuit diagram of the charging current supply of a four-stage relaxation oscillator in accordance with the invention ; Figure 17 is a circuit diagram of output flip-flops for use in a four-stage oscillator in accordance with the invention; Figure 18 is a diagram which represents signal waveforms which occur in a four-stage relaxation oscillator in accordance with the invention; Figure 19 is an electrical circuit diagram of stages for use in a six-or-more stage relaxation oscillator in accordance with the invention; Figure 20 is a diagram which represents signal waveforms which occur in a six- stage relaxation oscillator in accordance with the invention; Figure 21 is an electrical circuit diagram of the basic part of a stage for use in a three-stage relaxation oscillator in accordance with the invention; Figure 22 is an electrical circuit diagram of stages for use in a three-stage relaxation oscillator in accordance with the invention; Figure 23 is a diagram which represents waveforms which occur in a three- stage relaxation oscillator in accordance with the invention; Figure 24 is an electrical circuit diagram of a charging current supply with current routing for a four-stage relaxation oscillator in accordance with the invention; and Figure 25 is an electrical circuit diagram of a stage with switched-bias technique for use in a relaxation oscillator in accordance with the invention. Figure 1 is a functional diagram of a prior-art relaxation oscillator. A capacitor C is alternately connected to a charging current source 4 and a discharging current source 6 by means of a switch 2. Both current sources 4 and 6 supply an equal current Ic which is controllable in practice. The voltage Vc across the capacitor C is monitored by a Schmitt trigger 8 with internal threshold voltages V H and V L . Thus, as is shown in Figure 2, the direction of the charging current of the capacitor C is reversed when the voltage Vc passes one of the threshold voltages V H and V L - The tangent of the angle of inclination α is determined by the quotient of the charging current Ic and the capacitance of the capacitor C. In the case of an ideal Schmitt trigger the oscillation period Tosc only depends on the angle of inclination α and on the voltage difference (V H - V L ) between the threshold voltages V H and V L , SO that there is a linear relationship between the charging current I c and the oscillation period Tosc and, as a consequence, between the charging current Ic and the oscillation frequency Fosc- However, in practice, owing to the finite bandwidth the Schmitt trigger 8 introduces a certain delay To in the decision whether the capacitor voltage Vc passes the threshold value V H or V L . As a result, the capacitor voltage Vc overshoots the value V H - In Figure 3 this effect is illustrated in more detail. The result is that a fixed amount is added to the ideal oscillation period, which amount is independent of the charging current Ic- This leads to a non-linear relationship between the charging current Ic and the oscillation frequency Fosc which relationship is shown in Figure 4. The linearity can be improved by speeding up the Schmitt trigger 8. However, this also leads to an increase in bandwidth of the noise voltage V N of the equivalent input noise voltage source 10 of the Schmitt trigger 8. This, in turn, results in an increase of the phase jitter of the oscillator, which is caused by the sampling action of the Schmitt trigger 8. The equivalent input noise voltage V N may be added to the threshold voltages V H and V L . Figure 5 shows the variation of the capacitor voltage Vc, where for the sake of simplicity only noise has been added to the threshold voltage V H - At the decision levels V H and V the noise is sampled by the Schmitt trigger, which leads to a variation ΔTosc in the nominal oscillation period. Owing to the random nature of the noise the variation ΔTosc is different each time and gives rise to phase jitter. Only two sinusoidal components of the noise are shown, which both give rise to the same variation ΔTosc- Thus, it appears that different noise components having a given mutual frequency relationship can lead to the same variation in the oscillation period Tosc- Therefore, an increasing bandwidth results in an increasing number of frequency components which give rise to a given value of the ΔTosc- In other words, the phase jitter increases as the bandwidth increases. The improvement in linearity as a result of the increased bandwidth of the Schmitt trigger is attended by an undesirable increase of the phase jitter of the oscillator. Figure 6 shows a known two-stage relaxation oscillator, charging of the capacitor C2 of the one stage being started when the voltage VI across the capacitor Cl of the other stage passes a threshold voltage V ref . Once the one capacitor is charged the other capacitor is discharged. Charging is effected with a constant current whose magnitude is adjustable. Discharging is effected by means of a discharge switch