Revisting multistage amplifier consists of Common Source-Common Base-Emitter Follower in cascading, I found the attached page of MPS-H85 PNP transistor that is proposed special for common base application.
Is any unique characteristic for CB amplifiers?
Surpriselly, when I used many transistors in simulation, I found very few that can give a good gain and low distortion in CB configuration even at 1MHz
Best Answer
The ability to give a better frequency response in common base configuration than in common emitter one was a characteristic typical of old BJTs constructed by using old semiconductor processes. To clarify the phenomenon, let us recall the formula of the common base current gain cutoff frequency \$f_\alpha\$ deduced by using the Giacoletto (Hybrid-Pi) model of the BJT: $$ f_\alpha = (\beta_o + 1)f_\beta\simeq \beta_o f_\beta=f_T.\label{1}\tag{1} $$ where \$\beta_o\$ is the ordinary low frequency common emitter current gain, \$f_\beta\$ is its cutoff frequency and \$f_T\$ is the ordinary transition frequency of the BJT, i.e. the frequency at which \$\beta(\omega)\simeq 1\$.
If we try to experimentally check the accuracy of \eqref{1}, we get the following relation instead: $$ f_\alpha\simeq (1+\lambda) f_T\label{2}\tag{1'} $$ where \$\lambda\$ is an empirical parameter which accounts for the differences between the two measured values of \$f_\alpha\$ and \$f_T\$ and varies from \$0.2\$ to \$1.0\$ when using BJTs made with different processes. The discrepancy between \eqref{1} and \eqref{2} is due to the fact that the hybrid-pi model is accurate only up to frequencies less than half of the \$f_T\$ and nevertheless not more than few hundreds \$\mathrm{MHz}\$.
So when in a datasheet you see stated that a RF BJT is "designed for common base (pre-)amplification", this is due to the fact that its constructive technology allows for nicer high frequency performances than its \$f_T\$ may suggest: this is most explicitly seen in old UHF germanium transistors as Siemens AF239: here the typical \$f_T\$ is \$\simeq700\mathrm{MHz}\$, but the device is accurately characterized as an amplifier at frequencies up to \$900\mathrm{MHz}\$, where it has a typical \$10.5\mathrm{dB}\$ power gain.
Notes
For a given BJT, the transition frequency \$f_T\$ can be extrapolated by measuring \$\beta(f)\$ for two sufficiently different frequencies \$f_1\$ and \$f_2\$, just above \$f_\beta\$, and finding the intersection of the \$10\mathrm{dB}/\text{decade}\$ slope line found by these two measures with the \$\beta=1\$ line in a Log-Log plot: and if you have a BJT with \$\beta_o\simeq 100\$, this means only doing two measures at frequencies \$f_1, f_2\sim f_T/100\$, getting rid of all risks of high frequency (setup induced) spurious oscillations caused by the necessity of dynamically short circuit the collector and the emitter of the device under test. This kind of measure can be quite easily arranged in order to easily test full production batches.
On the contrary, \$f_\alpha\$ can only be measured directly and this implies that the producer should put extreme cure and skill on the construction of its testbeds in order to avoid setup induced errors while keeping a fast measurement speed: thus, even if the common base current gain cutoff frequency would give a better characterization of HF performance of a BJT, it is almost never provided.
References
[1] J. R. Finch and J. C. Haenichen, "Annular - A new semiconductor device structure," 1963 International Electron Devices Meeting, Washington, DC, USA, 1963, pp. 98-98, doi: 10.1109/IEDM.1963.187416.
[2] Mario Gasparini and Domenico Mirri, Dispositivi e circuiti elettronici, 3rd Ed., Bologna: Edizioni Calderini, 1982, ISBN 8-8701-9427-2, ISBN-13 978-8-8701-9427-2.