Abstract:
A method for assisting the oscillating starting process of an electromechanical oscillator ( 10 ) has the following steps: detection of oscillator oscillations ( 1   b   , 1   c ) which occur in the output signal ( 1   a ) from the electromechanical oscillator ( 10 ); generation of an excitation pulse ( 3   b ) on the basis of a detected oscillator oscillation ( 1   c ); and feeding ( 3   a ) of the excitation pulse ( 3   b ) to the electromechanical oscillator ( 10 ).

Description:
PRIORITY 
     This application claims priority from German Patent Application No. DE 10 2005 001 684.7, which was filed on Jan. 13, 2005, and is incorporated herein by reference in its entirety. 
     TECHNICAL FIELD 
     The invention relates to a method and an apparatus for assisting the oscillation starting process of electromechanical oscillators, in particular crystal oscillators. 
     BACKGROUND 
     In order to interchange data between different communication terminals, an identical clock or oscillator signal is required for the transmission and reception of data in the subscriber appliances. When interchanging data via radio links, this is generally a radio-frequency clock or oscillator signal (for example at 2 GHz or more). This clock or oscillator signal must be produced in the various communication terminals independently of one another, for which reason the individual clock signals must be highly frequency stable, in order to maintain synchronicity between the subscriber appliances. Thus, in general, electromechanical oscillators, such as oscillating crystals or similar piezoelectric oscillators, are used to produce the stable-frequency clock or oscillator signal. 
     Crystal oscillators have a high power consumption, which is particularly disadvantageous in battery-powered terminals or terminals which are independent of the mains system, such as mobile telephones, since the comparatively high energy consumption shortens the operating time of such terminals which are independent of a mains system. The oscillating crystals which define the frequency are therefore not generally operated permanently but only at those times at which data is actually being interchanged, or when such an interchange is intended to be possible. 
     If the intention is just to ensure the capability to interchange data (for example during the standby mode of mobile telephones), then the subscriber appliance is generally briefly switched to reception at regular intervals, for which purpose the radio-frequency clock signal is required. In consequence, the crystal oscillator is likewise switched on for short periods at regular intervals. The radio-frequency clock signal is in this case generally required only for a few milliseconds. However, it must be remembered that the crystal oscillator itself also has an oscillation starting period of several milliseconds. 
       FIG. 1  illustrates the measured oscillation starting process of a known crystal oscillator. The supply voltage is switched on at t=0, and the oscillating crystal has stabilized after about 4 ms. The radio-frequency clock signal is therefore not available until several milliseconds after the oscillating crystal has been switched on. If the radio-frequency clock signal is likewise required only for a few milliseconds, then the oscillation starting process of the crystal oscillator is lengthened, during which process the radio-frequency clock signal, whose overall operating time is significant, is not yet available. The overall operating time and thus the energy consumption of the crystal oscillator when operated for short periods in this way are governed to a considerable extent by the duration of the oscillation starting process. 
     SUMMARY 
     One object of the invention is, thus, to specify a method and an apparatus for assisting or speeding up the oscillation starting process of crystal oscillators. A further object of the invention is to specify an oscillator circuit having an apparatus for assisting the oscillation starting process. 
     This object can be achieved by a method for assisting the oscillation starting process of an electromechanical oscillator, comprising a feedback method with the following steps: 
     a) detecting oscillator oscillations which occur in an output signal from the electromechanical oscillator; 
     b) generating an excitation pulse on the basis of a detected oscillator oscillation; and 
     c) feeding of the excitation pulse to the electromechanical oscillator. 
     The detection of the oscillator oscillations may comprise the following steps:
         amplifying oscillator oscillations which occur in the output signal from the electromechanical oscillator; and   generating a clock signal on the basis of the amplified oscillator oscillations.       

     The excitation pulse can be generated as a function of an enable signal, with a time at which the enable signal causes the generation of the excitation pulse being predetermined. The enable signal can be produced with the aid of the clock signal. A plurality of excitation pulses can be fed to the electromechanical oscillator, by carrying out the feedback method repeatedly. Groups of excitation pulses can be fed to the electromechanical oscillator periodically, with each group comprising at least one excitation pulse. A predetermined number of excitation pulses can be fed to the electromechanical oscillator within one group of excitation pulses, with the excitation pulses in the groups being generated on the basis of successive, detected oscillator oscillations. No excitation pulses can be fed to the electromechanical oscillator during the time period between the feeding of the groups of excitation pulses. The oscillator oscillations of the electromechanical oscillator which exceed a threshold value can be detected. The electromechanical oscillator may comprise a piezoelectric oscillator, in particular a crystal oscillator. 
