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1.
Abstract

A novel 10-Gbps × 12-channel pluggable parallel optical transceiver is designed and fabricated. Compared with other optical transceivers, this transceiver emphasizes small size, high-density, low power consumption, and high transmission speed. Most importantly, its optical coupling structure is simplified to promote cost-effective large-scale production. This transceiver is electrically pluggable and consists of transmitter and receiver modules linked by parallel multi-mode fibers. Each module consists of a six-layered high-speed, high-density printed circuit board, the size of which is 30 mm × 18 mm × 1 mm, packaged with optoelectronic devices and corresponding control chips. The printed circuit boards not only provide a high-speed electrical connection between the I/O interfaces and high-speed chips, but they also supply power and ground planes to those chips. End-to-end error-free transmission at 10.3125 Gbps was obtained for a 231 ? 1 non-return-to-zero pseudo-random bit sequence.  相似文献   

2.
In this paper, a low-power optical receiver front-end which consists of a transimpedance amplifier (TIA) and three stages of limiting amplifier (LA) for 2.5 Gb/s applications is proposed in 0.18 µm CMOS technology. The proposed TIA benefits from a modified inverter structure, in which the input resistance is properly reduced due to the use of diode-connected transistors in comparison with conventional inverter circuit. Also, an active inductor is used in parallel with a diode-connected transistor at the output node, which provides a low output resistance, while it resonates with the load capacitance to extend the ?3 dB frequency bandwidth. Moreover, three stages of LAs are used to obtain extra gain, in which each LA cell uses active inductor load. However, HSPICE simulations for the proposed TIA circuit show a 42.24 dBΩ transimpedance gain, 1.96 GHz frequency bandwidth, 11.7 pA/√Hz input referred noise, and only 972 µW of power consumption at 1.5 V supply. Also, simulation results for the whole receiver system show a 75.6 dB gain, 1.7 GHz frequency bandwidth, and 6.54 mW of power consumption at 1.5 V supply. Finally, simulation results indicate that the proposed receiver system has good performances to be used as a low-power optical receiver front-end.  相似文献   

3.
This paper presents an active patch array designed at 24 GHz. It can be used as a front-end component for a phased array. A series resonant array structure is chosen which is compact and easy excite. With 5 elements, the array proved a 12-dB antenna gain. A power amplifier and a low noise amplifier are designed on a single GaAs chip (PALNA). Bias switch is used in the PALNA, which greatly reduces the switch loss in a transceiver and increases the efficiency. 20-dB small signal gain is achieved in both power amplifier and low noise amplifier. The active patch array is built by the combination of the patch array and PALNA. The measured active gain of this antenna is 35-dB for the PA mode and 31-dB for the LNA mode. This active patch array can obtain an EIRP of 34 dBm with a total radiated power of 22dBm and a maximum PAE of 32%. To check the noise performance, we applied sources at both normal temperature and 77K (liquid nitrogen) and extracted the noise figure (3.5 dB) of the active antenna by the Y factor method. The results proved that the active antenna is working efficiently as both a transmitting and receiving antenna.  相似文献   

4.
In this paper, a new low-power optical receiver front-end is proposed in 90 nm CMOS technology for 5 Gb/s AApplications. However, to improve the gain-bandwidth trade-off, the proposed Trans-Impedance Amplifier (TIA) uses an active modified inverter-based topology followed by a common-source amplifier, which uses active inductive peaking technique to enhance the frequency bandwidth in an increased gain level for a reasonable power consumption value. The proposed TIA is analyzed and simulated in HSPICE using 90 nm CMOS technology parameters. Simulation results show a 53.5dBΩ trans-impedance gain, 3.5 GHz frequency bandwidth, 16.8pA/√Hz input referred noise, and 1.28 mW of power consumption at 1V supply voltage. The Optical receiver is completed using three stages of differential limiting amplifiers (LAs), which provide 27 dB voltage gain while consume 3.1 mW of power. Finally, the whole optical receiver front-end consumes only 5.6 mW of power at 1 V supply and amplifies the input signal by 80 dB, while providing 3.7 GHz of frequency bandwidth. Finally, the simulation results indicate that the proposed optical receiver is a proper candidate to be used in a low-power 5 Gbps optical communication system.  相似文献   

