共查询到20条相似文献,搜索用时 31 毫秒
1.
基于光纤环形镜的L-波段掺铒光纤放大器增益的提高 总被引:3,自引:0,他引:3
提出了一种基于光纤环形镜作为反射器的反射式L-波段掺铒光纤放大器(EDFA)结构。光纤环形镜不但可以反射后向放大自发辐射(ASE)作为二次抽运源,而且还可以反射信号,使信号得到二次放大。当抽运功率为115mW时。在1570~1605nm波长范围内,反射式L-波段掺铒光纤放大器的平坦小信号增益达到29.14dB,与前向抽运方式L-波段掺铒光纤放大器相比(保持平坦性不变)。增益提高了5.33dB。分别输入波长为1580nm和1600nm的信号,反射式L-波段掺铒光纤放大器的饱和输出功率为7.63和7.6dBm.与前向抽运方式L-波段掺铒光纤放大器相比分别提高了2.98和3dB。 相似文献
2.
A praseodymium doped fluoride fiber amplifier (PDFFA) exhibiting efficient operation in both the large- and the small-signal regimes is described. The amplifier, based on a high NA fluoride fiber, exhibited a maximum small-signal gain of 29 dB and a low-pump small-signal. efficiency of 0.13 dB/mW. In the saturated regime a maximum output power of 212 mW was achieved. In this format, the signal-out versus pump-in characteristic, exhibited a slope efficiency of 30%, representing the most efficient conversion from pump to signal yet reported. Detailed spectral characterization reveals small-signal gain in excess of 20 dB over a wavelength range of almost 50 nm and in excess of 100 mW of saturated output available over a 30-nm wavelength range 相似文献
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The performance of a long wavelength‐band erbium‐doped fiber amplifier (L‐band EDFA) using 1530nm‐band pumping has been studied. A 1530nm‐band pump source is built using a tunable light source and two C‐band EDFAs in cascaded configuration, which is able to deliver a maximum output power of 23dBm. Gain coefficient and noise figure (NF) of the L‐band EDFA are measured for pump wavelengths between 1530nm and 1560nm. The gain coefficient with a 1545nm pump is more than twice as large as with a 1480nm pump. It indicates that the L‐band EDFA consumes low power. The noise figure of 1530nm pump is 6.36dB at worst, which is 0.75dB higher than that of 1480nm pumped EDFA. The optimum pump wavelength range to obtain high gain and low NF in the 1530nm band appears to be between 1530nm and 1540nm. Gain spectra as a function of a pump wavelength have bandwidth of more than 10nm so that a broadband pump source can be used as 1530nm‐band pump. The L‐band EDFA is also tested for WDM signals. Flat Gain bandwidth is 32nm from 1571.5 to 1603.5nm within 1dB excursion at input signal of –10dBm/ch. These results demonstrate that 1530nm‐band pump can be used as a new efficient pump source for L‐band EDFAs. 相似文献
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Bo-Hun Choi Hyo-Hoon Park Moojung Chu Seung Kwan Kim 《Photonics Technology Letters, IEEE》2001,13(2):109-111
A 1530-nm band has been studied as a pump wavelength for the long-wavelength-band erbium-doped fiber amplifier (L-band EDFA). The pump source is built using a tunable light source and cascaded conventional-band (C-band) EDFA. The L-band EDFA uses a forward pumping scheme. Within the 1530-nm band, the 1545-nm pump demonstrates 0.45-dB/mW gain coefficient, which is twice better than that of conventional 1480-nm pumped EDFA. The noise figure of the 1530-nm pump is at worst 6.36 dB, which is 0.75 dB higher than that of the 1480-nm pumped EDFA. Such high-gain coefficient indicates that the L-band EDFA consumes low power 相似文献
6.
报道了一种新型基于环形激光腔的增益钳制掺铒光纤放大器。得到了较好的增益钳制效果和增益平坦度,利用980nm半导体激光器泵浦12m长掺铒光纤形成激光增益,观测到
30nm增益带宽。通过反馈1520nm 激光,在可变衰减器不同值测量了输入信号从- 40 ~10dBm的增益,其小信号增益被钳制在16dB。可为40个波分复用(WDM)信道波长提供增益钳制及平坦的放大功能。 相似文献
7.