     The object can also be achieved by an apparatus for assisting the oscillation starting process of an electromechanical oscillator, comprising a detection unit for detection of oscillator oscillations which occur in an output signal from the electromechanical oscillator, and a pulse generator for generation of an excitation pulse on the basis of a detected oscillator oscillation which is fed to the electromechanical oscillator. 
     The detection unit can be designed to amplify oscillator oscillations which occur in the output signal from the electromechanical oscillator, and to generate a clock signal on the basis of the amplified oscillator oscillations. The detection unit may comprise an inverter chain and at least one of the inverters in the inverter chain is operated at the triple point. The first inverter in the inverter chain may detect those oscillator oscillations in the electromechanical oscillator which exceed a threshold value, and this first inverter is in the form of a Schmitt trigger. The pulse generator may comprise a univibrator, and an RC element can be arranged in the delay path of the univibrator. The apparatus may further comprise a unit for production of an enable signal, with the pulse generator being designed to receive the enable signal and feeding the excitation pulse or pulses to the electromechanical oscillator as a function of the enable signal, and a counter which uses the clock signal to determine the time or times at which the enable signal causes the excitation pulse or pulses to be fed to the electromechanical oscillator. The counter can be operable to produce the enable signal with the aid of the clock signal. The unit for production of the enable signal can be designed to cause a plurality of excitation pulses to be fed to the electromechanical oscillator. The unit for production of the enable signal can be designed to cause groups of excitation pulses to be fed to the electromechanical oscillator periodically, with each group comprising at least one excitation pulse. The unit for production of the enable signal can be designed to cause a predetermined number of excitation pulses to be fed to the electromechanical oscillator within one group of excitation pulses, with the excitation pulses in the groups being generated on the basis of successive detected oscillator oscillations. The unit for production of the enable signal can be designed to ensure that no excitation pulses are fed to the electromechanical oscillator during the time periods between the generation of the groups of excitation pulses. The electromechanical oscillator may comprise a piezoelectric oscillator, in particular a crystal oscillator. An oscillator circuit may comprise such an apparatus and an oscillator unit with an electromechanical oscillator. The oscillator unit can be in the form of a Colpitz oscillator. 
     The method according to the invention for speeding up and assisting the oscillation starting process of an electromechanical oscillator comprises a feedback method. In a first step of the feedback method, voltage variations and oscillator oscillations which occur in the output signal from the electromechanical oscillator are detected. In a second step, a detected oscillator oscillation is used to generate an excitation pulse, which is fed to the electromechanical oscillator in a third step. 
     Immediately after the supply voltage for the crystal oscillator has been switched on, the crystal oscillator will not yet have been stabilized, but it emits an output signal with voltage variations corresponding to the self-noise of the oscillating crystal, with noise effects and initial oscillations contained in it. These voltage variations are detected in the first step of the feedback method according to the invention. A detected voltage variation is used to produce an excitation pulse, which is emitted to the electromechanical oscillator. The time which passes from detection of a voltage variation to the feeding of the excitation pulse which is produced from it is in general negligible in comparison to the oscillation duration of the electromechanical oscillator. The excitation pulses are thus fed to the electromechanical oscillator instantaneously, on the timescale of the oscillator oscillation, after the detection of a voltage variation or of an oscillator oscillation in the output signal from the electromechanical oscillator. The voltage variation which is detected in the first step of the feedback method is thus amplified with the correct phase. As soon as voltage variations can be detected in the output signal from the electromechanical oscillator, these or the mechanical oscillations of the electromechanical oscillator on which they are based are deliberately amplified by using the instantaneously generated excitation pulses that are fed in to drive additional charges into the electromechanical oscillator. The oscillation amplitude of the voltage variation or of the oscillator oscillation of the electromechanical oscillator is increased in this way. 
