Open access peer-reviewed chapter

Perovskites-Based Nanomaterials for Chemical Sensors

Written By

Morteza Enhessari and Ali Salehabadi

Submitted: 28 September 2015 Reviewed: 17 February 2016 Published: 24 August 2016

DOI: 10.5772/62559

From the Edited Volume

Progresses in Chemical Sensor

Edited by Wen Wang

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The perovskite structure is adopted by many compounds in solid-state chemistry. The sensitivity, selectivity, and stability of many perovskite nanomaterials have been devoted the most attention for chemical sensors. They are capable to sense the level of small molecules such as O2, NO, and CO. This chapter provides a comprehensive overview of perovskite nanoscale materials that concentrate on chemical sensors. The perovskite structure, with two differently sized cations, is amenable to a variety of dopant additions. This flexibility allows for the control of transport and catalytic properties, which are important for improving sensor performance. We devote the most attention on the synthesis, structural information, and sensing mechanism. We will later elaborate on the development mechanism of chemical sensors based on perovskite nanomaterials. We conclude this chapter with the personal perspectives on the directions toward future works on a novelty of nanostructured chemical sensors.


  • Perovskite
  • Nanomaterial
  • Chemical sensor
  • Gas sensing material
  • Semiconductor

1. Introduction

The 3D-metal monooxides such as MnO, FeO, CoO, and NiO are semiconductors with low electrical conductivities. In general, the as-mentioned metal oxides have such large band gaps that they are insulators. The structure with general formula ABX3, containing 12-coordinate hole of BX3 is occupied by a large A ion (A: Ni, Pb, Fe, Co, Zn, etc) are known as perovskites. The tetragonal structure of perovskites showing the local displacements leads to the variation in electric behavior of this material (Figure 1).

Figure 1.

The local ion displacements of a tetragonal ABX3 structure [1].

Many applications of perovskites (here ABO3) are reported in electrodes of solid oxide fuel cells [2], metal–air batteries [3], gas sensors [4], and high-performance catalysts [5].

Metal-oxide semiconductors, such as semiconducting tin oxide (SnO2), have been used as chemical sensors for a number of years. Applications include environmental monitoring, fire detection, and vehicle monitoring [4]. The fundamental sensing mechanism of these metal-oxide-based gas sensors relies upon the change in electrical conductivity due to the interaction between the gases in the environment and oxygen in the grain boundaries.

A chemical sensor is a device that transforms chemical information into an analytically useful signal. The chemical information may originate from a chemical reaction of the analyte or from a physical property of the investigated system. They have applications in different areas such as medicine, home safety, environmental pollution, and many others. Chemical sensors are classified according to the operating principle of the transducer (Table 1).

A variety of chemical methods have been reported for the synthesis of semiconducting materials including perovskites, spinels, or illminites which include ball-milling [6, 7], combustion synthesis [810], co-precipitation [11], sol–gel [1215], radio frequency sputtering [1619], solid-state reaction [2022], and molten-salt method [23, 24].

In this chapter, we will review the routine reliable synthesis method, structural information, and gas sensing behavior of (mixed) metal-oxide semiconductors with tunable functionalities used in electrical devices for chemical sensors. Novel functional nanostructure semiconductors will be presented.

Type of
Source Example
Absorbance, reflectance
Opto-thermal effect
Light scattering
Voltammetric sensors
Potentiometric sensors
Chemically sensitized field effect
transistor potentiometric
solid electrolyte gas sensors
Electrical Electrical
Metal-oxide semiconductor
Organic semiconductor
Electrolytic conductivity
Electric permittivity
Mass change at a
specially modified surface
Piezoelectric devices
Surface acoustic wave devices
Magnetic Change of
Oxygen monitors
Thermometric Heat effects of a specific chemical
reaction or adsorption
Combustion reaction
Enzymatic reaction
Optothermal device
Radiation Change of Physical
X-, p- or r-radiation
Chemical composition

Table 1.

Classification of chemical sensors

1.1. Semiconductors chemistry

Semiconductors are insulators at absolute zero. Above this temperature and below the melting point of the solid, the metal acts as a semiconductor. Semiconductors are generally classified on the basis of their composition and particle size. Procreation of semiconductors with typical band gaps (a few eV’s corresponding to 100–200 kJ mol−1) usually occurs between p-block metals and group 13/14 metalloids in combination with chalcogenides and pnictides [1].