R.N. Ghosh J. Shmulovich C.F. Kane M.R.X. de Barros G. Nykolak A.J. Bruce P.C. Becker 《Photonics Technology Letters, IEEE》1996,8(4):518-520
We report on the gain characteristics of a low threshold (8 mW) Er/sup 3+/-doped planar optical waveguide amplifier. Net fiber to fiber gain of 4.5 dB is achieved at a signal wavelength of 1536 nm with 80 mW of 980-nm pump power. This device represents significant progress toward a planar amplifier module pumped by a single laser diode. 相似文献
8.
Teyo T.C. Shah N.S.M. Leong M.K. Poopalan P. Ahmad H. 《Photonics Technology Letters, IEEE》2002,14(9):1255-1257
The erbium-doped fiber amplifier (EDFA) with regenerative feedback is compared with the cofeedback scheme. Without the bandpass filter, the injected signal experiences regenerative amplification and results in a higher signal gain. Such an above-threshold regenerative amplifier also exhibits a lower noise figure due to a higher inversion for the transition corresponding to the signal wavelength of 1550 nm. A near quantum-limited noise figure of 3.1 dB is achieved at the maximum pump power of 134.5 mW, showing nearly complete inversion at the EDF input end in the regenerative-feedback scheme. A low (<10/sup -10/) bit-error rate has been achieved with saturation input signal power above -12 dBm. 相似文献
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Improvement of gain and noise figure in double-pass L-band EDFA by incorporating a fiber Bragg grating 总被引:2,自引:0,他引:2
L.L. Yi L. Zhan J.H. Ji Q.H. Ye Y.X. Xia 《Photonics Technology Letters, IEEE》2004,16(4):1005-1007
An obvious improvement on both the gain and noise figure (NF) is demonstrated in the new double-pass L-band erbium-doped fiber amplifier (EDFA) with incorporating a fiber Bragg grating (FBG). Compared with the conventional L-band EDFAs, the gain is improved by about 6 dB in the new configuration for a 1580-nm signal with an input power of -30 dBm at 60 mW of 980-nm pump power. It is important that the NF is greatly reduced in the new configuration, as the FBG greatly compresses the backward amplified spontaneous emission. For the economical utility of pump power and erbium-doped fiber length, such a configuration may be a very competitive candidate in the practical applications of L-band EDFAs. 相似文献
13.
C波段和980 nm抽运的两段级联L波段掺铒光纤放大器 总被引:2,自引:3,他引:2
提出了由C波段和传统的 980nmLD两段级联抽运L波段信号的结构 ,C波段的功率和波长由掺铒光纤激光器控制。从实验和理论上分析了注入不同波长和功率的C波段对其增益的影响。设计的掺铒光纤放大器(EDFA)结构 ,在C波段波长为 15 2 5nm ,注入功率为 5mW时 ,功率为 - 2 0dBm ,波长为 15 80nm的信号增益提高了 7 7dB。 相似文献
14.
In this paper, a high-power erbium-doped fiber amplifier (EDFA) for the temperature sensor system is theoretically designed and experimentally demonstrated. It consists of an erbium-doped fiber that is pumped bidirectionally with two 980-nm high-power laser diodes (LDs). At the EDFA input, an optical isolator (ISO) is used to ensure that the signal pulse transmits forward only. After that, a wavelength division multiplexer (WDM) is employed to combine the forward pump laser (980 nm) and incident optical pulse (1550nm) into the erbium-doped fiber for direct amplification in the optical domain. At the EDFA output, another WDM couples the backward pump laser (980 nm) into the erbium-doped fiber and outputs the amplified optical pulse (1550 nm) with an ISO followed to isolate the backscattering light. According to this structure, we carried out the experiment in the condition as follows. For 980 nm pump LD, the operating current is 590 mA, and the setting temperature is 25℃. For EDFA, the length of erbium-doped fiber is 12.5 m, and the power of 1550 nm input signal is 1.5 mW. As a result, the power of pump LD is 330 mW, and the power uncertainty is 0.5%. The power of EDFA output at 1550 nm is 300 mW, and the power uncertainty is ±3 mW. 相似文献
15.
