2.2 Design of the proposed 24 GHz CMOS LNA
Fig. 2 shows the proposed low-power low noise-noise 24-GHz CMOS LNA. This LNA is implemented
using the 65 nm RF CMOS process. This process has been retained because of its good
low noise performance, the unity current gain cut-off frequency ($f_{T}$) of 120 GHz
and the maximum oscillation frequency ($f_{max}$) of 140 GHz. Successful integration
of the LNA at 24 GHz depends on minimizing parasitic capacitances and losses to maintain
adequate gain, designing with low voltage swing for low breakdown devices, and achieving
sufficient linearity required for low spectrally efficient and variable envelope modulation
scheme.
Providing a resistive input impedance of 50 Ω is one critical requirement of an LNA.
The 50 Ω termination is required mainly by the previously band select filter $L_{3}$
with parasitic capacitance and transistor $M_{1}$ is biased by adding parasitic capacitance
to the input impedance matching. The third-order non-linear transconductance coefficient
$g_{m3}$ is performed by gate-drain and gate-source capacitances of basic components,
and it reduces linearity performance. To improve noise figure and linearity, we propose
a CG (common gate) NMOS-PMOS inverter scheme for the cascode LNA as a linearizer.
The proposed linearization method accepts NMOS and PMOS transistors into common gate
configuration with the second-order and third-order nonlinearity to improve the linearity
performance (9,10).
Fig. 3. Ideal view of the inverter stage.
To reach very low third-order distortion and low power, it is very important to reduce
the second-order and third-order nonlinearities. It is very important to minimize
or cancel $g_{m2}$ and $g_{m3}$ to decrease the third-order intermodulation distortion
and to improve IIP3 (third-order input intercept point). The inductor $L_{2}$, and
the parasitic capacitances at the drain of $M_{2}$ and $M_{4}$ form provide broadband
network.
Let’s consider drain current $I_{d_{total}}$ of $M_{1}$ through the $M_{2}$ and $M_{3}$
transistors as shown in Fig. 3. For $M_{4}$, $V_{g4}$ = $V_{dd}$, $V_{s4}$ = $V_{d3}$, $I_{d4}$ = ($V_{dd}$-$V_{d4}$)/$R_{out}$,
$I_{d4}$ = $I_{d3}$ and $I_{d4}$ = 0, since $M_{1}$ is connected to the ground through
capacitor $C_{1}$ for $d_{1}$ = 0. From KCL, $I_{s3}$ = $d_{1}$ + $I_{s2}$, $I_{s2}$
= $I_{s3}$, $V_{dd}$-$I_{d4}$$R_{out}$-$V_{ds4}$-$V_{ds3}$ = $V_{ds2}$, and $V_{dd}$
= $I_{d4}$$R_{out}$ + $V_{d4}$, and we obtain Eqs. (1)-(3).
Since $V_{gs3}$ is a function of $V_{gs2}$, it is expressed to power series of $V_{gs2}$
as expressed by Eq. (4).
where $C_{i}S$ are generally frequency dependent. In practice, the π-network cancels
the effects of $c_{2}$ and $c_{3}$ at the frequency of interest. To find the coefficient
$C_{i}S$, we should solve the equation after expanding $I_{d_{total}}$ as a power
series of $V_{gs2}$ and replacing it with Eq. (4), and then we obtain Eq. (5) (4).
where $g_{m1}$, $g_{m2}$ and $g_{m3}$ are the main transconductance, second-order
and third-order nonlinearity coefficients, respectively (4). The second order nonlinearity is canceled in output due to cut off phase signal
by NMOS and PMOS. The optimum biasing is used to obtain a high IIP3 by reducing the
total $g_{m3}$, and the IIP3 can be calculated by Eq. (6) (8).
The $g_{m3,d3}$ changes from positive to negative when the transistor moves from weak
to strong inversion region. In other words, by changing gate bias voltage of PMOS
transistor, the parameter $C_{1}$ can be varied. It can be deduced from Eq. (4).
