S.M. Alavi
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19 records found
1
The design and implementation of a test system are described, along with the development of an occupancy grid map capable of representing data from both LiDAR and ultrasonic sensors. To enhance the accuracy and reliability of the environmental representation, the occupancy grid map incorporates an inverse sensor model in combination with Bayesian statistical methods. ...
The design and implementation of a test system are described, along with the development of an occupancy grid map capable of representing data from both LiDAR and ultrasonic sensors. To enhance the accuracy and reliability of the environmental representation, the occupancy grid map incorporates an inverse sensor model in combination with Bayesian statistical methods.
In the initial chapters, the overall architecture of the VNA is outlined, with specific attention to the power budget and system requirements. The RF generation principles are examined, and a range of RF generators are tested to ensure they meet the signal quality standards, such as spurious emissions and harmonic content. The performance of various RF mixers is also evaluated and found to be sufficient for the RF system.
Experimental results demonstrate the system’s capability to measure the S21 parameter of a resonator cavity, comparable to commercial VNAs. This validates that the RF system meets the specified requirements and can be effectively used in quantum research.
Future work suggested includes the measurement of generator frequency/phase stability over time and exploring the feasibility of implementing power sweeps to enhance the system’s functionality. The findings of this thesis contribute to the development of accessible and flexible tools for quantum technology research, promoting further advancements in the field. ...
In the initial chapters, the overall architecture of the VNA is outlined, with specific attention to the power budget and system requirements. The RF generation principles are examined, and a range of RF generators are tested to ensure they meet the signal quality standards, such as spurious emissions and harmonic content. The performance of various RF mixers is also evaluated and found to be sufficient for the RF system.
Experimental results demonstrate the system’s capability to measure the S21 parameter of a resonator cavity, comparable to commercial VNAs. This validates that the RF system meets the specified requirements and can be effectively used in quantum research.
Future work suggested includes the measurement of generator frequency/phase stability over time and exploring the feasibility of implementing power sweeps to enhance the system’s functionality. The findings of this thesis contribute to the development of accessible and flexible tools for quantum technology research, promoting further advancements in the field.
6G Beamforming Antenna-in-Package
Improving Efficiency using Direct Impedance Matching
This work demonstrates a novel analysis of PA-antenna co-design at 96 GHz using a 8x8 cavity-backed dual-polarized pin-fed stacked patch array. Two versions of this antenna array are designed in Ansys HFSS, one with an antenna impedance of 50 Ω, the benchmark, and one with a lower impedance of 25 Ω. Both designs are made on a custom package laminate stack-up and are compatible with pin-fed AiP technology. Using Keysight ADS, the antenna designs are co-simulated with an RF front-end circuit comprised of a single tone AC signal, ideal 1-64 channel power divider, ideal continuous phase shifters and realistic SiGe Class A cascode power amplifiers. In this setup, the 50 Ω reference antenna is connected to the PA’s with a matching network in between. Because the 25 Ω antenna array matches the optimal output impedance of the PA, it is directly connected. The performance of both antenna arrays are compared, with the focus on PAE and radiation characteristics. The results show that by going for a directly matched antenna the PAE of the system increases by 15.6% for a broadside beam and 30.4% with a scanned beam (θ = 45◦, φ = 45◦). EIRP for broadside and scanned beams increased from 50.3 W to 56.3 W and from 31.1 W to 37.9 W respectively. Bandwidth, gain, radiation efficiency and side-lobe levels were similar in both arrays but the 25 Ω antenna had 4 dB higher levels of cross-polarized radiation and a 4 dB stronger back-lobe behind the antenna. The advantage of higher efficiency and radiated power outweighs these drawbacks and makes direct impedance matching a good design strategy for 6G beamforming AiP technology. ...
