5 research outputs found

    Integrating Metal-Oxide-Decorated CNT Networks with a CMOS Readout in a Gas Sensor

    Get PDF
    We have implemented a tin-oxide-decorated carbon nanotube (CNT) network gas sensor system on a single die. We have also demonstrated the deposition of metallic tin on the CNT network, its subsequent oxidation in air, and the improvement of the lifetime of the sensors. The fabricated array of CNT sensors contains 128 sensor cells for added redundancy and increased accuracy. The read-out integrated circuit (ROIC) was combined with coarse and fine time-to-digital converters to extend its resolution in a power-efficient way. The ROIC is fabricated using a 0.35 ฮผm CMOS process, and the whole sensor system consumes 30 mA at 5 V. The sensor system was successfully tested in the detection of ammonia gas at elevated temperatures

    Nanostructured Gas Sensors for Health Care: An Overview

    Get PDF
    Nanostructured platforms have been utilized for fabrication of small, sensitive and reliable gas sensing devices owing to high functionality, enhanced charge transport and electro-catalytic property. As a result of globalization, rapid, sensitive and selective detection of gases in environment is essential for health care and security. Nonmaterial such as metal, metal oxides, organic polymers, and organic-inorganic hybrid nanocomposites exhibit interesting optical, electrical, magnetic and molecular properties, and hence are found potential gas sensing materials. Morphological, electrical, and optical properties of such nanostructures can be tailored via controlling the precursor concentration and synthesis conditions resulting to achieve desired sensing. This review presents applications of nano-enabling gas sensors to detect gases for environment monitoring. The recent update, challenges, and future vision for commercial applications of such sensor are also described here

    Contact Metal-Dependent Electrical Transport in Carbon Nanotubes and Fabrication of Graphene Nanoribbons

    Get PDF
    In this thesis, we fabricate and characterize carbon nanotube (CNT) and graphene-based field effect transistor devices. The CNT-based work centers on the physics of metal contacts to CNT, particularly relating the work function of contact metals to carrier transport across the junction. The graphene work is motivated by the desire to utilize the high carrier mobility of graphene in field effect transistors. We introduce a surface-inversion channel (SIC) model based on low temperature and electrical measurements of a distinct single-walled semiconducting CNT contacted by Hf, Cr, Ti and Pd electrodes. Anomalous barrier heights and metal-contact dependent band-to-band tunneling