Abstract:
The present invention relates to a method and device for reducing the phase noise of a laser signal from a laser source. This device comprises a first current generator for supplying a driving current to the laser source in view of producing the laser signal. A phase noise detector is responsive to the laser wavelength for generating a phase error signal and a second current generator is responsive to the phase error signal for generating a compensation current added to the driving current supplied to the laser source for generating a phase-adjusted laser signal. The device therefore defines a phase stabilization loop formed by the phase noise detector and the second current generator, for reducing the phase noise of the laser signal.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
     This application is the U.S. National Phase Application of International Patent Application Serial No. PCT/CA06/001673, filed Oct. 12, 2006, published under PCT Article 21(2) in English, which claims priority to and the benefit under 35 U.S.C. Section 119(e) of U.S. Provisional Patent Application Ser. No. 60/725,665, filed Oct. 13, 2005, the entire disclosures of each of which are incorporated by reference herein. 
    
    
     FIELD OF THE INVENTION 
     The present invention relates generally to a method and device for reducing phase noise of a laser source. More specifically, but not exclusively, the present invention relates to a method and device for effectively reducing the phase noise by 20 to 40 dB in the low frequency range of conventional distributed feedback diode laser and gain chip based external cavity laser (ECL), etc. for, as an example, fiber optic sensors based on interferometric principles, RF signal generation and coherent communications. 
     BACKGROUND OF THE INVENTION 
     In oil and gas exploration industries, seismic survey is a technique for determining the detailed geographic structure underlying a particular area by propagating acoustic shock waves into the strata and detecting and measuring the reflected seismic wave signal. The seismic survey technology is now recognized as a crucial area for oil and gas exploration and production industries in order to increase capital efficiency, minimize the risks for capital investment, eliminate the dry holes and increase oil production throughput. 
     Fiber optic based seismic survey sensing technology improves penetration through salt domes by reaching beyond 10,000 feet in depth with a resolution of less than 50 feet. This improved performance helps to discover additional new oil or gas reserves. 
     The core components in a fiber optic seismic system are the low phase noise laser sources and sensitive seismic fiber optic sensors (e.g., accelerometers, hydrophones or geophones) based on interferometric principles. The laser sources need to show not only low phase noise, but also low sensitivity to external vibration disturbance due to harsh environment. 
     Conventional high power telecom grade diode lasers exhibit narrow linewidth and low sensitivity to vibrations due to its small size. These characteristics make them suitable for use as coherent light source for interferometer-based applications. But they exhibit high phase noise in the seismic sensors working frequency range, typically 1-1000 Hz. Other types of lasers such as optical fiber lasers exhibit low phase noise but their phase noise increases dramatically in the field environment due to the sensitivity of the optical fiber (fiber length to be exact) to acoustic or mechanical vibrations (causing jitter and wavelength drift), which makes their use difficult without isolating the optical fiber lasers from harsh environmental disturbances. 
     These technical challenges and difficulties may hinder further development of fiber optic seismic sensing systems. In order to fulfill the need of fiber optic seismic sensing functions, vibration insensitive low phase noise laser sources are needed. 
     Other applications, such as precision spectroscopic measurements, hydrophone sensors, LIDAR, RF signal generation, coherent communications may also require low phase noise laser sources. 
     Furthermore, due to the high wavelength density nature of fiber optic seismic sensing systems, there is still a need to design and manufacture laser sources capable of both wavelength tuning and self-calibration to provide sufficient wavelength accuracy. 
     SUMMARY OF THE INVENTION 
     Therefore, according to an aspect of the present invention there is provided a method for reducing a phase noise of a laser signal from a laser source. This method comprises generating a main driving current to be supplied to the laser source for producing the laser signal; detecting a phase noise in the laser signal; generating a phase error signal in response to the detected phase noise; and generating a compensation current in response to the error signal to be added to the main driving current supplied to the laser source for producing a phase-adjusted laser signal. The operations of detecting the phase noise in the laser signal, generating the phase error signal in response to the detected phase noise and generating the compensation current in response to the error signal define a phase stabilization loop for reducing the phase noise of the laser signal. 