Perovskites are an example of especial class of semiconductors (Figure 2). In this structure, the unit cell is not centrosymmetric and the crystal develops a permanent electric polarization as a result of ion displacements (refer to Figure 1). Barium titanate, BaTiO3, is one of the interesting examples of perovskite. This compound, at above 120°C, exhibits a cubic structure while a lower symmetry, that is, a tetragonal unit cell at room temperature due to ions displacement. Fe2TiO5 [25], NiTiO3 [26, 27], CoTiO3 [15, 28], BaZrO3 [12], La2CuO4 [29], LaMnO3 [5], MnTiO3 [14], and PbTiO3 [30] are some important examples of common perovskite oxide semiconductors.

Figure 2.

Schematic representation of (a) perovskite (ABX3) structure, (b) emphasizes of octahedral sites, and (c) its respective projection [1].

1.2. Semiconducting Chemical Sensors

Chemical sensors are generally classified according to the shape of metal oxides to nanotubes, nanorods, nanobelts, and nanowires [16]. A nanotube sensors include metal-oxide tubes such as Co3O4 (superior gas sensing capabilities toward H2), SnO2 (gas sensor to ethanol), and TiO2 (hydrogen sensor). Nanorod-based sensors are involved in metal oxides such as ZnO, MoO3, and tungsten oxide nanosensors, polymer nanorods such as poly(3,4-ethylene-dioxythiophene)-nanosensor, and metal nanorods such as Au nanosensor. As for nanobelt-based sensors, the attentions have been devoted on metal oxides such as ZnO (Co and O2 sensors), SnO2 (NO2 sensors), and V2O5 (stable ethanol sensor) nanosensors, especially on ZnO nanobelts sensors. Nanowire metal oxides such as In2O3, SnO2, ZnO, and Ga2O3 are used in NO2 sensor, O2 and CO sensors, NH3 sensor, and ethanol sensor, respectively.

Perovskites with a general formula of ABO3, a typical band gap of 3–4 eV and good thermal stability, are interesting choices for gas sensing materials [6]. A suitable material for a chemical sensor particularly gas sensors must not only have an appropriate electronic structure but also a good affinity with the target reactant which satisfies a number of other requirements such as manufacturability, hydrothermal stability, poisoning resistance, and adaptability with existing technologies. A wide variety of techniques are capable of synthesizing perovskites (nano)- materials. Sol–gel, impregnation, and precipitation are some of the most promising ones from efficiency and scale-up perspectives.

Many researchers have reported the gas sensing devices for dangerous gases such as carbon oxides (CO, CO2), nitrogen oxides (NO, NO2), and sulfur dioxide (SO2) released from high-temperature combustion processes. CH4 is another potent greenhouse gas that leads to global warming [3134].

The perovskite oxide generally used in oxygen sensors is SrTiO3 [35]. The oxygen partial pressure dependence of the conductivity of undoped SrTiO3 contains both n-type and p-type regimes.

Gas sensing properties of nanocrystalline perovskite, LaFeO3 [36] and BaTiO3 [37], were successfully involved in previous literatures. It is concluded that the sensor based on the LaFeO3 powders has a considerable sensing response to carbon dioxide. On the other hand, the BaTiO3 sensor has a good selectivity to LPG against CO2, H2, NH3, C2H5OH, and Cl2. The BaTiO3 thin films exhibit rapid response recovery which is one of the main features of this sensor. The defect structure and conduction properties of BaTiO3 are also similar to those of SrTiO3. However, the conductivity of BaTiO3 is higher than that of SrTiO3 in the p-type regime.

Hydrogen-sensitive semiconductor SrCe0.9Yb0.1O3 nanopowders with tunable sensing functionalities toward H2 and H2S were synthesized in our group [13]. We observed a noticeable gas sensing behavior of the perovskite at room temperatures with semi-spherical and porous structures of nanoparticles.

High sensitivity and selectivity of mixed potential sensor based on Pt/YSZ/SmFeO3 for NO2 gas are investigated by Giang et al. [38]. They concluded that the high sensing performances of the as-mentioned sensor to NO2 could be related to high catalytic active of the sensing material, that is, SmFeO3. The adsorption of exposed gases on the surface of SmFeO3 has been considered the factor that affects on the performance of the sensor Pt/YSZ-8/SmFeO3.

CO sensitive nanocrystalline LaCoO3 and La1−xCexCoO3 perovskite sensor were investigated by Dhivia et al. [6] and Ghasdi et al. [31]. They inferred that the oxygen mobility increased by increasing the surface area. Moreover, the maximum response ratio of CO exhibited a good correlation with the total amount of desorbed oxygen.

