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1.1. Gas Sensors: An Introduction A sensor is a device that receives a signal, either in the form of physical, chemical or biological and converts into electrical signal. Depending on the input signal, there are various types of sensors, such as optical, electrical, thermal, mechanical, chemical, and so on. So, chemical sensor is a device which converts a chemical signal into an electrical one. In a chemical sensor (which consists of two parts, the sensing element and the transducer), the sensing element changes the chemical properties in accordance with the ambient and the transducer transforms this chemical change into electrical one. The gas sensors are included in chemical sensors group. So gas sensor is a device which can detect the presence of various toxic and combustible gases present in the environment. The interaction between the test gas and the sensing surface can be detected by the measurements of change in resistance, capacitance, work function, mass, optical characteristics etc. There are a numerous use of these gas sensors. Particularly, using these gas sensors human beings can be saved from potential dangers. Hence the gas sensors play important roles in various sectors, which include industry, medical, environmental applications, and domestic applications for monitoring toxic and flammable gases [1]. Some of the important applications of gas sensors are summarized in Table 1. Table-1: Application of gas sensors in various fields Applications Safety Fire detection Leak detection Toxic/flammable/explosive gas detectors Boiler control Personal gas monitor Environmental control Weather stations Pollution monitoring Automobiles Car ventilation control Filter control Gasoline vapor detection Alcohol breath tests Medicine Fermentation control Process control 1 Food Food quality control Process control Packaging quality control (off-odors) Indoor air quality Air purifiers Ventilation control Cooking control Industrial production Fermentation control Process control The present chapter provides a brief introduction about various types of solid state gas sensors. The properties of ZnO and its suitability as an effective gas sensing material are discussed. 1.2. Solid State Gas Sensors In the last few decades, the demands for highly efficient gas sensors, together with the challenge to detect the toxic gases in harsh environment have invoked the development of various types of solid state gas sensors. These solid state gas sensors include acoustic wave gas sensors, metal-oxide-semiconductor field effect transistor (MOSFET) gas sensors, optical fiber gas sensors, electrochemical gas sensors, chemi-resistive gas sensors etc. The sensing principle, type of sensing elements and application field of these gas sensors are briefly discussed as follows [2]. Acoustic wave gas sensors: In these sensors chemically selective sensing layers are coated on piezoelectric substrates, such as quartz, ZnO etc. which can act as resonant elements. When these sensing elements are exposed to any test gas environment, the adsorption of gaseous species on the sensing layer results a mass loading in the resonant element leading to a reduction in the resonant frequency. As a result there is a shift in the value of the frequency, which can be detected and measured accurately. A variety of gases can be detected using these sensors depending on the type of the sensing layers used. However, the main disadvantages of these sensors are the requirement of high frequency and very complex circuit for its operation [3-4]. Metal-oxide-semiconductor field effect transistor (MOSFET) gas sensors: These sensors consist of a source, drain and gate. Usually the gate is a metal (catalytic metals such as Pd, Pt etc.) contact which acts as the sensing element. Next to the gate there exist 2 an oxide insulator and at the opposite side of the insulator there exist a semiconductor. The source provides and the drain collects the charge carriers (may be holes or electrons depending on the type of the MOSFET). The amount of charge carriers (or current) can be controlled by controlling the electric field in the semiconductor. The change in current, results from the change in work function of the metal and semiconductor, in presence of the test gas. Hence the efficiency of MOFET gas sensors depends on the type of metal used and the operating temperature (as the carriers in a semiconductor changes with the temperature). There are a number of advantages of these sensors as they are small in size and can be reproduced easily. However, these sensors are mostly used to detect H2 gas [5-6]. Optical gas sensors: In optical gas sensors the sensing layer is usually a polymer based layer. Upon exposure of these sensors to a test gas environment, results in the change in optical parameters (e.g. refractive index, absorption coefficient, etc.), due to the interaction of the test gas with the sensing layer [1, 7]. These sensors work efficiently and offer faster response. It has wider gas sensing capability when combined with Raman