Synthesis of Nanosized Zinc-Doped Cobalt Oxyhydroxide Parties by a DroppingMethod and Their CarbonMonoxide Gas Sensing Properties

Two nanostructures of cobalt oxyhydroxide (CoOOH) and Zinc-(Zn-) doped CoOOH (1–4% Zn) are prepared from Co(NO3)2 solution via microtitration with NaOH and oxidation in air. e X-ray diffraction (XRD) analysis results show that a pure state of nano-CoOOH can be obtained at an alkalinity (OH/Co) of 5 with 40C heat treatment aer 6 h. e Zn ions preferentially substitute Co ions in the CoOOH structure, resulting in a decrease of its crystallinity.e disc-like CoOOH nanostructure exhibits good sensitivity to carbonmonoxide (CO) in a temperature range of 40–110Cwithmaximum sensitivity to CO at around 70–80C. When CoOOH nanostructure is doped with 1% Zn, its sensitivity and selectivity for CO gas are improved at 70–80C; further Zn doping to 2% degraded the CO sensing properties of nano-CoOOH. e results of a cross-sensitivity investigation of the sensor to various gases coexisting at early stages of a �re show that the sensitivity of Zn-doped nano-CoOOH is the highest toward CO. Zn-doped nano-CoOOH �lm exhibits a high sensitivity to CO at room temperature, making it a promising sensor for early-stage �re detection.


Introduction
Fire detection systems are designed to respond to the smoke, heat, and electromagnetic radiation generated during smoldering and �aming combustion.It is known that decomposed gases, which are emitted in the preliminary stage of a �re, are generated before smoke.erefore, numerous studies have developed gas sensors for �re detection [1].Based on European standard EN 54, CO is a major by-product at early stages of a �re for all 6 typical �re scenarios [2].Highly sensitive CO sensors can provide early �re detection and reduce false alarm rates [3].
Early �re detection requires that all major by-products of complete and/or incomplete combustion (including CO) should be detected rapidly in a relatively low temperature range of 60-100 ∘ C (i.e., when a �re has just started).Several semiconducting metal oxides have been used in CO gas sensors, including SnO 2 , ZnO, Fe 2 O 3 , BaTiO 3 , TiO 2 , In 2 O 3 , and Zn 2 SnO 4 [4].However, these CO gas sensors require relatively high operating temperatures (above 400 ∘ C) [5][6][7].erefore, CO gas sensors that operate at a relatively low temperature are desirable.
CoOOH (cobalt oxyhydroxide), a high-conductivity active material used in conjunction with nickel hydroxide in Ni-H cells, has been proposed as an alternative material for CO detection at low temperatures [8].In contrast to Co 3 O 4 , CoOOH is a nonstoichiometric oxide; Co has a higher oxidation state (+3) than that of Co 3 O 4 (+2).Some studies on the oxidation of CO [9,10] have shown that cobalt Co (+3) ions are active in the reaction.Results revealed that although response and recovery rates at low temperatures are an issue, the temperature for the maximum CO sensitivity level for CoOOH could be decreased down to 80 ∘ C [11].
Many approaches have been proposed for modifying the sensing properties of semiconductor oxide CO sensors to achieve high sensitivity and selectivity.Grain size reduction is another approach to enhancing gas sensitivity.Zhuiykov and Dowling [12] showed that dumbbell-like CoOOH nanostructures exhibit high sensitivity to CO at room temperature as well as good reproducibility and short response/recovery times.e gas sensitivity is expected to increase when the grain size becomes smaller than the space charge depth [13].us, in this study, nanosized CoOOH was synthesized by a modi�ed dropping method using a peristaltic pump to avoid excessive volume of sodium hydroxide solution drop into cobalt nitrate solution resulting in the rapid growth of precursor particles.
Noble metals (Ag, Au, Pt, and Pd) are well known for enhancing the rate of response and increasing selectivity to a single gas.Shimizu and Egashira [14] indicated that CO sensitivity and selectivity of a nanostructured CoOOH CO sensor can be increased by Au nanoparticle addition.e results also showed that Au nanoparticles enhance the reaction kinetics at low temperature.In addition, Bahlawane et al. [15] indicated that the addition of nickel or zinc affects the conductivity of Co 3 O 4 , generating metal vacancies and decreasing resistivity.Similar results for the addition of SnO 2 to Co 3 O 4 sensor materials were reported [16].SnO 2 addition to Co 3 O 4 leads to an increase in sensor resistance compared to that of undoped Co 3 O 4 .us, it was considered that similar promotion effects can be obtained for nano-CoOOH doped by Zn or Ni.erefore, we attempted to further improve the CO sensing properties by the development of a nanostructure of CoOOH doped with Zn in this study.

