SLOS451D December 2004 – March 2026 THS4631
PRODUCTION DATA
High slew rate, unity gain stable, voltage-feedback operational amplifiers typically achieve high slew rate at the expense of a higher-input noise voltage. However, the 7nV/√Hz input voltage noise for the THS4631 is much lower than comparable amplifiers while achieving high slew rates. The input-referred voltage noise and the input-referred current noise term combine to give low output noise under a wide variety of operating conditions. Figure 8-1 shows the amplifier noise analysis model with all the noise terms included. In this model, all noise terms are taken to be noise voltage or current density terms in either nV/√Hz or fA/√Hz.
Figure 8-1 Noise Analysis
ModelThe total output noise voltage is computed as the square root of all square output noise voltage contributors. Equation 1 shows the general form for the output noise voltage using the terms shown in Figure 8-1.

Equation 2 shows that dividing this expression by the noise gain [NG = (1+ Rf/Rg)] gives the equivalent input-referred spot noise voltage at the noninverting input.

High resistor values can dominate the total equivalent input-referred noise. Use a 3kΩ source-resistance (RS) value to add a voltage noise term of approximately 7nV/√Hz. This noise term is equivalent to the amplifier voltage noise term. Higher resistor values dominate the noise of the system. Although the THS4631 JFET input stage is advantageous for high-source impedance because of the low-bias currents, the system noise and bandwidth is limited by a high-source (RS) impedance.