5.
In this paper, we have proposed a novel approach to generate optical carrier suppression (OCS) mm-wave with signal only carried by one first-order sideband using a dual-parallel MZM in radio-over-fiber (RoF) system, and the transmission performance was also investigated. As the optical mm-wave signal is transmitted along the fiber, there is no time shift of the data symbols resulting from the group velocity dispersion in the fiber because the signal is only modulated on one sideband. The simulation results showed that the eye diagram keeps open and clear even when the optical mm-wave signals are transmitted over 96-km and the power penalty is about 1-dB after fiber transmission distance of 60-km, which is quite consistent with our theoretical analysis. Furthermore, the proposed OCS optical mm-wave generation approach is also used in a full-duplex RoF link based on wavelength reuse at the base station for the uplink due to another pure sideband without carrying data. The bidirectional 2.5-Gbit/s data is successfully transmitted over 40-km standard single mode fiber with less than 0.5-dB power penalty in the simulation. Both the unidirectional RoF downlink and the full-duplex RoF system have good performance.  相似文献   

6.
In the visible light communication (VLC) system which combines lighting and communication functions, the 3-dB modulation bandwidth is mainly limited by the light-emitting diode (LED) suffered high-frequency response attenuation. An optimized photoelectric receiver was proposed to enhance the 3-dB modulation bandwidth. The frequency response of the photoelectric receiver was derived. Theoretical analysis predicted that a gain peak would appear in the high-frequency response of the photoelectric receiver. The value of the gain and the frequency point of the gain peak can be adjusted by selecting appropriate values of feedback resistor and capacitor. Then, the measurement platform of 3-dB modulation bandwidth for blue-LED VLC system was established. Experimental measurements demonstrated that the photoelectric receiver with proper sets of feedback resistor and capacitor can compensate the high-frequency response attenuation of a normal LED. The 3-dB modulation bandwidth obtains 56% enhancement if the photoelectric receiver was replaced from a commercial one to our optimized design. In order to further expand the 3-dB modulation bandwidth, an equalization circuit consists of two-stage transistor amplifier and an emitter-follower was introduced to suppress the low-frequency response. The 3-dB modulation bandwidth for the VLC system with our optimized photoelectric receiver can be expanded to 241 or 281 MHz, while the circuit was, respectively, arranged as pre-equalization or post-equalization.  相似文献   

7.
A large-diameter PIN photodiode (400 μm) with antireflection coating optimized for wavelength 650 nm was integrated with an automatic gain control transimpedance amplifier, linear post amplifier and 50Ω linear driver. The presented optical receiver shows a high linearity in receiving multilevel signals. A sensitivity of ?29.5dBm (BER = 10?9) at 200 Mb/s with binary signal was achieved. By using four-level pulse amplitude modulation (4-PAM) a data rate of 400 Mb/s and a sensitivity of ?21.5 dBm (SER = 10?9) was achieved.  相似文献   

8.
双向掺铒光纤放大器的特性分析   总被引:1,自引:0,他引:1  
讨论了双向掺铒光纤放大器的结构方案,利用考虑放大的自发辐和北员耗影响的双向掺铒光纤放大器稳态放大速率方程模型分析的增益与掺铒光纤长度、输入信号光功率、帛运光功率及抽运方式等参数之间的关系,研究了单向和双向等功率抽运下正反向噪声系数随正反向信号光输入功率的变化行为。  相似文献   

9.
We report a flexible all-optical gain controlled bidirectional optical amplifier. The device achieves constant gain and low noise figure over a large input power range. Moreover, the device removes Rayleigh backscattered light and amplifier noise.  相似文献   

