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HIP9022AM Datasheet(PDF) 8 Page - Intersil Corporation |
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HIP9022AM Datasheet(HTML) 8 Page - Intersil Corporation |
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8 / 10 page ![]() 4-8 Circuit Block Descriptions Laser Drive Circuitry In Figure 3, the gate of the external current source Power FET, Q2 is driven via the Operational Transconductance Amplifier (OTA), A2 on the IC. The voltage on the current sense resistor, RS in the source of the Power FET is monitored by a X10 gain of the feedback amplifier, A1. The stability of the current loop is established with an external 0.1 µF capacitor to ground at the gate of the Power FET. The sampled voltage range is 0 to 0.5V when the proper value of sense resistor, RS is chosen (typically 0.25Ω for 2A). The OTA, A2 compares the X10 gain signal toa0to5Vreference signal from an on-chip Sample and Hold (First S/H) circuit. The Q2 drain current (Laser Drive current), IDL is: where VIN(DL) is the programmed VIN for the First S/H voltage reference signal. The S/H reference for the Laser Drive Current current is updated with other multiplexed S/H circuits from a serial bus and an off-chip D/A converter. Laser constant current is fully controllable by the multiplex analog S/H bus, allowing accurate calibration of the laser output and corrections as the laser ages. In Figure 1, the laser drive current from Q2 is digitally switched to either flow through or is shunted around the laser diode by switching the external Shunt Power FET, Q3 on or off. The gate of the Shunt FET is switched between two voltages (Upper and Lower) which are provide by 2nd and 3rd S/H circuits. These Shunt FET gate drive levels are fully programmable via the multiplexed analog S/H bus. By adjusting these levels to account for the laser power supply, the Shunt FET threshold and channel resistance; minimum Shunt FET gate drive power levels can be established. The Upper and Lower gate voltage driver circuits are two high current OTA amplifiers with two filter capacitors. The upper voltage is programmable in the 0V to VCC range at the input of amplifier A4. The lower voltage is programmable in the range of -4V to VCC. The -4V extension is accomplished by an optional on-chip voltage inverter circuit. The input to amplifier A3 is either direct from the S/H input or inverted by amplifier A5. The maximum laser on-off switching speeds are dependent on the selection of Shunt FETs. A Harris dual complementary MOSFET, RF3V49092 or RF3S49092 has been designed specifically for this application. With the constant current set at 0.8A, a typical laser switching speed of 20ns has been measured. Thermal Compensation A 4th S/H circuit is used to set the amplitude of an optional thermal compensation signal which can be used to modulate the constant laser current source as a two pole filtered effect of the laser on-off data. This feature may be disabled when it is not required. This circuit is designed to compensate for the temperature variations in the laser as the laser is turned on and off. The bypass capacitors at the Thermal Comparator (CTCx-10K, CTCx-27K) represent the respective poles for the filter. A laser cools after it has been off for a period of time and is more efficient when it is turned-on. Compensation for the increased efficiency is made by slightly reducing the current level of the constant current source FET. The level will be reduced by a programmable amount of 0 to 5% of full scale. The programmable amount is fixed by the level of compensation to S/H addresses 7 and 8 (see Table 1). The percent of modulation (change) in drive current is calculated as follows: For example, if we control the Laser Drive current with 2V programmed with address 1 and 2 for the First S/H’s, given that VIN(DL) = 2V and RS = 0.25Ω. Then, from EQ. 1, IDL = VIN(DL)/(RS x 10) = 2/(0.25 x 10) = 0.8A. If 2V is programmed to addresses 7 and 8 as Thermal Compensation, VIN(TC) for the 4th S/H’s, then, Mod.% = (2/2) x 5% = 5%. In Figure 3, the correction is applied from the output of the Thermal Compensation circuit (where the current is 2V/20k Ω = 0.1mA) to the input of amplifier A2. The 0.1mA is forced into the 1k Ω resistor (and the low Z output of A1) to increase the voltage at the inverting input of A2 by 0.1V or 5% of the +VIN(DL) input (2V) to A2. The modulation input is limited by the 0 to VCC input range of S/H maximum VIN. Input Data I DL V IN DL () R S 10 × () ------------------------- = (EQ. 1) Modulation °°⁄ V IN TC () V IN DL () --------------------- 5 °°⁄ × = (EQ. 2) FIGURE 3. LASER CONSTANT CURRENT SOURCE DRIVER WITH OVER CURRENT DETECTION AND THERMAL COMPENSATION S/H SYS + - +- X10 CC2 XTEN2+ XTEN2- 53 54 55 0.25 Ω A1 A2 Q2 RS 1k Ω O. C. COMP. + - 49 0.1 µF 12k Ω 30k Ω 51 VOLT. TO CURRENT 52 VOLT. TO CURRENT OC2 CTC2-27K CTC2-10K THERMAL COMP. 10k Ω 27k Ω 20k Ω 0.1 µF 0.02 µF HIP9022 |
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