This work demonstrates a novel analysis of PA-antenna co-design at 96 GHz using a 8x8 cavity-backed dual-polarized pin-fed stacked patch array. Two versions of this antenna array are designed in Ansys HFSS, one with an antenna impedance of 50 Ω, the benchmark, and one with a lower impedance of 25 Ω. Both designs are made on a custom package laminate stack-up and are compatible with pin-fed AiP technology. Using Keysight ADS, the antenna designs are co-simulated with an RF front-end circuit comprised of a single tone AC signal, ideal 1-64 channel power divider, ideal continuous phase shifters and realistic SiGe Class A cascode power amplifiers. In this setup, the 50 Ω reference antenna is connected to the PA’s with a matching network in between. Because the 25 Ω antenna array matches the optimal output impedance of the PA, it is directly connected. The performance of both antenna arrays are compared, with the focus on PAE and radiation characteristics. The results show that by going for a directly matched antenna the PAE of the system increases by 15.6% for a broadside beam and 30.4% with a scanned beam (θ = 45◦, φ = 45◦). EIRP for broadside and scanned beams increased from 50.3 W to 56.3 W and from 31.1 W to 37.9 W respectively. Bandwidth, gain, radiation efficiency and side-lobe levels were similar in both arrays but the 25 Ω antenna had 4 dB higher levels of cross-polarized radiation and a 4 dB stronger back-lobe behind the antenna. The advantage of higher efficiency and radiated power outweighs these drawbacks and makes direct impedance matching a good design strategy for 6G beamforming AiP technology.
This thesis presents a new phase noise filter, which can filter both the DLL and PI phase noise. The proposed phase noise filter is inspired by the noise transfer function from the phase detector’s input to the delay locked loop(DLL) output of a type-II DLL, which shows a first-order low-pass transfer function. The noise suppression pole frequency is adjustable and can be modified by changing the
gain of each component in the circuit. In addition, by carefully placing the frequency of the LDO’s pole, second-order noise filtering can be realized.
During design, a 10-bit DTC is constructed first and the proposed filter is placed behind the DTC to verify the effectiveness of the filter. The design achieves the post-layout level. The simulation results show that the DTC’s phase noise drops from 1.099 psrms to 315.9 fsrms with the filter. The area is 695 μm × 693.5 μm. The design consumes 42.3 mW with 1.8V supply in 180nm BCD technology. ...
This thesis presents a new phase noise filter, which can filter both the DLL and PI phase noise. The proposed phase noise filter is inspired by the noise transfer function from the phase detector’s input to the delay locked loop(DLL) output of a type-II DLL, which shows a first-order low-pass transfer function. The noise suppression pole frequency is adjustable and can be modified by changing the
gain of each component in the circuit. In addition, by carefully placing the frequency of the LDO’s pole, second-order noise filtering can be realized.
During design, a 10-bit DTC is constructed first and the proposed filter is placed behind the DTC to verify the effectiveness of the filter. The design achieves the post-layout level. The simulation results show that the DTC’s phase noise drops from 1.099 psrms to 315.9 fsrms with the filter. The area is 695 μm × 693.5 μm. The design consumes 42.3 mW with 1.8V supply in 180nm BCD technology.
To drive the gate segments in this custom VT LDMOS technology with a gate-to-source voltage (VGS) swing of 2.2 V, a driver is proposed comprising: inverter chains, a level shifter, and a high-voltage output buffer. This driver is fully digital and can be implemented using thin-oxide bulk CMOS devices whose VDD is limited to 1.1 V. A model of the DTX comprising only the drivers and DPA at the circuit level is created in ADS to evaluate the output power, drain efficiency, and system efficiency. The DTX is simulated at 3.5 GHz full power and achieves an output power of 19.79 W/23.43 W, a drain efficiency of 67.28%/59.22%, and a system efficiency of 60.34%/54.48% with a non-empirical and empirical model of LDMOS, respectively. Rise and fall times of around 20% of the RF cycle (tr = tf = 0.2/fc) are found to be the most suitable in terms of power consumption and system efficiency. ...
To drive the gate segments in this custom VT LDMOS technology with a gate-to-source voltage (VGS) swing of 2.2 V, a driver is proposed comprising: inverter chains, a level shifter, and a high-voltage output buffer. This driver is fully digital and can be implemented using thin-oxide bulk CMOS devices whose VDD is limited to 1.1 V. A model of the DTX comprising only the drivers and DPA at the circuit level is created in ADS to evaluate the output power, drain efficiency, and system efficiency. The DTX is simulated at 3.5 GHz full power and achieves an output power of 19.79 W/23.43 W, a drain efficiency of 67.28%/59.22%, and a system efficiency of 60.34%/54.48% with a non-empirical and empirical model of LDMOS, respectively. Rise and fall times of around 20% of the RF cycle (tr = tf = 0.2/fc) are found to be the most suitable in terms of power consumption and system efficiency.