Smart R.G. Zyskind J.L. Sulhoff J.W. DiGiovanni D.J. 《Photonics Technology Letters, IEEE》1993,5(5):523-525
The effect of pump wavelength around 1480 nm on the performance of saturated erbium-doped fiber amplifiers (EDFAs) suitable for use as in-line amplifiers for terrestrial and submarine systems is investigated experimentally. The results show that for high-gain amplifiers (25 dB) with high output powers (15 dBm), operating around 10 dB in compression, the performance is relatively insensitive to pump wavelength. However, for lower gain amplifiers (12 dB), pumped at low (15 mW) powers, the compression of the amplifier is found to decrease significantly with increasing pump wavelength, while the noise figure shows a weak minimum for a pump wavelength near 1480 nm 相似文献
16.
Percival R.M. Szebesta D. Williams J.R. Lauder R.D.T. Tropper A.C. Hanna D.C. 《Electronics letters》1994,30(19):1598-1599
A fully connectorised diode laser pumped first window amplifier has been constructed, for the first time, around a thulium doped fluoride fibre. For a 780/806 nm combination of pump and signal wavelengths, small signal gains of 25-26 dB and gain efficiencies of 2.4 dB/mW have been achieved. In addition, output powers approaching +13 dBm are possible for a launched pump power of 31 mW, which corresponds to a conversion efficiency of around 650% 相似文献
17.
用于传感的具有平坦带宽掺Er光纤超荧光光源的研究 总被引:1,自引:0,他引:1
设计和实现了一种双程后向泵浦结构的掺Er光纤(EDF)超荧光光源。通过1×2端的980nm耦合器和980nm的LD,实现了单管双泵浦作用,改善了光源输出光谱、带宽和平坦度,在未加滤波器的情况下,最高功率可达41.48mW(16.18dBm),3dB带宽可达40nm,平坦度为±1.5dB。该光源结构简单、易于实现,应用于光纤光栅(FBG)传感系统,可实现多FBG传感信号峰值功率均衡。 相似文献
18.
Brinkmann R. Dinand M. Baumann I. Harizi C. Sohler W. Suche H. 《Photonics Technology Letters, IEEE》1994,6(4):519-521
The first integrated optical amplifying acoustically tunable wavelength filter in Er-doped LiNbO3 is reported. At the signal wavelength of λs=1531 nm a maximum gain of 4.8 dB has been obtained with a coupled pump power of 160 mW (λp =1484 nm). Lossless signal transmittance has been achieved with a pump power as low as 13.5 mW for λs>1561 nm 相似文献
19.
Optimal pump wavelength in the4I 15/2-4I 13/2 absorption band for efficient Er3+-doped fiberamplifiers
Zyskind J.L. Giles C.R. Desurvire E. Simpson J.R. 《Photonics Technology Letters, IEEE》1989,1(12):428-430
The authors report the measured gain of a highly efficient erbium-doped fiber amplifier pumped at wavelengths between 1.46 and 1.51 μm. The optimal pump wavelength, λopt, was determined to be 1.475 μm. At this wavelength, the maximum gain coefficients for signals at 1.531 and 1.544 μm were 2.3 and 2.6 dB/mW, respectively. At λopt, high gains ranging from 32 dB at pump power P p=20 mW up to 40 dB at P p=80 mW were obtained. These modest pump powers are within the capabilities of currently available 1.48-μm diode lasers. The width about λopt for 3-dB gain variation exceeded 27 nm for P p=10 mW and 40 nm for P p >20 mW. With this weak dependence on pump wavelength, single-longitudinal-mode lasers do not have a significant advantage over practical Fabry-Perot multimode pump lasers 相似文献
20.
A highly efficient Er-doped fibre amplifier pumped by GaAlAs laser diodes is reported. Using a low Er-cluster content fibre with a high numerical aperture, the EDFA attains 39 dB signal gain for double LD pumping and 30 dB for single LD pumping at 1.536 mu m. A maximum gain coefficient of 1.3 dB/mW was achieved at the 0.827 mu m pump band.<> 相似文献