<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">WJET</journal-id><journal-title-group><journal-title>World Journal of Engineering and Technology</journal-title></journal-title-group><issn pub-type="epub">2331-4222</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/wjet.2024.121005</article-id><article-id pub-id-type="publisher-id">WJET-130760</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject><subject> Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Design of a Low Power Low-Noise Amplifier with Improved Gain/Noise Ratio
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Raja</surname><given-names>Mahmou</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Khalid</surname><given-names>Faitah</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Engineering Sciences and Technology Laboratory (LABSTI), Private University of Marrakech (UPM), Marrakech, Morocco</addr-line></aff><aff id="aff2"><addr-line>Laboratory of Engineering Sciences for Energy (LabSIPE), National School of Applied Sciences (ENSAJ), El Jadida, Morocco</addr-line></aff><pub-date pub-type="epub"><day>27</day><month>12</month><year>2023</year></pub-date><volume>12</volume><issue>01</issue><fpage>80</fpage><lpage>91</lpage><history><date date-type="received"><day>29,</day>	<month>November</month>	<year>2023</year></date><date date-type="rev-recd"><day>23,</day>	<month>January</month>	<year>2024</year>	</date><date date-type="accepted"><day>26,</day>	<month>January</month>	<year>2024</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  This work details the development of a broad-spectrum LNA (Low Noise Amplifier) circuit using a 65
   
  nm CMOS technology. The design incorporates an inductive degeneracy circuit, employing a theoretical approach to enhance gain, minimize noise levels, and uphold low power consumption. The progression includes a shift to a cascode structure to further refine LNA parameters. Ultimately, with a 1.8
   
  V bias, the achieved performance showcases a gain-to-noise figure ratio of 16 dB/0.5 dB, an IIP3 linearity at 5.1 dBm, and a power consumption of 3 mW. This architecture is adept at operating across a wide frequency band spanning from 0.5 GHz to 6 GHz, rendering it applicable in diverse RF scenarios.
 
</p></abstract><kwd-group><kwd>LNA</kwd><kwd> Degeneracy</kwd><kwd> Noise Figure</kwd><kwd> Linearity</kwd><kwd> Power Consumption</kwd><kwd> Gain</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In an RF reception chain, the Low Noise Amplifier (LNA) plays a critical role, since it brings the useful signal from the receiving antenna to a high-level signal that will be correctly processed by the blocks located downstream of the RF chain. Positioned upstream (<xref ref-type="fig" rid="fig1">Figure 1</xref>), it requires higher gain, and its noise factor significantly determines the overall noise factor of the system.</p><p>When designing LNAs, four main types exist regardless of the technology used [<xref ref-type="bibr" rid="scirp.130760-ref2">2</xref>] : resistance termination, resistive feedback, 1/gm termination, and inductive degeneration. Unlike other architectures, the last one adapts perfectly without adding noise to the system.</p><p>Recent research indicates a predominant preference for employing the LNA architecture with inductive degeneration, for example: [<xref ref-type="bibr" rid="scirp.130760-ref3">3</xref>] focuses on designing</p><p>for high linearity while maintaining low power consumption in biomedical instruments, the objective of this following work [<xref ref-type="bibr" rid="scirp.130760-ref4">4</xref>] is to enhance the gain without deterioration in other parameters by cascode LNA using an extra capacitor, another study centers on a PVT compensation to reduce the sensitivity of the circuit to PVT variations [<xref ref-type="bibr" rid="scirp.130760-ref5">5</xref>] , then a novel configuration in an inductor-less ultra-wideband LNA for cognitive radio systems [<xref ref-type="bibr" rid="scirp.130760-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.130760-ref7">7</xref>] proposes a technique to enhance linearity for large input signals with a new composites transistor, then [<xref ref-type="bibr" rid="scirp.130760-ref8">8</xref>] uses the Advanced Compact MOSFET (ACM) model alongside a Lookup <xref ref-type="table" rid="table">Table </xref>(LUT) to encompass transistor behavior across various operational modes, enabling seamless integration into digital computing environments.