     The present invention also relates to a device for reducing a phase noise of a laser signal from a laser source. The device comprises a first current generator, a phase noise detector and a second current generator. The first current generator supplies a main driving current to the laser source for producing the laser signal. The phase noise detector is responsive to the laser signal for generating a phase error signal. The second current generator is responsive to the phase error signal for generating a compensation current added to the main driving current supplied to the laser source for generating a phase-adjusted laser signal. The phase noise detector and the second current generator form a phase stabilization loop for reducing the phase noise of the laser signal. 
     The present invention is further concerned with a detector for detecting wavelength drifting of a laser signal, comprising a wavelength discrimination filter, a first photodetector and a second photodetector. The wavelength discrimination filter is supplied with the laser signal and is so configured as to reflect a portion of the laser signal and to transmit a portion of the laser signal. The first photodetector is connected to the wavelength discrimination filter for measuring the transmitted portion of the laser signal, and the second photodetector is connected to the wavelength discrimination filter for measuring the reflected portion of the laser signal. The wavelength discrimination filter is a periodic high slope wavelength discrimination filter, the periodic high slope wavelength discrimination filter is a Fabry-Perot filter and the Fabry-Perot filter is made of two Bragg gratings spaced apart by a gap and formed inside an optical fiber. Measurements of the transmitted and the reflected laser signal portions are usable for detecting the wavelength drifting of the laser signal. Each of the transmitted and reflected laser signal portions are laser reference signals for each other. 
     The foregoing and other objects, advantages and features of the present invention will become more apparent upon reading of the following non restrictive description of illustrative embodiments thereof, given by way of example only in connection with the accompanying drawings. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       In the appended drawings: 
         FIG. 1  is a block diagram of a laser phase noise reducing device comprising a laser current driving control, a laser temperature control, a wavelength drifting detector and a wavelength locking current generator; 
         FIG. 2  is a block diagram of the laser phase noise reducing device, comprising an optical laser wavelength variation detector including a three-port fiber optic circulator, an in-line all-fiber Fabry-Perot cavity filter and two photodetectors; 
         FIG. 3A  is a portion of reflection spectrum of a fiber Fabry-Perot cavity filter formed by a set of two identical broadband chirped fiber Bragg gratings as shown in  FIG. 2 ; 
         FIG. 3B  is an example of transmission spectrum of a fiber Fabry-Perot filter formed by a set of two identical broadband chirped fiber Bragg gratings as shown in  FIG. 2 ; 
         FIG. 3C  is an example of a reduced vibration sensitivity fiber Fabry-Perot filter packaging design; 
         FIG. 3D  is a schematic diagram of a high slope wavelength discrimination filter based on an all-fiber Michelson interferometer forming an alternative design for the fiber Fabry-Perot cavity filter of  FIG. 2 ; 
         FIG. 4  is a typical optical normalized spectrum recorded simultaneously on both photodetectors of  FIG. 2 , wherein the cross points are used as wavelength references to lock the laser wavelength; 
         FIG. 5  is an alternative design using a fiber tap coupler at the laser front output to collect a laser beam portion for feeding the laser wavelength stabilization loop; and 
         FIG. 6  is another alternative design integrating a second edge-filter and two additional photodetectors for setting and tuning the laser operating wavelength. 
     
    
    
     DETAILED DESCRIPTION 
     Laser phase noise at low frequency can be reduced by sending laser light into a high slope wavelength discrimination filter and convert wavelength drifting into intensity variation. By measuring the intensity variation with a photodiode and comparing the measured intensity variation with a laser reference intensity, a error signal is generated. Based on this error signal, a compensation current is generated and is then added to a laser source driving current. In this manner, the laser wavelength is locked within a bandwidth of the resulting laser phase stabilization loop. It is to be understood that depending on the polarity of the compensation current, the compensation current may increase or decrease the value of the laser source driving current. 