     The method according to the invention deliberately amplifies noise effects and initial oscillations of the electromechanical oscillator, and the oscillation amplitude of the electromechanical oscillator increases considerably faster than in the case of known methods for switching on an electromechanical oscillator. In consequence, the full oscillation amplitude of the electromechanical oscillator, that is to say the steady state, is reached considerably more quickly, and the oscillation starting process is thus significantly shortened. The useable radio-frequency clock or oscillator signal is thus available considerably more quickly after the electromechanical oscillator has been switched on, and the time in which the electromechanical oscillator is not emitting any useable radio-frequency clock signal even though it is consuming power is reduced. The electromechanical oscillator is thus operated in a considerably more energy-saving manner, since the overall operating time of the electromechanical oscillator is reduced. The method according to the invention lengthens the possible operating time of communications terminals which are independent of the mains system. 
     In one advantageous refinement of the method according to the invention, the detection of the voltage variation or of the oscillator oscillations in the output signal from the electromechanical oscillator comprises the amplification of oscillator oscillations which occur in the output signal from the electromechanical oscillator, and the production of a clock signal on the basis of the amplified oscillator oscillations. The clock signal may in this case be an analogue or else a digital clock signal. A clock signal (initially irregular) is thus formed from the noise and from the initial oscillations of the electromechanical oscillator, from which excitation pulses are subsequently generated for feeding to the electromechanical oscillator. 
     In a further advantageous refinement of the method according to the invention, the excitation pulses are produced as a function of an enable signal. The enable signal determines whether an excitation pulse is generated on the basis of a detected oscillator oscillation and is then fed to the electromechanical oscillator, and thus predetermines the times at which the generation and feeding of one or more excitation pulse or pulses is caused. 
     In one preferred refinement, the enable signal is produced with the aid of the clock signal which is emitted from the detection unit. The coupling of the enable signal to the clock signal results in the enable signal being matched to the possibly still irregular clock signal and to the already existing oscillator oscillations. 
     In a further advantageous refinement of the method according to the invention, the feedback method is carried out repeatedly. In consequence, a plurality of excitation pulses are produced and are fed to the electromechanical oscillator. The plurality of excitation pulses are generated on the basis of a plurality of voltage variations detected, or oscillator oscillations occurring, in the output signal from the electromechanical oscillator, and/or on the basis of the clock signal which is derived from them. The excitation pulses may be generated on the basis of successive clock signals or oscillator oscillations in the output signal from the electromechanical oscillator, or else on the basis of non-successive clock signals, so that an excitation pulse is not fed to the electromechanical oscillator on the basis of each detected voltage variation or oscillator oscillation. There are therefore gaps or pauses between such separated, successive excitation pulses, with these gaps or pauses covering one or more detected oscillator oscillations. The enable signal is advantageously used to control the production of the excitation pulses. 
     However, the feeding of an excitation pulse to the electromechanical oscillator excites not just the intended oscillation frequency but also harmonics and other undesirable oscillations. The insertion of pauses or gaps between successive excitation pulses allows the undesirable harmonics to decay, and thus contributes to the electromechanical oscillator oscillating only at the intended oscillator frequency. Carrying out the feedback method according to the invention repeatedly results in the oscillation amplitude of the electromechanical oscillator being additionally amplified, and accordingly makes a contribution to further shortening the oscillation starting time. 
     In a further preferred refinement of the method according to the invention, groups of excitation pulses with a predetermined number of excitation pulses are produced, and are fed to the electromechanical oscillator. The groups comprise at least one excitation pulse. If each of the groups comprises a plurality of excitation pulses, then the excitation pulses in the group are produced on the basis of successive, detected oscillator oscillations or on the basis of separated, non-successive detected oscillator oscillations or clock signals. One group is separated from the previous group and from the subsequent group by a number of detected oscillator oscillations or clock signals, which are not used as the basis for generation and feeding of any excitation pulse. In one particularly preferred refinement, the successive groups of excitation pulses have an identical structure and are separated or spaced apart by an identical number of detected oscillator oscillations, thus resulting in a periodic group structure of excitation pulses. 