or IR spectroscopy and are environmental friendly as no electric requirement is needed. However, these sensors have often poor life time. Electrochemical gas sensors: Electrochemical gas sensors consist of two electrodes (one sensing electrode and another reference electrode) separated by a thin layer of electrolytes. These electrodes are made up of noble metals or gold which can catalyze the test gas and the electrolytes carries the charges across the electrodes. When these gas sensors are exposed to the test gas environment, the gas is either oxidized or reduced at the sensor electrode [1, 8] and the resulting current is measured. From the value of the measured current the concentration of the test gases can be estimated. Electrochemical sensors are divided into three types; amperometric, potentiometric, and conductometric gas sensors. In potentiometric gas sensors the generated signal is independent of the size of the sensor, whereas in amperometric gas sensors the current is proportional to the size of the electrode and hence sensors having smaller size produce lesser current. The primary uses of the potentiometric gas sensors are oxygen sensors or λ-sensors, which are used to monitor the air/fuel ratio in automotive combustion engines. The air/fuel ratio is determined by comparing the partial pressure of oxygen in the exhaust and that in the ambient air. In amperometric gas sensors a zero oxygen concentration is maintained at the cathode by applying a high voltage 3 externally. Now the diffusion of oxygen from cathode to anode determines the efficiency of these sensors. Chemi-resistive gas sensors: In chemi-resistive gas sensors the sensing layer can be either of a variety of materials, like semiconducting metal oxides (SMO), composites, carbon nanotubes, polymers etc. [9-13]. The principle of operation of these sensors is primarily based on the changes in resistances upon exposure to the target gas. Though the polymer based sensors offer reasonably good sensitivity, however, the poor life time of these sensors limits their use [14]. On the other hand, the SMO based sensors are useful, due to their low cost, ease of preparation, high sensitivity, and long term stability. However, the poor selectivity and higher operating temperature sometimes limits their use in different applications [15-16]. Among all the gas sensing materials, SMO based resistive gas sensors (e.g. SnO2, ZnO, WO3 etc) have been extensively studied due to their lower cost, ease of synthesis and simplicity in use. In the following section the properties of ZnO as an efficient gas sensing material is discussed. 1.3. ZnO as a Gas Sensing Material ZnO is one of the earliest discovered SMO gas sensing materials. It is a very promising material for gas sensors because of its good response to various gases, high chemical stability, and feasibility to doping, non toxicity, and low cost. Bulk and thin films of ZnO have demonstrated high sensitivity for toxic gases [17-18]. ZnO gas sensors can be used not only for detecting the toxic and inflammable gases but also for detecting volatile organic components such as, alcohol, petrol, etc [18]. 1.3.1. Properties of ZnO ZnO is an II-VI compound semiconductor having a stable wurtzite structure of lattice constants a = 3.25 Å and c = 5.2 Å; their ratio c/a ~ 1.60 is close to the value for an ideal hexagonal cell c/a = 1.633 [19]. It has a direct and wide band gap (3.37 eV) in the near-UV spectral region [20], and a large free-exciton binding energy of 60 meV (sufficiently larger than the thermal energy at room temperature (26 meV)) [20], which makes the excitonic emission possible at or even above room temperature [21]. Some of its physical properties that make it particularly attractive for electronic devices are summarized below, in table 2 [22]. Table 2: Properties of ZnO 4 Crystal structure Hexagonal, Wurtzite Molecular weight Zn:65.38, O:16 and ZnO:81.38 Lattice constant a = 3.246 Å, c = 5.207 Å Density 5.67 g/cm3 or 4.21 ×1019 ZnO molecules/mm3 Cohesive energy Ecoh = 1.89 eV Melting point Tm = 2250ok under pressure Heat of fusion 4470 cal/mole Thermal conductivity 25 W/mK at20oC Thermal expansion coefficients 4.3 × 10-6 /oK at 20oC 7.7 × 10-6 /oK at 600 oC Band gap at RT 3.37 eV Refractive index 2.008 Electron and hole effective mass me* = 0.28, mh* = 0.59 Debye temperature 370oK Lattice energy 964 kcal/mole Dielectric constant ε0 = 8.75, ε∞ = 3.75 Exciton binding energy Eb = 60 meV Pyroelectric constant 6.8 Amp/sec/cm2/oK × 1010 Piezoelectric coefficient D33 = 12 pC/N The above remarkable physical properties of ZnO has attracted intensive research efforts in numerous applications, such as semiconductor devices [23-24], transparent conductors [25], solar cell [26], varistors [27], liquid-crystal displays [28], spintronic applications [29], gas sensors [30-31], etc. Due to the above cited applications and hence the motivation of device miniaturization, large effort has been focused on the synthesis, characterization and device applications of ZnO nanomaterials. 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