MO5/MO7 in such short time that the period Tosc of a cycle and, consequently, the frequency of the relaxation oscillator is determined only by the sum of the charging times of the two capacitors. Figure 7 shows the sawtooth-shaped waveforms of the voltages VI and V2 across the two capacitors Cl and C2. For a more comprehensive description of the operation of this known relaxation oscillator reference is made to the afore-mentioned article in IEEE Journal of Solid State Circuits, Vol. 27, No. 7, July, 1992, pp. 982-987. In this type of relaxation oscillator the delay time and the noise bandwidth of the comparators 12 and 14 have a similar influence on the linearity and the phase jitter. As shown in Figure 8, in order to reduce the phase jitter in accordance with the invention, each new rising edge of the sawtooth voltage across a capacitor is started gradually when the rising edge of the sawtooth voltage across another capacitor passes the threshold voltage V H . These instants are marked by means of arrows Al and A2. A capacitor is discharged when the rising edge of the sawtooth voltage of another capacitor passes the other threshold voltage V L - This is indicated by the arrows A3 and A4. The gradual starting results in an effective filtering of the noise at the level V H - This is because the decision to start the charging of the capacitor with a given charging current is now spread in time. Each sawtooth voltage is generated in a stage by a capacitor which is charged and discharged. Since the sawtooth voltages control one another, this configuration of stages is called a coupled sawtooth oscillator. Figure 9 shows a possible implementation of a stage bearing the sequence number i in the coupled sawtooth oscillator. The stage comprise a differential pair of PMOS transistors Ml and M2 having their first main elecrodes or sources interconnected and coupled to a charging current source CS, which supplies a charging current Ic- The current from the second main electrode or drain of the transistor Mi flows into a capacitor C,. The current from the drain of the transistor M 2 is drained to ground. An NMOS discharging transistor M 3 is connected in parallel with the capacitor C, and has its control electrode or gate connected so as to receive the capacitor voltage Vc, ι+ ι from a subsequent stage. The transistor Mi has its gate connected to the threshold voltage V H , which is supplied by a bias voltage source, and the transistor M 2 has its gate connected so as to receive the capacitor voltage Vc, , + ι from a preceding stage. Figure 10 shows the relationship between the input voltage V, n of the differential pair and the drain current I] of the transistor Mi for two different values Ici and Ic of the charging current Ic- The characteristic curve ensures a gradual increase of the current Ii to the capacitor C„ as a result of which the voltage Vc,, becomes as shown in Figure 8. The transistor M 3 assures that the capacitor C, is discharged at the instant at which the voltage Vc, i + i in the adjacent stage passes threshold voltage V L . In this case the threshold voltage V L is equal to the source threshold voltage Wj of the NMOS transistor M 3 . The simplicity of the differential pair has the additional advantage that only little noise V N is added to the decision threshold V H - Figure 11 shows how a capacitor C 2 elsewhere in the coupled sawtooth oscillator controls a stage. When the voltage Vc 2 across the capacitor C 2 comes within the control window W (see Figure 10) of the differential pair Mι-M 2 , which control window is centered about the voltage V H on the gate of the transistor Mi, charging of the capacitor Ci is started. The voltage V ( in series with the gate of the transistor Mi represents the equivalent input noise of the transistors Mi and M 2 as well as the noise present on the threshold voltage VH- The use of a differential pair not only reduces the phase jitter but it also guarantees the linearity of the oscillator. This is because the transfer characteristic of the differential pair is point-symmetrical in the control window W. See also Figure 12, which shows the linearized transfer characteristic of the differential pair. The drain current Ii increases from the maximum value Ic when the input voltage V ιn increases within the control window W. The transfer characteristic then exhibits a transconductance g m = tan ( ) = Ic/W. Owing to the point-symmetry the curved portion in the sawtooth voltage which appears across the capacitor during the gradual start-up does not give rise to an error in the timing of the subsequent linear portion of this rising edge of the sawtooth voltage. See Figure 8: the linear portions of the rising edge shown as a dotted line and the actual edge coincide. Figure 13 represents the variation of the capacitor voltages as a function of time around the starting instant of the capacitor Ci in Figure 11. The curved portion of the capacitor voltage Vcι(t) appears during a switching time whose value