     In a further preferred refinement of the method according to the invention, the only voltage variations and oscillator oscillations that occur in them which are detected and amplified in the output signal from the electromagnetic oscillator are those which exceed a predetermined threshold value. This threshold value is set, for example, such that the detected voltage variations or oscillator oscillations on the basis of which the clock signal is generated can, with a specific confidence level, no longer be added to the (statistical) self-noise of the electromechanical oscillator. By way of example, this threshold value may be in the range between 2 and 10 mV. 
     In a further preferred refinement of the method according to the invention, the electromechanical oscillator comprises a piezoelectric oscillator, in particular a crystal oscillator or an oscillating crystal. 
     The apparatus according to the invention for assisting the oscillation starting process of an electromechanical oscillator and for carrying out the method according to the invention comprises a detection unit for detection of oscillator oscillations which occur in the output signal from the electromechanical oscillator and of voltage variations which are present in the self-noise of the electromechanical oscillator and are caused, for example, by noise effects and initial oscillations, as well as a pulse generator for production of an excitation pulse on the basis of a detected oscillator oscillation, which excitation pulse is fed to the electromechanical oscillator. In general, the signal delay times through the detection unit and the pulse generator of the apparatus according to the invention are negligible in comparison to the oscillation duration of the electromechanical oscillator, so that the excitation pulse which is produced on the basis of a detected oscillator oscillation is fed to the electromechanical oscillator instantaneously, on the timescale of the (slower) oscillator oscillation, and thus with the correct phase. This results in additional charges being driven into the crystal, and the oscillation amplitude of the electromechanical oscillator is increased. 
     In one particularly preferred refinement of the apparatus according to the invention, the detection unit amplifies the voltage variations and oscillator oscillations which occur in the output signal from the electromechanical oscillator, and uses them to generate a clock signal. This clock signal is supplied to the pulse generator. The clock signal thus represents the voltage variations and oscillator oscillations detected in the output signal from the electromechanical oscillator, and can thus be used to produce excitation pulses with the correct phase in the pulse generator. 
     In one particularly preferred refinement of the apparatus according to the invention, the detection unit comprises an inverter chain for amplification of oscillator oscillations which occur in the output signals from the electromechanical oscillator, and for production of the clock signal. In a further preferred refinement, at least one of the inverters in the inverter chain, but in particular all of the inverters in the inverter chain, is or are operated at the triple point, that is to say the output of the respective inverter is fed back through a high impedance to its input. The input and the output of the inverter thus assume the same voltage level in the rest state, with this being between the two logic voltage levels. The inverter is thus in a state in which it produces the highest gain and can quickly amplify voltage variations which occur. This analogue operation of an inverter, in particular of a CMOS inverter, results in a faster amplifier of simple design. 
     In a further preferred refinement of the apparatus according to the invention, the first inverter in the inverter chain detects and amplifies only those voltage variations and oscillator oscillations in the electromechanical oscillator which exceed a predetermined threshold value. For this purpose, the first inverter in the inverter chain is preferably in the form of a Schmitt trigger. This means that the only voltage variations which are detected and amplified are those for which, for example, there is a specific confidence level that they cannot be added to the self-noise of the electromechanical oscillator. 
     In a further preferred refinement of the apparatus according to the invention, the pulse generator comprises a univibrator. The pulse generator receives the clock signal, with the clock signal preferably being in digital form. The univibrator comprises two signal paths, via which signals are supplied to a logic gate. The input signal or the received clock signal is supplied directly to the logic gate via the first signal path. There are an (odd) number of inverters in the second signal path, the delay path, and these have a specific signal delay time (gate delay time). The signal through the delay path thus reaches the logic gate only with a certain delay, with the signal delay time by the inverter chain also governing the pulse duration of the pulse which is emitted at the output of the logic gate. Depending on the nature of the logic gate, a signal pulse is produced at its output when a rising or a falling flank occurs, or on both flanks of the input signal of the univibrator, that is to say of the received clock signal. In one particularly preferred refinement, an RC element which precedes the inverter or inverters is located in the delay path of the univibrator, additionally delays the switching of the inverter or inverters following a flank in the clock signal, and thus additionally governs the pulse duration at the output of the logic gate. 
     In a further preferred refinement of the apparatus according to the invention, the pulse generator is designed to receive an enable signal, and the apparatus according to the invention also comprises a unit for production of an enable signal. The pulse generator generates the excitation pulse or pulses as a function of the received enable signal. The enable signal thus controls whether an excitation pulse is generated in response to an oscillator oscillation detected in the output signal from the electromechanical oscillator or in response to a flank occurring in the clock signal, and whether this is or is not fed to the electromechanical oscillator. 