phenomena are utilized to show that dependent upon contact work function and gate field, transport occurs either directly between the metal and CNT channel or indirectly via injection of carriers from the metal-covered CNT region to the CNT channel. The model is consistent with previously contradictory experimental results, and the methodology is simple enough to apply in other contact-dominant systems. We further develop a model explain Isd-Vsd tendencies in CNT FETs. Using experimental and analytical analysis, we demonstrate a relationship between the contact metal work function and electrical transport properties saturation current (Isat) and differential conductance in ambient exposed CNT. A single chemical vapor deposition (CVD)-grown 6 millimeter long semiconducting single-walled CNT is electrically contacted with a statistically significant number of Hf, Cr, Ti, Pd, and Ti, Au electrodes, respectively. The observed exponentially increasing relationship of Isat and with metal-contact work function that is explained by a theoretical model derived from thermionic field emission. Next, a performance analysis on CNT Schottky diodes using source-drain current anisotropy is explored. An analytical model is derived based on thermionic field emission and used to correlate experimental data from Pd-Hf, Ti-Hf, Cr-Hf, Ti-Cr, and Pd-Au mixed metal devices fabricated on one single 6 mm-long CNT. Results suggest that the difference in work functions of the two contact-metals, and not a dominant Schottky contact, determines diode performance. Results are further applied and demonstrated in a reversible polarity diode. Lastly, we investigate the effect of UV irradiation of graphene, CNT, and graphene/CNT hybrids in an oxygen environment. Samples were irradiated by 254/185 nm UV light in an oxygen environment for up to two hours. Results suggest a unique method to generate graphene nanoribbons using aligned carbon nanotubes (CNT) as a graphene etch mask. Ambient and cryogenic Gsd-Vg measurements of resulting ultra-thin graphene nanoribbons show p-type character and field effect GOn/GOff > 10^4

    CMOS์™€ ์ง‘์  ๊ฐ€๋Šฅํ•œ ์ƒํ™”ํ•™ ์„ผ์„œ๋ฅผ ์œ„ํ•œ ์ธํ„ฐํŽ˜์ด์Šค ํšŒ๋กœ์— ๊ด€ํ•œ ์—ฐ๊ตฌ

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2012. 8. ๊น€์ˆ˜ํ™˜.๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” CMOS์™€ ์ง‘์  ๊ฐ€๋Šฅํ•œ ์ƒํ™”ํ•™์„ผ์„œ์˜ ์‹ ํ˜ธ๊ฒ€์ถœ์— ์ ํ•ฉํ•˜๋„๋ก ์—ฌ๋Ÿฌ๊ฐ€์ง€ ์ธํ„ฐํŽ˜์ด์ŠคํšŒ๋กœ๋ฅผ ๊ณ ์•ˆํ•˜๊ณ  CMOS ์ƒ์—์„œ IC๋กœ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋งŽ์€ ๊ฒฝ์šฐ์— ์žˆ์–ด์„œ, ์ง‘์  ๊ฐ€๋Šฅํ•œ ์šฉ๋Ÿ‰์„ฑ ์„ผ์„œ์˜ ๊ฒฝ์šฐ์—๋Š” MEMS ๊ณต์ •์„ ํ†ตํ•ด์„œ ์ œ์ž‘์ด ๋˜๊ณ , ์ง‘์  ๊ฐ€๋Šฅํ•œ ์ €ํ•ญ์„ฑ ์„ผ์„œ์˜ ๊ฒฝ์šฐ์—๋Š” ๋‚˜๋…ธ-์™€์ด์–ด๋ฅผ ํ™œ์šฉํ•ด์„œ ์ œ์ž‘์ด ๋œ๋‹ค. ์ด์ฒ˜๋Ÿผ, ์ง‘์ ์„ ํ†ตํ•œ ์„ผ์„œ์˜ ๊ณ ๋ฐ€๋„ํ™” ๊ฐ€๋Šฅ์„ฑ์„ ์‹ญ๋ถ„ ํ™œ์šฉํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ์–ด๋ ˆ์ด ๊ตฌ์กฐ๊ฐ€ ๋งค๋ ฅ์ ์ด๋ผ ํ•  ์ˆ˜ ์žˆ๋‹ค. ์šฉ๋Ÿ‰์„ฑ ์„ผ์„œ์˜ ์‹ ํ˜ธ๋ฅผ ๊ฒ€์ถœํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ์ „ํ•˜์ฆํญ๊ธฐ๋ฅผ ํ™œ์šฉํ•œ ์ผ๋ จ์˜ ๋ฐฉ๋ฒ•๋“ค์„ ์ œ์•ˆํ•˜์˜€๊ณ , ์ €ํ•ญ์„ฑ ์„ผ์„œ์˜ ์‹ ํ˜ธ๋ฅผ ๊ฒ€์ถœํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ์ „๋ฅ˜-๋ชจ๋“œ ๊ฒ€์ถœ์„ ํ™œ์šฉํ•œ ์ผ๋ จ์˜ ๋ฐฉ๋ฒ•๋“ค์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ๋˜ํ•œ ๋‘ ๊ฐ€์ง€ ๋ชจ๋‘์˜ ๊ฒฝ์šฐ์— ์žˆ์–ด์„œ, ์–ด๋ ˆ์ด ๊ตฌ์กฐ์—์„œ ๋ฐœ์ƒํ•  ์ˆ˜ ์žˆ๋Š” ์„ผ์„œ ์ดˆ๊ธฐ๊ฐ’์˜ ๋„“์€ ์‚ฐํฌ๋ฅผ ๋ณด์ƒํ•  ์ˆ˜ ์žˆ๋„๋ก ๋™์  ์˜์—ญ์„ ํ™•์žฅ์‹œํ‚ค๋Š” ๋ฐฉ๋ฒ•์„ ๊ตฌํ˜„ํ•˜๊ณ ์ž ํ•˜์˜€๋‹ค. ์šฉ๋Ÿ‰์„ฑ ์„ผ์„œ์˜ ๊ฒ€์ถœ์„ ์œ„ํ•œ ์ฒซ ๋ฒˆ์งธ ์—ฐ๊ตฌ์—์„œ๋Š”, ํ•จ๊ป˜ ์ง‘์ ๋  ์ฐจ๋™ ์šฉ๋Ÿ‰ ์„ผ์„œ์— ์ ํ•ฉํ•˜๋„๋ก ๋ฐ˜๋ณต์ ์ธ ์ „ํ•˜ ์ ๋ถ„์„ ํ™œ์šฉํ•จ์œผ๋กœ์จ, ๋ณต์žก๋„๋Š” ๋‚ฎ์ถ”๋ฉด์„œ๋„ ์ •ํ™•๋„๋Š” ๋†’์ธ CMOS ๊ฒ€์ถœ ํšŒ๋กœ๋ฅผ ์ œ์•ˆํ•˜์˜€๋‹ค. ๋‘ ๋ฒˆ์งธ ์—ฐ๊ตฌ์—์„œ๋Š”, ์ ๋ถ„ ์บํŒจ์‹œํ„ฐ๋ฅผ ๋ฐฉ์ „์‹œํ‚ฌ ๋•Œ ์ž”์—ฌ ์ „ํ•˜๋ฅผ ๋ณด์กดํ•จ์œผ๋กœ์จ, ์ •ํ™•์„ฑ์ด ๋”์šฑ ํ–ฅ์ƒ๋œ ๊ฒ€์ถœ ํšŒ๋กœ๋ฅผ ์ œ์•ˆํ•˜์˜€๋‹ค. ์„ธ ๋ฒˆ์งธ ์—ฐ๊ตฌ์—์„œ๋Š”, ๋‚ฎ์€ ๋ณต์žก๋„๋Š” ์œ ์ง€ํ•˜๋ฉด์„œ๋„ ํ•ด์ƒ๋„๋ฅผ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•ด ๋ธํƒ€-์‹œ๊ทธ๋งˆ ๋ณ€์กฐ ๊ธฐ๋ฒ•์„ ํ™œ์šฉํ•˜๋ฉด์„œ, ์บํŒจ์‹œํ„ฐ์˜ ์ดˆ๊ธฐ๊ฐ’์„ ๋ณด์ƒํ•จ์œผ๋กœ์จ ๊ฒ€์ถœ ๊ฐ€๋Šฅํ•œ ๋™์  ์˜์—ญ์˜ ์†์‹ค์„ ์ค„์ด๋Š” ํšŒ๋กœ๋ฅผ ์ œ์•ˆํ•˜์˜€๋‹ค. ์ €ํ•ญ์„ฑ ์„ผ์„œ์˜ ๊ฒ€์ถœ์„ ์œ„ํ•œ ์ฒซ ๋ฒˆ์งธ ์—ฐ๊ตฌ์—์„œ๋Š”, ๋ฐฐ์—ด ๊ตฌ์กฐ์˜ CNT ์„ผ์„œ์— ์ ํ•ฉํ•˜๋„๋ก ๋™์  ์˜์—ญ ํ™•์žฅ ๊ธฐ๋Šฅ ๋ฐ ์ „๋ฅ˜-๋ชจ๋“œ ๋ธํƒ€ ์‹œ๊ทธ๋งˆ ๋ณ€์กฐ ๊ธฐ๋ฒ•์„ ํ™œ์šฉํ•œ ๊ฒ€์ถœ ํšŒ๋กœ๋ฅผ ์ œ์•ˆํ•˜์˜€๊ณ , ๋‘ ๋ฒˆ์งธ ์—ฐ๊ตฌ์—์„œ๋Š” TDC๋ฅผ ํ™œ์šฉํ•œ ํšŒ๋กœ๋ฅผ ์ œ์•ˆํ•จ๊ณผ ๋™์‹œ์— CNT-SnO2 ์„ผ์„œ๋ง์„ ๊ตฌํ˜„๋œ CMOS ํšŒ๋กœ์ƒ์— ํ•จ๊ป˜ ์ง‘์ ํ•˜์—ฌ, ํ†ตํ•ฉ๋œ ์‹œ์Šคํ…œ์œผ๋กœ NH3 ๊ฐ€์Šค ๊ฒ€์ถœ์„ ์„ฑ๊ณต์ ์œผ๋กœ ์‹œํ–‰ํ•˜์˜€๋‹ค.In this study, several methods were invented and verified by the silicon for the readout of CMOS-integrable bio-chemical sensors. These sensors are generally capacitive or resistive. In many cases, integrable capacitor-type sensors are in the form of micro-electro-mechanical system (MEMS) sensors and integrable resistor-type sensors are in the form of various nanowire sensors. To get benefit from high-density CMOS-integration and to characterize the sensing environment sufficiently, these sensors are made into array. For the detecting of signals from capacitor-type sensors, the scheme using charge amplifier has been invented and developed. For the detecting of signals from resistor-type sensors, schemes using current-mode detection have been invented and developed. In any type of sensors, schemes to extend dynamic range or methods to compensate for the variation of sensors