is equal to the quotient of the capacitance value of the capacitor and the afore-mentioned transconductance g m . As the noise voltage Vκ(t) is integrated in the capacitor Ci during the switching time T , it is achieved that the noise voltage is effectively filtered , as a result of which in particular high- frequency components in the noise voltage V N (I) will contribute to a smaller extent to the deviation ΔTosc in the period Tosc- Figure 14 shows the electrical circuit diagram of the first stage of a four-stage coupled sawtooth oscillator, of which Figure 15 shows the circuit diagram of the second, the third and the fourth stage and of which Figure 16 shows the charging current supply for the four stages. The first stage in Figure 14 comprises a differential pair of MOS transistors Mi and M having their sources connected to a terminal Si from which a charging current Ic issues. The transistor Mi of the differential pair has its gate connected to a terminal V REFI which receives a first threshold voltage from a reference voltage source (not shown). The other transistor M 2 of the differential pair has its gate connected to the terminal C 4 of the fourth stage. The stage has a capacitor CAPi connected between the drain of the transistor Mi and a negative supply terminal Vss- The voltage across the capacitor CAPi is available on a terminal Ci . The transistor M 2 has its drain connected to the negative supply terminal Vss via the main current path of an NMOS starting transistor M 5 . The gate of the starting transistor M 5 receives an inverted starting signal on a terminal STRT, which signal has been inverted by means an inverter INV. The starting signal is briefly high when the oscillator circuit is started. An NMOS transistor M 3 arranged in parallel with the capacitor CAPi allows the capacitor CAPI to be discharged. The gate of the transistor M 3 is driven by a comparator CMP, whose output signal is available on a terminal CPi. The drive to the gate of the transistor M 3 can be inhibited by means of an NMOS transistor M 4 , whose main current path is connected between the gate of the transistor M 3 and the negative supply terminal Vss and whose gate is connected to the terminal C of the fourth stage. The comparator CMP has inputs, of which a positive input is connected to the terminal C3 of the third stage and of which a negative input is connected to a terminal V REF2 , which supplies a second threshold voltage obtained from a reference voltage source (not shown). The second threshold voltage VR EF2 is smaller than the first threshold voltage VREFI - Figure 15 shows the structure of the second, the third and the fourth stage, where i = 2, 3 or 4. The structure of these stages is substantially similar to that of the first stage. However, in the present structure the transistor M 2 has its drain connected directly to the negative supply terminal Vss and an NMOS starting transistor M 6 arranged in parallel with the capacitor CAPj has its gate connected to the terminal STRT to receive the starting signal. The sources of the differential pair M)-M 2 are connected to a terminal Sj from which a charging current Ic issues. The transistor M 2 has its gate connected to the terminal C M , i.e. to the terminal Q of the stage whose sequence number is 1 lower. The positive input of the comparator CMP is connected to the terminal Cj+ 2 , i.e. to the terminal C; of the stage whose sequence number is 2 higher. However, if this results in a sequence number greater than four, it must be decremented by four. The transistor M has its gate connected to the terminal +3 , i.e. to the terminal of a stage whose sequence number is 3 higher. In this way, the stages form a ring of coupled sawtooth generators. Figure 16 shows the charging current supply for the four stages. The terminals Si and S 3 are coupled to a positive supply terminal V DD via PMOS current source transistors Ti and T 3 . The current source transistors Ti and T 3 together with a PMOS transistor T 5 form a current mirror. A PMOS transistor T arranged in series.with the transistor T 5 has its gate connected to the terminal VR EFI • An NMOS transistor T arranged in series with the transistor T 6 has its source connected to a node Nj and has its gate connected to a terminal V Q . The transistors Tj, T 3 and T 5 all have their gates connected to the node N 2 of the transistors T 6 and T 7 . The terminals S 2 and S 4 are coupled to the positive supply terminal V DD via PMOS current source transistors T and T 4 . The current source transistors T 2 and T 4 together with a PMOS transistor T form a current mirror. A PMOS transistor To arranged in series with the transistor T has its gate connected to the terminal V REFI • An NMOS transistor T 10 arranged in series with the transistor To has its source connected to the node Ni and has its gate also connected to the terminal V REFI - The transistors T , T 4 and T 8 all have their gates connected to the node N of the transistors To and Tι 0 . The node