     In a further preferred refinement, the unit for production of the enable signal is in the form of a counter, which determines the times at which the enable signal causes the generation of the excitation pulse or pulses from the clock signal by the pulse generator. 
     In one particularly preferred refinement of the apparatus according to the invention, the counter is designed to produce the enable signal on the basis of the clock signal which is produced by the detection unit. By way of example, the counter is operated with the aid of the clock signal. 
     In one particularly preferred refinement of the apparatus according to the invention, the electromechanical oscillator comprises a piezoelectric oscillator and is, in particular, in the form of a crystal oscillator or an oscillating crystal. 
     The oscillator circuit according to the invention comprises an oscillator unit with an electromechanical oscillator, as well as an apparatus according to the invention for assisting the oscillation starting process of an electromechanical oscillator. The addition of the apparatus according to the invention for assisting the oscillation starting process of an electromechanical oscillator to the known oscillator unit ensures that a stable-frequency clock or oscillator signal is produced even after an oscillation starting period of the electromechanical oscillator which is considerably shorter than that in the prior art. 
     In one particularly preferred refinement, the oscillator circuit is in the form of a Colpitz oscillator. The electromechanical oscillator is in this case the element of the Colpitz oscillator which determines the frequency. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       The invention will be explained in more detail in the following text with reference to drawing figures and data curves, in which: 
         FIG. 1  shows the measured oscillation starting process of an electromechanical oscillator according to the prior art; 
         FIG. 2  shows an exemplary embodiment of the apparatus according to the invention; 
         FIG. 3  shows a simulation of the oscillation starting response when using the method according to the invention; and 
         FIG. 4  shows a comparison of the oscillation starting response which results from the use of the method according to the invention, with the known oscillation starting response. 
     
    
    
     DETAILED DESCRIPTION 
       FIG. 2  shows the circuit diagram of one exemplary embodiment of the oscillator circuit according to the invention. The oscillator circuit comprises an oscillator unit  1  with a crystal oscillator or oscillating crystal  10 . A controlled current source  12  supplies a switching transistor  11 , whose gate is controlled by the oscillating crystal  10 . The controlled current source  12  may be controlled, for example, in such a way that it emits a higher voltage during the oscillation starting process, in order to speed up the oscillation starting process. A stabilized-frequency clock signal is emitted at the connection  1   e  of the switching transistor. The output signal from the oscillating crystal  10  is supplied via the supply line  1   a  (XTAL) to a detection unit  2 . A pulse generator  3  feeds excitation pulses  3   b  with the correct phase via the supply line  3   a  (LOAD PIN) to the oscillator unit  1 . 
     Immediately after the supply voltage for the oscillator unit  1  is switched on, the oscillating crystal  10  has not yet stabilized, and the output signal from the oscillating crystal  10  (on the supply line  1   a ) essentially contains the self-noise of the oscillating crystal  10  as well as noise effects and initial irregular oscillations, which are detected in the detection unit  2  and are mapped to form a digital clock signal. 
     In the present exemplary embodiment, the detection unit  2  for this purpose contains an inverter chain comprising three inverters  21 ,  24 ,  27 , which are DC-isolated from one another and the oscillator unit  1  by means of coupling capacitors  23 ,  26 ,  29 . The inverters  21 ,  24 ,  27  are operated at the so-called triple point, that is to say the output of the inverters  21 ,  24 ,  27  is fed back via resistors  22 ,  25 ,  28  with a high impedance to the respective input. High-impedance transistors can also be used in each case, instead of the resistors  22 ,  25 ,  28 . The high-impedance feedback  22 ,  25 ,  28  of the individual inverters  21 ,  24 ,  27  is designed in such a way that, in the rest state, the voltage at the input and output of an inverter  21 ,  24 ,  27  is identical. The resistance value is typically 200 kΩ. The voltage at the input and output is in this case in the middle between the two logic voltage levels, that is to say, if the two logic voltage levels are, for example, 0 and 2.5 V, then the high-impedance feedback for the inverters  21 ,  24 ,  27  results in a voltage of 1.25 V being produced at their inputs and outputs. The inverters  21 ,  24 ,  27  thus operate as fast amplifiers. When voltage fluctuations occur at the input of the first inverter  21  as a consequence of noise effects, or initial oscillations of the oscillation crystal  10  occur, then these are amplified and are passed to the next inverter  24 . If, for example, voltage variations of 10 mV occur at the input of an inverter  21 ,  24 ,  27 , then these are typically amplified to about 100 mV. The gain is limited by the logic voltage level, which typically at the same time represents the supply voltage for the inverters  21 ,  24 ,  27  as well as earth. The detection unit  2  thus emits a digital clock signal  2   a , which is produced on the basis of the analogue output signal from the oscillating crystal  10 . 