10.
An X-band dielectric Cerenkov maser amplifier experiment is reported. The amplifier system consisted of a solid, thermionically generated electron beam propagating through a cylindrical waveguide partially filled with an annular, dielectric liner. The input signal was provided by a tunable (9-10.3 GHz) magnetron with power up to 10 kW. Electron beam voltages and currents of up to 250 kV and 100 A could be generated for 1 μs pulse durations. The system was configured to operate in the TM01 mode of the dielectric-lined waveguide. In this experiment the gain of the system with respect to the length of the dielectric liner was studied at a fixed input frequency of 10.3 GHz. At electron beam parameters of 160 kV and 60 A, a power gain of 24 dB over 56 cm of interaction length was measured for an input power of 4.5 kW, corresponding to a maximum RF amplified power of 1.15 MW and 12% efficiency  相似文献   

11.
高巍  万里兮  李志华  李宝霞  宋见 《应用光学》2011,32(6):1275-1281
 介绍了一款基于系统级封装技术的低成本、收发一体、可带电热插拔的12通道小型光模块的研制。该光模块采用850 nm垂直腔面发射激光器阵列及其驱动器作为发射端,光电探测器阵列及其跨阻放大器作为接收端,通过光路无源对准实现了低成本光互连。高速度、高密度封装下的瞬态同步开关噪声、芯片间电磁干扰、通道间串扰、反射等电学问题是实现模块整体性能的难点。基于埋入技术的新型滤波器的使用实现了封装尺寸小型化且改善了电源网络的完整性;基于电磁场、传输线理论的信号完整性设计减小了通道间串扰且通过补偿阻抗不连续结构增加了通道带宽。模块背靠背眼图测试结果显示6.25 Gbps速率下系统传输零误码。  相似文献   

12.
李轩  赵尚弘  朱子行  韩磊  赵静 《应用光学》2013,34(3):547-552
针对外调制星间微波光子链路输出信噪比优化问题,建立了基于双电极马赫 曾德尔调制器的强度调制直接探测星间微波光子链路模型,通过优化调制器调制方式来提高链路性能。用数值模拟方法得到了单边带、双边带和推挽式3种调制方式下链路输出信噪比,利用曲面投影法求得了最优调制方式时一定信噪比要求下发射端所需最小光放大器增益和对应的调制器直流偏置相位。结果表明:相同输入射频信号功率和发射光功率情况下,双边带调制输出信噪比比单边带调制高3 dB,低直流偏置相位推挽调制可以进一步优化输出信噪比。输入射频信号功率为-20 dBm,输出信噪比为17.3 dB时,所需最小光放大器增益为43.9 dB,对应的直流偏置相位为0.87。  相似文献   

13.
Lin  J. M.  Ho  W. J. 《Laser Physics》2012,22(4):765-769
We propose and demonstrate a C-band Erbium-doped fiber amplifier (EDFA) using amplified spontaneous emission (ASE) power peaking-selective and feedback to achieve highly stabilized and wide dynamic range gain clamping performances. The gain of 16.20 ± 0.13 dB is obtained with the input signal power dynamic range of 30 dB and the maximum noise figure (NF) was 6.6 dB with the input signal power from −35 to −10 dBm. To investigate the gain variation for the probe signals, we applied a saturation tone signal to simulate 16-channel DWDM signals as it is added (dropped) into (from) EDFA. The gain variation of the proposed scheme at a appropriate ring-cavity loss (VOA = 5 dB) is less than 0.13 dB for the input signal power from −35 to −5 dBm and wavelength from 1530 to 1564 nm.  相似文献   

14.
The equalization circuit in the visible light communication (VLC) system has large impacts on the frequency response and can greatly improve the 3-dB modulation bandwidth. The optimization of the two-stage common-emitter transistor amplifier for equalization circuit is presented in detail and the design rules are disclosed. At first, the frequency response of the single-stage amplifier is derived and the simulated characteristic curves illustrated the changing regularity of four main factors are given. Subsequently, the frequency response of the two-stage amplifier is investigated by simulation. It is shown that the capacitors in the resistance–capacitance (RC) network has large impacts on the low-frequency range, while the resistors in the RC network can adjust the high-frequency, and the resistors in the emitter can adjust the low-frequency. Experimental measurements of the fabricated equalization circuit demonstrated the simulation results. Then, the two-stage amplifier is induced as post-equalization circuit (post-EQC) or pre-equalization circuit (pre-EQC) and the measured frequency response curves are given. The equalization circuit with proper sets of capacitors and resistors would flatten the frequency response curve of the VLC system. It is shown that the 3-dB modulation bandwidth of the VLC system equipped with post-EQC or pre-EQC can be expanded to 292 MHz or 304 MHz, respectively. Moreover, if the photoelectric receiver and the post-EQC are combined in the optimization, the 3-dB modulation bandwidth can be expanded to 375 MHz.  相似文献   