Ni is coupled to the negative supply terminal Vss via a bias current source I t . The oscillation frequency of the coupled sawtooth generator is controlled by means of the bias current source I t . The four-stage oscillator further comprises two flip-flops shown in Figure 17. The first flip-flop FFi has its set input S connected to the terminal CPi of the first stage and its reset input R to the terminal CP 3 of the third stage. The output Qi of the flip-flop FFi supplies a first squarewave output signal OUTl . The second flip-flop FF 2 has its set input S connected to the terminal CP 2 of the second stage and has its reset input R connected to the terminal CP of the fourth stage. The output Qi of the flip-flop FF 2 supplies a second squarewave output signal OUT 2 which is 90 degrees phase-shifted with respect to the first output signal OUTl. This phase shift can be influenced by means of the voltage on the terminal V Q in the charging current supply of Figure 16. The starting means in the stages are required to impose the correct initial state, after which the oscillator can further operate autonomously. Starting is effected by briefly making the terminal STRT high with respect to the negative supply voltage terminal Vss- Figure 18 illustrates the variation of the capacitor voltages Vci, V C2 , Vc 3 and Vc in the four stages. Charging of the capacitor CAP 2 is started gradually if the voltage Vci passes the threshold voltage V REFI , which is indicated by means of an arrow Al. Charging of the capacitor CAP 3 is started gradually if the voltage Vc 2 passes the threshold voltage V REFI , which is indicated by means of an arrow A2. Charging of the capacitor CAP 4 is started gradually if the voltage Vc 3 passes the threshold voltage V REFI , which is indicated by means of an arrow A3. Charging of the capacitor CAPi is started gradually if the voltage V C4 passes the threshold voltage V REFI , which is indicated by means of an arrow A4. Discharging of the capacitor CAP] begins if the voltage Vc 3 passes the threshold voltage V REF2 , which is indicated by means of an arrow A5. For this purpose, the comparator CMP of the first stage drives the transistor M 3 of the first stage into conduction, as a result of which the capacitor CAP] is discharged rapidly. As the voltage Vc 3 on the terminal C 3 will remain higher than V R E F2 for a substantial time the comparator CMP of the first stage will still sustain conduction of the discharging transistor M 3 at the instant at which the gradual charging of the capacitor CAP] should begin again. In order to preclude this situation the transistor M 4 ensures that, under control of the voltage Vc from the fourth stage (at the instant indicated by an arrow A6), the drive to the discharging transistor M 3 is canceled. The transistor M is turned on if the voltage Vc 4 exceeds the internal threshold voltage V T of the MOS transistor M4. The output Qi of the flip-flop FFi and, consequently, the output signal OUTl goes high when the voltage on the terminal CPi goes high, i.e. when the voltage Vc 3 on the terminal C 3 exceeds the threshold voltage V REF2 - This instant is indicated by means of the arrow A7. The output Qi of the flip-flop FFi and, consequently, the output signal OUTl goes low when the voltage on the terminal CP goes high, i.e. when the voltage Vci on the terminal Ci exceeds the threshold voltage V R E F2 - This instant is indicated by means of the arrow A8. A similar analysis applies to the output signal OUT2, which explains that the signals OUTl and OUT2 are 90 degrees out of phase when the terminal V Q carries the same voltage as the terminal V EFI (see Figure 16). In that case all the charging currents are equal and the timing is identical for all stages. The phase difference can be influenced by slightly varying the voltage on the terminal V Q around the value of the voltage on the terminal V REF I - However, this does not affect the oscillation frequency Fosc- It appears that only the rising edges in the voltages across the capacitors CAPj (i = 1..4) define the duration of the actual oscillation period Tosc- Consequently, the discharging instant of a capacitor is non-critical and possible jitter at this instant does not play a part. Figure 19 shows the circuit diagram of a coupled sawtooth oscillator having six or more stages. The number of stages is represented by k (k > = 6) and the number of the stage is represented by i (i = l..k). The first stage (i=l) is largely identical to the first stage of the four-stage oscillator shown in Figure 14. The difference is that the comparator CMP and the transistor i are dispensed with and the discharging transistor M 3 has its gate connected directly to the terminal C 3 . The other stages (i = 2...k) are largely identical to the stages shown in Figure 15 and in this case the transistor M 3 has its gate connected directly to the terminal +2 . As a result of the larger number of stages the measure with the comparator CMP and the additional transistor