## Abstract

We theoretically analyze gain guiding in large-core Bragg fibers, to be used for large-mode-area laser amplifiers with single-transverse-mode operation. The signal is gain-guided in a low-index core, whereas the pump is guided by the photonic bandgap of the Bragg cladding to achieve good confinement. The high-index layers in the Bragg cladding are half-wave thick at the signal wavelength in order to eliminate Bragg reflection, reducing the Bragg fiber effectively to a step-index fiber for gain guiding.

©2009 Optical Society of America

## 1. Introduction

Recently laser oscillation in gain-guided and index-antiguided fibers [1,2] has been demonstrated to exhibit near-diffraction-limit beam characteristics with core diameter up to 400 µm [3,4]. In an index-antiguided (IAG) fiber the core has a lower refractive index relative to the surrounding cladding, and light propagating in the core eventually leaks into the cladding. For the signal radiation, single-transverse-mode operation can be achieved by balancing the leakage loss and the provided gain inside the core [2]. However, such lasers are not efficient under end pumping since most of the launched pump power leaks into the cladding due to index antiguiding [5]. To mitigate this problem, we have proposed a scheme based on gain guiding in photonic bandgap (PBG) waveguides in which the pump is confined inside the core via the PBG effect, while the signal is gain-guided and index-antiguided in the same core. This scheme was illustrated in a one-dimensional transverse grating waveguide [6]. Since the signal and the pump share the same core, one can expect a large overlap factor between the modes of the signal and the pump. Gain-guided photonic bandgap waveguides, therefore, could have ultra-large mode area, robust single-transverse-mode operation, and high pump efficiency. Photonic bandgap fibers, such as Bragg fibers, would serve as more practical waveguides for gain guiding. A Bragg fiber [7] is composed of concentric layers of alternating high- and low-index materials (Bragg cladding) surrounding a core, followed by a uniform outer cladding (see Fig. 1
). Bragg fibers have been fabricated by drawing [8,9] or deposition [10–12]. Most studies have focused on modal characteristics inside the PBG of the Bragg cladding, where the lowest loss mode could be either TE_{01} [13] or HE_{11} [11,12], depending on the fiber configuration.

In this paper, we investigate gain guiding in Bragg fibers in which the signal is gain-guided and index-antiguided in a low-index core, while the pump is confined by the PBG effects of the Bragg cladding. Gain-guided Bragg fibers can be used for large-mode-area laser oscillators or amplifiers. Here the Bragg cladding serves two purposes. Firstly, it has a wide bandgap at the pump wavelength to confine the pump efficiently with a finite number of Bragg layers, which usually requires a large contrast in refractive indices between high- and low-index layers. Secondly, the Bragg cladding has a passband at the signal wavelength such that the Bragg fiber becomes equivalent to an IAG fiber, where the HE_{11} mode has the lowest loss for a modest index contrast [14]. For an IAG fiber to have large modal gain while remain single transverse mode, large modal loss is essential, which requires small index contrast between the core and the cladding [2]. These two requirements on the Bragg cladding seem to be incompatible. We resolve this issue by making the high-index layer in the Bragg cladding half-wave thick at the signal wavelength. We show that, under such condition, the Bragg fiber reduces to a step-index fiber for the signal, and the properties of the Bragg cladding can be considered independently for the signal and the pump.

## 2. Theoretical analysis

For a large-core fiber with relatively thin Bragg layers, the Bragg cladding can be considered approximately planar, and its optical properties can be understood using the theory of light propagation in one-dimensional periodically stratified media [15,16]. The Bloch wavenumber *K* in the Bragg cladding (with refractive indices *n*
_{1} and *n*
_{2}) can be determined by [15]

where Λ = *d*
_{1} + *d*
_{2} is the period of the Bragg layers, ${k}_{j}=\sqrt{{\left(2\pi /\lambda \right)}^{2}{n}_{j}^{2}-{\beta}^{2}}$ (*j* = 1, 2) is the transverse component of the wavevector in each layer, and *β* is the complex propagation constant of modes in the fiber.