</p><p>The present work utilizes the inductive degeneracy source in the LNA topology as a reference by adopting a theoretical approach that allows for an adjustment between gain and noise figure while maintaining low power consumption. The LNA designs developed in this paper are based on 65 nm CMOS technology, beginning with a simple structure and then refined through a second assembly employing a two-stage structure.</p></sec><sec id="s2"><title>2. Methodology for Enhancing Gain-to-Noise Ratio</title><sec id="s2_1"><title>2.1. Circuit Gain</title><p>The LNA structure with inductive degeneration, being illustrated by <xref ref-type="fig" rid="fig2">Figure 2</xref>, whose general gain formula is expressed by Equation(1):</p><p>G = V o u t V i n (1)</p><p>The signal V i n being received from the antenna, the gain (G) increases if the amplitude of the signal V O U T increases. According to the <xref ref-type="fig" rid="fig2">Figure 2</xref>: knowing that V D S is the voltage between the drain and the source of the MOSFET transistor, and that V D S is the potential of its source:</p><p>V o u t = V D S + V S (2)</p><p>The CMOS works in the ohmic zone then [<xref ref-type="bibr" rid="scirp.130760-ref9">9</xref>] :</p><p>V D S = R o n I D S where R o n = 1 μ n c O X W L ( V G S − V t n ) (3)</p><p>With Ids is the Drain-Source current</p><p>The voltage V S is across the terminals of the inductance L<sub>s</sub>, I<sub>s</sub> represents the current flowing through it, where I<sub>g</sub> represents the gate G current (<xref ref-type="fig" rid="fig2">Figure 2</xref>):</p><p>V s = L s ω I s (4)</p><p>I S = I G + I D S (5)</p><p>And</p><p>I G = V i n ( L G + L S ) ω (6)</p><p>According to Equation (1), and knowing that the input signal V i n (<xref ref-type="fig" rid="fig2">Figure 2</xref>) is fixed by the antenna, increasing the gain G is directly linked to increasing the amplitude of the output signal V O U T , since this latter is the sum of the voltages V D S and V S (Equation (2)). Therefore, an enhancement in V O U T amplitude is attributed to the improved V D S and V S .</p><p>Depending on the chosen technology (CMOS 65 nm), the length L of the MOSFET channel is set at 65 nm, while keeping the other parameters fixed, the choice of a relatively wide MOSFET channel (W) will improve the V D S voltage amplitude.</p><p>Regarding the voltage V S :</p><p>V S = L S ω I S (7)</p><p>From Equation (6) and Equation (7), it’s enough to fix the impedance L<sub>g</sub> and increase L<sub>s</sub>, in other words; current Is is increased if I<sub>g</sub> is increased. We can keep (L<sub>s</sub> + L<sub>g</sub>) low; if we set Ls to a value, we can minimize the value of L<sub>g</sub> (L<sub>s</sub> is fixed, L<sub>g</sub> is small, W is large).</p><p>We can keep the sum L<sub>s</sub> + L<sub>g</sub> small; if we fix L<sub>s</sub> to a value, we can minimize the value of L<sub>g</sub> (L<sub>s</sub> is fixed, L<sub>g</sub> is small, W is large).</p></sec><sec id="s2_2"><title>2.2. Technique for Enhancing Gain</title><p>In order to improve the gain of the chosen LNA circuit, we can add an impedance Z in series (<xref ref-type="fig" rid="fig3">Figure 3</xref>), which will improve the V O U T voltage relative to <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>Since V i n is fixed by the antenna, if we increase V O U T , according to <xref ref-type="fig" rid="fig3">Figure 3</xref>, V D S will be:</p><p>V D S = R o n I D S + | Z | I D S (8)</p><p>In terms of noise, it’s crucial to study the impact of noise associated with the C, L, and R components of impedance Z through simulation. Ideally, introducing only a resistor R whose noise impact is comparatively lower than that of L and C would be preferable.</p></sec><sec id="s2_3"><title>2.3. Technique for Noise Minimization</title><p>The noise figure (NF) is generally represented by formula (Equation (9)), N O U T represents the amplitude of the noise signal at the output, N i n is the noise at the input, and G represents the gain of the circuit:</p><p>N F = N o u t N i n ⋅ 1 G (9)</p><p>N i n depends on the V i n input signal, according to Equation (9), to reduce the noise figure we can increase the gain G while reducing N O U T , to do this, we can adjust the parameters of the MOSFET and the impedances L<sub>s</sub> and L<sub>g</sub> within the circuit.