Superfluorescent source stabilization

Abstract: A wavelength stabilization apparatus (10) and method for a superfluorescent source comprising a SFS (superfluorescent source) comprising a fibre with a core doped with lazing material. The SFS source produces SFS light with an SFS wavelength when pumped with pump light from a pump light source (14) having a pump light wavelength. An output controller responds to a sample of the SFS light and operates to maximize the power of the sample of SFS light by automatically adjusting the pump light wavelength. The output controller also has a pump power controller (27) responsive to a sample of the pump light from the pump light source for stabilizing the output power of the sample of the pump light with respect to the predetermined reference output power level.

Description: This invention relates to the field of optics and more particularly to the field of light sources, also called amplified spontaneous emission (ASE) lasers useful in applications such as interferometric sensors such as a fiber optic gyro. U.S. Patent 4,637,025 for a "Super Radiant Light Source" issued Jan. 13, 1987 to E. Snitzer et al describes the use of a single mode optical fiber having a core doped with an active laser material such as neodymium. The fiber is pumped with pump light sufficient to produce amplification of spontaneous emissions. In one embodiment, a dichroic mirror is used to provide a double pass for light in the fiber core for extra gain. Snitzer does not show or suggest a control process for controlling the wavelength of the pump source light. Fiber Laser Sources and Amplifiers II, SPIE Procs. Vol. 1373, 18 September 1990, pp. 234-245 and Electronics Letters, Vol. 13, No. 584, 21 June 1990, pp 870-879 propose a superfluorescent fiber source system as a broadband source comprising a SFS (superfluorescent source) means for producing SFS light having a SFS wavelength when pumped with pump light from a light source having a pump light wavelength. They discuss the stabilisation of the SFS output wavelength. Temperature sensitivity of the mean wavelength is suggested as being dependent upon various parameters and it is suggested that, by selecting the values of those parameters, one can achieve a stable operating point, i.e. reduce substantially to zero a relationship between those parameters defining the temperature sensitivity. According to a first aspect of the invention there is provided a superfluorescent fiber source system comprising: a SFS (superfluorescent source) means for producing SFS light having an SFS wavelength when pumped with pump light from a light source having a pump light wavelength, the system being characterised by control means comprising: an output controller means responsive to a sample of light from the SFS means to tend to maximize the power of said SFS light by automatically adjusting said pump light wavelength. In one embodiment the output controller means has a pump light source temperature control means responsive to a thermal drive signal for controlling the temperature of the pump light source, and an output sense and control means for sensing the power of a sample of said SFS light and for controlling the thermal drive signal to vary the temperature of the pump light source around an operating temperature, the variation in pump light source temperature resulting in a corresponding variation in pump light source wavelength, said SFS source being responsive to the variation in pump light source wavelength to provide a corresponding variation in the power of the sample of the SFS light, the output sense and control means being responsive to the variation in the power of the sample of the SFS light for adjusting the thermal drive signal to adjust the operating temperature of the pump light source to maximize the power of the sample SFS light. In another embodiment, the output controller means has a pump light source temperature control means responsive to a thermal drive signal for controlling the temperature of the pump light source and an output sense and control means for sensing the power of a residual pump ray exiting the SFS means and for adjusting the thermal drive signal to adjust the operating temperature of the pump light source to minimize the power of the residual pump ray. According to a second aspect of the invention there is provided a stabilization method for stabilizing a superfluorescent fibre source comprising the steps of: pumping a SFS (superfluorescent source) fibre to produce SFS light having an SFS wavelength with pump light from a pump light source having a pump light wavelength, characterised by sampling light from the SFS and maximizing the power of the SFS light by automatically adjusting the pump light wavelength. For a better understanding of the invention, and to show how the same may be carried into effect, reference will now be made, by way of