An N-channel JFET has a low bias current when its gate is
  biased negative to the source. However, this requires either
  that the gate voltage be biased negative with respect to the source
  voltage or that source voltage be biased positive with respect to
  the gate voltage. For ac amplifier designs, gate biasing can be made
  self-biased by using an RC network at the source to hold the positive
  voltage for a period longer than the time period of the input
  pulse/frequency source.
 
 In the design described here, the JFET source is constantly
  biased. Hence, its frequency response is excellent from dc to 10
  MHz. This improvement is due to stable diode biasing. Diode
  biasing exhibits only a 2-mV/°C drop in voltage with increasing
  temperature from 0°C to 100°C. This is excellent stability.
 In this example of a pulsed amplifier design, the signal source has
  been biased by a 1-GO resistance to ground, and the JFET source
  is biased using a fast diode, a 1N4148, at a source-drain current
  of about 5 mA. The gate is maintained at ground potential so that
  no bias voltage is injected into the input dc circuit. This scheme
  makes the gate remain at zero voltage unless a signal to be amplified
  changes it.
 This technique is illustrated in the figure, where the input
  impedance of the circuit is maintained at 1 GO, unless it’s shunted
  by the impedance of the signal source. The JFET’s output current
  is kept significantly high—at 5 mA—to let the JFET drain voltage
  remain at its mid-operating point, about 5 V. This enables the
  JFET to work for both positive and negative input signals.
 In this circuit, a J309 or IFN152 JFET is the most suitable
  device, with an input bias current of about 100 pA. The amplifier
  delivers a good signal response to about 10 MHz. A 2N4117A
  JFET would reduce the input bias current but also reduce the highfrequency
  response considerably.
 This circuit makes an excellent input-stage amplifier for oscilloscopes,
  where input impedance isn’t greater than 1 MO. The
  amplifier improves the input stage to 1 GO. The circuit is most
  suitable for piezoelectric detectors, photodiode-based radiation
  detectors, and low-capacitance sensors with a very small charge in
  the range of 10 fC to 1 pC.