</p><p>Generally, there are three types of noise in a MOSFET transistor [<xref ref-type="bibr" rid="scirp.130760-ref9">9</xref>] : 1/f noise, noise induced in the grid: which can be neglected because the Cgs capacity is quite low, and noise of the drain current: in the ohmic zone the latter has no great effect.</p><p>According to Equation (10) [<xref ref-type="bibr" rid="scirp.130760-ref9">9</xref>] , to have fairly a low 1/f noise, simply increasing the value of W slightly, this method has no influence either on the gain or on the power consumed by the circuit.</p><p>i &#175; n f 2 = K f g m 2 W L C o x 2 Δ f (10)</p></sec></sec><sec id="s3"><title>3. Simulation Results</title><sec id="s3_1"><title>3.1. Basic Inductive Degeneration Circuit</title><p>The M1 and M2 MOSFETs in <xref ref-type="fig" rid="fig4">Figure 4</xref> are chosen from the BSIM4 65 nm model, the channel width of NMOS M1 is 10 μm, The voltage and bias resistance are respectively set at 1.8 V and 1 kΩ. The impedances L<sub>g</sub> and L<sub>s</sub> are respectively equal to 0.5 nH and 10 nH.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> and <xref ref-type="fig" rid="fig6">Figure 6</xref> illustrate the signals V i n ( t ) and V O U T ( t ) :</p><p>From <xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref>: at 1.9 GHz (cellular telecommunications for example), the simulation leads to a gain G of 13.7 dB, a noise figure NF equal to 1.6 dB and the 3rd order interception point (IIP3) corresponds to 2.4 dBm.</p><p>From <xref ref-type="fig" rid="fig9">Figure 9</xref>, the power consumption of the circuit will be around 3 mW ( V d d = 1.8 V I D C = 1.524 &#160;mA ).</p></sec><sec id="s3_2"><title>3.2. Inductive Degeneration Circuit in Cascode Configuration</title><p>As illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>0, this structure allows both on-board adaptation and low noise, additionally, share the bias current and thus increase efficiency [<xref ref-type="bibr" rid="scirp.130760-ref2">2</xref>] .</p><p>Maintaining the same values of frequency, amplitude, and DC component of the input signal V i n as mentioned in the previous paragraph. Thus, by sharing the same bias current (R2 = 1 kΩ) between both MOSFETs 1 and 3 (chosen to be identical with L = 65 nm and W = 10 um). This allowed, following simulations in various modes (using Agilent ADS tool),to observe the responses: Figures 11-15, respectively represent the time-domain responses of signals V i n and V o u t , the gain and noise figure, the third-order intercept point, and the power consumed by the cascoded LNA circuit.</p></sec><sec id="s3_3"><title>3.3. Comparison of Results for the Two Selected Structures</title><p>The table below (<xref ref-type="table" rid="table">Table </xref>1) summarizes the values obtained in simulation for these two different proposals, compared with the typical characteristics of an LNA circuit [<xref ref-type="bibr" rid="scirp.130760-ref10">10</xref>] . It is noticeable that the cascode inductive degeneration circuit maintains a low power consumption and exhibits both a better linearity and a good gain/noise ratio.</p></sec></sec><sec id="s4"><title>4. Comparison with Recent Works</title><p>The table below (<xref ref-type="table" rid="table">Table </xref>2) summarizes the simulation results of the last proposed circuit (proposed work 2) and compares them, within a similar frequency range, with those of some more recent achievements, including the typical characteristics [<xref ref-type="bibr" rid="scirp.130760-ref10">10</xref>] of LNA, and the work done by the simple inductive degeneration LNA (Proposed work 1) (section 2, paragraph 1). Our introduced LNA demonstrates notably: an elevated IIP3 (thanks to the cascoded configuration), and among the best voltage gains, a minimal noise figure. Positioning it as a superior choice for low-noise, controlled consumption, high-gain, and linearity receiver designs.