     Several elements are taken into account for designing the phase noise reduction loop and maximizing the loop performance.
         First, the phase noise characteristics of telecommunication grade laser diodes are different from each vendor. The laser noise spectrum and tuning response with injection current need to be tested in order to tune the wavelength locking loop adequately.   Second, the wavelength locking loop stability should not be affected by the variation of laser power sent into the loop, therefore logarithm amplifiers are used to amplify the photodiode current and generate wavelength locking current.   Third, since the noise of wavelength discrimination filter will be transferred into wavelength locking loop. This noise could be caused by filter&#39;s instability due to external disturbance and by filter&#39;s polarization dependent response.       

       FIG. 1  illustrates a functional block diagram showing a phase noise reduced laser source module according to a first non restrictive illustrative embodiment of the present invention. 
     The main driving current  117  of the laser  110  is supplied by a first current generator in the form of a laser driving current controller  114  and the operating temperature of the laser  110  is controlled by a temperature controller  113 . Both the driving current controller  114  and temperature controller  113  are connected to a micro-controller  116 . The main driving current  117  is a DC current with minimum variation. 
     The laser  110  has a first front output that emits a laser signal  101  and a second rear output that emits a laser signal  102 . The laser signal  102  from the second rear output of the laser  110  is sent to a phase noise detector in the form of an optical wavelength drifting detection circuit  120 . The electrical signal generated by this circuit  120  is supplied to a second current generator in the form of a laser wavelength locking current generator  115  which generates a relatively small compensation current  118  to be added to the main driving current  117  to yield a total driving current  116  supplied to the laser  110 . The compensation current  118  therefore stabilizing the laser output wavelength  101  and reducing the phase noise of the laser  110 . 
     In other words, the laser wavelength drifting detector  120  and the wavelength locking current generator  115  form a phase stabilization loop that reduces the phase noise of the laser signal  101 . 
       FIG. 2  illustrates a functional block diagram showing in more detail the implementation of the phase stabilization loop of  FIG. 1 . The laser signal  102  collected from the second pigtailed output of the laser  110  is used as an input optical signal projected through a three-port circulator  121 . The optical signal from the transmission port  121 A passes through a reflective wavelength discrimination filter  122  and an attenuator  123  before reaching a first photo-detector in the form of a photodiode  128 A. The optical signal from the reflective port  121 B is directly routed into a second photo-detector in the form of a photodiode  128 B. The attenuator  123  between the discrimination filter  122  and the photodiode  128 A is used to compensate the additional insertion loss of the reflection port  121 B of the circulator  121 . Only at certain wavelengths the intensity of the power measured by both photo-diodes  128 A and  128 B can be equal, as will be described hereinbelow. 
     In the illustrative embodiment described herein, the laser  110  is a distributed feedback (DFB) laser diode packaged with both front and rear output pigtails using conventional diode packaging technologies. Alternatively, the laser  110  can also be an external cavity laser which consists of a diode gain chip and one or two fiber Bragg gratings to form the laser cavity. 
     The high frequency variation of the current at the output of both photodiode  128 A and  128 B is filtered out by respective low-pass filters  129 A and  129 B. The bandwidth of the low pass filters  129 A and  129 B determine the bandwidth of the phase stabilization loop bandwidth. 
     The reflective wavelength discrimination filter  122  is a filter which contains two sets of identical broadband chirped fiber Bragg gratings  122 A and  122 B formed in an optical fiber and spaced apart from each other by a gap  122 C. Each set of gratings operates like a broadband reflector, and together operate as a Fabry-Perot cavity. The free spectral range (FSR) of the Fabry-Perot cavity depends on both the fiber index and the gap  122 C. 