For the signal to be gain-guided in a single transverse mode, its wavelength needs to be located inside the passing zones of the Bragg cladding for both TE and TM polarizations. One possible way to accomplish this is to impose *k*
_{1}
*d*
_{1} = *π* in Eq. (1) (*i.e.*, half-wave condition at the signal wavelength) such that cos(*K*Λ) = −cos(*k*
_{2}
*d*
_{2}), which ensures the same real wavenumber in the Bragg cladding for both polarizations. Given glancing incidence of low-order modes in a large-core (with refractive index *n*
_{0}) fiber where *β* ≈ω*n*
_{0}/*c* (*i.e*., the core light line), the thickness *d*
_{1} can be determined from the half-wave condition at the signal wavelength *λ*
_{s} to be

It is well known in thin-film optics that when a dielectric layer is half-wave thick, it becomes an absentee layer such that its presence does not affect optical properties of the whole structure [17]. Since in the current Bragg fibers the *n*
_{1} layers are half-wave thick, we expect that they become absentee layers to the low-order modes such that the Bragg cladding reduces effectively to a uniform cladding with refractive index *n*
_{2}. This can be seen by examining the mode fields and the dispersion equation of a Bragg fiber under the conditions of *R*
_{0} >> Λ and *k*
_{1}
*d*
_{1} = *π.* The radial dependence of the *E _{z}* field in a Bragg fiber can be written as (in the cladding the asymptotic expressions are used for the Hankel functions) [16],

*n*

_{2}(

*n*

_{1}) layer of the

*l*-th period in the cladding. Similar expressions can be written for the

*H*field with another set of expansion coefficients, and all other field components can be obtained from

_{z}*E*and

_{z}*H*. In the asymptotic limit, the coefficients

_{z}*a*and

_{l}*b*in the adjacent

_{l}*n*

_{2}layers are related by a transfer matrix as in planar stratified media [15,16],

Under the half-wave condition *k*
_{1}
*d*
_{1} = *π*, *B*
_{TM} is zero and the transfer matrix becomes diagonal. This indicates that the outgoing wave and incoming wave in the *n*
_{2} layers are decoupled. Since there is no incoming wave at infinity, we have *b _{n}* = 0 for all the

*n*

_{2}layers. Similarly, there is no incoming wave for the

*H*field in the

_{z}*n*

_{2}layers. Consequently, the field expressions in the

*n*

_{2}layers of the Bragg fiber reduce to those of a step-index fiber. In addition, by matching the boundary conditions and keeping only the (

*k*)

_{j}r^{(−1/2)}terms for

*E*and

_{θ}*H*[17], we obtain the following dispersion equation provided that

_{θ}*R*

_{0}>> Λ and

*k*

_{1}

*d*

_{1}=

*π*,

This dispersion equation is equivalent to the one for a step-index fiber in Ref [14], as in the asymptotic limit we have ${{H}^{\prime}}_{m}^{(1)}\left({k}_{2}{R}_{0}\right)/{H}_{m}^{(1)}\left({k}_{2}{R}_{0}\right)$→ *i*. Since both the field expressions and propagation constants are identical, the Bragg fiber indeed behaves like a step-index IAG fiber with a core index *n*
_{0} and a cladding index *n*
_{2}. The leakage loss of the signal in the Bragg fiber then follows that of the corresponding IAG fiber, which is determined by the dimensionless index parameter $\Delta N={\left(2\pi /{\lambda}_{s}\right)}^{2}\cdot {R}_{0}^{2}\cdot \left({n}_{2}^{2}-{n}_{0}^{2}\right)$ [2]. Such leakage loss has shown to be critical in determining the saturated power in gain-guided IAG waveguides [18].

We now turn to the bandgap properties at the pump wavelength *λ*
_{p}. To confine the pump efficiently, the Bragg cladding needs to have a complete bandgap at the pump wavelength, and it is beneficial to have a numerical aperture (NA) as large as possible to facilitate the coupling of the pump light into the Bragg fiber. Since the low-order modes of the pump also approach glancing incidence, the bandgaps of the one-dimensional Bragg cladding satisfy the following requirement [15] under the constraint of Eq. (3) [cf. Equation (1)],

*φ*

_{1}=

*πλ*

_{s}

*/λ*

_{p},

*φ*

_{2}= 2

*πd*

_{2}(

*n*

_{2}

^{2}-

*n*

_{0}

^{2})

^{1/2}

*/λ*

_{p}. Equation (8) can be used to select the parameters of

*n*

_{1}and

*d*

_{2}to ensure that there is a complete bandgap at the pump wavelength. Since the bandgaps of the TE polarization usually cover those of the TM polarization, we may examine Eq. (8) for the TM polarization only.

## 3. Example and discussion

We apply the above principle to a Bragg fiber with 6 pairs of Bragg layers followed by an infinite outer cladding with the same refractive index as the low-index layer [see Fig. 1(b)]. The fiber has a core radius *R*
_{0} = 50 µm, refractive indices *n*
_{0} = 1.56, and *n*
_{2} = 1.57. The pump wavelength is *λ*
_{p} = 0.803 µm (as for a typical wavelength of diode lasers), and the signal wavelength is *λ*
_{s} = 1.055 µm (as for a Nd-doped glass fiber).