example, to the accompany drawings in which: Figure 1 is a block diagram of the control system for a broadband super fluorescent light source (SFS); Figure 2 is a graphical schematic representation of the pump absorption by the SFS fiber measured as the ratio of the residue pump power leaving the super fluorescent source fiber to the power into the SFS fiber as a function of the pump wavelength. Figure 3 is a graphical schematic representation of the SFS fiber emission power as a function of pump wavelength with pump power being held constant; Figure 4a is a graphical schematic representation of the SFS fiber emission wavelength as a function of pump wavelength with pump power held constant at a first and second level; Figure 4b is a graphical schematic representation that shows that the SFS fiber emission wavelength Ls of the SFS emission ray 32 varies as a function of the pump light ray 16 pump light power PMPPWR; Figure 5 is a graphical schematic representation of the pump wavelength as a function of temperature; Figure 6 is a graphical schematic representation of the SFS emission wavelength Ls as a function of the temperature of the SFS fiber source; Figure 7 is a block diagram of an alternate embodiment of the control system for a broadband super fluorescent light source (SFS); Figures 8a, 8b and 8c are graphical schematic representations showing the values of SFS fiber emission power that result at the extremes of a fixed variation in the temperature of the pump in response to variations in the TEC temperature; Figure 9 is a graphical schematic representation of the TDITHER drive voltage from the reference oscillator as a function of time; Figure 10 is a block diagram of an embodiment of the output controller for the control system for a broadband super fluorescent light source (SFS); Figure 11 is a more detailed block diagram of an embodiment of the output controller for a broadband super fluorescent light source (SFS); Figure 12 is a block diagram of an embodiment of the pump power controller for the control system for a broadband super fluorescent light source (SFS); Figure 13 is a block diagram of an embodiment of a temperature controller for the SFS fibre source. Figure 1 is a block diagram of a preferred embodiment of a system 10 for stabilizing the wavelength of a SFS fiber source 12. Pump light source 14 provides a pump light ray 16 at pump wavelength PMPLNTH and with pump power PMPPWR to the SFS (super fluorescent source) fiber 12 via a pump light optical path 18 to WDM (wavelength division multiplexer) 20. The WDM 20 splits the pump light ray 16 by a predetermined ratio and couples a first portion of the pump light ray 16, referred to as pump monitor light ray 22 with pump power Pp1, via a pump monitor fiber port 24, to pump monitor fiber port 25, to a pump monitor detector 26. Pump power controller 27 represents a pump power control means responsive to a pump detector signal from pump monitor detector 26 for adjusting the amplitudes of the pump drive current IPMDRV to maintain the pump monitor light ray 22 from pump monitor fiber port 25 at constant power. A second portion of pump light ray 16, referred to as main ray of pump light 28 with pump power Pp2 is coupled into the SFS fiber source 12 via optical path 30. The SFS fiber source 12 contains a single mode optical fiber having a core doped with at least one active laser material such as neodymium or erbium. The SFS fibre is pumped by the main ray of pump light 28 via optical path 30 with sufficient power Pp2 to produce amplification of spontaneous emission of the active laser material to provide an SFS emission ray 32 of light that exits the SFS fiber source 12 via SFS optical path 30. A dichroic mirror 58 formed on the end surface of the SFS fiber source 12 reflects light at the wave-length of the SFS emission ray 32 to provide a double pass for SFS light in the SFS fiber source for extra gain. The dichroic mirror 58 is designed to pass a residual pump light ray 36 through the dichroic mirror 58 to avoid reflection of the unabsorbed portion of the main ray of pump light 28 back to the WDM 20. Use of the dichroic mirror 58 improves operation of the invention; however, the system will operate without it but with reduced efficiency. The SFS emission ray 32 returns to the WDM 20 via SFS optical path 30 with an SFS emission power Ps and with the SFS emission wavelength Ls. The WDM 20 directs the SFS emission ray 32 via the WDM output path 38 as SFS output emission ray 39 to the coupler input 40 of coupler 42. Coupler 42 splits the SFS output emission ray 39 into an SFS output ray 44 at SFS system output 46 and into an SFS sense ray 47 output at SFS sense output 48. Coupler 42 is typically designed to provide over 90% of the power of the SFS output emission ray 39 to the SFS system output 44 and less than 10% of the power to the SFS sense output 48. The SFS sense