     The Fabry-Perot cavity is configured to have a very small FSR and a high contrast. A small FSR allows the locked laser wavelength to be very close to the initially set wavelength of the laser  110  and to improve the filter&#39;s sensibility to laser wavelength drifting. 
     As will easily be understood by one skilled in the art, the wavelength discrimination filter  122  reflects one portion of laser signal to the photodiode  128 B and transmits another portion of the laser signal to the photodiode  128 A. 
       FIG. 3A  and  FIG. 3B  show respectively, as an example, a portion of the reflection spectrum  300  and of the transmission spectrum  310  of an exemplary fiber Fabry-Perot cavity. The FSR is designed to be 10 picometers with maximum reflection about 90%. The reflection spectrum is detected by photodiode  128 B and the transmission spectrum is detected by photodiode  128 A. 
     The fiber Bragg grating based reflective wavelength discrimination filter  122  is so packaged that its sensitivity to vibration is reduced to a level close to laser diode.  FIG. 3C  shows an illustrative example of the design of the package. The portion of the fiber containing the reflective wavelength discrimination filter  122  is inserted into a small size groove  321  inside a solid metal body  320  without any applied tension thereonto. The groove is filled with polymer similar fiber&#39;s coating material (not shown). The two apertures of the body  320  are filled with epoxy  322 ,  323 , to adequately maintain the fiber therein. Accordingly, any strain applied on the fiber outside the body  320  will not be transferred to the fiber inside the body  320 . Since the dimension of the body is quite small, vibration in low frequency range will not be effectively transferred to the fiber inside. The temperature stability of reflective wavelength discrimination filter  122  is controlled by the temperature control of the whole body  320  which sits on a thermoelectric cooler (not shown). The thermoelectric cooler control circuit is tuned to have low frequency response in order to minimize filter&#39;s high frequency noise. 
       FIG. 3D  shows a high slope wavelength discrimination filter that can be used as the reflective wavelength discrimination filter  122 . Basically, it is a 3 dB fiber coupler  330  based asymmetric Michelson interferometer. Two identical broadband chirped fiber Bragg gratings  331 ,  332  are used as high reflectivity mirrors. The filter output in the wavelength domain is sinusoidal curve, its slope depend on position imbalance of fiber Bragg gratings  331 ,  332  on the two arms. 
     The reflective wavelength discrimination filter  122  and pigtailed photodiode  128 A,  128 B exhibit polarization dependent response which reduces the wavelength locking loop stability when the fiber is under vibration disturbance. Therefore, it is preferable that the second output of the laser  110  is connected to the circulator  121  via a polarization maintaining (PM) fiber pigtail. Similarly, the circulator  121  is pigtailed with PM fiber, the reflective wavelength discrimination filter  122  is PM fiber based and the photodiodes  128 A,  128 B are also connected by PM fiber pigtails. 
       FIG. 4  shows an example of combined spectrum detected respectively by photodiode  128 B and photodiode  128 A. The crossing points  410  are used as reference wavelengths to lock the wavelength of the laser  110 . So if the wavelength of the laser  110  doesn&#39;t match one of the reference wavelengths, the power detected by the photodiodes  128 A and  128 B will be not equal, and an error signal will be generated by the wavelength locking current generator  114 . Indeed, as can be seen from  FIG. 2 , the output of the low-pass filters  129 A and  129 B are supplied to the wavelength locking current generator  115  that may calculate the error signal in the low frequency range. 