M is no longer necessary. Figure 20 shows the variation of the capacitor voltages Vci, c 2 , Vc 3 , Vc 4 , Vc 5 and V 6 in a six-stage version (k=6). The gradual starting of the charging of the capacitor of a subsequent stage is initiated when the capacitor voltage of the preceding stage passes the threshold voltage V REFI - These starting instants are indicated by means of the arrows Al to A6. The capacitor CAPi of the first stage is discharged when the voltage Vc 3 on the capacitor CAP 3 in the third stage exceeds the threshold value V REF2 - This instant is indicated by means of the arrow A7. In the present case this threshold value V REF2 is equal to the internal threshold voltage of the NMOS transistor M 3 of the relevant stage. The capacitor CAPi in the first stage remains short-circuited by the transistor M 3 as long as the voltage Vc 3 is higher than the threshold voltage V REF2 - This is represented by means of a shaded area in the diagram of the voltage Vc 3 . The capacitor CAP 3 , in its turn, is discharged when the voltage Vc 5 passes the threshold voltage V REF2 - This instant is indicated by means of an arrow A8. The charging current supply can be of a design similar to that shown in Figure 16 but having two additional PMOS current source transistors. It will be evident from the above examples that the capacitor which drives the transistor M 2 should not be discharged during the charging process of the capacitor to be charged, which is coupled to the transistor M 2 . Consequently, the voltage on the driving capacitor should not be changed to such an extent that the differential pair prematurely interrupts the charging process of the capacitor to be charged. In the three-stage coupled sawtooth generator described hereinafter measures are taken to preclude this. Figure 21 shows the second stage of a three-stage coupled sawtooth oscillator. The transistors Mi, M 2 , M 3 and the capacitor CAP] are arranged in a manner corresponding to that shown in the first stage (i = 1) of Figure 19. However, the transistor M 2 has its drain coupled to the negative supply terminal Vss via an NMOS transistor M . This transistor M 7 has its gate connected to the terminal C 2 via an inverter INV. The transistors Mi, M 2 , M 3 have their gates connected to the terminals V REFI , Ci and C 3 , respectively. When during charging of the capacitor CAP the voltage on the terminal C 2 reaches a given value, the output of the inverter goes low and the transistor M 7 is turned off. The whole charging current Ic then keeps flowing through the transistor Mi regardless of a possible premature decrease of the voltage on the terminal Cj. Figure 22 shows the circuit diagram of a coupled sawtooth oscillator having 3 stages. The structure of the first stage (i = 1) is similar to that of Figure 21, except that the inverter INV has been replaced by a logic NOR-circuit NOR having two inputs, of which one input is connected to the terminal Ci and of which the other input is connected to the terminal STRT to receive a starting signal similar to that in the preceding embodiments. In the first stage the transistor M 2 has its gate connected to the terminal C 3 and the transistor M has its gate connected to the terminal C 2 . The structure of the second and the third stage (i = 2, 3) is similar to that of Figure 21 but an NMOS starting transistor M 8 has been added, which transistor is arranged in parallel with the capacitor CAPj and has its gate connected to the terminal STRT. In the second stage the gates of the transistors M 2 and M 3 are connected to the terminals Ci and C 3 , respectively , and in the third stage these gates are connected to C 2 and Figure 23 shows the variation of the capacitor voltages V C ι, Vc 2 , and Vc 3 . The gradual starting of the charging process of the capacitor of a subsequent stage is initiated when the capacitor voltage of the preceding stage passes the threshold voltage V REFI - These starting instants are indicated by means of the arrows Al, A2 and A3. The capacitor CAP] of the first stage is discharged when the voltage V C on the capacitor CAP 2 in the second stage exceeds the threshold value V REF2 - In the present case, this threshold value V REF2 is equal to the internal threshold voltage of the NMOS transistor M of the relevant stage. This instant is indicated by the arrow A4. The capacitor CAPi remains short-circuited as long as the voltage Vc is higher than the threshold voltage V REF2 - A stage need to be provided with current only during time periods in which the capacitor of that stage is being charged. Taking the first stage of the six-stage coupled sawtooth oscillator shown in Figures 19 and 20 as an example, it appears that this stage only needs current during the time period T A in which the capacitor CAPi is charged. In other words, this stage only needs current during the rising edge of the sawtooth voltage Vci- In the remainder of the time, i.e. during the time period Tβ, the capacitor has to be discharged within