initial values in array structure are considered and developed. In the first study for the readout of capacitive sensors, a low-complexity CMOS circuit for reading out monolithically integrated differential capacitive sensors has been proposed. It directly converts the differential capacitance of a MEMS sensing device to a frequency by accumulating the charges produced by repeated charge integration and charge conservation. A prototype chip was designed and fabricated in 0.35ฮผm CMOS technology. Experimental results show that differential capacitance is linearly converted to output frequency. In the second study for the readout of capacitive sensors, a more accurate capacitance-to-frequency converter has been presented, which produces a single pulse stream in a wide range of frequencies. This circuit saves residual charges and accumulates them when discharging an integrator capacitor. Implemented in 0.35ฮผm CMOS technology, the proposed circuit improves the accuracy from about 6% to 0.13%. In the third study for the readout of capacitive sensors, a low-complexity interface circuit for capacitive sensors has been presented which are integrated into sensor microsystems. To reduce hardware cost while keeping high resolution, a first-order delta-sigma modulator (DSM), which balances the charge from the capacitive difference between the sense and reference capacitors with the charge from a fixed-quantity capacitor, is employed. A charge-mode digital-to-analog converter and a successive approximation register are utilized to automatically calibrate the zero point of the interface circuit, which may shift further than a dynamic range. A prototype circuit fabricated in a 0.35ฮผm CMOS process. Its DSM operates at a sampling frequency of 1MS/s with an oversampling ratio of 128. This circuit can read a capacitive difference from -0.5pF to +0.5pF with a 0.49fF resolution. Capacitive offset that causes the zero point to shift can be cancelled in the range from -2pF to +2pF with a 31.25fF resolution. In the first study for the readout of resistive sensors, a sensor readout integrated circuit for the carbon nanotube (CNT) bio-sensor array has been presented. The heart of the proposed circuit is the low-power current-input continuous-time ฮ”ฮฃ modulator that is capable of dynamic range extension. Experimental results show that the prototype chip, designed and fabricated in 0.18ฮผm CMOS process, achieves a dynamic range of 87.746dB and has a readout rate of 160kHz, which guarantees 1k sample/s per each sensor. It consumes 8.94ฮผW/cell considering the 16x10 sensors and its core area is 0.085mm2. In the second study for the readout of resistive sensors, a tin-oxide-decorated CNT network gas sensor system has