Hydrocarbon gas sensing of nanocrystalline perovskite oxides, LnFeO3, shows a superior response to gas sensing characteristics containing methane, propane, and n-hexane. Moreover, the rare earth elements of the as-mentioned perovskite play an important role to gas sensitivities [39].

Nanostructured perovskite, CdTiO3 films for methane sensing, is one of the recent studied examples of semiconductor for chemical sensors [40]. The gas sensing mechanism of CdTiO3 sensor is of surface-controlled type. The variation in the resistance of sensing material caused by the adsorption and desorption of gas molecules such as O2. The oxygen adsorption on the CdTiO3 film surface depends on the temperature. At high temperatures, O2 dissociates into atomic oxygen Oads-(Eq. 1)


The chemistry image, the classification of perovskites applicable as gas sensing materials, the fabrications, and the performance mechanism of gas sensors will be discussed in the following sections. It must be noted that in this chapter the perovskites classes are named based on “B” site in general formula of ABO3, such as stanate (BaSnO3), titanate, and niobate.


2. Classification of perovskites

As mentioned before, the typical chemical formula of the perovskite structure is ABO3 and AB2O4, where A and B denote two different cations. The ilmenite structure has the same composition as the perovskite, that is, ABO3; however, A and B in this structure are cations of approximately the same size that occupy an octahedral site.

Compound Lattice parameter/× 10 nm
A B c
Cubic structure
KTaO3 3.989
NaTaO3 3.929
NaNbO3 3.949
BaMnO3 4.040
BaZrO3 4.193
SrTiO3 3.904
KMnF3 4.189
KFeF3 4.121
Tetragonal structure
BiAlO3 7.61 7.94
PbSnO3 7.86 8.13
BaTiO3 3.994 4.038
PdTiO3 3.899 4.153
TlMnCl3 5.02 5.04
LaAlO3 type
LaAlO3 5.357 α=60° 06
LaNiO3 5.461 α=60° 05
BiFeO3 5.632 α=60° 06
KNbO3 4.016 α=60° 06
GdFeO3 type
GdFeO3 5.346 5.616 7.668
YFeO3 5.283 5.592 7.603
NdGaO3 5.426 5.502 7.706
CaTiO3 5.381 5.443 7.645
NaMgF3 5.363 5.503 7.676

Table 2.

Typical perovskite compound [41]

Various combinations of charged cations in the A and B sites of perovskite compounds such as 1 + 5 and 2 + 4 have been reported. However, a complex combinations are also investigated, such as M(B′1/2B″1/2)O3, where M can be Pb or La, B′ can be Sc, Fe, Ni, or Mg and B″: Nb, Ta, Ru(IV), or Ir(IV). Typical perovskite compounds with various lattice structures are listed in Table 2.

In Table 3, the as-reported elements that can be incorporated within the perovskite structure are listed (Self-test: to be completed by the readers). It is obvious that almost all elements except noble gases can be occupied either A or B lattice structure in the perovskite lattice. The crystal structure of perovskites is dependent on the size and the nature of the A and B atoms. Simplifying the possible lattice interaction between elements forms a perovskite structure for gas sensing materials.

B/A Na K Rb Ca Sr Ba Y La Hf Ag Cd Ln Tl Pb Ce Th Pr Nd Sm Eu Gd Tb Dy Ho Er Tm Yb Lu Th
Fe *

Table 3.

(Self-test) elements that can occupy perovskite structure (ABO3, AB2O4)

“✓” Represents the available, as-synthesized gas sensing perovskites; “*” corresponds to LaFeO3 [42].

Another class of perovskites forms by the replacement of B-site elements with a dopant. The as-mentioned structure with general formula A3MB2O9 is called as superstructure perovskites. In fact, large differences in ionic radii lead to the formation of this huge structure. Here, M can be Fe, Co, Ni, Zn, or Ca like Ba3SrTa2O9. Moreover, a new class of superstructure perovskite is invented where the ordering of cation vacancies located on A sites: for example, MNb3O9 (M-La, Ce, Pr, Nb) and MTa3O9 (M-La, Ce, Pr, Nd, Sm, Gd, Dy, Ho, Y, Er).