Mismatch errors of the coarse DACs in CTP ADC are very critical as they introduce distortion and leak the quantization noise of the coarse stages to the output. Conventional calibration techniques such as dynamic element matching (DEM) linearize the DACs by converting the DAC distortion to white noise. However, after the linearization, the residual gain errors of the DACs remain. As a result, the quantization noise of the coarse quantizers leak to the output and degrade the performance of the CTP. Therefore, the residual gain errors of the DACs need to be estimated and calibrated. A resistive DAC architecture is proposed in the first stage of the CTP. The proposed architecture employs conventional DEM technique and is verified within the first stage of the CTP.
Furthermore, two new innovative techniques are presented in this thesis. The first technique, advanced dynamic element matching (ADEM), translates both the distortion and the gain errors due to element mismatch of the DACs in multi-stage CTP ADC into white noise. The second technique, advanced data weighted averaging (ADWA), noise shapes both the the distortion and the gain errors of the DACs. Therefore, the presented techniques do not require additional digital calibration for element mismatch errors. Finally, a DAC architecture is presented that allows a feasible implementation of the presented techniques. The techniques are verified using simulations in MATLAB and Cadence. However, The presented techniques require the CTP stages to have equal impedances. ...
This
thesis provides an investigation of the architecture and the design of the
coarse DACs in continuous time pipeline (CTP) ADC to achieve high SFDR
performance within a large bandwidth at sampling frequency of 4.8 GHz
in TSMC 28nm technology.
Mismatch
errors of the coarse DACs in CTP ADC are very critical as they introduce
distortion and leak the quantization noise of the coarse stages to the output.
Conventional calibration techniques such as dynamic element matching (DEM)
linearize the DACs by converting the DAC distortion to white noise. However,
after the linearization, the residual gain errors of the DACs remain. As a
result, the quantization noise of the coarse quantizers leak to the output and
degrade the performance of the CTP. Therefore, the residual gain errors of the
DACs need to be estimated and calibrated. A resistive DAC architecture is
proposed in the first stage of the CTP. The proposed architecture employs
conventional DEM technique and is verified within the first stage of the
CTP.
Furthermore,
two new innovative techniques are presented in this thesis. The first
technique, advanced dynamic element matching (ADEM), translates both the
distortion and the gain errors due to element mismatch of the DACs in
multi-stage CTP ADC into white noise. The second technique, advanced data
weighted averaging (ADWA), noise shapes both the the distortion and the gain
errors of the DACs. Therefore, the presented techniques do not require
additional digital calibration for element mismatch errors. Finally, a DAC
architecture is presented that allows a feasible implementation of the
presented techniques. The techniques are verified using simulations in MATLAB
and Cadence. However, The presented techniques require the CTP stages to have
equal impedances.
It employs a capacitive digital-to-analog converter (CDAC) to minimize noise. Mismatch in the CDAC is addressed through mismatch shaping techniques. Additionally, an open-loop transconductance stage is incorporated into the loop filter, enhancing dynamic range and striving for optimal performance. Extra paths are introduced in the loop filter to guarantee that amplifier swings are maintained within the designated range.
...
It employs a capacitive digital-to-analog converter (CDAC) to minimize noise. Mismatch in the CDAC is addressed through mismatch shaping techniques. Additionally, an open-loop transconductance stage is incorporated into the loop filter, enhancing dynamic range and striving for optimal performance. Extra paths are introduced in the loop filter to guarantee that amplifier swings are maintained within the designated range.
The proposed design incorporates a novel circuit technique for improving the dynamic response of linear voltage regulators. In this thesis, the theory and analysis of current amplifier-based NMOST linear voltage regulators is introduced. In order to maximize the dynamic performance, multiple implementations are analyzed and their drawbacks are presented. Adaptive biasing has been implemented in order to improve the slew rate at the gate of the pass transistor and to increase the voltage loop gain bandwidth. The current loop is stabilized by means of bandwidth enhancement resistors, reaching a unity gain frequency of over 500MHz at maximum load current condition.
The linear voltage regulator occupies an area of 0.0078 mm2, consumes a quiescent current of 8.5µA and has a current capability of 10 mA. The circuit operates at supply levels varying between 7 to 18V, provides an output regulated voltage of 1.8V and is scalable in terms of the load capacitance and the load current. This design achieves a FOM of 0.613ps and is comparable to state-of-the-art designs. ...
The proposed design incorporates a novel circuit technique for improving the dynamic response of linear voltage regulators. In this thesis, the theory and analysis of current amplifier-based NMOST linear voltage regulators is introduced. In order to maximize the dynamic performance, multiple implementations are analyzed and their drawbacks are presented. Adaptive biasing has been implemented in order to improve the slew rate at the gate of the pass transistor and to increase the voltage loop gain bandwidth. The current loop is stabilized by means of bandwidth enhancement resistors, reaching a unity gain frequency of over 500MHz at maximum load current condition.