been implemented on a single die. The deposition of metallic tin on the CNT networks, its subsequent oxidation in air, and the improvement of the lifetime of the sensors have also been shown. The fabricated array of CNT sensors contains 128 sensor cells for added redundancy and increased accuracy. The read-out integrated circuit (ROIC) combines coarse and fine time-to-digital converters to extend its resolution in a power-efficient way. The ROIC is fabricated using a 0.35ยตm CMOS process, and the whole sensor system consumes 30mA at 5V. The sensor system was successfully tested in the detection of ammonia gas at elevated temperatures.ABSTRACT I CONTENTS IV LIST OF FIGURES VII LIST OF TABLES X CHAPTER 1 INTRODUCTION 1 1.1 CMOS-INTEGRABLE BIO-CHEMICAL SENSORS 1 1.1.1 CAPACITIVE BIO-CHEMICAL SENSOR 1 1.1.2 RESISTIVE BIO-CHEMICAL SENSOR 4 1.1.3 REQUIREMENTS FOR HIGH-DENSITY INTEGRATION ON CMOS 8 1.2 THESIS ORGANIZATION 10 CHAPTER 2 INTERFACE CIRCUITS FOR CAPACITIVE BIO-CHEMICAL SENSORS 11 2.1 A CMOS DIFFERENTIAL-CAPACITANCE-TO-FREQUENCY CONVERTER UTILIZING REPETITIVE CHARGE INTEGRATION AND CHARGE CONSERVATION 11 2.1.1 INTRODUCTION 11 2.1.2 CIRCUIT DESIGN 12 2.1.3 PROTOTYPE DESIGN AND EXPERIMENTAL RESULTS 17 2.2 IMPROVING THE ACCURACY OF CAPACITANCE-TO-FREQUENCY CONVERTER BY ACCUMULATING RESIDUAL CHARGES 19 2.2.1 INTRODUCTION 19 2.2.2 PROPOSED CAPACITANCE-TO-FREQUENCY CONVERTER 22 2.2.2.1 CIRCUIT OPERATION 22 2.2.2.2 MATHEMATICAL ANALYSIS 26 2.2.3 EXPERIMENTAL RESULTS 30 2.3 A DELTA-SIGMA INTERFACE CIRCUIT FOR CAPACITIVE SENSORS WITH AN AUTOMATICALLY CALIBRATED ZERO POINT 35 2.3.1 INTRODUCTION 35 2.3.2 PROPOSED INTERFACE CIRCUIT FOR CAPACITIVE SENSORS 38 2.3.2.1 DELTA-SIGMA INTERFACE CIRCUIT 38 2.3.2.2 AUTOMATIC CALIBRATION OF THE ZERO POINT 41 2.3.3 EXPERIMENTAL RESULTS 44 CHAPTER 3 INTERFACE CIRCUITS FOR RESISTIVE BIO-CHEMICAL SENSORS 48 3.1 A CMOS READOUT INTEGRATED CIRCUIT WITH WIDE DYNAMIC RANGE FOR A CNT BIO-SENSOR ARRAY SYSTEM 48 3.1.1 INTRODUCTION 48 3.1.2 CIRCUIT ARCHITECTURE 51 3.1.3 CIRCUIT IMPLEMENTATION 53 3.1.3.1 CURRENT DAC 54 3.1.3.2 INTEGRATOR AND COMPARATOR 55 3.1.3.3 BACK-END LOGIC 55 3.1.4 EXPERIMENTAL RESULTS 57 3.2 INTEGRATING METAL-OXIDE-DECORATED CNT NETWORKS WITH A CMOS READOUT IN A GAS SENSOR 60 3.2.1 INTRODUCTION 60 3.2.2 EXPERIMENTAL: CARBON NANOTUBE SENSING CELL FABRICATION 63 3.2.3 THE ROIC ARCHITECTURE 68 3.2.3.1 THE CNT CELL ARRAY STRUCTURE 68 3.2.3.2 ANALOG FRONT-END CIRCUIT 70 3.2.3.3 DLL-BASED TDC 75 3.2.4 CALIBRATION AND ERROR REDUCTION 77 3.2.4.1 DEVICE MISMATCH AND CALIBRATION 77 3.2.4.2 QUANTIZATION ERROR AND NOISE 79 3.2.5 SYSTEM ARCHITECTURE 81 3.2.6 MEASUREMENT AND RESULTS 82 CHAPTER 4 CONCLUSIONS 85 BIBLIOGRAPHY 88 ABSTRACT IN KOREAN 95Docto
    corecore