Patent Publication Number: US-2023134631-A1

Title: Asymmetric chirped fiber bragg grating for diode laser of fiber amplifier

Description:
BACKGROUND OF THE DISCLOSURE 
     Laser diodes are used for optical fiber amplifiers, and fiber Bragg gratings (FBG&#39;s) are used with the laser diodes to lock them to a pump wavelength. Some common types of fiber Bragg gratings include a uniform fiber Bragg grating and a chirped fiber Bragg grating. The uniform fiber Bragg grating has grating elements uniformly spaced along a length of a fiber member. By contrast, the chirped fiber Bragg grating has grating elements that increase in spacing along a length of a fiber member. 
     Both of these types of fiber Bragg gratings have their own benefits and uses. As one example, a fiber Bragg grating, such as a chirped fiber Bragg grating, can offer wider bandwidths and can increase the number of laser modes captured within the envelope of the fiber Bragg grating when used with a laser diode. The spectral bandwidth of the resulting laser output creates more incoherent light that can improve output power variation for the optical fiber amplifier. In essence, the wider bandwidth from the chirped fiber Bragg grating allows for more modes to be captured within the envelope of the fiber Bragg grating, thus increasing the power sharing across an increased number of modes. 
     Although existing fiber Bragg gratings used with laser diodes in optical fiber amplifiers may be effective, the subject matter of the present disclosure is directed to improving implementations, such as optical fiber amplifiers having laser diodes. 
     SUMMARY OF THE DISCLOSURE 
     An optical device disclosed herein is used with a laser diode. The laser diode has an end facet and is configured to output light at a selected wavelength. The optical device comprises an optical fiber segment configured to optically interact with the output light. The optical fiber has a fiber Bragg grating, which has a plurality of refractive index variations. The refractive index variations have a chirped period changing spatially along a length of the fiber Bragg grating. The refractive index variations in the chirped period have a first reflectivity for a short wavelength region of the fiber Bragg grating. The first reflectivity is shifted asymmetrically from a central wavelength region of the fiber Bragg grating, is greater than a second reflectivity of the central wavelength region, and is greater than a third reflectivity of the other of the long wavelength region. 
     A fiber amplifier disclosed herein is used to amplify seed light having a seed wavelength. The fiber amplifier comprises a laser diode, an optical fiber segment, and a doped fiber. The laser diode is configured to generate pump light at a pump wavelength. The laser diode has front and back end facets. The front end facet has a front reflectivity, and the back end facet has a back reflectivity. 
     The optical fiber segment is in optical communication with the pump light from the second end facet. The optical fiber segment has a fiber Bragg grating configured to lock the pump light to the pump wavelength. The fiber Bragg grating has a length and has a plurality of refractive index variations, which have a chirped period changing spatially along the length of the fiber Bragg grating. The refractive index variations in the chirped period have a first reflectivity for a short wavelength region of the fiber Bragg grating. The first reflectivity is shifted asymmetrically from a central wavelength region of the fiber Bragg grating, is greater than a second reflectivity for the central wavelength region, and is greater than a third reflectivity for a long wavelength region. The doped fiber is doped with an active dopant. The fiber is in optical communication with the seed light and is in optical communication with at least a portion of the pump light from the laser diode. The pump wavelength of the pump light is configured to interact with the active dopant of the fiber and thereby amplify the seed light. 
     A method is disclosed herein to amplify seed light having a seed wavelength. The method comprises: generating pump light with a laser diode, the pump light having a pump wavelength different from the seed wavelength, the laser diode having a front facet with a front reflectivity; coupling the pump light from the front facet of the laser diode with an optical fiber segment having a fiber Bragg grating, the fiber Bragg grating having a length and having a plurality of refractive index variations, the refractive index variations having a chirped period changing spatially along the length of the fiber Bragg grating; locking the pump light of the laser diode to the pump wavelength by reflecting at least a portion of the pump light back to the front facet using the fiber Bragg grating, the refractive index variations in the chirped period having a first reflectivity for a short wavelength region of the fiber Bragg grating, the first reflectivity being shifted asymmetrically from a central wavelength region of the fiber Bragg grating, being greater than a second reflectivity for the central wavelength region, and being greater than a third reflectivity for a long wavelength region; transmitting the seed light and at least a portion of the pump light to a doped fiber; and amplifying the seed light by interacting the pump light with the doped fiber. 
     The foregoing summary is not intended to summarize each potential embodiment or every aspect of the present disclosure. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG.  1 A  illustrates an optical fiber amplifier according to the present disclosure. 
