• Title/Summary/Keyword: Gain grating

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Lasing Modes of LD-Pumped Fiber Grating Lasers

  • Park, Dong-Wook;Hwang, Joon-Hwan
    • Journal of the Optical Society of Korea
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    • v.6 no.3
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    • pp.108-116
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    • 2002
  • Lasing modes of laser-diode-pumped fiber grating lasers are analyzed by coupled-mode theory. First, a power series solution of the coupled-mode equations is derived under the assumption of an exponentially-decreasing longitudinal modal gain profile for a laser-diode-pumped grating section, followed by determination of the transfer matrix for such a section. Based on these results, an eigenvalue equation for oscillation is then derived and solved numerically for the lasing modes of uniform and phase-shifted fiber grating lasers. Comparisons made with the uniform-gain results indicate that, surprisingly, the lasing mode characteristics are not as significantly altered as might be expected in most cases, even for a highly nonuniform gain profile. In the case of a phase-shifted grating, the phase-shift position appears to have a much greater impact on determining the threshold gain, the modal field distribution, and the front-to-back output power ratio.

Effect of grating structures and mirror postions on characteristics of 1.55$\mu\textrm{m}$ DFB lasers-II (1.55.$\mu\textrm{m}$ DFB 레이저의 특성에 미치는 Grating 구조와 Mirror 위치의 영향 -II)

  • Kwon, Kee-Young
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.32A no.2
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    • pp.48-56
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    • 1995
  • The operating characteristics, such as, the threshold gain, lasing frequency, and longitudinal intensity profile, etc., of 1.55$\mu$m DFB laser diode with index and/or gain grating structures and with one side AR-coated mirror have been analyzed. From this analysis, the optimum design parameters have been shown that ${\Delta}{\Omega}$ (the phase difference between index grating and gain grating) is 0 or ${\pi}$, (xL)$_{r}$=1~3 and (xL)$_{i}$=0.5~0.9. It has been also shown that the modal selectivity and intensity uniformity of the DFB lasers with .DELTA..OMEGA.=0 are ~1.2 times better thatn those of the DFB lasers with ${\Delta}{\Omega}$= ${\pi}$.

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Optimization of Grating Structures in Complex-Coupled MQW DFB Lasers with Absorptive Gratings (흡수 회절격자를 가지는 복소결합 다중양자우물 DFB 레이저의 회절격자 구조의 최적화)

  • Cho, Sung-Chan;Lee, Dong-Chan;Kim, Boo-Gyoun
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.36D no.7
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    • pp.80-91
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    • 1999
  • We present various optimal grating structures which give the low threshold gain, good modulation characteristics, small effective linewidth enhancement factor, and large fabrication tolerance in complex-coupled MQW DFB lasers with absorptive gratings. To obtain these, we calculate the complex coupling coefficients using the extended additional layer method and the threshold gain including the modal loss in the absorptive grating region for rectangular and trapezoidal gratings. Based on the comparison of the results for various possible absorptive grating structures, the design guidelines are presented to obtain the low threshold gain or large fabrication tolerance. Among the grating structures studied, the double grating structure consisting of the absorptive grating on the index grating has the largest fabrication tolerance for the threshold gain and the coupling strength. The fabrication tolerance for the coupling ratio is very large for all the grating structures studied.

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Effect of Grating Phase in DFB Lasers with an Anti-reflection Coated Mirror (AR 코팅된 DFB 레이저에서 격자 위상의 영향)

  • Kwon, Kee-young;Ki, Jang-geun;Cho, Hyun-mook
    • The Journal of the Convergence on Culture Technology
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    • v.7 no.3
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    • pp.463-468
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    • 2021
  • In this paper, when a refractive index grating and a gain grating were simultaneously present in a DFB laser having a wavelength of 1.55 ㎛, a dielectric film coating was applied so that reflection did not occur on the right mirror surface, so that 𝜌r=0. In case of 𝛿L>0, the characteristics of the oscillation frequency and oscillation gain were analyzed. When the grating phase of the left mirror surface continues to decrease from 𝜋, the graph lines of each mode gradually shift to the left. In case of 𝜅L=10, the threshold gain of the oscillation mode is the lowest. In this case, the mode selectivity is relatively low. From 𝜅L=0.5 to 𝜅L=6, the mode selectivity and the frequency stability are excellent. In the case of DFB lasers with an anti-reflection coated mirror, the threshold gain of the oscillation mode increases but the mode selectivity is about twice as excellent, compared with DFB lasers of having two cleaved facets.

Simulation and Examination for DFB Lasers with Grating Phase of π/2 on One Mirror Face (한쪽 거울면의 격자 위상이 π/2인 DFB 레이저의 시뮬레이션과 검정)

  • Kwon, Kee-Young
    • Journal of Software Assessment and Valuation
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    • v.15 no.2
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    • pp.101-109
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    • 2019
  • Lasers for optical broadband communication systems should have excellent frequency selectivity and modal stability. DFB(Distributed Feedback) lasers have low lasing frequency shift during high speed current modulation. In this paper, I have developed a simulation software and analysed threshold gain and lasing frequency of a lasing mode in longitudinal direction of an 1.55um DFB laser with two mirrors and without anti-reflection coatings, that have both an index- and gain-gratings. The grating phase on a left mirror face is fixed as π/2 and the grating phase on a right mirror face is varied. As the phases of the index and gain gratings on the right mirror facet are π and 0, κL should be in the range of 2~6 in order to enhance the frequency stability. In order to reduce the threshold current of a lasing mode, κL should be greater than 8, regardless of the grating phases on the mirror faces.