Typical polymorphs of the perovskite structure are brownmillerite (A2B2O5). This is oxygen deficient type of perovskite, the oxygen vacancy is ordered [41, 43]. In this structure, as the content of oxygen drops, the phase changes from the cubic perovskite to tetragonal, to orthorhombic, and finally to the brownmillerite structure. These phases are in fact a repeating sequence of octahedral and tetrahedral layers [44]. In the typical example of a non-stoichiometric ternary oxide such as SrFeO2.5+x (0 < x <0.5), there is a series of phases that is derived from the perovskite structure. Stepwise dropping of the oxygen content, the phase changes from the cubic (x = 0.5) to tetragonal (x = 0.35), to orthorhombic (x = 0.25), and to the brownmillerite structure (x = 0) [43, 44]. The as-mentioned phenomenon can be observed clearly in the reaction isotherm profiles (Figure 3). In the regions where two phases co-exist, the x-value increases greatly for the small increase in oxygen pressure.

Figure 3.

Reaction isotherm of SrFeO2.5+x in a substituted SrFe0.9Cu0.1O2.5 [44].

Ruddelsden–Popper compounds are a group of perovskite with the general formula (ABO3)nAO (Figure 4). Some examples of this structure are Sr3Ti2O7 and Sr4Ti3O10.

Figure 4.

Ruddelsden–popper structure [41].


3. Sensing materials and mechanism

Sensor technology has widely distributed as a basic enabling technology in many instances. Many applications of sensing devices particularly in intelligent manufacturing processing have been reported ranging from assessing the integrity of aircraft to monitoring the environment for hazardous chemicals [45, 46]. The oxygen deficient crystal structure in semiconducting oxide materials is responsible for the change in resistance an oxide sensor [1]. This is due to the adsorbed surface species [41]. The reducing gas develops a shrink charge region which allows better charge movement.

A chemical/gas sensor provides an electrical/optical output in response to chemical and physical interactions with chemicals/gases. In particular, the gas sensors have been used for various industrial and/or safety applications and chemical such as a) determination of gas leakage [41, 4749], novel LPG sensitive materials working in the entire range of least explosive limit (LEL) to upper explosive limit (UEL) [3032]. Nanostructured perovskite materials can improve the sensing properties of the sensor due to high surface-to-volume ratio characteristics. Knowledge of nanoscale perovskite sensing materials have been achieved a great attraction to serve as a novel gas sensing materials at the lower working temperatures.

How does a sensing materials work? Band theory is a principle of chemical sensors technology which postulates that when atoms or molecules are aggregated in the solid state, the outer atomic orbitals are split into bonding and antibonding orbitals and mix to form two series of closely spaced energy levels. In general, in a gas sensor, the gas species react with metal-oxide particle surfaces thereby trapping electrons (Figure 5). This is the process of chemisorptions. A resistance layer from an electron-depleted space (cloud) charge on the n-type (the majority of charge carriers are electrons) particle surface or conducting layer from accumulated holes on the p-type (the positive holes being the majority of charge carriers) particle [50]. Continued reaction between gas molecules and chemisorbed oxygen causes electrons to release from oxygen back to oxide. The current changes the electrical conductivity in the space charge layer. The conductivity increases in the case of n-type oxides, as a greater charge carrier (electron) concentration, and decreases in p-type oxides, as electrons recombine with holes. Time-by-time changing of conductivity in the space charge layer varies the overall electrical resistance of the oxide. Hence, the space (cloud) charge surrounding the bulk material directly influenced the sensitivity, that is, thicker the space charge layer higher the sensitivity. The change of sensor resistance depends on a type of metal-oxide semiconductors, here perovskites. The changes in sensor resistance upon exposure to the target gas/reducing gas in the cases of n-type and p-type perovskite sensors are reported by Choopon et al. [51] as illustrated in Figure 6.

Figure 5.

Mechanism of gas sensing [50].

Figure 6.

Change of sensor resistance upon exposure to the target gas [51].


4. Application of perovskite nanomaterials in gas sensor

Variety of component and high chemical stability are two important characteristic of perovskite nanomaterials applicable for catalysts in various reactions. It is impractical to consider the classification of perovskites without their applications in sensing devices. The advent of high-performance solid-state gas sensors has motivated several scientists in searching the new perovskite materials and investigating their gas sensing properties. In general, the perovskites are either oxidation catalysts or oxygen-activated catalysts as an alternative to catalyst containing precious metals, or a model for active sites. The stability of the perovskite structure allows the invention of new compounds with an unusual valence state of elements or a high extent of oxygen deficiency [41]. In Table 4, we summarize the as-reported perovskite nanomaterials in sensing device. We mentioned that the high catalytic activity of perovskite oxides is based on the high surface activity to oxygen reduction ratio or large number of oxygen vacancies in the particular structure. Among the various catalytic reactions studied, automobile exhaust gas, various pollutant gases such as H2S, and NH3, NOx decomposition reaction gas, hydrogen gas, methanol, and LP gas attract particular attention. The perovskite materials can be used as a thin film (nanocomposites) or nanopowders.