     The first inverter  21  is preferably in the form of a Schmitt trigger, which amplifies voltage oscillations at the input only above an adjustable threshold value, and preferably has hysteresis in its gain response. 
     The detection unit  2  thus detects noise effects and oscillator oscillations  1   b  which occur in the output signal from the oscillating crystal  10 , and uses them to form a digital clock signal  2   a , which is emitted at the output of the detection unit  2 . 
     The digital clock signal  2   a  is passed to a counter  4  and to the pulse generator  3 . 
     The pulse generator  3  contains a univibrator  31 ,  32 , which comprises an inverter (flank detector)  31  and a differentiating circuit  32  with whose aid short pulses  3   b  are produced from the digital clock signal  2   a . When a logic 1 is applied to the input of the pulse generator  3 , then a logic 0 is produced at the output of the inverter  31 . A logic 0 and a logic 1 are thus applied to the inputs of the NOR gate  32 , so that the NOR gate  32  emits a logic 0. When the digital clock signal  2   a  changes to the logic value 0, then a logic 0 is first of all still produced at the output of the inverter  31  (owing to the gate delay time in the inverter  31 ). A logic 0 is thus applied to both inputs of the NOR gate  32 , and the NOR gate  32  emits a logic 1. After the gate delay time of the inverter  31 , its output changes to logic 1, and the output of the NOR gate  32  changes back to the logic value 0. The NOR gate  32  thus emits short pulses, whose duration depends on the signal delay time in the delay path. In addition, the inverter  31  is preceded by an RC element  33 , which delays the switching of the inverter  31  and further extends the pulse duration at the output of the NOR gate  32 . 
     The output of the NOR gate  32  is connected to one input of a NAND gate  34 . The second input of the NAND gate  34  is coupled to a supply line  4   a . When the enable signal (logic 1) is applied to the supply line  4   a , the pulses which are produced at the output of the NOR gate  32  are passed through the NAND gate  34 . The output of the NAND gate  34  changes to the logic value 0 during the pulse duration, and thus opens the gate of a PMOS transistor  35 . In consequence, excitation pulses  3   b  are generated and are emitted via the supply line  3   a  to the oscillator unit  1  and/or to the oscillating crystal  10 . The signal delay time through the detection unit  2  and the pulse generator  3  is governed only by the gate delay times and is thus negligible in comparison to the oscillation duration of the oscillating crystal  10 , so that the excitation pulses  3   b  which are emitted to the oscillating crystal are emitted synchronously in phase with respect to the detected oscillation  1   c  of the oscillating crystal  10 , so that additional charges are driven into the crystal oscillator  10 . Noise effects and initial oscillations of the oscillating crystal  10  are amplified instantaneously, and thus in the correct phase. 