ray 47 is directed via SFS output fiber 50 through SFS output detector port 51 to SFS output detector 52. SFS output controller 54 represents a temperature control means responsive to an SFS output sense signal represented by phantom line 55 from SFS output detector 52 for adjusting the wavelength of the pump light ray 16 by adjusting the pump temperature Tp of the pump light source 14 to maximize the amplitude of the SFS sense ray 47 by adjusting the drive current ITHERMDV to a thermal electric cooler (TEC) 56. Pump power controller 27 represents a pump power control means responsive to a pump detector signal from pump monitor detector for adjusting the amplitude of the pump drive current IPMDRV to maintain the pump monitor light ray 22 from pump monitor fiber port 25 at constant power. Figure 2 is a graphical schematic representation of the pump absorption by the SFS fiber measured as the inverse ratio of the residual pump power in sense ray 36 leaving the super fluorescent source fiber via dichroic mirror 58 to the power delivered to the SFS fiber 12 by main ray of pump light 28 via SFS optical path as a function of the pump wavelength PMPLNTH of the pump light ray 16. The peak in the absorption of pump power at "A" was obtained using a sample of Erbium doped alumino-silicate fiber. The peak at "A" was observed to occur at approximately 980 nano meters as the pump wavelength PMPLNTH is swept from 900 nano meters to 1000 nano meters while holding the power in the pump monitor light ray 22 in Figure 1 substantially constant. A laser diode with a center wavelength at 980 nano meters was selected for use in the pump light source 14; however, in alternate embodiments, laser diodes with wavelengths centered at 810, 980 or 1475 nanometers can be used depending on the requirements of the particular embodiment. A model OL452A diode purchased from OKI in Japan was suitable for the application. Figure 3 is a graphical schematic representation of the SFS fiber emission power in SFS emission ray 32 as a function of pump wavelength with pump power being held constant. This graph shows that the peak output power of the SFS emission ray 32 to WDM 20 also coincides with a pump wavelength of 980 nanometers. Figure 4a is a graphical schematic representation of data that shows that the SFS fiber emission wavelength Ls of the SFS emission ray 32 varies as a function of the pump light ray 16 pump light wavelength PMPLNTH. Variation of the SFS fiber emission wavelength Ls as a function of pump wavelength is shown with the SFS emission power held constant at a first level of 4 mW and second level of 10 Mw. Figure 4a shows that the stability of the SFS wavelength is greatest where the change in SFS wavelength with respect to a change in the pump wavelength is least. The point of greatest stability also occurs when the pump wavelength PMPLNTH is at or near 980 nano meters. Figure 4b is a graphical schematic representation of data that shows that the SFS fiber emission wavelength Ls of the SFS emission ray 32 varies as a function of the pump light power PMPPWR of the pump light ray 16. By way of example, the power level of this ray is typically in the order of 30 mW. A pump power stability of about 1% is required to achieve an SFS emission wavelength stability of approximately 30 ppm. Figure 5 is a graphical schematic representation that shows that the pump wavelength PMPLNTH varies as a function of pump temperature. The wavelength PMPLNTH of the pump light ray 16 is controlled by a means for controlling the pump source temperature such as the thermoelectric cooler (TEC) 56. Figure 5 also shows that as the TEC 56 temperature is modulated over a controlled range, the pump wavelength varies accordingly. Figure 6 graphically depicts in schematic fashion that the SFS emission wavelength Ls varies also as a function of the temperature of the SFS fiber source. Since the pump light source 14 is typically a diode with a dissipation that is dependent on its forward voltage drop and the drive current passing through it, and since there is no mechanism or process present to link the temperature of the SFS fiber source 12 to that of the pump light source 14, contributions to a change in the wavelength of the SFS source 12 due to changes to the temperature of the pump light source 14 which changes PMPLNTH and changes to the SFS source wavelength Ls from changes in the temperature of the SFS fiber source 12 are substantially independent of each other. Equation 1, below, shows that the variation of the SFS emission ray wavelength DLs is a function of the partial derivative of Ls with respect to pump power PMPPWR times an incremental change in pump power DPMPPWR, plus the partial derivative of Ls with respect to pump wavelength PMPLNTH times an incremental change in pump wavelength DPMPLNTH, plus the partial derivative of Ls with respect to the temperature of the SFS source