         FIG.  1 B  illustrates a submarine repeater having optical fiber amplifiers according to the present disclosure. 
         FIG.  1 C  illustrates a Master Oscillator Power Amplifier (MOPA) system having an optical fiber amplifier according to the present disclosure. 
         FIG.  2 A  illustrates an asymmetric chirped fiber Bragg grating according to the present disclosure. 
         FIG.  2 B  graphs wavelength versus reflected power for an envelope of the disclosed asymmetric chirped fiber Bragg grating. 
         FIG.  2 C  graphs wavelength versus reflectivity for the disclosed asymmetric chirped fiber Bragg grating in more detail. 
         FIG.  3 A  graphs a standard envelope of power relative to wavelength for a uniform fiber Bragg grating. 
         FIG.  3 B  graphs a dominant mode in the standard envelope. 
         FIGS.  4 A- 4 B  graph envelopes for a standard chirped fiber Bragg grating that provides wider bandwidth. 
         FIG.  5 A  graphs a dominant mode in the envelope for the standard chirped fiber Bragg grating. 
         FIG.  5 B  graphs a skewed reflectivity envelope for the disclosed asymmetric chirped fiber Bragg grating of the present disclosure. 
         FIG.  6 A  graphs gain and carrier distribution for a laser operating at lower current/optical power. 
         FIG.  6 B  graphs gain and carrier distribution for a laser operation at high current/optical power that produces spectral hole burning. 
         FIG.  6 C  graphs gain and reflectivity for wavelengths when feedback is provided by an external fiber Bragg grating with finite reflectivity and width in the presence of spectral hole burning. 
         FIG.  7 A  graphs reflectivity in a standard profile along with a net gain without spectral hole burning and another net gain with spectral hole burning. 
         FIG.  7 B  graphs reflectivity in another profile according to the present disclosure along with a net gain without spectral hole burning and another net gain with spectral hole burning. 
         FIG.  8 A  graphs power variation for a laser driven by a drive current when locked using a standard chirped fiber Bragg grating and an asymmetric chirped fiber Bragg grating of the present disclosure. 
         FIG.  8 B  graphs spectral width for a laser driven by a drive current when locked using a standard chirped fiber Bragg grating and an asymmetric chirped fiber Bragg grating of the present disclosure. 
         FIG.  9 A  illustrates a uniform fiber Bragg grating known in the art. 
         FIG.  9 B  graphs wavelength versus reflected power for an envelope of the uniform fiber Bragg grating. 
         FIG.  10 A  illustrates a standard chirped fiber Bragg grating known in the art. 
         FIG.  10 B  graphs wavelength versus reflected power for an envelope of the standard chirped fiber Bragg grating. 
         FIG.  10 C  graphs wavelength versus reflectivity for the standard chirped fiber Bragg grating in more detail. 
     
    
    
     DETAILED DESCRIPTION OF THE DISCLOSURE 
       FIG.  1 A  illustrates an optical amplifier  10  having a pump laser  20  outputting pump light P for a doped fiber  18 . Source or seed light S passing along an optical path  12 , which can include optical fibers, passes through an isolator  14  to a combiner  16 . The isolator  14  may be configured to prevent or at least reduce back reflection from the combiner  16 . For its part, the combiner  16  combines the seed light S with the pump light P received from the pump laser  20  via a pump path, which includes an optical fiber segment  30  and an asymmetric chirped fiber Bragg grating (FBG)  50  according to the present disclosure. In general, the combiner  16  can be a dichroic pump coupler, fused-fiber coupler, or other coupler configured to combine the pump light P with the seed light S. 
     The pump laser  20  is a laser diode having a waveguide  22 , an active layer, cladding layers, a cathode  26 , an anode  28 , a substrate, and other necessary components. Other mounting configurations are possible. The waveguide  22  has a laser cavity formed by front and back mirrors on its end facets  24   b ,  24   f . The front and back mirrors on the end facets  24   b ,  24   f  have power reflectivities of Rf and Rb, respectively, for which Rf&lt;Rb. 
