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LTC6602 Datasheet(PDF) 20 Page - Analog Devices |
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LTC6602 Datasheet(HTML) 20 Page - Analog Devices |
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20 / 40 page ![]() LTC6601-2 20 66012f APPLICATIONS INFORMATION Table 1 lists the amplifier input referred noise for the LTC6601-2. Tables 2 to10 list the noise referred to the input pins of the IC for common configurations of the LTC6601-2. To determine the spot noise at the output, simply multiply the noise by the Gain = R2/R1. To estimate the integrated noise at the output, multiply the noise by the gain, and the square root of the noise bandwidth. The noise bandwidth depends on the filter configuration. For Figure 2, the noise bandwidth is 100MHz, or approximately 7 times the filter bandwidth. Improvements in SNR can be made by adding an additional RC filter at the output to band limit wide band noise before feeding ADCs. See the section “Interfacing the LTC6601 to ADC Converters” for more detail. Table 1. Amplifier (Input Referred) Noise Characteristics for the LTC6601-2 BIAS PIN PULLED TO V+ BIAS PIN FLOATING eni nV/√Hz in pA/√Hz eni nV/√Hz in pA/√Hz 4.7 3 5.2 2.1 LAYOUT CONSIDERATIONS Because the LTC6601 is a very high speed amplifier, it is sensitive to both stray capacitance and stray inductance. It is critical that close attention be paid to supply bypass- ing. For single supply applications, it is recommended that a high quality 0.1μF surface mount ceramic bypass capacitor be placed between Pins 14 and 13 with direct short connections. Pin 13 and the Exposed Pad, Pin 21, should be tied directly to a low impedance ground plane with minimal routing. For dual (split) power supplies, it is recommended that an additional high quality, 0.1μF ceramic capacitor be used to bypass pin V+ to ground and V– to ground, again with minimal routing. For driv- ing large differential loads (<200Ω), additional bypass capacitance may be needed between V+ and V– for opti- mal performance. Note that small geometry (e.g., 0603) surface mount ceramic capacitors have a much higher self resonant frequency than capacitors with leads, and perform best in high speed applications. The VOCM pin should be bypassed to ground with a high quality ceramic capacitor whose value exceeds 0.01μF, with direct, short connections. In split supply applications, the VOCM pin can be either bypassed to ground or directly hardwired to ground. Be careful not to violate the output common mode range specifications for the VOCM pin. Stray parasitic capacitances to unused component pins that set up the filter’s characteristics, should be kept to an absolute minimum. This prevents deviations from the ideal frequency response. An ideal layout technique would be to remove the solder pads for the unused component pins, and strip away the ground plane underneath these pins to lower capacitance to an absolute minimum. Floating unused component pins which set up the filter characteristics will not reduce the reliability of the LTC6601. At the output, always keep in mind the differential nature of the LTC6601, and that it is critical that the load impedances seen by both outputs (stray or intended), should be as bal- anced and symmetric as possible. This will help preserve the natural balance of the LTC6601, which minimizes the generation of even order harmonics and preserves the rejection of common mode signals and noise. – + 66012 F05 R1 R1 R3 * * eni2 eno2 enR32 R3 * enR32 R2 * enR22 R2 * enR22 * enR12 * enR12 In+2 In–2 Figure 5. Differential Noise Model of the LTC6601 |
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