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Question

If Z × L is the total channel area and C'par is the total input parasitic capacitance, then for microwave performance the cut off frequency can be defined as :

(A) \(\dfrac{g_{m}}{2\pi\left(C'_{ca}+C'_{par}\right)}\)
(B) \(\dfrac{g_{m}}{2\pi C_{gs}}\)
(C) \(\dfrac{g_{m}}{2\pi C_{gd}}\)
(D) \(\dfrac{g_{m}}{2\pi\left(ZLC_{ox}+C'_{par}\right)}\)

Choose the most appropriate answer from the options given below :

This question was previously asked in
UGC NET 2023 Electronic Science Question Paper (13-Dec-2023) (Shift 1)
The correct answer is

(A) and (D) Only

 Statements (A) and (D) are the same expression written two ways — option 4 — and recognising that is the whole point of the question.

The cut-off frequency is the frequency at which the device's current gain falls to unity:

\(f_{T}=\dfrac{g_{m}}{2\pi C_{in}}\)

where \(C_{in}\) is the total capacitance the gate must drive.

Why (A) and (D) are identical. The channel capacitance is the oxide capacitance per unit area multiplied by the channel area:

\(C'_{ca}=Z\times L\times C_{ox}\)

Substituting that into (A) gives (D) exactly. The question defines \(Z\times L\) as the channel area in its own preamble, which is the hint that the two are meant to be recognised as one.

StatementCapacitance usedVerdict
(A)Channel + parasitic✓ Complete
(B)Cgs alone✗ Ignores the parasitics
(C)Cgd alone✗ The wrong capacitance entirely
(D)ZLCox + parasitic✓ The same as (A)

Why the parasitic term cannot be dropped, which rules out (B). The intrinsic channel capacitance is only part of what the gate drives. Overlap capacitance where the gate extends over the source and drain diffusions, fringing capacitance from the gate edges, and the capacitance of the interconnect all add to it — and as devices are scaled down the intrinsic part shrinks while the overlap and fringing parts do not shrink as fast, so the parasitics come to dominate. An expression that omits them overestimates \(f_{T}\) badly for a real microwave device.

Why (C) is wrong in principle. \(C_{gd}\) is the feedback capacitance from output back to input. It matters greatly — through the Miller effect it is multiplied by the gain when referred to the input — but it is not the input capacitance, and it appears in the maximum oscillation frequency \(f_{max}\) rather than in \(f_{T}\).

How to raise fT : shorten the channel, which raises \(g_{m}\) and lowers \(C_{ca}\) together, giving roughly \(f_{T}\propto1/L^{2}\) in the long-channel limit — which is why the drive to shorter gates has been as much about speed as about density.

Hence, the correct statements are (A) and (D).

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