     During operation of the optical fiber amplifier  10 , the seed light S has a seed wavelength λ S , and the pump light P received at the combiner  16  has a pump wavelength λ Pump . The value of the pump wavelength λ Pump  is selected to provide optical amplification to the seed light S operating at the seed wavelength As in the presence of a specific rare-earth dopant within the doped fiber  18 . The dopant may be erbium, ytterbium, or other dopant. When the dopant is erbium, the wavelength λ Pump  of the pump light P emitted by the laser  20  may be about 980 nanometers (nm) (e.g., 970 nm to 990 nm), such as a wavelength of 972 nm, 974 nm, 976 nm, or 978 nm. In some embodiments, the pump light P at the wavelengths λ Pump  of about 980 nanometers may be configured to provide amplification in the doped fiber  18  to the seed lights S when the seed wavelengths λ S  of the seed light S is about 1550 nm, such as wavelengths in the C band (˜1525 nm to 1570 nm), or about 1590 nm, such as wavelengths in the L band (˜1570 nm to 1625 nm). 
     The combiner  16  outputs the seed light S combined with the pump light P to the doped fiber  18 . The pump light P at the pump wavelength λ Pump  energizes ions in the doped fiber  18 , and the seed light S at the seed wavelength λ S  interacts with the energized ions. In particular, photons of the seed light S at the seed wavelength λ S  stimulates emission of photons from the energized ions at the seed wavelength λ S  to generate the amplified light S A . The amplified light S A  can then pass through an isolator  14  to an output. The system  10  may include additional pump lasers  20 , combiners  16 , and the like, such as shown here. 
     According to the present disclosure, the laser diode  20  uses the asymmetric chirped fiber Bragg grating  50  of the optical fiber segment  30  for wavelength feedback. In particular, the pump light emitted through the front facet  24   f  is coupled into the optical fiber segment  30 . To increase the coupling efficiency, a lens or lens structure  32  having an antireflection coating can be fabricated on the fiber tip of the optical fiber segment  30 . For example, the lens or lens structure  32  can include a taper or cone fabricated on the fiber tip, but other structures can be used, such as cylinder, angled cleave, flat cleave, etc. 
     The pump light P propagates along the optical fiber segment  30  and is reflected by the fiber Bragg grating  50 , which has a grating reflectivity profile or envelope Rg. The fiber Bragg grating  50  is positioned at a given distance from the laser&#39;s end facet  24   f , and the front facet&#39;s mirror and the fiber Bragg grating  50  produce an external resonator cavity for the laser light. As will be appreciated, particular values for the reflectivities Rf, Rb, and Rg can depend on the implementation. In a general case, the values for reflectivities are Rb&gt;Rg&gt;Rf. The reflectivity bandwidth for Rf and Rb is much wider as compared to the reflectivity bandwidth of the Rg. Two main optical cavities are formed by the disclosure configuration. The first optical cavity is between Rb and Rf, while the second optical cavity is between Rb and Rg. For the purposes of the present teachings, the optical cavity between Rf and Rg is not under consideration. Instead, when the contribution of the external cavity (optical fiber segment  30  and fiber Bragg grating  50 ) dominates the reflectivity Rf, the laser diode  20  can be locked to wavelength(s) defined by the fiber Bragg grating  50 . 
     In general, the disclosed fiber Bragg grating  50  defines the gain of the laser diode  20  at λ B =λ Pump  over a wide range of operating conditions. To do this, the fiber Bragg grating  50  reflects a portion of the pump light P back to the laser diode  20  to lock the laser diode  20  to a narrow wavelength interval configured to overlap with an absorption band for the doped fiber  18 . 
     More particularly, the disclosed fiber Bragg grating  50  may be configured to reflect back a predetermined wavelength or multiple predetermined wavelengths that may “lock” the laser diode  20  to the predetermined wavelength(s) such that the laser diode  20  exhibits stable lasing at the predetermined wavelength(s). In other words, the fiber Bragg grating  50  is configured to reflect back one or more wavelengths, and the reflected light coupled through the end facet  24   f  into the laser diode  20  interacts generally with the laser diode  20  such that the laser diode  20  is locked to predetermined wavelength(s). 
     According to the present disclosure, the disclosed fiber Bragg grating  50  for the laser diode  20  includes an asymmetric chirped fiber Bragg grating, which is discussed in more detail below. The asymmetric chirped fiber Bragg grating  50  is different from a uniform fiber Bragg grating ( 40 :  FIG.  9 A ) and a standard chirped fiber Bragg grating ( 40 ′:  FIG.  10 A ) found in the existing art. Before discussing the asymmetric chirped fiber Bragg grating  50  of the present disclosure, the uniform fiber Bragg grating ( 40 :  FIG.  9 A ) and the standard chirped fiber Bragg grating ( 40 ′:  FIG.  10 A ) found in the existing art are initially discussed. 