fiber Ts times an incremental change in the temperature of the source fiber Dts. A net decrease in the maximum absolute value of DLs term at the left of the equation implies an increase in the stability of the SFS emission ray wavelength Ls. It is clear that the stability of the SFS emission ray wavelength Ls is greatest when the term DLs goes to zero. The DLs term is zero when the three terms on the right side of Equation 1 sum to zero. Equation 1. DLs = (DLs /DPMPPWR)*DPMPPWR + (DLs /DPMPLNTH)*DPMPLNTH + (DLs/DTs)*DTs Figure 7 shows a mechanization of an alternative preferred embodiment in which the third term in Equation 1 relating to the temperature of the SFS fiber source 12 is modeled out. Figure 1 shows a preferred embodiment in which the third term of Equation 1 is evaluated. Referring to Figure 1, SFS thermistor 59 senses the temperature of the SFS fiber source and provides an SFS temperature signal to a signal conditioner 60 within a using system within phantom block 62. Signal conditioner 60 converts the SFS temperature signal into a series of sampled digital values that are coupled via bus 61 to signal processor 64 for use in correcting factors sensitive to the wavelength of the SFS output signal via ray 44 from output port 46 of coupler 42. Using system 62, is typically an instrument such as an interferometer, fiber optic gyro, or triax fiber optic gyro that receives and uses the stabilized output light ray 44 at a receiving coupler 66 or other internal optics arrangement or instrument. The receiving coupler is used to output at least a first portion of the output signal 44 to at least a first internal instrument or system detector 68 using system 62. The output of each system detector 68 couples the signal to a conditioner 70. After amplification and conditioning by conditioner 70, the conditioned signal from conditioner 70 is also provided to the signal processor 64 where the compensating effects from the SFS temperature signal are used to compensate for variation in the system signal from conditioner 70 that are due to the influence of temperature effects on the SFS source. Referring to Figure 6, as the temperature of the SFS source 12 varies, the signal processor 64 refers to a relationship, such as the relationship of Figure 6, and the measured value of the temperature of the SFS fiber source 12 for a particular fiber and calculates the compensation required to cancel the effect of the third term in Equation 1. In another alternate embodiment of the invention, such as that shown in Figure 13, the SFS fiber source 12 is placed on a temperature controller such as SFS TEC 72. The SFS thermistor 59 senses the temperature and provides the SFS temperature signal to an SFS fiber temperature controller represented by phantom block 74 for controlling the temperature of the SFS fiber source 12. In the alternative embodiment of Figure 13, the SFS fiber temperature control means responds to the SFS temperature signal and to a predetermined temperature reference signal T s for stabilizing the temperature of the SFS fiber 12 to a value corresponding to the predetermined temperature reference signal T s . It is apparent from the block diagrams of Figures 1 and 7 that by sensing the temperature of the SFS fiber source 12, and by using temperature control process for the SFS fiber source 12 such as that described above in connection with Figure 13, it would be feasible to further stabilize the superfluorescent source by turning the third term in Equation 1 substantially to a constant bias term. In each of the above alternative embodiments, the associated wavelength error in the SFS system output signal 44 is optionally compensated by the subsequent using system 62 by software corrections made by the system signal processor 64. The control process that remains requires that the value of the first and second terms be as small as possible , or of equal magnitude and opposite sign. In the embodiment of Figure 1, the pump monitor detector 26 provides a signal representative of the amplitude of the first portion of the pump power Pp1 to the pump power controller 27. The pump power controller 27 represents a means responsive to the pump power signal from pump monitor detector 26 for regulating the value of IPMPDRV to fix the output power of the light from the pump light source 14 to a predetermined value. Thus, the first term in Equation 1 above is close to zero since (DPMPPWR ~ 0) by operation of the controller. Figure 12 shows an embodiment of the pump power controller 27 in which detector 26 senses light ray 22 which is proportional to the output power of the pump light source light applied to the SFS source 12. The signal from detector 26 is amplified and conditioned by amplifier KA. The output of the amplifier KA is low pass filtered by filter HI2(S). The filtered output is fed to the adder and summed with predetermined signal