     The wavelength and power of the laser  110  can be initially set by the laser driving current control circuit  114  and laser temperature control circuit  113 , but due to internal and external influence, the laser wavelength is not stabilized. Accordingly, the current detected by photodiodes  128 A and  128 B vary with time due to the drifting of the laser wavelength. By comparing the current signals generated by photodiode  128 A and  128 B through, for example, a comparator such as a differential amplifier (not shown), a small compensation current  118  is generated by the wavelength locking current generator  115  and then is added to the main driving current  117 , whereby the real current  116  supplied to the laser  110  is increased or decreased depending on the polarity of the compensation signal  118 . Once the current  116  is changed, the wavelength of the laser signal  101  from the laser  110  is adjusted accordingly. The circulator  121 , the reflective wavelength discrimination filter  122 , the attenuator  123 , the photodiodes  128 A,  128 B, and the wavelength locking current generator circuit  115  form a phase stabilization loop which keeps the phase of the laser locked and stabilized to a closest reference wavelength defined by reflective wavelength discrimination filter  122 ; therefore the laser phase noise is reduced. 
     By detecting and comparing both transmitted and reflected laser signals instead of detecting only one of the transmitted and reflected laser signals and comparing it with a reference laser signal collected directly from the laser output, the sensitivity of the generated phase error signal to laser wavelength drifting is improved. 
       FIG. 5  shows a phase noise reduced laser source module according to a second non-restrictive illustrative embodiment of the present invention. The laser source illustrated in  FIG. 5  is very similar to the laser source illustrated in  FIG. 2  and described hereinabove. Accordingly only the differences between these two laser sources will be described herein. The main difference between the two laser sources is that the laser  110 A of  FIG. 5  has only one output. Accordingly, the laser signal supplied to the phase stabilization loop is a small portion of the laser&#39;s output collected by using a fiber tap coupler  150 , preferably a PM based tap coupler. 
       FIG. 6  shows a phase noise reduced laser source module according to a third non-restrictive illustrative embodiment of the present invention. Again, the laser source illustrated in  FIG. 6  is very similar to the laser source illustrated in  FIG. 2  and described hereinabove. Accordingly only the differences between these two laser sources will be described herein. 
     The 3-port circulator  121  of the embodiment of  FIG. 2  is replaced by a 2×2 fiber coupler  130 , thereby providing a supplemental port  132 . The supplemental port  132  of the coupler  130  is followed by a 1×2 fiber coupler  140 . One output port  141  of fiber coupler  140  is connected to a large bandwidth wavelength discrimination filter  144  which covers the laser wavelength tuning range, then projected to a photodiode  148 . An isolator  143  is provided between the port  141  and the filter  144  to prevent eventual back reflection light from the large bandwidth wavelength filter  144  from reaching the photodiode  148 . The other output port  142  of the coupler  140  is directly connected to another photodiode  149 . The signals from the photodiodes  148  and  149  are supplied to the micro-controller  116  through an electronic circuit, for example a differential amplifier circuit  152 , and then used for several purposes. More specifically, the signals from the photodiodes  148  and  149  are used to set the laser&#39;s initial operating wavelength through the laser driving current control circuit  114  and laser temperature control circuit  113  and to monitor the laser output power. These signals are also used to measure the laser wavelength when the laser driving current control circuit  114  and laser temperature control circuit  113  are used to tune the laser wavelength. 
     In accordance with the above description, the present invention discloses a technique to stabilize laser wavelength and to reduce laser phase noise by locking the wavelength to a reference wavelength by controlling in real time the current passing through laser diode. The reference wavelength is realized, for example, by an in-line all fiber Fabry-Perot cavity with small FSR and high contrast. Such a filter allows the power detected by photodiodes to be extremely sensitive to input wavelength changes. In addition, the Fabry-Perot cavity filter is loosely packaged inside a small dimension metal body, so that its optical performance will not be affected by acoustic and mechanical vibration. 
     The present invention further discloses a method and device to control the current passing through the laser diode based on the signals supplied by the wavelength drift detection loop. The small correction current is added directly to the main driving current feeding the laser diode. This technique allows fine tuning of the current for stabilizing the laser wavelength, to therefore reduce the laser phase noise level. 
     Although the present invention has been described in terms of a non-restrictive illustrative embodiment, it is to be understood that such disclosure is not to be interpreted as limitative. Various alternatives and modifications will no doubt become apparent to those skilled in the art upon reading the above disclosure.