       FIG.  9 A  illustrates a uniform fiber Bragg gating  40  as known in the art, and  FIG.  9 B  graphs wavelength versus reflected power for an envelope  48  of the uniform fiber Bragg gating  40 . In the uniform fiber Bragg grating  40 , a number (N) of grating elements  46  are formed at a uniform period (A) along a length (L) of a core  44  of a fiber having a cladding  42 . The grating elements  46  are variations in the refractive index of the fiber core  44 . 
     For the uniform fiber Bragg grating  40  (assuming no strain or temperature variation), the Bragg wavelength is equal to: 
       λ B =2Λ n   eff  
 
     where Λ is the period of the refractive index modulation, and n eff  is the effective refractive index of the fiber core  44 . As shown in  FIG.  9 B , the envelope  48  of the reflected power for the uniform fiber Bragg grating  40  is centered at the Bragg wavelength λ B . 
     In contrast to the uniform fiber Bragg grating  40 , a standard chirped fiber Bragg grating  40 ′ as shown in  FIG.  10 A  has grating elements  46  arranged in a chirped pattern defined by a function Λ(z) so that an overall spectrum of the fiber Bragg grating  40 ′ is produced by the spectrum of each section of the fiber Bragg grating  40 ′. The period Λ(z) of the chirped fiber grating  40 ′ linearly changes along the longitudinal length (L) of the grating  40 ′. The chirped grating  40 ′ can be manufactured using a chirped phase mask that modifies the grating depth. 
     When light is incident on the chirped fiber grating  40 ′, different spectral components of the light are reflected by different parts of the grating  40 ′. Depending on the orientation of the grating  40 ′ relative to incident light, long-wavelength light having slow propagation speed light may be reflected after short-wavelength light having fast propagation speed, or vice versa. The reflection wavelength of the chirped fiber grating  40 ′ (i.e., the Bragg wavelength of each grating element) is spatially varying and has a linear dependence upon the grating length (L). Accordingly, different wavelengths are reflected at different grid periods. As shown in  FIG.  10 B , an envelope  48  of reflected power for the chirped fiber Bragg grating  40 ′ is centered at the Bragg wavelength and has a wider bandwidth (BW) than the envelope for the uniform fiber Bragg grating ( 40 :  FIG.  9 A- 9 B ). 
       FIG.  10 C  graphs the envelope  48  of wavelength versus reflectivity for the standard chirped fiber Bragg gating  40  in more detail. As generally illustrated, wavelength feedback is shown for regions of the grating elements  48 . Short wavelength feedback produces a short wavelength reflectivity region (R 1 ), center wavelength feedback produces a center wavelength reflectivity region (R 2 ), and long wavelength feedback produces a long wavelength reflectivity region (R 3 ). For the standard chirped fiber Bragg grating  40 , the reflectivity regions center about a center wavelength with the center wavelength reflectivity region (R 2 ) being greater than the short and long wavelength reflectivity regions (R 1  &amp; R 3 ). 
     As noted above with reference to  FIG.  1 A , the asymmetric chirped fiber Bragg grating  50  of the present disclosure can be useful in an optical amplifier  10  having a pump laser  20  outputting pump light P for a doped fiber  18 . Other implementations can benefit from the asymmetric chirped fiber Bragg grating  50 . For example,  FIG.  1 B  illustrates a submarine repeater  60  having optical fiber amplifiers according to the present disclosure. The same numerals are used for comparable components in  FIG.  1 A . 
     The repeater  60  includes two pumps  20   1-2 , a splitter  62 , and doped fiber amplifiers  18  for transmit and receive signal lines  12   1-2 . Each line  12   1-2  includes a multiplexer  64 , a doped fiber amplifier  18 , and a filter  66 . The two pumps  20   1-2  at two wavelengths λ 1-2  feed pump light into the splitter  62 , which splits the pump light for the signal lines  12   1-2 . 
     The submarine repeater  60  relies on pump splitting for redundancy. In the repeater  60 , significant back reflection can come from the splices downstream from the multiplexers  64  and the fiber amplifiers  18 . If the pumps  20   1-2  develop a level of coherence, then the repeater  60  produces strong interference at the output of the 50/50 splitter  62 . The back reflection can go all the way back to a given pump  20   1-2  and can then be reflected back to the splitter  62 , thus interfering with itself or the other pump  20   1-2 . The asymmetric chirped fiber Bragg gratings  50  are used on the fibers  30  for the pumps  20   1-2  to counteract this. 
