Data Sheet
Comlinear CLC1605, CLC2605, CLC3605 1.5GHz Ampliers Rev 1E
©2007-2013 Exar Corporation 14/21 Rev 1E
General Information - Current Feedback
Technology
Advantages of CFB Technology
The CLC1605 Family of ampliers utilize current feedback
(CFB) technology to achieve superior performance. The
primary advantage of CFB technology is higher slew rate
performance when compared to voltage feedback (VFB)
architecture. High slew rate contributes directly to better
large signal pulse response, full power bandwidth, and
distortion.
CFB also alleviates the traditional trade-off between
closed loop gain and usable bandwidth that is seen with
a VFB amplier. With CFB, the bandwidth is primarily
determined by the value of the feedback resistor, Rf. By
using optimum feedback resistor values, the bandwidth
of a CFB amplier remains nearly constant with different
gain congurations.
When designing with CFB ampliers always abide by these
basic rules:
• Use the recommended feedback resistor value
• Do not use reactive (capacitors, diodes, inductors, etc.)
elements in the direct feedback path
• Avoid stray or parasitic capacitance across feedback
resistors
• Follow general high-speed amplier layout guidelines
• Ensure proper precautions have been made for driving
capacitive loads
Figure 1. Non-Inverting Gain Conguration with First
Order Transfer Function
VOUT
VIN
= − Rf
Rg
+1Eq. 2
1+Rf
Zo(jω)
VIN
VOUT
Zo*Ierr
Ierr
RL
Rf
x1
Rg
Figure 2. Inverting Gain Conguration with First Order
Transfer Function
CFB Technology - Theory of Operation
Figure 1 shows a simple representation of a current
feedback amplier that is congured in the traditional
non-inverting gain conguration.
Instead of having two high-impedance inputs similar to a
VFB amplier, the inputs of a CFB amplier are connected
across a unity gain buffer. This buffer has a high impedance
input and a low impedance output. It can source or sink
current (Ierr) as needed to force the non-inverting input
to track the value of Vin. The CFB architecture employs
a high gain trans-impedance stage that senses Ierr and
drives the output to a value of (Zo(jω) * Ierr) volts. With
the application of negative feedback, the amplier will
drive the output to a voltage in a manner which tries to
drive Ierr to zero. In practice, primarily due to limitations
on the value of Zo(jω), Ierr remains a small but nite
value.
A closer look at the closed loop transfer function (Eq.1)
shows the effect of the trans-impedance, Zo(jω) on the
gain of the circuit. At low frequencies where Zo(jω) is very
large with respect to Rf, the second term of the equation
approaches unity, allowing Rf and Rg to set the gain. At
higher frequencies, the value of Zo(jω) will roll off, and
the effect of the secondary term will begin to dominate.
The -3dB small signal parameter species the frequency
where the value Zo(jω) equals the value of Rf causing the
gain to drop by 0.707 of the value at DC.
For more information regarding current feedback
ampliers, visit www.exar.com for detailed application
notes, such as AN-3:
The Ins and Outs of Current
Feedback Ampliers
.
VOUT
VIN
=1+Rf
Rg
+1Eq. 1
1+Rf
Zo(jω)
VIN VOUT
Zo*Ierr
Ierr
Rg
RL
Rf
x1