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table">Table </xref>1</label><caption><title> Summary of results compared with typical values</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Reference</th><th align="center" valign="middle" >Technology</th><th align="center" valign="middle" >RF (GHz)</th><th align="center" valign="middle" >Gmax (dB)</th><th align="center" valign="middle" >NFmin (dB)</th><th align="center" valign="middle" >IIP3 (dBm)</th><th align="center" valign="middle" >P (mW)</th><th align="center" valign="middle" >Impedance (Ω)</th></tr></thead><tr><td align="center" valign="middle" >Typical characteristics [<xref ref-type="bibr" rid="scirp.130760-ref10">10</xref>]</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−10</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >LNA inductive degeneration</td><td align="center" valign="middle" >65 nm</td><td align="center" valign="middle" >0.5 - 6</td><td align="center" valign="middle" >14.7</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >2.4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >LNA inductive degeneration (Cascoded)</td><td align="center" valign="middle" >65 nm</td><td align="center" valign="middle" >0.5 - 5.4</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5.1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >50</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table">Table </xref>2</label><caption><title> Summary of results compared with recent works</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Reference (1<sup>st</sup> Author)</th><th align="center" valign="middle" >Year</th><th align="center" valign="middle" >Technology</th><th align="center" valign="middle" >Frequency (GHz)</th><th align="center" valign="middle" >Gain (dB)</th><th align="center" valign="middle" >NF (dB)</th><th align="center" valign="middle" >IIP3 (dBm)</th><th align="center" valign="middle" >P (mW)</th><th align="center" valign="middle" >Vdd (V)</th><th align="center" valign="middle" >S/M</th></tr></thead><tr><td align="center" valign="middle" >Proposed Work 2</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >65 nm</td><td align="center" valign="middle" >1.9 (0.5 - 6)</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >5.1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.8</td><td align="center" valign="middle" >S</td></tr><tr><td align="center" valign="middle" >Proposed Work 1</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >65 nm</td><td align="center" valign="middle" >1.9 (0.5 - 6)</td><td align="center" valign="middle" >13.7</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >2.4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.8</td><td align="center" valign="middle" >S</td></tr><tr><td align="center" valign="middle" >Typical [<xref ref-type="bibr" rid="scirp.130760-ref10">10</xref>]</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >-10</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Didem Erol As [<xref ref-type="bibr" rid="scirp.130760-ref3">3</xref>]</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >40 nm</td><td align="center" valign="middle" >2.4</td><td align="center" valign="middle" >11.5</td><td align="center" valign="middle" >3.38</td><td align="center" valign="middle" >-0.7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >S</td></tr><tr><td align="center" valign="middle" >F. Gozalpour [<xref ref-type="bibr" rid="scirp.130760-ref4">4</xref>]</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >180 nm</td><td align="center" valign="middle" >2.4</td><td align="center" valign="middle" >15.5</td><td align="center" valign="middle" >2.42</td><td align="center" valign="middle" >0.84</td><td align="center" valign="middle" >3.2</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >S</td></tr><tr><td align="center" valign="middle" >S.Nejadhasan [<xref ref-type="bibr" rid="scirp.130760-ref5">5</xref>]</td><td align="center" valign="middle" >2022</td><td align="center" valign="middle" >65 nm</td><td align="center" valign="middle" >2.32</td><td align="center" valign="middle" >15.4</td><td align="center" valign="middle" >2.3</td><td align="center" valign="middle" >−14.05</td><td align="center" valign="middle" >0.57</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >S</td></tr><tr><td align="center" valign="middle" >M. M. Farahani [<xref ref-type="bibr" rid="scirp.130760-ref6">6</xref>]</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >180 nm</td><td align="center" valign="middle" >0.05 - 10.8</td><td align="center" valign="middle" >10.6</td><td align="center" valign="middle" >2.24</td><td