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HFA1115IP

225MHz, Low Power, Output Limiting, Closed Loop Buffer Amplifier

Intersil 

HFA1115

The HFA1115’s closed loop gain implementation provides

better gain accuracy, lower offset and output impedance,

and better distortion compared with open loop buffers.

Closed Loop Gain Selection

This “buffer” operates in closed loop gains of -1, +1, or +2, and

gain selection is accomplished via connections to the ±inputs.

Applying the input signal to +IN and floating -IN selects a gain

of +1 (see next section for layout caveats), while grounding -IN

selects a gain of +2. A gain of -1 is obtained by applying the

input signal to -IN with +IN grounded through a 50Ω resistor.

The table below summarizes these connections:

GAIN

(AV)

-1

+1

+2

CONNECTIONS

+INPUT (PIN 3)

-INPUT (PIN 2)

50Ω to GND

Input

Input

NC (Floating)

Input

GND

Unity Gain Considerations

Unity gain selection is accomplished by floating the -Input of

the HFA1115. Anything that tends to short the -Input to

GND, such as stray capacitance at high frequencies, will

cause the amplifier gain to increase toward a gain of +2. The

result is excessive high frequency peaking, and possible

instability. Even the minimal amount of capacitance

associated with attaching the -Input lead to the PCB results

in approximately 3dB of gain peaking. At a minimum this

requires due care to ensure the minimum capacitance at the

-Input connection. .

TABLE 1. UNITY GAIN PERFORMANCE FOR VARIOUS

IMPLEMENTATIONS

APPROACH

PEAK-

ING

(dB)

BW

(MHz)

+SR/-SR

(V/μs)

±0.1dB

GAIN

FLATNESS

(MHz)

Remove Pin 2

2.5

400 1200/850

20

+RS = 620Ω

0.6

170 1125/800

25

+RS = 620Ω and

0

165 1050/775

65

Remove Pin 2

Short Pins 2, 3

0

200 875/550

45

100pF cap. be-

0.2

190 900/550

19

tween pins 2, 3

Table 1 lists five alternate methods for configuring the

HFA1115 as a unity gain buffer, and the corresponding

performance. The implementations vary in complexity and

involve performance trade-offs. The easiest approach to

implement is simply shorting the two input pins together, and

applying the input signal to this common node. The amplifier

bandwidth drops from 400MHz to 200MHz, but excellent

gain flatness is the benefit. Another drawback to this

approach is that the amplifier input noise voltage and input

offset voltage terms see a gain of +2, resulting in higher

noise and output offset voltages. Alternately, a 100pF

capacitor between the inputs shorts them only at high

frequencies, which prevents the increased output offset

voltage but delivers less gain flatness.

Another straightforward approach is to add a 620Ω resistor

in series with the positive input. This resistor and the

HFA1115 input capacitance form a low pass filter which rolls

off the signal bandwidth before gain peaking occurs. This

configuration was employed to obtain the datasheet AC and

transient parameters for a gain of +1.

Non-inverting Input Source Impedance

For best operation, the DC source impedance seen by the

non-inverting input should be ≥50Ω. This is especially

important in inverting gain configurations where the non-

inverting input would normally be connected directly to GND.

Pulse Undershoot and Asymmetrical Slew Rates

The HFA1115 utilizes a quasi-complementary output stage to

achieve high output current while minimizing quiescent supply

current. In this approach, a composite device replaces the

traditional PNP pulldown transistor. The composite device

switches modes after crossing 0V, resulting in added

distortion for signals swinging below ground, and an

increased undershoot on the negative portion of the output

waveform (see Figures 9, 13, and 17). This undershoot isn’t

present for small bipolar signals, or large positive signals.

Another artifact of the composite device is asymmetrical slew

rates for output signals with a negative voltage component.

The slew rate degrades as the output signal crosses through

0V (see Figures 9, 13, and 17), resulting in a slower overall

negative slew rate. Positive only signals have symmetrical

slew rates as illustrated in the large signal positive pulse

response graphs (see Figures 7, 11, and 15).

PC Board Layout

This amplifier’s frequency response depends greatly on the

care taken in designing the PC board. The use of low

inductance components such as chip resistors and chip

capacitors is strongly recommended, while a solid

ground plane is a must!

Attention should be given to decoupling the power supplies.

A large value (10μF) tantalum in parallel with a small value

(0.1μF) chip capacitor works well in most cases.

Terminated microstrip signal lines are recommended at the input

and output of the device. Capacitance directly on the output

must be minimized, or isolated as discussed in the next section.

For unity gain applications, care must also be taken to

minimize the capacitance to ground at the amplifier’s

inverting input. At higher frequencies this capacitance tends

to short the -INPUT to GND, resulting in a closed loop gain

which increases with frequency. This causes excessive high

frequency peaking and potentially other problems as well.

An example of a good high frequency layout is the

Evaluation Board shown in Figure 2.

5

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