Mechanically induced long-period fiber grating devices and EDFA gain flattening (기계적으로 유도된 장주기 광섬유격자 소자와 이를 이용한 EDFA 이득평탄화)

  • 김륜경;조준용;이경식
    • Korean Journal of Optics and Photonics
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    • v.14 no.1
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    • pp.8-11
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    • 2003
  • For the first time to our knowledge we have developed compact mechanically-induced long-period fiber grating devices which have an excellent tunability in the center wavelength and the depth of the notch. The compactness and ease to tune allow us to include them in other optical devices or systems. The devices were characterized by measuring their transmission spectra with different grating periods and applied pressures. We have also demonstrated the EDFA gain flattening using the mechanically-induced long-period fiber grating devices.

All-optical gain control in erbium-doped fiber amplifier using a fiber grating (광섬유격자를 이용한 Erbium 첨가 광섬유 증폭기의 광학적 이득제어)

  • 박희갑
    • Korean Journal of Optics and Photonics
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    • v.8 no.1
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    • pp.58-62
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    • 1997
  • A new, simple lasing loop configuration employing a fiber grating was proposed and demonstrated for all-optical gain control of erbium-doped fiber amplifier. The lasing loop was designed such that the fiber grating acts as a notch filter to cutoff the lasing light as well as selects the lasing wavelength. The operating gain was clamped to the same level as the loop loss and it could be varied with a tunable directional coupler in the loop. It is believed that this type of gain-controlled erbiumdoped fiber amplifier can have several advantages when used in wavelength-division-multiplexed transmission systems.

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Effect of Grating Structures and Mirror Positions on Characteristics of 1.55$\mu\textrm{m}$ DFB Lasers (1.55 $\mu\textrm{m}$ DFB 레이저의 특성에 미치는 Grating구조와 Mirror 위치의 영향)

  • Kwon, Kee-Young
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.31A no.9
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    • pp.128-138
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    • 1994
  • In 1.55.mu.m DFB lasers with two non-AR mirrors, I have analyzed the effect of the sturctures of indes and/or gain gratings and mirror positions on the threshold gains, the lasing frequencies, and the beam profiles in longitudinal direction of lasers. I have obtained the optimum condition of static characteristics that ${\Delta}{\Omega}$(the phase difference betweeen index grating and gain grating is 3${\pi}$/4, $({\kappa}L)_{i}$=4~6 in case of $({\kappa}L)_{i}$=0.9 and $({\kappa}L)_{i}$=3~5 in case of $({\kappa}L)_{i}$=0.7. The modal selectivity and intensity uniformity of this optimum condition are 2~2.5 times better than those of the gain-coupled DFB lasers ${\Delta}{\Omega}$=0). The gain-coupled DFB lasers${\Delta}{\Omega}$=0) have 10$^{10) times better modal selectivity and intensity uniformity than the loss-coupled DFB lasers(TEX>${\Delta}{\Omega}$=${\pi}$).

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Beam Profile Analysis of DFB Laser for High Speed Communications (고속 통신용 DFB 레이저의 빔 분포 해석)

  • Kwon, Keeyoung
    • The Journal of the Convergence on Culture Technology
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    • v.6 no.3
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    • pp.419-425
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    • 2020
  • In this paper, when a refractive index grating and a gain grating are simultaneously present in a DFB (Distributed Feedback) laser for a 1.55 um wavelength with two mirror surfaces without an anti-reflective coating, an analysis program was developed to determine the beam distribution of the oscillation mode in the longitudinal direction. As the phases of the index and gain gratings on the mirror faces are varied, the lasing gain and the beam profiles |R(z)| and |S(z)| of the lasing mode with the emitted power ratio Pl/Pr are analyzed and examined in case of δL<0. In order to reduce the threshold current of a oscillation mode and enhance the frequency stability, κL should be greater than 8, regardless of the grating phase values at the mirror surface.

Lasing mode and Beam Profile Analysis of DFB Laser with an Anti-reflection Coated Mirror (무반사 면을 갖는 DFB 레이저의 발진 모드와 빔 분포 해석)

  • Kwon, Keeyoung
    • The Journal of the Convergence on Culture Technology
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    • v.6 no.4
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    • pp.727-732
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    • 2020
  • In this paper, when a refractive index grating and a gain grating were simultaneously present in a DFB laser having a wavelength of 1.55 ㎛, a dielectric film coating was applied so that reflection did not occur on the right mirror surface, so that 𝜌r=0. In case of δL > 0, the threshold gain and the beam distribution in the longitudinal direction and the radiated power ratio Pl/Pr of the oscillation mode were compared for the cases of the phase of 𝜌l=π and π/2. If the phase of 𝜌l=π, in order to obtain a low threshold current and high frequency stability, κL should be greater than 8. In the case of the phase of 𝜌l= π/2, when κL is larger than 4.0, the oscillation gain starts to be lower than when the phase of 𝜌l=π. In order to lower the threshold current of a oscillation mode and enhance the frequency stability, κL should be greater than 8.