     In another example,  FIG.  1 C  illustrates a fiber laser used in a Master Oscillator Power Amplifier (MOPA) system  160 . The system  160  includes a pump  162  for a single mode that provides a seed input. The seed input is combined with input from multi-mode pumps  164  that connect via a coupling  165  and filter  166 . The laser light passes to an active fiber  168 , and the amplified laser light is then output by a fiber laser output optic  172  connected by a delivery fiber  170 . 
     For example, a module having the seed pump  162  pulsed at 1064 nm can be used as the seed laser for an industrial ytterbium doped fiber laser used in marking, micromachining, soldering, etc. For a majority of applications, the seed laser pulses can be a couple of hundreds nanoseconds long with an amplitude of ˜1 W. At high optical power levels achievable in the fiber laser, Stimulated Brillouin Scattering (SBS) can be triggered during the amplification, which can deteriorate the performance and reliability of the system  160 . Having a spectrally broad seed laser during the pulse can be helpful because the SBS gain can be reduced by decreasing the spectral density of the seed laser. For this reason, increasing the spectral width of the seed laser using the approach disclosed herein can be beneficial in reducing the SBS and can increase the fiber laser operating power. Accordingly, asymmetric chirped fiber Bragg gratings  50  can be used on the pumps  162 ,  164 . 
     In contrast to the uniform fiber Bragg grating  40  and the standard chirped fiber Bragg grating  40 ′, discussion turns to the asymmetric chirped fiber Bragg grating  50  of the present disclosure. 
       FIG.  2 A  illustrates an asymmetric chirped fiber Bragg gating  50  according to the present disclosure.  FIG.  2 B  graphs an envelope  58  of wavelength versus reflected power for the asymmetric chirped fiber Bragg gating  50 , and  FIG.  2 C  graphs the envelope  58  of wavelength versus reflectivity in more detail. 
     As schematically shown in  FIG.  2 A , a number (M) of grating elements  56  are formed at a period (Λ(z*)) along a length (L) of a core  54  of a fiber having a cladding  52 . The grating elements  56  are variations in the refractive index of the fiber core  54 . 
     The grating elements  56  are arranged in a chirped pattern defined by a function Λ(z*) so that an overall spectrum of the fiber Bragg grating  50  is produced by the spectrum of each section of the fiber Bragg grating  50 . The period Λ(z*) of the chirped Fiber grating  50  changes along the longitudinal length (L) of the grating  50 , but further details of the grating  50  are different from the standard chirped fiber Bragg grating ( 40 ′;  FIG.  10 A ). 
     In general, the fiber Bragg grating  50  can be fabricated using conventional techniques, such as using masking, step-by-step fiber translation, etc. For example, the core  54  of the fiber element can be illuminated with ultraviolet (UV) laser light, which produces modifications in the refractive index of the core  54 . For example, a high-power ultra-violet (UV) laser can be used to create refractive index changes within the fiber core  54 . The irradiated regions produce the grating elements  56  that provide reflective interfaces to feedback light to a laser diode. By controlling the level of irradiance used to produce each of these elements  56 , the reflectivity caused by the change in the refractive index for each element  56  can be controlled. As will be appreciated by one skilled in the art having the benefit of the present disclosure, parameters for the fabrication of the grating  50  depend on a number of factors in a given implementation, such as the laser power, the UV frequency, and the pulse light used for irradiation; the fiber material used; the length of the disclosed fiber Bragg grating  50 ; etc. 
     Variable spacing is used between the grating elements  56 , and variable reflectivities in the refractive indices are used for the grating elements  56 . At the start of the fiber Bragg grating  50 , a short distance between these elements  56  leads to reflections at the short wavelength end of the spectrum, corresponding to a short wavelength region. Whereas, at the end of the fiber Bragg grating  50 , the longer spacing between grating elements  56  means the long wavelength end of the spectrum is reflected corresponding to a longer wavelength region. A central wavelength region lies between the short and long wavelength regions. The variation in spacing between the grating elements  56  effectively broadens the bandwidth of the fiber Bragg grating&#39;s response, and the variation in the reflectivities for the grating elements  56  shifts the peak wavelength away from the central wavelength of the grating structure. 
     For an implementation of a fiber Bragg grating that is targeted at reflecting the same wavelength and the same bandwidth of reflected light, the spacings for the standard chirped fiber Bragg grating ( FIG.  10 A ) and the asymmetric chirped fiber Bragg grating ( FIG.  2 A ) can be generally the same. For the standard chirped fiber Bragg grating ( 40 ′:  FIG.  10 A ), however, the reflectivity is highest at the central region (center wavelength) of the fiber Bragg grating&#39;s structure. By contrast, the reflectivity for the asymmetric chirped fiber Bragg grating  50  in  FIGS.  2 A- 2 C  is configured to be highest at the short wavelength region of the fiber Bragg grating&#39;s structure. 