align="center" valign="middle" >−2.3</td><td align="center" valign="middle" >6.12</td><td align="center" valign="middle" >1.8</td><td align="center" valign="middle" >Post-Layout</td></tr><tr><td align="center" valign="middle" >W. Liu [<xref ref-type="bibr" rid="scirp.130760-ref11">11</xref>]</td><td align="center" valign="middle" >2022</td><td align="center" valign="middle" >0.25 &#181;m</td><td align="center" valign="middle" >4 - 15</td><td align="center" valign="middle" >17 - 21</td><td align="center" valign="middle" >1.6 - 2.1</td><td align="center" valign="middle" >&lt;−7</td><td align="center" valign="middle" >266.5</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >Post-Layout</td></tr><tr><td align="center" valign="middle" >E. Salighe [<xref ref-type="bibr" rid="scirp.130760-ref7">7</xref>]</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >0.18 &#181;m</td><td align="center" valign="middle" >0.85 - 0.95</td><td align="center" valign="middle" >11.9</td><td align="center" valign="middle" >2.46</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >5.4</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >Post-Layout</td></tr><tr><td align="center" valign="middle" >G. Britton [<xref ref-type="bibr" rid="scirp.130760-ref8">8</xref>]</td><td align="center" valign="middle" >2022</td><td align="center" valign="middle" >28 nm</td><td align="center" valign="middle" >2*<sup> </sup></td><td align="center" valign="middle" >~17*</td><td align="center" valign="middle" >~3*</td><td align="center" valign="middle" >~−1*</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >Post-Layout</td></tr><tr><td align="center" valign="middle" >S. Babak Hamidi [<xref ref-type="bibr" rid="scirp.130760-ref12">12</xref>]</td><td align="center" valign="middle" >2023</td><td align="center" valign="middle" >0.18 &#181;m</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >31</td><td align="center" valign="middle" >3.6</td><td align="center" valign="middle" >−11</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >M</td></tr><tr><td align="center" valign="middle" >BM. Jafari [<xref ref-type="bibr" rid="scirp.130760-ref13">13</xref>]</td><td align="center" valign="middle" >2020</td><td align="center" valign="middle" >65 nm</td><td align="center" valign="middle" >1.4 - 4.5</td><td align="center" valign="middle" >25.7</td><td align="center" valign="middle" >2.7</td><td align="center" valign="middle" >10.1</td><td align="center" valign="middle" >0.87</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >S</td></tr><tr><td align="center" valign="middle" >M. Mudavath [<xref ref-type="bibr" rid="scirp.130760-ref14">14</xref>]</td><td align="center" valign="middle" >2020</td><td align="center" valign="middle" >45 nm</td><td align="center" valign="middle" >1-5</td><td align="center" valign="middle" >32.5</td><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >3.74</td><td align="center" valign="middle" >16.9</td><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >S</td></tr></tbody></table></table-wrap><p>S: Simulation Result; M: Measurement Result; *: observed results from simulation figures.</p></sec><sec id="s5"><title>5. Conclusions</title><p>The theoretical approach focuses on optimizing LNA voltage gain by introducing an impedance Z in series with the MOSFET’s Drain and adjusting parameters based on characteristic equations. Managing noise figure involves addressing prevalent noise types, particularly 1/f noise linked to MOSFET parameters (W and L). Precision tuning of these parameters effectively mitigates this noise.</p><p>The initial simulation of a simple inductive degeneration circuit demonstrated the effectiveness of the adopted technique. This led to a subsequent transition towards an advanced cascode structure to consider linearity. The comparative simulation of the final circuit with other studies showcased the performance advantages of this approach, particularly in terms of gain-to-noise ratio (16/0.5 dB), linearity (5.1 dBm), and power consumption (3 mW). As a result, this proposed design demonstrates applicability across a wide frequency band (0.5 - 6 GHz).</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Mahmou, R. and Faitah, K. (2024) Design of a Low Power Low-Noise Amplifier with Improved Gain/Noise Ratio. 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