Sample Preparation.
In a typical synthesis of CoOOH nanomaterials, 100 mL of 2.5 M NaOH solution was added dropwise into 100 mL of 0.5 M cobalt nitrate (Co(NO 3 ) 2 ⋅6H 2 O) solution with a peristaltic pump to form a Co(OH) 2 precursor.e pH value was kept below 9 during the mixing process.e red color of Co(NO 3 ) 2 ⋅6H 2 O gradually changed to deep blue and �nally to pink.�hen the pH was increased to 9 <pH < 14, the color of the Co(OH) 2 precipitate turned brown with the formation Co(OH) 3 ⋅CoOOH was obtained from Co(OH) 3 by holding in 40 ∘ C water bath for 1∼6 hr.e �nal brown precipitate was �ltered and washed with deionized water three times, then dried at 60 ∘ C for 2 days, and collected as CoOOH.
CoOOH nanopowders doped with Zn were synthesized by a hydrothermal method.Some of the CoOOH nanopowders were ultrasonically dispersed into methanol (200 mL) at about 60 ∘ C. Subsequently, 0.01 M Zn(Ac) 2 was dissolved into the above solution.en, a 0.03 M solution of KOH (65 mL) in methanol was added dropwise.e reaction mixture was stirred for 2 h.e resulting solution was concentrated by the evaporation of the solvent.e resulting white product was centrifuged and then washed with deionized water and ethanol to remove any remaining ions in the �nal product.e CoOOH nanopowders doped with Zn of Zn : Co molar ratios of 0, 1, 2, 3, and 4% were prepared.2.2.Sample Characterization.ermogravimetric/differential thermal analysis (TG/DTA) of the CoOOH-based nanostructure was conducted using a differential thermal analyzer (Setaram Setsys Evolution 1600, France).A gas �ow rate of 100 cm 3 /min was maintained for all experiments.e temperature was increased at a rate of 10 ∘ C/min from room temperature up to 1000 ∘ C. e crystalline phase was identi�ed using an X-ray diffractometer (XRD, Model Rad IIA, Rigaku Co., Tokyo, Japan) with Cu K radiation and an Ni �lter, operated at 30 kV, 20 mA, and a scanning rate of 4 ∘ /min.e surface morphology of the CoOOH-based powders was examined by a �eld-emission scanning electron microscope (FE-SEM, XL-40 FEG SEM, Philips, Eindhoven, Holland).

Gas Sensing Experiments.
Sensing material was prepared in the form of a paste by mixing an appropriate amount of glycerol, 3 g CoOOH or Zn-doped CoOOH powder, and 1mL tetraethyl orthosilicate (TEOS) binder.Nanostructured layers of Zn-doped CoOOH and pure CoOOH were deposited onto indium tin oxide (ITO) substrates between attached Pt electrodes by using an organic binder.Figure 1 shows the structure of the sensing element.
Gas sensing experiments were carried out in a selfdesigned conventional �ow apparatus equipped with heating facility.Each sensor was exposed to a constant �ow of dry air (100 cm 3 /min) or a sample gas (CO or other calibrated gases in dry air), while the electrical resistance of the sensor was monitored by an Agilent 34970A multimeter, which was connected to a PC.e sensor responses was de�ned as    for pure CoOOH and Zn-doped CoOOH nanostructures, where  and  denote the sensor electrical resistance in a sample gas and in air, respectively.Measurements were performed between room temperature and 100 ∘ C with CO content of 100 ppm.e temperature was carefully measured using a K-type thermocouple located adjacent to the CO sensor.e cross-sensitivity of the cobalt oxyhydroxide-based sensors to various gaseous pollutants that are usually by-products of �res was examined.A 100 ppm concentration was chosen for all gases that included CO, except carbon dioxide.3(a) shows that the initial compound is composed of many nanoparticles that were created during the titration reaction.Since the surface energy of nanomaterials tends to aggregate in large particles, CoOOH precursors aggregated into an irregular plated form; the plate size was 50-150 nm in length and 30-40 nm in width.However, some rod-like structures were scattered all over the corner region.ey may be CoOOH nanostructures in a linear plated form.Aer hydrothermal treatment, Co(OH) 3 transformed into a CoOOH structure.e surface morphology is shown in Figure 3(b).e OH functional groups were removed by the heating process, resulting in the irregular plate structure transforming into a disc-like structure.e particle size was 100-150 nm in diameter.e crystalline grain boundaries became obvious.e nanostructure increased the powder surface area and enhanced the sensitivity of the gas sensor.