     As generally illustrated in  FIG.  2 C , wavelength feedback is shown for regions of the grating elements  56 . Short wavelength feedback produces a short wavelength reflectivity region (R 1 ), center wavelength feedback produces a center wavelength reflectivity region (R 2 ), and long wavelength feedback produces a long wavelength reflectivity region (R 3 ). For one implementation of the asymmetric chirped fiber Bragg grating  50 , the reflectivity regions can be blue-shifted with the short wavelength reflectivity region (R 1 ) being greater than the center and long wavelength reflectivity regions (R 2  &amp; R 3 ), and specifically R 1 &gt;R 2 &gt;R 3 . 
     Thus, the optical fiber segment  30  shown in  FIGS.  2 A and  2 C  having the asymmetric chirped fiber Bragg grating  50  is configured to optically interact with or communicate with a laser diode&#39;s pump light (P). The fiber Bragg grating  50  has a length (L) and has a plurality of variations  56  in refractive index produced in the core  54 . The variations  56  have a chirped period changing spatially (e.g., linearly) along the length of the fiber Bragg grating  50 . The chirped period has a first reflectivity for one of a short or a long wavelength region (R 1 , R 3 ) of the fiber Bragg grating  50 . The first reflectivity is shifted asymmetrically from a central wavelength region (R 2 ) of the fiber Bragg grating  50 . As illustrated in  FIG.  2 C , the first reflectivity of the short wavelength region (R 1 ) is greater than a second reflectivity of the central wavelength region (R 2 ) and is greater than a third reflectivity of the other of the long wavelength region (R 3 ). Although the asymmetric chirped fiber Bragg grating  50  could alternatively be redshifted to the long wavelength reflectivity region (R 3 ) being greater than the short and center wavelength reflectivity regions (R 1  &amp; R 2 ), such an implementation would not be necessarily usable in most applications because the implementation would produce narrower net gain, which would be less beneficial as discussed below. 
     The blue-shifted asymmetric structure can compensate for long wavelength modes that dominate the light from a laser diode ( 20 ) in a given implementation. In this way, the center wavelength is blue-shifted away from a lone peak wavelength that can tend to dominate in the given implementation. Clearly, for a standard chirped fiber Bragg grating ( 40 ′:  FIG.  10 C ), the center wavelength would be the same as the peak wavelength. Here, however, the blue-shift is made significant enough to provide the desired compensation and to ensure there are no dominant long wavelength peaks. (Further details of this are discussed with reference to  FIGS.  4 A to  5 B  specifically.) 
     In one implementation, the reflectivity width for the grating  50  containing more than 10 modes at Full-Width Half Maximum (FWHM) (if the distance between modes is about 30 pm) would give FWHM about 0.3 nm. The asymmetry that blue shifts the center wavelength from the peak wavelength can be defined as: Δλ=λ center −λ peak &gt;0.2×FWHM. Other implementations can be configured differently. 
     Looking back at the system of  FIG.  1 A , the asymmetric chirped fiber Bragg grating  50  as disclosed herein can be used with a 980-nm pump laser diode  20  where good power stability performance is required, particularly when combining outputs from multiple pump laser diodes  20  for the optical fiber amplifier  10 , such as illustrated in  FIG.  1 A . 
     In particular, outputs from the multiple pump laser diodes  20  as in  FIG.  1 A  can produce “coherent” laser output, which can cause interference and reduce output power. The desire is to make the laser outputs more “incoherent” to reduce interference and reduce power instabilities in the amplifier output. Using a standard chirped fiber Bragg grating ( 40 ′ as in  FIG.  10 A ) on a laser diode  20  does not guarantee that an “incoherent” laser output will be produced because the standard chirped fiber Bragg grating ( 40 ′:  FIG.  10 A ) can still generate a dominant mode within the FBG&#39;s envelope. In particular, the combination of laser gain peak, front facet reflectivity, and an imperfect Gaussian FBG profile can lead at Iop&gt;&gt;Ith to a dominant laser mode biased to one side of the FBG envelope. This is due to spectral hole burning. 
     In contrast, the asymmetric chirped fiber Bragg grating  50  as disclosed herein skews the FBG reflectivity envelope to the short wavelength side. This promotes gain values for the less dominant modes, therefore decreasing the coherence of the laser diode  20  and improving the output power stability. 