     In the present exemplary embodiment, the counter  4  has five series-connected toggle flipflops  41 ,  42 ,  43 ,  44 ,  45 , which are connected such that they divide the respectively applied clock signal (input C) by a factor of 2. The counter  4  can thus assume 2 5 =32 different states. Each flipflop  41 ,  42 ,  43 ,  44 ,  45  has a Set-S and a Reset-R input, and the output Q is fed back to the respective data input D. The digital clock signal  2   a  is applied to the clock input C of the first flipflop  41 . The output of the flipflops  41 ,  42 ,  43 ,  44  is applied to the clock input C of the respective subsequent flipflop  42 ,  43 ,  44 ,  45 . Furthermore, the output signal Q from the four “higher-value” flipflops  42 ,  43 ,  44 ,  45  is supplied to a NOR gate  46 . When a logic 0 is applied to all four inputs of the NOR gate  46 , then the enable signal is supplied to the pulse generator  3 , in the form of a logic 1 via the supply line  4   a . The enable signal is thus emitted to the pulse generator  3  only during the count states  30  and  31  of the counter  4 . When the enable signal is not applied to the supply line  4   a  and a logic 0 is produced there, then the NAND gate  34  blocks the pulses emitted from the NOR gate  32 , and no excitation pulses are generated and fed to the oscillating crystal  10 . This design of the counter  4  produces three excitation pulses (on changing to the count states  30 ,  31  and  0 ) for every 32 detected oscillator oscillations  1   b  in the output signal from the oscillating crystal  10 . However, the design of the counter  4  can be changed as required, so that different excitation pulse sequences are emitted to the oscillating crystal  10 . For example, the outputs of the flipflops  41 ,  42 ,  43 ,  44 ,  45  can be combined as required at the input of the NOR gate  46  in order to emit the desired number and sequence of pulse sequences for each counter run to the oscillating crystal  10 . It is also feasible for the number of flipflops  41 ,  42 ,  43 ,  44 ,  45  to be varied in order to increase or to reduce the number of states of the counter  4 . Furthermore, it is also possible to use more complex counters. 
     The Set-S and Reset-R inputs of the flipflops  41 ,  42 ,  43 ,  44 ,  45  are controlled via external supply lines  47 ,  48 . The counter  4  and the feeding of the excitation pulses can thus be switched on and off externally. 
     The lower part of  FIG. 3  shows a simulation of the output signal  1   a  (XTAL) from the oscillating crystal  10  when using the method according to the invention. The pulses which are emitted by the pulse generator  3  on the supply line  3   a  (LOAD PIN) are shown in the upper part of  FIG. 3 . Three excitation pulses  3   c  are emitted per cycle of the counter  4 , that is to say in the present case with five flipflops  41 ,  42 ,  43 ,  44 ,  45  per 2 5 =32 for oscillator oscillations  1   b  detected in the output signal  1   a  from the oscillating crystal  10 . This excitation pulse sequence  3   c  is repeated with each cycle of the counter  4 , and is annotated by the reference symbols  3   d ,  3   e ,  3   f  in  FIG. 3 . The individual excitation pulses  3   b  in a pulse sequence  3   c  correspond to three successive detected oscillator oscillations  1   d  of the oscillating crystal  10 . In the present exemplary embodiment, the oscillation frequency of the oscillating crystal  10  is about 26 MHz, that is to say one counter cycle, which corresponds to 32 oscillator oscillations  1   d , lasts for slightly more than 1 μs. As can be seen from the lower part of  FIG. 3 , the oscillation amplitude of the oscillating crystal  10  increases significantly in each counter cycle, that is to say for every pulse sequence  3   c ,  3   d ,  3   e ,  3   f  which is emitted, so that the oscillation amplitude of the oscillating crystal  10  has increased considerably even after a few microseconds and after a small number of excitation pulses  3   b  have been fed to the crystal oscillator  10 . 
     An oscillation frequency of about 26 MHz corresponds to an oscillation duration of about 38 nanoseconds, while the signal delay time through the detection unit  2  and the pulse generator  3  is in the region of 1 nanosecond. The excitation pulses are thus fed to the crystal oscillator  10  with a delay which is negligible in comparison to the oscillation duration and is thus sufficiently in the correct phase. 
       FIG. 4  shows a comparison of the oscillation starting processes of an oscillating crystal  10  according to the prior art (upper part) and that of an oscillating crystal  10  when using the method according to the invention (lower part). As has already been mentioned above, the oscillator amplitude of the oscillating crystal  10  rises considerably within a few microseconds when using the method according to the invention. In comparison, the oscillator amplitude of the oscillating crystal  10  rises only slightly in the same time period when the oscillations are started according to the prior art (the scaling of the graph in the upper part of  FIG. 4  is irrelevant in this case). 
     After the end of the oscillation starting process, that is to say as soon as the oscillation of the oscillating crystal  10  has risen above a specific amplitude, the detection unit  2 , the pulse generator  3  and the counter  4  are switched off.