Results and Discussion
Figure 4 shows TG/DTA measurements of nano-CoOOH in air.TGA data illustrate that aer the initial loss of moisture, accumulated in the nanostructured CoOOH, the loss of weight from 200 to 400 ∘ C was due to a gradual decomposition of CoOOH.Co 3 O 4 formed via the decomposition of CoOOH, with O 2 and H 2 O also produced, when the temperature was above 300 ∘ C. Reaction ( 1) is an exothermic process, as con�rmed by DTA analysis Co 3 O 4 was converted into CoO and O 2 aer a further increase of temperature via the following endothermic reaction: Reaction ( 2) is endothermic.Co 3 O 4 is thermodynamically more stable than CoO.e weight losses in reactions ( 1) and (2) are 10.36% and 6.1%, respectively.e results obtained experimentally are in good agreement with the calculated values of 12.7% and 6.6%, respectively.Figure 6 shows the surface morphology of nano-CoOOH with various Zn doping amounts.e plate and disclike structures of nano-CoOOH gradually transformed into spherical particles as the Zn doping amount increased from 1% to 2%.When the Zn amount was increased to 3%, the nanoparticle size decreased to 30-40 nm in diameter.However, the nanoparticles tended to aggregate and the particle size increased with the Zn doping amount for concentrations above 4%.Some necking structures were found between particles.Added impurities may in�uence the size and morphology of a given crystal by participating in the nucleation and growth, in which many overall factors integrate to dominate the process.Meanwhile, the real behavior of crystal growth in nanocrystalline semiconductors may vary between fractal aggregation in the inauguration period and the subsequent diffusion process [17].Change in morphology would be affected by the nucleation and growth process that would depend upon the above parameters as well as the charge status of the surface states and the dangling bonds.Compared to undoped sample, doped CoOOH nanocrystals shows individual grains clearly and its average particle size shrinks with different impurities.200-400 ∘ C was the decomposition behavior similar to that of nano-CoOOH.It gradually lost its weight (6%) when the Zn doping amount was 1%.However, the weight loss of the nanocomplex signi�cantly decreased (2% and 0.3%) when the Zn doping amount was increased to 2% and 3%.XRD analysis results con�rm that Zn 2+ doped into the crystal lattice CoOOH host, resulting in a signi�cantly reduced amount of nano-CoOOH decomposition.According to the results of XRD, SEM, and TGA/DTA, the Zn doping amount was set to below 3% for subsequent CO sensing tests.temperature was above 70 ∘ C, the electrons hopped between the surface defects of CoOOH, resulting in a decreased resistance.is behavior is similar to the semiconductor conduction mechanism.Figure 8 also shows that the resistance of nano-CoOOH decreased with temperature when the Zn doping amount was increased to 1% in the range of 40 to 100 ∘ C.However, the resistance of nano-CoOOH increased with temperature when the Zn doping amount was over 1%.is indicates that appropriate zinc ion addition can reduce the resistance of nano-CoOOH.In addition, a low doping amount of zinc ions results in a small change in resistance with temperature.However, a rapid increase in resistance with temperature in the range of 60-70 ∘ C was found when the Zn doping amount was over 1%.Excess zinc oxide formed in the CoOOH structure for a high Zn doping amount.erefore, the electron hopping in the metal oxide was easily blocked, resulting in higher resistance.��D analysis results con�rm that the addition of zinc ions resulted in some structural distortion in CoOOH.Hence, the conductivity of Zn-doped CoOOH decreased with temperature in the range of 40 to 60 ∘ C.