     In addition to the benefits for pump laser diodes as in  FIG.  1 A , the asymmetric chirped fiber Bragg grating  50  can also be used in 10xx nm seed lasers, where the asymmetric chirped fiber Bragg grating  50  can provide a broader optical spectrum in a pulsed mode, which can counteract nonlinear effects in fiber lasers. Additionally, the broad emission spectrum of the asymmetric chirped fiber Bragg grating  50  as disclosed herein is also useful in a fiber laser for a submarine repeater ( FIG.  1 B ), for a master oscillator power amplifier (MOPA) system ( FIG.  1 C ), or for other configurations. Namely, the broad spectrum increases the threshold for the nonlinear effect in the fiber and hence allows higher optical power to be produced. 
     As noted above, the asymmetric chirped fiber Bragg grating  50  of the present disclosure can be used to reduce coherence of pump lasers, such as the 980 nm pump laser diodes as in  FIG.  1 A . To lay this out in more detail, discussion turns to  FIGS.  3 A through  5 B . 
     Power variation in a FBG-locked, 980 nm pump laser diode ( 20 ) that is locked by a fiber Bragg grating can be an issue for particular applications. Power variation is generally caused by the coherence of the laser diode ( 20 ) and is a result of mode hopping within the envelop of the fiber Bragg grating, which leads to changes in ex-fiber power. For an FBG-locked Fabry Perot laser diode, coherence is determined by how many spectral modes of power are shared across the envelope of the fiber Bragg grating. The less modes there are: the more coherent the laser light becomes, and the higher the power variation will be. 
       FIG.  3 A  shows a standard envelope  70  of power relative to wavelength for a uniform fiber Bragg grating. A number of spectral modes  72  of power are shown. As noted, the less modes  72  there are: the more coherent the laser light becomes, and the higher the power variation will be. As shown in  FIGS.  3 B , higher coherence also arises when one spectral mode  74  dominates in the standard envelope  70  and when adjacent modes are suppressed in the standard envelope  70 . 
     One solution to reduce the coherence of the laser light is to use a standard chirped fiber Bragg grating ( 40 ′) that provides wider bandwidth.  FIGS.  4 A- 4 B  show envelopes  80  for standard chirped fiber Bragg gratings ( 40 ′) that provide wider bandwidth ( 84 ;  FIG.  4 B ). As shown, more modes  82  can be captured within the envelopes  80 , thus increasing the power sharing across an increased number of modes  82 . 
     As shown in  FIG.  5 A , however, even a standard chirped fiber Bragg grating ( 40 ′) does not guarantee that incoherent laser light will be produced because the standard chirped fiber Bragg grating ( 40 ′) can still generate a dominant mode  92  within the envelope  90 . At high operating currents (Iop&gt;&gt;Ith), the combination of laser gain peak, front facet reflectivity, and an imperfect Gaussian FBG profile can lead to the dominant laser mode  92  biased to one side of the envelope  90 . This is due to spectral hole burning, which is discussed in more detail later. 
     As shown in  FIG.  5 B , however, an asymmetric chirped fiber Bragg grating ( 50 ) of the present disclosure has a reflectivity envelope  94  shifted or skewed to the short wavelength side compared to the standard envelope  90 . The shifted reflectivity envelope  94  limits gain of a dominant laser mode  92  and promotes gain of the less dominant modes  96 , therefore decreasing the coherence of the laser light and improving the output power stability. Again, although the asymmetric chirped fiber Bragg grating ( 50 ) could alternatively be shifted or skewed to the long wavelength reflectivity side, such an implementation would not be usable in most applications because the implementation would produce narrower net gain, which would be less beneficial as discussed below. 
     As mentioned briefly above, the asymmetric chirped fiber Bragg grating ( 50 ) of the present disclosure suppresses spectral hole burning. The reflectivity profile of the asymmetric chirped fiber Bragg grating ( 50 ) is biased to higher energy (shorter wavelength) side. This broadens the net gain for modes on the long wavelength side of the envelope as compared to the net gain that these modes would see from a standard chirped FBG profile ( 40 ′). 
     In the event of spectral hole burning, the asymmetric chirped fiber Bragg grating ( 50 ) will end up with a much broader net gain peak, resulting in a broader emission spectrum for both a pulsed signal and a continuous wave CW signal. Broader spectrum for the continuous wave (CW) signal will also reduce the noise originating from the mode switching during any instabilities in the laser cavity of the laser diode ( 20 ). 