ISET representing the desired current in the pump power source. The output of the adder is integrated by GI(S) and the integrated output is fed back via HI1(S) to the adder. The output of the integrator is used to drive current to the pump power source. Figure 13 shows an embodiment of the SFS fiber temperature controller in which thermistor T1 senses the temperature of the SFS fiber 12. The SFS temperature signal from the thermistor T1 is conditioned by amplifier KB and is proportional to the temperature of the SFS fiber source 12. The SFS temperature signal is low pass filtered by filter HF2(S). The filtered output is fed to the adder and summed with predetermined signal Ts representing the desired temperature of the SFS fiber source 12. The output of the adder is integrated by GF(S) and the integrated output is fed back via HF1(S) to the adder. The output of the integrator is used to drive the TEC 72 to control the temperature of the SFS fiber source 12. With reference again to Figure 1, an embodiment of the invention is best characterized as a wavelength stabilization apparatus for a superflourescent source 10. A SFS fiber source 12 represents an SFS (superfluorescent source) means for producing SFS light having an SFS wavelength when pumped with pump light from a pump light source 14 having a pump light wavelength, typically in range of 978 to 983 nano meters. In a simple form, the embodiment has an output controller means represented by output controller block 54 that is responsive to a sample of the SFS light at ray 47 for maximizing the power of said sample of SFS light by automatically adjusting said pump light wavelength. By maximizing the power of ray 47, the output controller means maximizes the stability of the SFS fiber source output. The performance of the stabilization apparatus for the superfluorescent source improves by adding a pump power controller means 27 to the output controller means to sample the pump light from said pump light source via ray 22 exiting fiber pump monitor fiber port 25, for stabilizing the output power of the sample of said pump light with respect to a predetermined reference output power level. In each of the preferred embodiments of the wavelength stabilization apparatus for the superfluorescent source, the SFS fiber source contains a single mode optical fiber having a core doped with at least one active laser material selected from the group of rare earth materials such as neodymium or erbium or aluminum. Referring again to the embodiment of Figure 1 and Figure 7, the SFS output controller 54 can be viewed as representing an output controller means having a pump light source temperature control means such as the TEC (thermal electric cooler) 56 that is responsive to a thermal drive signal such as ITHERMDV for controlling the temperature of the pump light source 14, and an output sense and control means 54 for sensing the power of the sample of said SFS light via SFS sense ray 47, or residual ray 36, and for dithering the thermal drive signal by superimposing a small oscillatory signal on ITHERMDV to slightly vary the temperature of the pump light source around an operating temperature. A variation in pump light source temperature results in a corresponding variation in pump light source wavelength in pump light ray 16. The SFS fiber source 12 responds to the variation in pump light source wavelength and provides a corresponding variation in the power of the SFS sense ray 47 sample of the SFS light. Figures 8a through 8c show how the SFS emission power varies in response to a variation in the temperature of the pump light source 14 at three different temperatures in synchronization with the reference signal waveform from the OSC1 oscillator in Figure 9. The OSC 1 reference oscillator 112 is shown and discussed in connection with in Figures 10 and 11. Figure 8a shows the condition of the dither range DT on the independent variable axis centered at the desired temperature To. Figure 8b illustrates the condition of the dither range DT on the independent variable axis being displaced to an operating range centered at a temperature below the desired temperature To. The difference between the amplitude of the SFS emission power at the high temperature limit B2 of the dither range minus the value of the emission power at the low limit of the temperature range BI results in a positive value. Alternatively, Figure 8c shows that the difference between the amplitude of the SFS emission power at the high temperature limit C2 of the dither range minus the value of the emission power at the low temperature limit of the temperature range C1 results in a negative value. The SFS output controller of Figure 1 responds to the variation in the power of the sample of the SFS light at SFS sense ray 47 by adjusting the thermal drive signal ITHERMDV to adjust the operating temperature of the pump light source 14 