Sensing Properties of Nano-CoOOH and Zn-Doped Nano-CoOOH.
Figure 9 shows the sensor response to 1000 ppm CO in air for CoOOH and Zn-doped nano-CoOOH as a function of temperature.CoOOH exhibited a larger response (  6.87) over the temperature range of 70-80 ∘ C. e CO sensing mechanism of CoOOH has been proposed to take the form of gas-phase CO adsorption and desorption at active sites on the nano-CoOOH surface and the form of a surface oxidation reaction between adsorbed CO and adsorbed oxygen atoms (O − ) [21].e surface oxidation reaction of CO − with O − produces CO 2 (3).erefore, the active vacant sites on the CoOOH surface decrease, resulting in a decreased conductivity However, when the temperature exceeded 70 ∘ C, the sensitivity of nano-CoOOH decreased with temperature.CO adsorption is an exothermic reaction, so it is unfavorable to proceed when the temperature exceeds a certain critical point.erefore, the best operating temperature of nano-CoOOH is 70-80 ∘ C for CO detection.Figure 9 also shows that the CO sensitivity of Zn-doped nano-CoOOH-based devices initially increases with temperature, with maximum values (  7.88) at around 70 ∘ C. e results presented in Figure 9 are consistent with similar results recently obtained by Wu et al. [22] and Zhuiykov [23].However, the magnitude of the sensor response to 1000 ppm CO for the nano-CoOOH and 1% Zn-doped nano-CoOOH-based device was  greater than that for those CoOOH thin-�lm screen-printed on the alumina substrate.is is probably due to a much higher surface-to-volume ratio provided by nanotechnology [12].For Zn-doped nano-CoOOH, the maximum sensor response was obtained for the device doped with 1% Zn. 2% Zn doping degraded the CO sensitivity substantially.e results obtained during this investigation agree with published results for an H 2 sensor based on Co-doped SnO 2 nano�bers [24].With excess Zn content, the p-type characteristics of CoOOH regress, and the p-type response decreases accordingly.is indicates that Zn promotes the sensor response to CO until its content in the nanostructure exceeds a critical value.e response and recovery time of sensors based on 1% Zn-doped nano-CoOOH were investigated for different CO concentrations at a measuring temperature of 70 ∘ C as Figure 10 show.e sensor response changed rapidly from the base level upon switching to the different CO concentrations.e steady-state repeatable measuring values were attained at each measuring cycle.Typically, the 90% response and recovery times to 1000 ppm CO at an operating temperature of 70 ∘ C were 20 and 45 s, respectively.A low working temperature of 70 ∘ C combined with high CO sensitivity of 1% Zn-doped nano-CoOOH as well as good response and recovery rate is very attractive for using cobalt oxyhydroxide as a sensor material for semiconductor CO sensors.e promoting effects of Zn in the present sensors are likely to be associated with the enhancement of the conductivity of CoOOH nanostructures.Figure 11 shows response changes as the CO concentration varies from 1 to 1000 ppm.It was revealed that the linearity of the line formed by plotting log  against log [CO] was  2 = 0.9936.e main effects of doping in CoOOH nanoparticles are the change in electronic conductivity and the introduction of defects into the nanoparticles.ese factors play an important role to enhance the sensitivity in nanoparticles sensors.Defects within the crystal structure can improve the adsorption of gas molecules on the nanoparticle surface and the change in the conductivity will change the position of Fermi level in the energy band diagram which governs the electronic transportation between gas molecule and nanoparticle material [25].In addition, the electrical detection of any chemical species is dependent on the surface reactions between the nanoparticles and the chemical molecules.Since the amount of Zn insertion into the nanoparticles was found to be small (1%), it is unlikely that solely chemical affinity can lead to the signi�cant CO gas detection enhancement.Conse�uently, the interference effect experiments were carried out using for sensors based on 1% Zn-doped nano-CoOOH.

