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LTC5100EUF Datasheet(PDF) 20 Page - Linear Technology |
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LTC5100EUF Datasheet(HTML) 20 Page - Linear Technology |
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20 / 52 page ![]() LTC5100 20 sn5100 5100fs Figure 17 depicts the current ranges for the source cur- rent. The guaranteed full scale is 6mA per range. The minimum operating level should be limited to 1/16 of full scale to avoid the coarse relative quantization seen in any ADC or DAC when operated at low levels. The source range, Is_rng, should be selected as low as possible such that the source current, IS, stays within the guaranteed current limits over temperature, considering the laser temperature characteristics. From Equation 1 we can see that the source current is the sum of the laser bias and the average modulation currents: IS = IB+ IM (15) Is_rng should be chosen to support the total current required for laser bias and modulation, taking temperature changes in IB and IM into account. Figure 18 depicts the current ranges for the average modulation current. This is the average modulation cur- rent at the MODA and MODB pins of the chip (recall that the MODA and MODB pins are connected on-chip). The peak- to-peak modulation at the pins of the chip is twice the average. Guaranteed full scale is 3mA average or 6mA pp per range. The minimum operating level should be limited to 1/8 of full scale to preserve the quality of the eye diagram. Operating below 1/8 full scale causes increased overshoot and undershoot. The modulation range, Im_rng, should be selected as low as possible such that the modulation current, IM, stays within the guaranteed cur- rent limits over temperature. The modulation current varies over temperature to compensate the loss in slope efficiency typical of most VCSELs. Therefore, the choice of Im_rng should take temperature changes into account. High Speed Aspects of the Modulation Output The LTC5100 modulation output presents a resistive drive impedance with very low reflection coefficient. This output design suppresses ringing and reflections to maintain the quality of the eye diagrams in spite of laser impedance variations. The reflection coefficient is sufficiently low that the LTC5100 can drive the laser over an arbitrary length of transmission line, as shown in Figure 19. A well designed transmission line stretching the entire length of a typical transceiver module goes virtually unnoticed in this sys- tem. The only practical limitation on interconnect length to the laser is high frequency line loss. OPERATIO Figure 17. Ranges for the Source Current Figure 18. Ranges for the Modulation Current Figure 19. High Speed Details of the Modulation Output 0 9 Is_rng = 0 5100 F17 4.5 18 27 36 Is_rng = 1 RECOMMENDED MINIMUM IS 1/16 OF FULL SCALE Is_rng = 2 Is_rng = 3 IS (mA) 0 4.5 Im_rng = 0 5100 F18 9 13.5 18 Im_rng = 1 RECOMMENDED MINIMUM IS 1/8 OF FULL SCALE Im_rng = 2 Im_rng = 3 IM (mA) VSS IM LBWB M1 IS = IB + IM ZO = RT IB IS VDD SRC MODA MODB LTC5100 RT 50 Ω TYP CT 10nF 3.2Gbps MODULATOR TRANSMISSION LINE 14 11 10 C1 LBWA |
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