Sensing materials NOx CH4 NH3 LPG C2H5OH Acetone Refs.
Titanate Sr(Ti 0.65Fe0.35)O3, Pb(Zr0.2Ti0.8)O3 BaTiO3, CdTiO3, Na2Ti3O7 Li0.35La0.55TiO3 [5257]
Ferrite CuxFe3−xO4, Mg0.5Zn0.5Fe2O4 SrTi0.6Fe0.4O3−δ
La0.8Sr0.2Fe1−xCuxO3, Cu0.5Zn0.5W0.3Fe1.7O4 Co1−xNixFe2O4, Mg0.5Zn0.5Fe2O4 NiFe2O4 [17, 5862]
Cobaltite Bi10Co16O38, Ln1−xSrxCoO3 NdCoO3, Nd0.8Sr0.2CoO3 Bi12(Bi0.55Co0.45)O19.6 LnBaCo2O5+δ, Bi10Co16O38 Ba0.5Sr0.5Co0.8Fe0.2O3−δ [6369]
Cobaltate YCoO3, LaCoO3 La1−xCexCoO3 NdCoO3 [6, 35, 60, 6568]
Mangenate La0.8Sr0.2Al0.9Mn0.1O3, Ln1−xCa(Sr)xMnO3 [67, 70]
Cerate SrCeo.95Yb0.05O3−α, SrCeO3, SrCe0.95Tb0.05O3−δ BaCe0.90Gd0.1O3−δ [9, 7173]
Niobate FeNbO4 BaNbO3 FeNbO4 [74, 75]
Nickelate LaNi03 [76]
Stanate BaSnO3, Zn2SnO4, ZnSnO3 Ba1−xNixSnO3 Ba1−xLaxSnO3, ZnSnO3 BaSnO3 [7783]
Zirconate PbZrO3 CaZrO3 [20, 48, 84]
Chromate MgCr2O4 [85, 86]
Molybdate Bi2MoO6 Bi3FeMo2O12 ZnMoO4 Bi3FeO4(MoO4)2 NiMoO4, CuMoO4, PbMoO4 Bi3FeMo2O12 [8789]
Tungstate SnxWO3+x ZnWO4, MnWO4 CoWO4, SnxWO3+x, SnW04 [9096]
Sensing materials NOx CH4 NH3 LPG C2H5OH Acetone Refs.
Titanate ZnTiO3 CoTiO3, Cr1.7Ti0.3O3, Zn2TiO4, [97100]
Ferrite LaFeO3,
Co1−xMnxFe2O4, CoFe2O4
Mg0.5Zn0.5Fe2O4 NixZn1−xFe2O4 CuFe2O4, Ni1−xCoxFe2O4 Co1−xNixFe2O4, ZnFe2O4, NixZn1−xFe2O4, GaFeO3 Ni1−xCoxFe2O4 CoFe2O4, NiFe2O4, Ni1−xCoxFe2O4 [11, 23, 47, 95, 96, 98101]
Cobaltate YCoO3 YCoO3
Mangenate LaMnO3+δ, La0.6Ca0.4Mn1−xNixO3, [42, 102]
Niobate LiNbO3 CrNbO4, InNbO4 InNbO4, FeNbO4 AlNbO4, CrNbO4, InNbO4 [70, 97, 102107]
Nickelate LaNi03 [76]
Stanate Zn2SnO4 Zn2SnO4 CaSnO3, ZnSnO3 Zn2SnO4,
CaSnO3, Zn2SnO4, [7274, 108, 109]
Chromate LaCr1−xTixO3 [8]
Molybdate Bi2MoO6, NiMoO4 Bi3FeMo2O12 [110, 111]
Tungstate CuWO4, SnW04, MgWO4, ZnWO4, BaWO4 CoWO4 [8789, 110, 112]

Table 4.

Gas sensing perovskite oxides

From Table 4, it is obvious that the various combinations of elements are used to produce the perovskite nanomaterials for the as-mentioned sensing devices. Among them, the humidity, LPG, ethanol, and pollution gases have been achieved a great attention.