Figure 2(a)
shows the combination of *n*
_{1} and *d*
_{2} for which there is a complete bandgap for the pump at glancing incidence [*i.e*., for those *n*
_{1} and *d*
_{2}
Eq. (8) is satisfied]. The band diagram of an infinite Bragg cladding for *n*
_{1} = 2.2 [the corresponding thickness *d*
_{1} determined from Eq. (3) is 0.34 µm] and *d*
_{2} = 0.575 µm is shown in Fig. 2(b). At the signal wavelength, the light line of the core is located inside the passing zones for both TE and TM polarizations, indicating the low-order modes are lossy in a passive fiber. At the pump wavelength, there is a

complete bandgap covering the range of 1.50 < *n*
_{eff} < 1.56, implying a quite large acceptance angle for the pump [NA ≈1.56 × sin(cos^{−1}(1.50/1.56)) = 0.42]. Notice that the small gap located near *n*
_{eff} = 1.35 at the signal wavelength will not diminish the robustness of single- transverse-mode operation during the gain guiding, since these higher-order modes possess much higher loss in a Bragg fiber with a finite Bragg cladding. This is confirmed by examining the reflectance of a planar structure with the same index profile as in Fig. 1(b). As shown in Fig. 2(c), the signal has a much lower reflectance (~90%) near *n*
_{eff} = 1.35 than at glancing incidence (> 99%). Also indicated is the strong PBG effects at the pump wavelength (reflectance > 99% for both TE and TM polarizations) with only 6 pairs of Bragg layers.

Table 1
shows the complex effective indices of low-order modes of a Bragg fiber with 6 pairs of Bragg layers, calculated by a rigorous transfer matrix method based on the Bessel function expansion [7]. Also shown are results for the corresponding IAG fiber, calculated by the analytical formula in Ref [14]. The loss of the pump is overall three orders of magnitude smaller than that of the signal in the Bragg fiber, indicting good pump confinement. The complex effective indices are nearly identical for the Bragg fiber and the corresponding IAG fiber at the signal wavelength, indicating the high-index layers indeed have no effect in the Bragg fiber. This is further confirmed by the overlapped radial profiles of *S*
_{z} of the HE_{11} mode for both fibers, as shown in Fig. 3(a)
. The inset of Fig. 3(a) also shows the radial phase profile of the *H*
_{z} field in the Bragg cladding, indicating a *π*-phase shift over each *n*
_{1} layer. This is consistent with the imposed half-wave condition. Notice that the loss coefficient of the LP_{11} mode is about 2.5 times higher than that of the LP_{01} mode in the Bragg fiber, which is very promising for strong transverse mode discrimination during gain guiding [2]. Furthermore, the modal gain coefficient of the Bragg fiber is identical to that of the IAG fiber when the material gain is present in the core, as shown in Fig. 3(b). For the current example where *-ΔN* ~2000, the mode profile is expected to show little change before and after the onset of gain guiding [2].

It is also found that, when *d*
_{1} deviates from the designed value by −1% ~ + 3%, the loss coefficients of TE_{01}, TM_{01}, and HE_{21} modes for the signal remain close and are about 2 times larger than that of the HE_{11} mode. This suggests fairly robust gain guiding with single transverse mode in this Bragg fiber even if the thickness of the high-index layers deviates from the half-wave condition slightly. A more judicious selection of *n*
_{1} and *d*
_{2} could improve the tolerance further. For the present example, a threshold gain of 0.1 cm^{−1} would require a doping density of ~6 × 10^{20} ions/cm^{3} which may be obtained with 6 wt % Kigre Q98 glass. Bragg cladding of such design could be potentially realized using the techniques described in Refs. [8]. and [12].

## 4. Conclusion

We have analyzed theoretically gain guiding in a large-core Bragg fiber, in which the signal is gain-guided and index-antiguided in the fiber core, while the pump is confined in the same core by the photonic bandgaps of the Bragg cladding. We imposed a half-wave condition on the high-index layers in the Bragg cladding such that they have no effect on fiber modes at the signal wavelength. Under this condition, the low-order modes of the signal in the Bragg fiber and the corresponding IAG fiber have nearly identical propagation constants and mode fields, as well as modal gains when gain guiding. The loss at the signal wavelength can then be solely determined by the index contrast between the core and the low-index layers of the Bragg cladding, while the high-index layers are used to optimize the photonic bandgap at the pump wavelength. This half-wave condition is expected to substantially simplify the design of gain-guided Bragg fibers, which hold promise for high-power laser amplifiers and oscillators with robust single transverse mode and large mode area.

## Acknowledgments

This work is supported by DARPA under Young Faculty Award No. HR0011-08-1-0065 and National Science Foundation under Grant No. 0925992.

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