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CMOS Inverter Design and Analysis Using TSMC180nm

Description

The motive of this project is to familiarize users with the LTspice tool and experiment with the working of a CMOS inverter, exploring various parameters associated with it. The project utilizes the TSMC180nm model file and begins by analyzing MOSFET models. The goal is to understand different plots and extract important parameters related to MOSFETs. Subsequently, the project progresses to the analysis of a CMOS inverter, where the aim is to obtain relevant plots and extract key parameters associated with its performance.

1. MOSFET Models Analysis

1.1 NMOS Analysis

In this section, I start with our analysis of MOSFET models present in tsmc180nm. Here, Vdd=1.8V and L=180nm as in the case of digital circuits Length can be taken as a minimum, and width is generally taken greater than or equal to 1.5 times of length. So, first I am plotting Id vs vgs curve, and here is the LT spice setup for that.

setup_idvsvgs_nmos

The curve is plotted between Id vs vgs by sweeping vgs from 0 to 1.8Vfor different values of vds, for this use the commands shown in the schematic.

idvsvgs_curve_nmos

This shows us that the threshold value is between 600mV to 700mV but we are going to calculate it using setup also. Also from this curve, we can obtain the gm transconductance curve for NMOS, by editing the command in the waveform viewer in LT Spice as d(Id(M2)).The deriv() function takes the derivative with respect to the independent variable present at the current simulation. From the definition of Gm we are aware that it is dId/dVgs.

gm_nmos

Now, I am plotting Id vs vds curve, and here is the LT spice setup for that.

image

The curve is plotted between Id vs vds by sweeping vds from 0 to 1.8Vfor different values of vgs, for this use the commands shown in the schematic. and from this curve, we can obtain the ro_nmos for NMOS, by editing the command in the waveform viewer in LT Spice as d(Id(M2)).The deriv() function takes the derivative with respect to the independent variable present at the current simulation. From the definition of ro we are aware that it is dId/dVds. and now, we will calculate the Threshold voltage for NMOS vtn here is the LT Spice setup for that.

vtn_setup

Here, we have assumed a reasonable value of vgs ( greater than vtn) and using the spice error log we will find vtn and here we are taking width = 0.36u. Now, you can view the spice error log file in LT Spice by using ctrl + L and can see vtn value.

vtn_value

Hence, we now have all the important values we need. The same can be done for a PMOS.

pmos setup

The motive is the same, but especially to extract the value of the Aspect ratio for which the current is the same in both NMOS and PMOS. I have done some experimentation and found that at W/L of PMOS = 4 * (Aspect ratio of NMOS), the current value is pretty close. So, we found the NMOS had a current of 9.1 microamps while PMOS had a current of 9.5 microamps (both at |Vgs| = 0.65V). (NOT BAD!!)

1.2 STRONG O AND WEAK 1

What does the above mean? Look at the schematic and waveforms below, strong0weak1_nmos_setup strong0weak1_nmos

Here we can see that when a square wave is applied to the input of NMOS when it is logic LOW(0V), the output goes to HIGH(1.8V). But when the input is logic HIGH(1.8V), the output goes to a value that is much larger than 0V. This is because when Vgs is 1.8V, the NMOS is in the linear region. This is where the MOSFET acts as a voltage-controlled resistor. At this point, the output is connected to a Voltage Divider Configuration. That is the output takes the value which is defined by the voltage across the resistance of the MOSFET. Hence, NMOS can transmit STRONG 0, but not STRONG 1.

1.3 STRONG 1 AND WEAK 0

here also let us look at some schematic and waveforms in LT Spice

strong1weak0pmos_setup strong1weak0pmos Therefore, both NMOS and PMOS alone do not serve as effective inverters. Various configurations were considered, but ultimately, one emerged as the most popular circuit design using MOSFETs, known as a CMOS configuration.