to maximize the power of the sample SFS sense ray, i.e. the output sense signal at sense ray 47. The stability of the wavelength stabilization apparatus is increased by combining the use of a pump power controller means, discussed above in connection with block 27 in combination with a pump light source temperature control means, such as TEC 56. TEC 56 responds to a thermal drive signal to control the temperature of the pump light source 14. An output sense and control means, such as SFS output controller 54 discussed above, senses the power of the sample of the SFS light with SFS output detector diode 52 as it is illuminated starting with rays 39, via WDM 20 to fiber 38, to input 40 at output coupler 42, then via fiber 50 as SFS sense ray 47 incident on diode 52. Diode 52 is a conventional detector diode and may be hermetically mounted in a metal can containing a pre-amp and an input lens through which sense ray 46 is allowed to pass. Detector diodes are sometimes PIN diodes. In the alternative, diode 52 is contained within the SFS output controller 54. For this arrangement, sense ray 47 is extended to include ray 55 entering the SFS output controller 54 to be incident on a detector ( not shown ). Figure 10 shows an embodiment of an SFS output controller 54 or output sense and control process or circuit for receiving the sensed signal, as in Figure 7, via ray 36 via signal lines 114, 115. Block 116 represents an SFS emission output amplifier having a voltage gain typically in the range of 20 to 100. The amplified sense signal is coupled from amplifier output 118 to the input of a PSD (phase sensitive demodulator) 120 at a first input 122. The PSD is referenced to the output of OSC1 by signal FDITHER at second input 124. Figure 9 shows a typical waveform for OSC1. The demodulated output of the PSD 120 is fed to the LPF (low-pass filter) 126. The filtered sense signal is fed to integrator input 128 for integration by integrator HT2(S), 130. The demodulated, filtered, integrated sense signal is coupled to a first subtracting input 134 of adder 136 for subtraction from feedback signal from ITHERMDV via feedback element 138. The output of adder 136 is coupled to the first input 140 of second adder 142. A predetermined temperature reference signal at second adder input 144 from potentiometer 146 is added with the FDITHER signal from OS1 112 to form a combined signal or the feedback corrected demodulated, filtered, integrated sense signal at the input 148 of the GT(S) block 150. The GT(S) block 150 block filters and integrates the combined signal to form the ITHERMDV drive signal to the TEC 56. Note that the FDITHER signal is imposed on the input of the GT(S) control block 150 at a point that insures that the output of the GT(S) block will contain the dither signal desired. The control process 210 of Figure 11 contains many elements identical to those in the control process of Figure 10; but, also includes a provision for receiving a temperature feedback signal TOFF from the TEC thermistor on signal line 214. The control process of FIG. 11 also contains compensation block GC2(S) 216 and GC1(S) 218 with compensating poles and zeros introduced to accommodate the response characteristics of the TEC 56 when driven by ITHERMDV on signal line 220. The control process 210 provides a TEC thermal control in accordance with the control signal on signal line 222. The apparatus of Figure 1 provides a way to practice a method or process for the wavelength stabilization of a superfluorescent fiber source comprising the step of: A. pumping a SFS (superfluorescent source) to produce SFS light having an SFS wavelength with pump light from a pump light source having a pump light wavelength; B. sampling SFS light from the SFS and maximizing the power of the sample of SFS light by automatically adjusting the pump light wavelength; and C. repeating steps A and B. The apparatus of Figure 7 provides a way to practice the method for stabilizing a superfluorescent source comprising the steps of: A. producing SFS light from an SFS source having an SFS wavelength by pumping the SFS source with pump light from a pump light source having a pump light wavelength, a first portion of said pump light being absorbed in pumping the SFS source and a second portion of said pump light exiting the SFS source as a residue pump ray; followed by step: B. sensing the residue pump ray and responding to the residue pump ray to maximize the power of said sample of SFS light by automatically adjusting said pump light wavelength to minimize the power of the residue pump ray. Accordingly there has been described a wavelength stabilization apparatus and method for a superfluorescent fiber source. Although the invention has been disclosed and illustrated in detail, it is to be understood that the same is by way of illustration and example only and is not to be taken by way of limitation.