Humidity measurement is one of the most significant issues in various areas of applications such as instrumentation, automated systems, agriculture, climatology, and GIS. Molybdate- , stanate- , and titanate-based perovskites are three powerful groups of materials used in this criterion. When perovskite oxides are exposed to moisture, interaction occurs in three stages: (a) a few water vapor molecules are chemisorbed at the neck of the crystalline grains on activated sites of the surface and form hydroxyl groups. As a result of this interaction, the hydroxyl group of each water molecule is adsorbed on metal cations and possesses high charge carrier density and strong electrostatic fields, and producing mobile protons. The protons migrate on the surface and react with the neighbor surface oxygen to form a second hydroxyl group. The chemisorbed layer is the first formed layer. (b) After chemical completion of the first layer, subsequent water vapor layers are physisorbed on the first-formed hydroxyl layer. After forming the first physisorbed layer, another water molecule adsorbs via double hydrogen bonding to two neighboring hydroxyl groups. This is continued to form multilayer. (c) By forming the more layers, a large amount of water molecules is physisorbed and bonded water vapor molecules become mobile and form continuous dipoles and electrolyte layers between the electrodes to generate dielectric constant and bulk conductivity. Figure 7 shows the layer by layer adsorption of humidity on the ceramic intelligent surface.

Figure 7.

Mechanism of humidity sensing [113].

Ferrite and cobaltate/cobaltite are two main groups of materials used as active sites in CO sensing device. The mechanism of CO sensors is based on an anionic adsorption and the lattice oxygen atoms activities in the surface of perovskites ceramic. Here, the oxygen atoms are adsorbed and react with the available CO gases to form CO2 and generate a free electron [114] of following types (Eq. 2):


A possible mechanism of oxidation of CO by lattice oxygen ions on the surface of La-doped BaTiO3 is shown in Figure 8.

Figure 8.

Schematic representation of CO absorption.

LPG (LPG is a mixture of hydrocarbons like n-propane and n-butane), ethanol, and NH3 sensors are another classes of perovskite-based sensing devices with a variety of applications. The sensing mechanism follows almost the same mechanism. When the perovskite sensor is exposed to air, O2 adsorbs on the surface substrate and trap electrons from the conduction band of perovskites. This occurs due to the electronegativity of oxygen atom, negative-charged chemisorbed oxygen species, that is, O2− and O. As a result, the number of holes increased, the resistance decreased, and the concentration of available carrier achieves a higher value. By exposing the sensing materials to reducing gases, the gas molecules first reacted with the adsorbed oxygen, the carrier (holes) density depressed (due to electron donating nature of gases), and finally increasing the resistance. The reaction mechanisms of LPG (Eq. 3), ethanol (Eq. 4), and NH3 (Eq. 5) [115] are the following:


An example is LaCoxFe1−xO3 nanoparticles which used to investigate the ethanol sensing properties [116]. A careful consideration on the response curves indicates that the LaCo0.1Fe0.9O3 nanoparticles are very promising materials for fabricating ethanol sensors (Figure 9).

Figure 9.

Responses of LaFeO3, LaCo0.1Fe0.9O3, LaCo0.2Fe0.8O3, and LaCo0.3Fe0.7O3 nanoparticles to 500 ppm ethanol [116].

Miscellaneous applications of perovskites in solid-state sensors such as infrared, electro-optic, heat, magnetic field, and liquid-state sensors especially in health-care products such as glucose and cholesterol are reported (Table 5). The form of the substrate is thick film including a nanocomposite of perovskites and a polymer. Typical example of this class is La0.67Sr0.33MnO3 (LSMO). A 400 nm thick LSMO films grow on the lucalox (polycrystalline Al2O3 + Mg) substrates via vapor deposition technique. Mechanism of such sensors is based on the change of the film resistivity depending on the applied magnetic field magnitude [119]. Initial resistance and the sensitivity to magnetic field are two important factors depend on ambient temperature. This is a drawback for magnetic field measurements because a temperature compensation mechanism is required. Figure 10 shows a typical magnetic field LSMO sensor. Twisted wires solder to the parts of the electrodes above the substrate (uncovered). Some samples were covered with the polyethylene hot-melt adhesive.

Sensing materials Infrared Magnetic field Heat Electro-optic Glucose H2O2 Cholesterol NADH Acetone Refs.
Titanate Ba0.25Sr0.75TiO3 [117]
Ferrite LaTiO3, ZnFe2O4, CuFe2O4 CoFe2O4 NiFe2O4 CoFe2O4 CoFe2O4, NiFe2O4, Ni1−xCoxFe2O4 [47, 98100, 118121]
NixMn3−xO4 La0.67Sr0.33MnO3, La0.67Ba0.33O3 LaSrMnO, La2/3Sr1/3MnO3, La0.60Pb0.40MnO3 [119, 122126]
Niobate LiNbO3 KTa1−xNbxO3 [45, 127]
Zirconate Pb(Zr52Ti4S)O3 [18, 128]

Table 5.