     Spectral hole burning (SHB) is a known, nonlinear effect. To illustrate spectral hole burning,  FIG.  6 A  is a graph  100  of gain  102  and carrier distribution  104  for laser operation at lower current/optical power. These are shown relative to the parabolic band  106 . Meanwhile,  FIG.  6 B  is a graph  100  of gain  102  and carrier distribution  104  for the laser operation at high current/optical power that produces spectral hole burning. 
     Spectral hole burning occurs when a carrier thermalization rate is similar to or smaller than a radiative recombination rate. This occurs typically at high current/optical power level Iop&gt;&gt;Ith, when carrier capture/thermalization rate is slower compared to the photon generation rate at photon energy hv laser   0 , resulting in decreased gain at the photon energy hv laser   0  and corresponding shift of the photon energy towards the new net gain maximum at hv laser   1 . 
     For a situation in which the feedback is provided by an external fiber Bragg grating with finite reflectivity and width, the spectral hole burning will narrow the emission spectrum and corresponding red shift of λ FBG  further away from the reflectivity maximum, but still within the reflectivity spectrum. For example,  FIG.  6 C  graphs gain  110  and reflectivity  112  for wavelengths when feedback is provided by an external fiber Bragg grating with finite reflectivity and width. 
     Here, the asymmetric chirped fiber Bragg grating ( 50 ) supresses spectral hole burning by biasing the reflectivity profile to the higher energy (shorter wavelength) side. This broaden the net gain for modes on the long wavelength side of the FBG envelope as compared to the net gain these modes would see from a symmetrical chirped FBG profile ( 40 ′). 
     For comparison,  FIG.  7 A  graphs reflectivity  120  in a standard FBG profile. The reflectivity  120  has a peak at the center wavelength  122  and is symmetrical about the central region. A net gain  124  without spectral hole burning is also shown relative to another net gain  126  with spectral hole burning. Narrow net gain  126  can result in the dominant mode  128 . Meanwhile,  FIG.  7 B  graphs reflectivity  130  in an standard FBG profile according to the present disclosure. The reflectivity  130  has a peak blue-shifted from the center wavelength  132  and is asymmetrical about the central region. A net gain  134  without spectral hole burning is also shown relative to another net gain  136  with spectral hole burning. 
     In the event of spectral hole burning, therefore, the asymmetric chirped fiber Bragg grating ( 50 ) as shown in  FIG.  7 B  can still produce a much broader net gain peak  136 , resulting in broader emission spectrum, capturing more FP modes  138 , both in pulsed mode and in CW mode. Broader spectrum in the CW mode will also reduce the noise originating from the mode switching during possible instabilities in the laser cavity of the laser diode. 
     The asymmetric chirped fiber Bragg grating ( 50 ) of the present disclosure has some positive benefits on power variation and spectral width on a laser diode ( 20 ) locked by the asymmetric chirped fiber Bragg grating ( 50 ). The graph  140  in  FIG.  8 A  shows a power variation  142  for a laser driven by a drive current when locked using a standard chirped fiber Bragg grating ( 40 ′) versus another power variation  144  for a laser driven by a drive current when locked using an asymmetric chirped fiber Bragg grating ( 50 ) of the present disclosure. As can be seen, the asymmetric chirped fiber Bragg grating ( 50 ) provides more stable power variation  144  with drive current for a laser compared to the variation  142  of the standard chirped fiber Bragg grating ( 40 ′) when used on the same laser. The bandwidth is nominally the same for both fiber Bragg gratings ( 40 ′,  50 ) in this example. 
     The graph  150  in  FIG.  8 B  shows a standard spectral width  152  for a laser driven by a drive current when locked using a standard chirped fiber Bragg grating ( 40 ′) versus another spectral width  154  for a laser driven by a drive current when locked using an asymmetric chirped fiber Bragg grating ( 50 ) of the present disclosure. The improved power variation provided by the asymmetric chirped fiber Bragg grating ( 50 ) produces an increase in spectral width  154  not seen with the width  152  for the standard chirped fiber Bragg grating ( 40 ′). 
     The foregoing description of preferred and other embodiments is not intended to limit or restrict the scope or applicability of the inventive concepts conceived of by the Applicants. It will be appreciated with the benefit of the present disclosure that features described above in accordance with any embodiment or aspect of the disclosed subject matter can be utilized, either alone or in combination, with any other described feature, in any other embodiment or aspect of the disclosed subject matter. 
     In exchange for disclosing the inventive concepts contained herein, the Applicants desire all patent rights afforded by the appended claims. Therefore, it is intended that the appended claims include all modifications and alterations to the full extent that they come within the scope of the following claims or the equivalents thereof.