The linked schematic in the first post will work, but its more of an example circuit, or a building block than something thats ready to be used. However, given that there is no 'global' feedback, just the local feedback of the transistors, with correct biasing a simple transistor circuit like that would be stupidly high bandwidth compared to an audio amp.
http://sound.westhost.com/project3a.htm is an example of a buildable AB power amplifier. It looks complex but it is actually pretty simple if you break it down into functional blocks.
Q1/Q2 is a long tail pair, which functions as a differential amplifier, the bases of the transistors are the inverting and non inverting inputs, just like on an op-amp, and the collector of Q1 is the output. Q3/R7/D1 make up a constant current sink for the LTP, with the LED being used as a voltage reference so the current would be (Vled-Vbe)/R7
Q4 provides current gain to supply current for the resistor string and the next set of transistors. Q9/VR1/R16 adjusts the DC operating point by affecting how much the transistors are turned on with a 0V input. The more the output transistors are on at a 0V input, the higher the idle current of the amplifier, but it also generally reduces crossover distortion.
Q5/Q7 and Q6/Q8 are the output drivers and output transistors, arranged to the schematic in the first post. Then the output signal goes though R5/R4 which divide the signal back down (C3 blocks DC, so only AC signals get gained up, DC signals have a much lower gain, which helps control DC offset) before feeding it back into the long tail pair to provide global feedback. R15/C7 is the zobel network, which helps stabilized the amp with inductive loads, and C+ and C- are just simple decoupling caps for high frequency noise. This would run off a unregulated transformer/rectifier, and the amplifier power supply rejection ratio (PSRR) is what keeps the output quiet.
Even if it doesn't all make sense, hopefully you got some new keywords to look for.