a time period indicated by Tc. In embodiments with 4 or more stages the charge of the capacitors has to be maintained for a while before the capacitor is discharged. In Figure 20 the horizontal portions of the capacitor voltages indicate when the charge is maintained. During the time periods T B no charge current is needed, and in fact this current is dumped to the negative supply voltage terminal Vss by means of the transistor M 2 of the differential pair. From the point of view of power consumption it is advantageous to use this current for another purpose or to switch off this current entirely. In the former case, during the time period Tβ, the charge current of a stage can be routed to another stage by means of switches in order to use this current as a charging current for the other stage. This routed current should be available in that other stage before the differential pair of the other stage decides to start the charging of its capacitor. A further advantage of this current routing system is that the total current consumption remains constant. In the latter case the charging current Ic at terminal Si is switched off during the time period Tβ, preferably by short-circuiting the gate-source junctions of transistors in the current supply. As a result of the filtering of the noise at the level V H , the 1/f noise present in the charging current Ic now becomes the dominant contributor to the phase noise in the coupled sawtooth generator. It appears that this switched-bias technique considerably reduces the low frequency phase noise of the coupled sawtooth generator. Figure 24 shows an implementation of the current routing in a four-stage coupled sawtooth generator. The charging current supply circuit is similar to that of Figure 16. However, the transistors Ti and T 4 are dispensed with, the terminals S 2 and S 4 are coupled to the transistor T 2 through respective PMOS transistors of a differential pair DPI, and the terminals Si and S 3 are coupled to the transistor T 3 through respective PMOS transistors of a differential pair DP2. Differential pair DPI is driven by the complementary output signals OUTl and NOUT1 of the first flip-flop FFI (Fig. 17) and differential pair DP2 is driven by the complementary output signals OUT2 and NOUT2 of the second flip-flop FF2. The current from the transistor T 2 is now alternately used as a charging current for stage 2 and stage 4, and the current from the transistor T 3 is alternately used for stages 1 and 3. A similar appraoch can be applied to a six-stage coupled sawtooth oscillator. Figure 25 shows an implementation of the switched-bias technique in a stage which can be used, for example, in a six-stage coupled sawtooth generator. Only stage 1 is shown. The other stages are the same. The differential pair MpM receives charging current from a PMOS current source transistor Mio which forms a current mirror with a diode- connected PMOS transistor Mi i . The transistor Mi i in turn receives current from a NMOS transistor M J2A which forms a current mirror with a diode-connected NMOS transistor Mι 3 . The transistor M 13 receives the bias current source I t which may be tuneable to control the oscillation frequency of the coupled sawtooth generator. A PMOS transistor M 1 parallel to the transistor Mu has its gate connected to the output of a logic NOR-circuit NOR2 having two inputs, of which one input is connected to the terminal C, +2 and of which the other input is connected to the terminal C, + ι . However, the logic NOR-circuit NOR2 may be replaced by a logic inverter which has its input connected to the terminal C, +2 . Further NMOS transistors M J2B , M 12 c, etc., identically arranged as the transistor M I2A provide bias current to the other stages. In this manner each stage has its own bias current supply path, switchable by means of the transistor Mι 4 . In the implementation with the logic inverter the PMOS current mirror Mio-Mπ is switched off by means of transistor M 14 during the time period Tc (Fig. 20) in which the capacitor CAP, is discharged. In this way no change will be noticeable in the waveforms of the capacitor voltages and also the timing is not harmed. The timing signals for driving the bias-switching transistor M 1 of the stages are generated by the oscillator itself and need not to be generated with additional circuitry. In the implementation with the logic-NOR circuit NOR2 the time period for switching off the PMOS current mirror Mio-Mπ is extended to T D (Fig. 20), as a result of which the current consumption is reduced even more. The bias current is switched off if the voltage on terminals C, + ι and/or C I+2 is greater than the reference voltage V REF2 - The embodiments described by way of example employ unipolar (MOS) transistors. However, instead of these it is also possible to use bipolar transistors, the first main electrode, the second main electrode and the control electrode correspond to the emitter, the collector and the base of the bipolar transistor.