2.3 Small Signal Analysis
Fig. 4 shows simplified high-frequency small signal model of cascade topology with inductively
degenerated scheme for the LNA. By applying the KCL at source node, we obtain Eq. (7).
where W and L represent the transistor’s width and length, respectively, and $C_{ox}$
is gate capacitance per unit area.
By applying the KCL at drain node $d_{1}$ of $M_{1}$, we get Eqs. (8)-(13).
Fig. 4. High-frequency small signal model for the LNA.
Now let’s analyze the input impedance of the cascade topology using inductive source
degeneration technique. The transistor $M_{1}$ is replaced by a high-frequency small-signal
model consisting of gate-source capacitor $C_{gs1}$, gate-drain capacitor $C_{gd1}$,
$g_{m1}$ and source degeneration inductor $L_{1}$. By applying the KCL at source node
$s_{1}$, we also obtain Eqs. (14)-(16).
For AC analysis, $C_{in}$ can be shorted, and by neglecting the term $V_{d1}$ and
$V_{g1}$, and using Eqs. (14) and (15), we obtain Eqs. (17) and (18). $V_{in}$=$V_{s1}$ by inserting this value and rearranging, so the input impedance
$Z_{in}$ is expressed by Eq. (19).
where $Z_{in}$ and output impedance $Z_{out}$ of each stage are optimized at 24 GHz,
and we can simplify Eq. (19) into Eq. (20).
where $X_{L1}$ and $X_{C}=\frac{1}{j w\left(\frac{c_{g d_{1}} c_{g s 1}}{c_{g d_{1}}+c_{g
s 1}}\right)}$
By assuming $r_{0}=∞$, we get the simplified form of $Z_{in}$as shown below.
On deactivating the input source $V_{in}$ and applying KCL at the output node, we
can get output impedance $Z_{out}$. At the input node $s_{1}$, we also obtain Eqs. (22) and (23).
By applying KCL at the output node $d_{4}$, inserting $V_{d4}$=$V_{out}$, and rearranging,
we get Eqs. (24)-(26).
where $G_{\text {out}}=\frac{1}{R_{\text {out}}+j w L_{\text {out}}}$, by assuming
$r_{0}=∞$, we obtained the simplified form of $Z_{out}$ as shown in Eq. (28).
Now let’s get voltage gain. From the voltage and current of transistors $M_{1}$, $M_{2}$,
$M_{3}$ and $M_{4}$, we also obtain Eqs. (29)-(35).
By rearranging Eqs. (29) and (35), we get Eqs. (36)-(38).
The voltage gain of the LNA should be much larger to reduce the noise figure. From
high-frequency small signal model as shown in Fig. 4, we also obtain Eqs. (39)-(41).
If we assume that $r_{o1}=r_{o2}=r_{o3}=r_{o4}=r_{o}$, voltage gain is expressed by
Eq. (42).
By assuming $r_{0}=∞$, therefore we get Eq. (43).
Eq. (43) is also simplified as described in Eqs. (44) and (45).
where $X_{Lout}$= $j_{ω}L_{out}$, $X_{L3}$ = $j_{ω}L_{3}$ and $G_{T}$ = $g_{ml}g_{m3}$.
The noise figure ($NF$) in LNA determines the inherent LNA noise added to the desired
or wanted signal during the process of amplification. $NF$ is a function of source
admittance looking into the input terminal of the two-port network. To achieve the
$NF_{min}$, an optimum source admittance that results in minimum noise figure, namely
$Y_{opt}$, should be introduced to the network. The expressions for $NF_{min}$ and
$Y_{opt}$ can be derived for a MOS device by considering a two-port network model
for the MOS device. In this model the gate-source terminal is the input port, and
the drain-source terminal is the output port. When source admittance presented to
transistor ($Y_{s}$) is matched at $Y_{opt}$, the NF has almost $NF_{min}$ (11,12).
Fig. 5. Die photograph of the proposed LNA.