Interference Effect of Nano-CoOOH and Zn-Doped Nano-
CoOOH.e cross-sensitivity of CO sensors based on nano-CoOOH and 1% Zn-doped nano-CoOOH to various coexisting gases was investigated.e gases and method were chosen as described in the French Standard [26] because they are applicable to studies and investigations on the �re behavior of substances and materials.e sensor response to the gases was tested in addition to the sensor response to

Conclusion
CoOOH-based nanocomplexes were prepared from a Co(NO  ) 2 solution via a modi�ed dropping method with NaOH and oxidation in air.e optimum working temperature of the CoOOH material for CO detection was roughly 70 ∘ C (  ).Zn doping enhanced the CO sensitivity of the CO sensor based on nano-CoOOH.Zn doping concentrations of 1% to 2% improved the reaction mechanism at a low temperature.Zn-doped nano-CoOOH exhibited a higher CO response than that of nano-CoOOH.e optimal CO sensing was obtained when the sensor was operated at 70 ∘ C, at which the sample exhibited a large response (  ) to 100 ppm CO. e Zn-doped nano-CoOOH also exhibited a high selectivity for CO relative to H 2 ( CO / H 2 ∼ 4) in the CO concentration of 100 ppm.Zn-doped nano-CoOOH �lm exhibits high sensitivity and selectively to CO at room temperature, making it suitable for early �re detection.

F 1 :
Structure of sensing element.

2 F 2 :
XRD patterns of cobalt oxide samples that underwent hydrothermal treatment at 40 ∘ C for various holding times.

3. 1 .
Characterization of Nano-CoOOH.Figure2shows XRD patterns of cobalt oxide samples that underwent hydrothermal treatment at 40 ∘ C for various holding times.e main peaks were attributed to the Co(OH) 2 structure aer one hour.With increasing retention time, the peaks intensity of the Co(OH) 2 structure decreased and then gradually transformed into those of the CoOOH phase.A pure phase of nanosized CoOOH can be obtained with a retention time of 5 h or longer.e results were veri�ed by JC�D cards (JC�DC 14-0673).Figures3(a) and 3(b) show the morphology of CoOOH precursors and nanosized CoOOH prepared by hydrothermal treatment at 40 ∘ C for 6 h, respectively. Figure

F 3 :F 4 :
Morphology of (a) CoOOH precursors and (b) nanosized CoOOH prepared by hydrothermal treatment at 40 ∘ C for 6 h.TG/DTA curves of the nano-CoOOH in air.

Figure 7 (F 5 :
Figure6shows the surface morphology of nano-CoOOH with various Zn doping amounts.e plate and disclike structures of nano-CoOOH gradually transformed into spherical particles as the Zn doping amount increased from 1% to 2%.When the Zn amount was increased to 3%, the nanoparticle size decreased to 30-40 nm in diameter.However, the nanoparticles tended to aggregate and the particle size increased with the Zn doping amount for concentrations above 4%.Some necking structures were found between particles.Added impurities may in�uence the size and morphology of a given crystal by participating in the nucleation and growth, in which many overall factors integrate to dominate the process.Meanwhile, the real behavior of crystal growth in nanocrystalline semiconductors may vary between fractal aggregation in the inauguration period and the subsequent diffusion process[17].Change in morphology would be affected by the nucleation and growth process that would depend upon the above parameters as well as the charge status of the surface states and the dangling bonds.Compared to undoped sample, doped CoOOH nanocrystals shows individual grains clearly and its average particle size shrinks with different impurities.Figure7(a) shows TGA measurements of Zn-doped nano-CoOOH in air.e nanocomplex in the range of

Figure 7 (F 6 :
b) shows that the exothermic peak (327 ∘ C) tended to decrease as the Zn doping amount increased.is indicates that the reaction that Surface morphologies of nano-CoOOH with Zn doping concentrations of (a) 1%, (b) 2%, (c) 3%, (d) 4%, and (e) 0%.transformed some CoOOH into Co 3 O 4 gradually decreased as the Zn doping amount was increased.Moreover, during the �rst stage of 200-400 ∘ C, there is weight loss about 6% to 0.3%, indicating the formation of Zn  Co 3− O 4 nanocomplex.e sharp weight loss at 930 ∘ C has been con�rmed the complete decomposition of nanocomplex structure into ZnO and CoO[18].e CoOOH structure was disrupted when the Zn doping amount was above 2%, resulting in a decrease of high-activity reaction areas of nano-CoOOH.