Miscellaneous perovskites sensors

Figure 10.

Covered and uncovered LSMO sensor (top and cross-section view) [119].

High selectivity, good sensitivity, fast, and reversible response are the main advantages of enzymatic glucose sensors (EGS) [129]. However, some deficiencies prevented wide range applications of EG sensors like the lack of mechanical and thermal stability and also environmental concerns. Development of glucose sensors without using enzymes based on magnetic nanoparticles can play a significant role. The nanoperovskites can be a good candidate due to the high surface area, high catalytic efficiency, superior mass transport, and strong adsorption ability [120]. Here, an electrode is covered/modified by intelligence perovskite nanomaterials or polymer-perovskite nanocomposite to enhance the sensing properties. In a typical example, polypyrrole is used as shell in polypyrrole–ZnFe2O4 magnetic nanocomposites to induce a strict barrier and reduce the magnetic coupling effect between nanoparticles (Figure 11). Electro-oxidation mechanism of glucose on ZnFe2O4/PPy core shell electrode is also shown [121].

Figure 11

The illustration of (a) preparation process of modified electrode and (b) electro-oxidation mechanism of glucose on ZnFe2O4/PPy core-shell–glassy carbone modified electrode [121].


5. Fabrication of gas sensor

Various fabrication techniques have been developed in the production of metal-oxide semiconductor sensors. Purity, porosity, reliability, reproducibility, and expense are the most important factors in selecting the production technique [130]. The mechanism of gas sensors are discussed in previous sections. Thick film and thin film technologies have been popular techniques to minify various types of the sensors unifying in monolithic hybrid circuits. In the general definitions, thick film depositions are a process of surface modification by applying a thick coating on a substrate. The manufacture of such devices is multilayer coating film involving deposition of several layers deposition of conductor, resistor, and dielectric layers on the insulating substrate. Thin film technology is a process of deposition of required materials by applying a very thin coating layer often just a few nanometers thickness. Screen printing of ceramic powders, chemical vapor deposition (CVD), sol–gel techniques, spray pyrolysis, physical vapor deposition (PVD), and drop coating [130] are the main techniques for production of metal-oxide films for gas sensors.

5.1. Screen printing

Spiral shape sensing device (screen printing) is one of the simplest sensors in most of the as-reported research articles [13]. Intelligent ink pushes through a porous layer, and it contains the material to be deposited on the substrate. After complete deposition, the print is heated to remove the vehicle, leaving perovskites on the specific target area. Figure 12 indicates a unit of gas sensor containing metal oxide fabricated by screen printing.

Figure 12.

Unit of gas sensor fabricated by screen printing [113].

5.2. Chemical vapor deposition

A heated substrate is exposed to a precursor or controlled mixture of precursors in the vapor phase. The vapors finally interact on the substrate to form a film of the intelligent material. Figure 13 demonstrates a gas sensors fabricated by CVD.

Figure 13.

Gas sensor fabricated by chemical vapor deposition process.

5.3. Sol–gel

A film formation by sol–gel involves the formation of colloidal suspension of solid particles and cross-linking between particles, followed by evaporation, and finally heating the film to form a dense surface on the substrate (Figure 14).

Figure 14.

Gas sensing film fabricated via a sol–gel technique.

5.4. Spray pyrolysis

The reactants are sprayed on to the target substrate and then react on the surface by continuous heating to form film (Figure 15).

Figure 15.

Schematic representation of spray pyrolysis [131].

5.5. Physical vapor deposition

The starting materials are transferred into the gas phase by evaporation/sputtering. A reactive gas reacts with the metal vapor, to form a compound, which further deposited on the substrate (Figure 16).

Figure 16.

Unit of physical vapor deposition.

5.6. Drop coating

Drop coating is a process by where a paste is made of the desired perovskite powder and a solvent; the mixture is then deposited onto a substrate using an appropriate apparatus followed by the evaporation to form a film (Figure 17).

Figure 17.

Drop coating sensor fabrication.

How does a real gas-sensor response to the analyte? The gas-sensor performance measures from the Vout of RL that cascades Rs (the resistance of gas sensor). The resistance of gas sensor (Rs) and the sensor response (S) obtain from the (Eqs. 6 and 7), respectively;


where Ra is the resistance in air and Rg is the resistance in the air mixed with detected gases. The response time is the time required for the conductance to reach 90% of the equilibrium value after a test gas injection, and the recovery time was the time necessary for a sensor to attain a conductance 10% above its original value in air (Figure 18).