15.
Ku  H. -D.  Park  C. -S. 《Laser Physics》2012,22(5):972-976
This paper proposes a switchable wavelength fiber laser (SWFL) based on an arrayed waveguide grating (AWG) and a gain-saturated reflective semiconductor optical amplifier (RSOA). The SWFL was experimentally implemented in the C- and L-bands. In order to achieve narrow-linewidth oscillation, the SWFL was driven by bidirectional injection-locked RSOAs. The RSOA was operated in the gain-saturated region, using gain compression properties to obtain uniform power over a wide bandwidth. Based on this configuration, we obtained 40 C-band international telecommunication unit (ITU) wavelengths with 100-GHz channel spacing. The SWFL displayed a narrow 3-dB bandwidth (<0.06 nm), a high and uniform peak power (P max > 0.22 dB, ΔP max < 0.26 dB), and a high and uniform side mode suppression ratio (SMSR > 66 dB, ΔSMSR < 1 dB). The peak-power and wavelength stabilities were ±0.24 dB and ±0.01 nm, respectively, at room temperature over a 1 h period.  相似文献   

16.
A novel scheme of optical power equalization based on Fabry-Perot semiconductor optical amplifier (FPSOA) is proposed. Because of the gain characteristic of FP-SOA, real-time controlling mechanism according to input optical power is aborted in the scheme. The simulations show that 10-dB pulse peak power variation can be clamped in less than i dB. The influences of injecting current, pulse periods, and pulse width are discussed.  相似文献   

17.
We consider the structure of a small-size superheterodyne modulation-type radiometric receiver with a low-noise transistor amplifier (LNTA) at the input. With LNTA noise coefficient 3.5 dB, the fluctuation sensitivity of the radiometric receiving unit was 0.025 K in the input-frequency range 56-60 GHz for a time constant 1 s.  相似文献   

18.
Theoretical analysis of the spatial, noise, and energy characteristics of an amplifier has been performed in the mode of spectral and time selection using subnanosecond stimulated Raman Scattering gain of weak echo signals in crystalline active media that are known for high (up to 10–1 cm/MW) gain coefficients. The possibility to reach high gain values has been demonstrated for weak signals from objects at acceptable angular sizes of the field of vision of an amplifier. To provide a signal-to-noise ratio that exceeds unity over the entire field of vision, the number of photons at the input to an amplifier that is required has to exceed the number of its resolution elements. Accurate determination of the possibilities of recording of weak echo signals and quality of images of targets that are obtained using amplifiers under stimulated Raman Scattering requires additional special experiments.  相似文献   

19.
We propose a stable multi-longitudinal Brillouin/semiconductor fiber laser(BSFL) as the upstream source in a bidirectional single-fiber wavelength-division multiplexing-passive optical network(WDM-PON).The downstream wavelength serves as the pump of the BSFL.Brillouin-frequency-shifted(~10.8 GHz) upstream carrier is generated to suppress the Rayleigh backscattering and back reflection-induced crosstalk.The stable multi-longitudinal operation of the BSFL,attributed to the four-wave mixing(FWM) effect in the semiconductor optical amplifier(SOA) reduces the difficulty of generating a stable single-longitudinal fiber laser-based upstream carrier.Bidirectional symmetric transmission at 10 Gb/s over a 12.5-km single mode fiber with less than 2-dB power penalty is demonstrated.  相似文献   

20.
A 44-GHz amplifier using 0.25-m gate length and double-heterojunction structure HEMT devices is described. Higher gain and power performance have been obtained from the amplifier using this device at millimeter-wave frequencies. A spot gain of 9.4 dB and a 1-dB gain compression point of +7.5 dBm has been achieved at 43.5 GHz.This work was supported by the Air Force Space Division under Contract No. F04701-84-C-0113.  相似文献   

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