Claims: A superfluorescent fiber source system comprising: a SFS (superfluorescent source) means (12) for producing SFS light having an SFS wavelength when pumped with pump light from a light source (14) having a pump light wavelength, the system being characterised by control means comprising: an output controller means (54) responsive to a sample of light (39, 36) from the SFS means to tend to maximize the power of said SFS light by automatically adjusting said pump light wavelength. A system according to claim 1 and comprising a pump power controller means (27) responsive to a sample of the pump light from said pump light source (14) for stabilizing the output power of the sample of said pump light with respect to a predetermined reference output power level. A system according to claim 1 or 2, said output controller means comprising a pump light source temperature control means (56) responsive to a thermal drive signal for controlling the temperature of the pump light source (14). A system according to claim 3, and comprising an output sense and control means (54) for sensing the power of a sample of said SFS light and for dithering the thermal drive signal to slightly vary the temperature of the pump light source around an operating temperature, the variation in pump light source temperature resulting in a corresponding variation in pump light source wavelength, said SFS fiber source being responsive to said variation in pump light source wavelength to provide a corresponding variation in the power of the sample of the SFS light, the output sense and control means being responsive to the variation in the power of the sample of the SFS light for adjusting the thermal drive signal to adjust the operating temperature of the pump light source to maximize the power of the sample SFS light. A system according to claim 1, 2 or 3, and arranged so that a first portion of said pump light will be absorbed in pumping the SFS means and a second portion (36) of said pump light will exit said SFS means as a residual pump ray (36), the control means being responsive to the residual pump ray for maximizing the power of SFS light by automatically adjusting said pump light wavelength. A system according to claim 5, wherein the output sense and control means (54) is arranged for sensing the power of the residual pump ray, the power of the residual ray varying in an inverse function to the power of the SFS light output, the output sense and control means being responsive to the variation in power of the residual pump ray for adjusting the thermal drive signal to adjust the operating temperature of the pump light source to minimize the power of the residual pump ray. A system according to claim 5 or 6 wherein said SFS means comprises a dichroic mirror (58) for passing light at the pump wavelength and for reflecting light at the SFS source wavelength into the SFS source. A system according to claim 3 or to any one of claims 4 to 7 when appended to claim 3, said pump light source temperature control means comprises: a thermoelectric cooler (56) to which the pump light source is thermally coupled; and a thermistor (T2) for measuring the temperature of the pump light source and for providing a pump temperature signal corresponding to the temperature of the pump light source; said output sense and control means being responsive to the pump temperature signal for adjusting the thermal drive signal to adjust the operating temperature of the pump light source (14) to maximize the power of the SFS light. A system according to any one of the preceding claims wherein said superfluorescent source means (12) comprises a superfluorescent fiber source. A system according to claim 9 wherein said SFS fiber source contains a single mode optical fiber having a core doped with at least one active laser material selected from the group of rare earth materials comprising neodymium or erbium. A system according to any one of the preceding claims, the control means comprising: a temperature control means (62) responsive to a SFS temperature control signal for controlling the temperature of the SFS source to correspond with a predetermined fixed value; and a temperature control measuring means (59) coupled to the SFS source for providing said SFS temperature signal. A stabilization method for stabilizing a superfluorescent fibre source comprising the steps of: pumping a SFS (superfluorescent source) fibre to produce SFS light having an SFS wavelength with pump light from a pump light source having a pump light wavelength, characterised by sampling light from the SFS and maximizing the power of the SFS light by automatically adjusting the pump light wavelength. A stabilization method according to claim 12 comprising the steps of: pumping the SFS source with pump light so that a first portion of said pump light is absorbed in pumping the SFS source and a second portion of said pump light exits the SFS source as a residual pump ray: sensing the residual pump ray; and responding to the residual pump ray to maximize the power of said SFS light by automatically adjusting said pump light wavelength minimize the power of the residual pump ray.

Inventors: FIDRIC BERNARD G, LIBMAN DAVID F, FIDRIC, BERNARD G., LIBMAN, DAVID F.
Applicants: LITTON SYSTEMS INC, LITTON SYSTEMS, INC.
Application year: 1991
Main classification: H01S3
IPC codes: H01S3