F 7 :F 8 :
Figure 8 shows the electrical resistance of nano-CoOOH and Zn-doped nano-CoOOH in air as a function of temperature in the range of 40-100 ∘ C. e resistance of CoOOH increased with temperature in the range of 40 to 70 ∘ C.However, the resistance of CoOOH decreased with temperature for temperatures over 70 ∘ C. CoOOH can be regarded as a p-type semiconductor [19].erefore, the free electrons in CoOOH should become more active as the temperature increases, resulting in a decrease in the resistance of CoOOH.However, the resistance of CoOOH increased with temperature in the range of 40 to 70 ∘ C. According to Tobias et al. [20], CoOOH has a layered structure, and the high electrocatalytic activity of the inner sphere reactions on oxide materials is associated with surface defects.Active surface sites are found on step edges and corners of CoOOH.In the range of 40-70 ∘ C, the heat was insufficient to cause electron hopping in the layered structure, resulting in a conductive behavior of the metal oxide.However, when the TGA/DTA curves of Zn-doped nano-CoOOH in air.Electrical resistance of nano-CoOOH and Zn-doped nano-CoOOH in air as a function of temperature in the range of 40-100 ∘ C.

F 9 :
Sensor response to 1000 ppm CO in air for nano-CoOOH and Zn-doped nano-CoOOH as a function of temperature.
As the amount of Zn 2+ increases, the characteristic peak intensity of CoOOH decreases and additional peaks appear.e positions of the main diffraction peaks evidently shi to the smaller angle side with the increasing zinc content.is shi of diffraction angles indicates that Zn 2+ ions have been successfully doped into the crystal lattice of CoOOH host.ese phenomena can be explained in terms of the larger covalent radius of Zn 2+ (0.74 Å) than that of Co 3+ (0.63 Å). e Zn 2+ ions doped into the CoOOH matrix necessarily results in the expansion of the unit-cell volume of the Zn-doped CoOOH nanocrystals owing to the larger covalent radius of Zn 2+ ions.�n addition, the (003) peak exhibits signi�cant broadening, which may be attributed to the disorder in the (003) side of Zn-doped CoOOH nanocrystals.When the amount of Zn 2+ was higher than 2%, the characteristic peak (003) of CoOOH disappeared.is indicates that some Zn 2+ did not enter the crystal lattice of CoOOH, forming a ZnO structure.For Zn 2+ doping amounts higher than 2%, the crystallinity of ZnO increased.e changes in the structure from CoOOH to ZnO are not favorable for CO detection at low temperatures, as con�rmed by electrical conductivity results of the materials.
Zn-Doped Nano-CoOOH.Figure5shows XRD patterns as a function of the Zn doping amount in the nano-CoOOH lattice.e refraction peaks of CoOOH can be indexed to a rhombohedral structure.
[27]isting gases (NO 2 , CO 2 , CH 4 , H 2 , and SO 2 ) typical for various �re scenarios.Figure12shows that sensors using CoOOH have a maximum response (  2) near 70 ∘ C. At that temperature, the gases NO 2 , CO 2 , CH 4 , H 2 , and SO 2 (all 100 ppm) exhibit low interference with CO gas in a nano-CoOOH sensor.e�gurealsoshowsthat the relative response to CO and H 2 ( CO / H 2 ) of nano-CoOOH is near 2.5 (2.46) at 70 ∘ C. erefore, the nanostructures enhance the sensitivity and selectivity of the reaction.Figure9also shows that sensors using Zn-doped CoOOH have a maximum response (  4) near 70 ∘ C. Furthermore, the relative response to CO and H 2 ( CO / H 2 ) of Zn-doped CoOOH is near to 4 (3.64).It seems that the addition of zinc ions can effectively increase the sensitivity and selectivity for the CO gas.According to Potyrailo et al.[27], different parts of the nanoscales can affect the overall measurement upon interaction with different types of gaseous molecules, producing remarkably diverse and distinct differential reactions in real �re situations.erefore, obtaining the required scale of the CoOOH is the keyto achieving a highly selective response to individual gaseous molecules. the