The linear voltage regulator occupies an area of 0.0078 mm2, consumes a quiescent current of 8.5µA and has a current capability of 10 mA. The circuit operates at supply levels varying between 7 to 18V, provides an output regulated voltage of 1.8V and is scalable in terms of the load capacitance and the load current. This design achieves a FOM of 0.613ps and is comparable to state-of-the-art designs.
The project presents an automated design approach that utilizes “Ocean” and “Skill” code to automate parts of the design flow of the mm-wave power amplifier. The Ocean script, the scripting language used by the cadence environment to control the simulations, together with Matlab is applied for data handling and to automate lots of the recurring simulations. The Skill-code, which under the cadence’s environment is applied to automatically generate the tunable layouts to realize a DRC conform circuit design.
The design of a 170-GHz Power Amplifier in 0.13-μm SiGe BiCMOS applied the automation design flow is presented in this thesis. The gain-stage characteristics such as gain, stability, power-added-efficiency, saturated output power or 1dB-Compression are automatically generated and plotted. Specifically, this 170-GHz PA achieves a 15dB power gain and 11.7dBm output 1dB compression point. ...
The project presents an automated design approach that utilizes “Ocean” and “Skill” code to automate parts of the design flow of the mm-wave power amplifier. The Ocean script, the scripting language used by the cadence environment to control the simulations, together with Matlab is applied for data handling and to automate lots of the recurring simulations. The Skill-code, which under the cadence’s environment is applied to automatically generate the tunable layouts to realize a DRC conform circuit design.
The design of a 170-GHz Power Amplifier in 0.13-μm SiGe BiCMOS applied the automation design flow is presented in this thesis. The gain-stage characteristics such as gain, stability, power-added-efficiency, saturated output power or 1dB-Compression are automatically generated and plotted. Specifically, this 170-GHz PA achieves a 15dB power gain and 11.7dBm output 1dB compression point.
Multi-channel Waveform Agile Radar
Experimental performance evaluation of ASTAP radar system
An Ultra-Low Power Temperature to Digital Converter
For Medical Applications in 180 nm CMOS
Despite the manufacturing advantages of CMOS technology, the wind sensor has not attained commercial success in the market. This is due, in part, to process spread and packaging artifacts that have resulted in offset, nonlinearity and angle errors in detecting wind speed and direction. Because of this, expensive manual calibration is required to compensate these errors. Furthermore, its power consumption, in the order of tens of milliwatts, is not yet low enough to compete with its MEMS counterparts.
In this thesis, the design of a new version of the wind sensor is described, which aims to address the drawbacks of previous designs. Four extra resistors were added at each corner to electrically compensate for packaging artifacts, with the aim of reducing calibration costs. Larger thermopiles (a number of thermo- couples in series) were used, resulting in a greater signal-to-noise ratio (SNR). Internal signals were buffered to output pads to gain more insight into the magnitude of the sensor's internal signal swings. With these improvements, the resulting wind sensor chip consumes less than 30 mW of heating power and has an accuracy of ±0.6 m/s (speed) for wind speeds ranging from 1 to 25 m/s, and ±2.5°(direction) for a range of 4 to 25 m/s. ...
Despite the manufacturing advantages of CMOS technology, the wind sensor has not attained commercial success in the market. This is due, in part, to process spread and packaging artifacts that have resulted in offset, nonlinearity and angle errors in detecting wind speed and direction. Because of this, expensive manual calibration is required to compensate these errors. Furthermore, its power consumption, in the order of tens of milliwatts, is not yet low enough to compete with its MEMS counterparts.
In this thesis, the design of a new version of the wind sensor is described, which aims to address the drawbacks of previous designs. Four extra resistors were added at each corner to electrically compensate for packaging artifacts, with the aim of reducing calibration costs. Larger thermopiles (a number of thermo- couples in series) were used, resulting in a greater signal-to-noise ratio (SNR). Internal signals were buffered to output pads to gain more insight into the magnitude of the sensor's internal signal swings. With these improvements, the resulting wind sensor chip consumes less than 30 mW of heating power and has an accuracy of ±0.6 m/s (speed) for wind speeds ranging from 1 to 25 m/s, and ±2.5°(direction) for a range of 4 to 25 m/s.