Claims: CLAIMS 1. A relaxation oscillator comprising stages each having a capacitor (CAP,) and means for charging (Mi, M 2 , I c ) the capacitor (CAP,) as soon as a voltage of the capacitor of another stage passes a first threshold voltage (V REFI ), characterized in that the means for charging are adapted to gradually cause the charging of the capacitor to be started. 2. A relaxation oscillator as claimed in Claim 1 , characterized in that the means for charging include a comparator (Mi, M 2 ) for comparing the voltage of said capacitor of said other stage with the first threshold voltage, and a charging current source (I c ) coupled to the capacitor (CAP,) to supply a charging current to the capacitor, which charging current gradually increases to a final value in response to the comparison. 3. A relaxation oscillator as claimed in Claim 2, characterized in that the comparator comprises a differential pair comprising a first transistor (Mi) and a second transistor (M 2 ), each having a first main electrode, a second main electrode and a control electrode, the first main electrode of the first transistor (Mi) and the first main electrode of the second transistor (M 2 ) being coupled to the charging current source (Ic), the second main electrode of the first transistor (Mi) being coupled to the capacitor (CAP,), the control electrode of the first transistor (Mi) being connected to receive the first threshold voltage (V REFI ), and the control electrode of the second transistor (M 2 ) being connected to receive the voltage of said capacitor of said other stage. 4. A relaxation oscillator as claimed in Claim 3, characterized in that the stage includes a third transistor (M 3 ) having a main current path arranged in parallel with the capacitor (CAP,) to discharge the capacitor as soon as a voltage of the capacitor of another stage passes a second threshold voltage. 5. A relaxation oscillator as claimed in Claim 4, characterized in that the stage includes a further comparator (CMP) having inputs connected to receive the second threshold voltage (V R E F2 ) and the voltage of the capacitor of the other stage, and having an output connected to drive a control electrode of the third transistor (M 3 ). 6. A relaxation oscillator as claimed in Claim 5, characterized in that the stage includes means (Mi) for inhibiting the drive to the control electrode of the third transistor (M 3 ) in response to a voltage across the capacitor of a still other stage. 7. A relaxation oscillator as claimed in Claim 6, characterized in that the means for inhibiting include a fourth transistor (M ) having a main current path connected between the control electrode of the third transistor (M 3 ) and a reference terminal (Vss), and having a control electrode connected to receive the voltage across the capacitor of the still other stage. 8. A relaxation oscillator as claimed in Claim 3, characterized in that one of the stages includes means (M 5 ) for interrupting a current from the second main electrode of the second transistor (M 2 ) of the differential pair in response to a starting signal, and in that the other stages include means (M 6 ) for discharging the respective capacitor (CAP,) of these other stages in response to the starting signal. 9. A relaxation oscillator as claimed in Claim 4, characterized in that in each of the stages the second transistor (M 2 ) of the differential pair has its second main electrode coupled to a supply terminal (Vss) via t he main current path of a further transistor (M 7 ), which further transistor (M ) has a control electrode connected to the capacitor (CAP,) of the relevant stage via an inverter (INV). 10. A relaxation oscillator as claimed in Claim 9, characterized in that one of the stages includes means (NOR) for turning off the further transistor (M 7 ) in response to a starting signal, and in that the further stages include means (M 8 ) for discharging the respective capacitors (CAP,) of said further stages and for turning on the respective further transistor of said further stages in response to the starting signal. 11. A relaxation oscillator as claimed in Claim 1 , 2, 3 or 4, further comprising means (DPI, DP2, FFi, FF 2 ) for routing a charging current of the capacitor of one stage to another stage during time periods (Tβ) that no charging current is needed in the one stage. 12. A relaxation oscillator as claimed in Claim 1, 2, 3 or 4, further comprising means (I t , Mj 3 , M 12A , Mn, M 10 ) for providing bias current to a stage, and means (Mj , NOR2) for switching off the bias bias current during at least part of the time period (Tβ) that no charging current is needed in the stage.

Inventors: GIERKINK SANDER L J, VAN TUIJL ADRIANUS J M, GIERKINK, SANDER, L., J., VAN TUIJL, ADRIANUS, J., M.
Applicants: KONINKL PHILIPS ELECTRONICS NV, PHILIPS SVENSKA AB, KONINKLIJKE PHILIPS ELECTRONICS N.V., PHILIPS AB
Application year: 1999
Main classification: H03B5
IPC codes: H03K3, H03K4