Figure 18.

Electrical circuit diagram of a gas sensor [132].

For instance, YCoO3-based sensors (p-type semiconductor) were tested at temperature range of 100–380°C. The obtained response to the gas (here NO2) versus time can be given by the contribution of two different reactions: (a) oxidation and (b) reducing of the surface (Figure 19). The former is faster and favored at low temperature, and the latter is slower and favored at higher temperatures [133].

Figure 19.

Typical response to (a) NO2 and (b) CO at various temperature [133].

Artificial olfactory systems (AOS) based on metal-oxides chemiresistors is one of the devices which practically used for sensing the air pollutions. YCoO3 sensors doped with various metals were selected for CO and NO2 detection at different temperatures. At around 280°C, the sensor-doped Pd shows a satisfactory sensitivity with a large response speed to CO gas. The same electrode-doped Co was selected for NO2 pollution sensing. The results clearly indicate that a good sensitivity and a fast response (response time, T10–90% = 1 min, and recovery time, T 90–10% = 3 min) at a temperature close to 180 °C [133].

The selectivity toward various target gases such as sulfur dioxide (SO2), ammonia (NH3), hydrogen sulfide (H2S), nitrogen dioxide (NO2) has been discussed before. For instance, 95% sensing response of CoFe2O4 observes toward NO2 compared to other gases at an operating temperature of 150°C, 5 seconds response time and 117 seconds recovery time with NO2 gas [23]. Performing the same sensors for SO2, NH3, and H2S was given just 3%, 6%, and 7%, respectively. The ferrites such as NiFe2O4, ZnFe2O4, MgFe2O4, ZnAl2O4, CoAl2O4, and MgAl2O4 shows the gas response 10–20% for H2S and 1–10% for NH3 gas at 300°C operating temperature.

The sensing response of GaFeO3 toward ethanol vapor at 350°C demonstrates that the resistance declines rapidly in the alcohol atmosphere which exhibited n-type behavior. The response characteristics of the sensors below 350°C for 1 ppm of methanol, ethanol, and isopropanol do not show any significant output. This is due to low thermal energy of the molecules to react with the surface adsorbed oxygen species [105]. Table 6 illustrates some typical experimental results of gas sensing properties of perovskite-based materials.

Perovskite Sensing
Sensing response
Response time
Recovery time
Response temperature (°C) Refs.
LaCoO3 CO 95 423 377 250 [134]
AlNbO3 Ethanol 99 24 100 250 [109]
ZnSnO3 H2 95 1 12 >375 [135]
ZnWO4 H2O 98 15 158 R.T [90]
NiFe2O4 H2S 75 60 300 150 [136]
CoWO4 NH3 90 3 1 Elevated [118]
SmFe1−xCoxO3 O3 <80 600 R.T [137]
La1−xSrxFeO3 CO2 <80 660 300 380 [138]
LaFeO3 C4H10 93 250 [139]
CuFe2O4 LPG 86 5 68 350 [11]
Zn2SnO4 NO2 43 326 200 [79]

Table 6.

Practical efficiencies of some important perovskites-based sensors.


6. Summary and recommendation for future research

The oxygen partial pressure dependence of the point defect concentration, and its conductivity, in perovskite semiconductors allows for their application in sensors. The resistance of the as-mentioned semiconductors can be affected by other gases, such as O2, CO, NH3, hydrocarbons, and ethanol, which create opportunities for developing new chemical sensors.

In addressing diversity and establishing the current chapter, it is necessary to develop the sensors technology by routine reliable synthesis of self-assembled materials including inorganic materials or inorganic–organic nanocomposites for real-life applications and also commercialization. The need of novel perovskites sensing materials with suitable compositions from all reported perovskites (summarized in Tables 4 and 5) as a filler/cover for sensing device for an especial chemical. The need of high-accuracy sensing device in everyday life especially for health care and also environmental concerns requires a systematic management and researches. For example, a suitable combination of perovskite materials can be identified out of 15 components for ethanol sensors. Moreover, suitable manufacturing technologies, free choice of device geometrical properties to attain the indispensable dimensional efficiencies, optimization of surface for the occurrence of conductance, ease of production flow, and investment expenses are immediately required. It seems that the accurate optimization of perovskite materials applicable in gas sensor is influenced by temperature and partial pressure of oxygen. Therefore, the performance of gas sensor depends on the exact height from the sea level.


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Written By

Morteza Enhessari and Ali Salehabadi

Submitted: 28 September 2015 Reviewed: 17 February 2016 Published: 24 August 2016