2. CMOS INVERTER

2.1. Why Choose CMOS Circuits

In the preceding section, we made an interesting observation: neither NMOS nor PMOS alone can effectively generate both HIGH and LOW values. However, they exhibit a complementary relationship. This insight led to the concept of combining them. Leveraging PMOS as a Strong 1, we position it between VDD and Vout, while NMOS, functioning as a STRONG 0, is situated between Vout and GND. By doing so, each can serve as a load for the other transistor, ensuring they are never ON simultaneously (or are they?). This arrangement is known as the Complementary Metal Oxide Semiconductor (CMOS) Configuration, representing the simplest circuit called the CMOS Inverter.

cmosinv

CMOS Circuits typically involve a network divided into two segments: the upper section is referred to as the pull-up network and the lower half as the pull-down network. The former incorporates P-channel MOSFETs, while the latter employs N-channel MOSFETs. The rationale is straightforward: as one transistor turns on, the other turns off, eliminating the issue of a resistive path to the ground and minimizing voltage division (at least not significantly). This arrangement allows for easily achieving both Strong High and Strong Low outputs from the same network. The pull-up provides a low-resistance path to VDD, while the pull-down offers a low-resistance path to GND.

punand pdn

2.2. CMOS Inverter Design and Analysis using LT Spice

Before moving further, First, let us understand What is an Inverter? So, In layman's terms, We can say that that inverter is the circuit that performs the NOT function or we can say that inverts and it is characterized practically by various parameters such as Noise Margin and speed. Now, here I have designed an inverter in LT Spice, as we had already calculated the width of PMOS as 4 times the width of NMOS using that I have taken W_NMOS=0.36u and W_PMOS=1.44u. Here is its schematic in LT Spice.

cmosinv_sch

2.2.1 DC Analysis and Important Design Parameters

We are going to plot the Voltage Transfer Characteristics (VTC) curve for the inverter using DC analysis. Here we sweep the Vin from 0V to 1.8V and plot the vin and vout. using the following command .dc vin 0 1.8 1m Here is the resulting waveform:

vtc_inv

Here we can see from the curve that vin=vout at 0.903V which is approximately equal to vdd/2 later we will see that it is termed as the switching threshold of an inverter. Now let us understand, What other parameters can be calculated using this curve:

vtc_book

we can see from the above picture that the inverter has five regions of operation. Also, refer to the below picture:

nm_inv

Let us understand the important parameters of this device that are based on its VTC curve.

VOH - Maximum output voltage when it is logic '1'. VOL - Minimum output voltage when it is logic '0'. VIH - Maximum input voltage that can be interpreted as logic '0'. VIL - Minimum input voltage that can be interpreted as logic '1'. Vth - Inverter Threshold voltage (Switching Threshold which we have already calculated to be 0.903V using VTC) The above five are critical for an Inverter and can be seen on the VTC curve of an inverter. One thing to point out now would be,

Vth should be at a value of VDD/2 for maximum noise margins

Now, using the property when d(vout)/d(vin) = -1 we can calculate all these parameters by plotting the vout and then applying d( ) on it and using the marker for measuring in LT Spice.

vil_and_vih

From the above graph, VIL=0.78V and VIH=1.01V are calculated and now, using these values from VTC we can calculate VOL and VOH.

vol_and_voh

from the graph, we calculated VOL=0.1V and VOH=1.69V.

Now, Next is Noise Margins. Noise margins are defined as the range of values for which the device can work noise-free or with high resistance to noise. This is an important parameter for digital circuits, since they work with a set of specific values(2 for binary systems), so it becomes crucial to know what values of the voltages can sustain for each value. This range is also referred to as Noise Immunity. There are two such values of Noise margins for a binary system: NML(Noise Margin for Low) = VIL - VOL NMH(Noise Margin for HIGH) = VOH - VIH

So for our calculated values, the device would have, NML = 0.682V and NMH = 0.68V.

In our case, they are very accurate and equal but there can be cases where they are not the same, and as Vth can be not near to vdd/2. Here is the summary of our results.

Parameter Value
Vth 0.903V
VIL 0.78V
VIH 1.01V
VOL 0.1V
VOH 1.69V

Credits

This work is also the part of simulation tasks given to us in our VLSI Design and Technology course in the fifth semester and also in LT Spice Lab.

I also want to acknowledge Youtuber @whyRD whose videos served as a valuable resource when I started learning this open-source EDA software at the start year of college.