Ultra-Sensitivity Glucose Sensor Based on Field Emitters
- First Online:
- Cite this article as:
- Liu, H., Qian, X., Wang, S. et al. Nanoscale Res Lett (2009) 4: 1141. doi:10.1007/s11671-009-9372-0
A new glucose sensor based on field emitter of ZnO nanorod arrays (ZNA) was fabricated. This new type of ZNA field emitter-based sensor shows high sensitivity with experimental limit of detection of 1 nM glucose solution and a detection range from 1 nM to 50 μM in air at room temperature, which is lower than that of glucose sensors based on surface plasmon resonance spectroscopy, fluorescence signal transmission, and electrochemical signal transduction. The new glucose sensor provides a key technique for promising consuming application in biological system for detecting low levels of glucose on single cells or bacterial cultures.
KeywordsZnO nanorod arrays Glucose sensor Field emitter High sensitivity
The glucose sensors are becoming an increasingly active area of research due to their applications in biological, chemical analyze, and clinical detection . Many glucose sensors based on surface plasmon resonance (SPR) spectroscopy [2, 3], fluorescence signal transmission (FST) [4, 5, 6, 7, 8], and electrochemical signal transduction (EST) [9, 10, 11], have been reported. However, the sensitivity of these glucose sensors was mostly confined to the millimolar, which restricted their application in the case of lower glucose concentration, such as cellular signal transduction and protein biosynthesis in single cell or bacterial cultures. In order to further promote the sensitivity, intensive efforts have been made in the exploration of a glucose sensors based on nanostructured materials such as carbon nanotubes, semiconductor quantum dots, and nanowires [12, 13, 14, 15, 16].
Due to their unique properties of good biological compatibility and stability, nanomaterials of metal oxides could play an important role in adsorption of biomolecules. They are able to couple with different redox enzymes, which make them particular promising for their applications on biosensors and bioelectronics [17, 18]. Being an important n-type semiconductor with a wide band gap (3.37 eV), ZnO possesses many versatile properties: high optical transparency, semiconducting, piezoelectric, nontoxicity, chemical stability, and electrochemical activity. Recently, one dimensional (1D) ZnO nanostructures for nanodevices such as field emitter , nanopiezotronics , gas and pH sensor , biosensor , transistor , and temperature laser , have received more and more attention due to their distinguished performance, high specific surface area, and facile preparation. 1D ZnO nanostructures have been used as electron mediators and adsorption matrices in amperometric biosensors . Sun et al. [22, 25, 26] constructed a glucose amperometric biosensor using 1D ZnO nanostructures as supporting materials for glucose oxidase (GOx) loading, whose detection limit measured was 0.02 and 0.01 mM. Ren et al.  fabricated a ZnO nanorod-gated AlGa/GaN high electron mobility transistor for the detection of glucose, which showed a linear range from 0.01 to 3.45 mM. In this contribution, we present a new type of nanodevice, a glucose sensor based on field emitter of ZnO nanorod arrays (ZNA). The obvious changes of field emission properties of ZNA caused by surface energy band bending, which induced by surface adsorptions. This new ZNA field emitter-based sensor shows high sensitivity with an experimental limit of detection (LOD) of 1 nM glucose solution and a wide detection range from 1 nM to 50 μM in air at room temperature, which is lower than that of glucose sensor based on FST and EST.
Materials and Apparatus
GOx(100 U mg−1) was purchased from Amersco Inc. (USA). All other reagents (analytical-grade) were purchased from Beijing Chemical Regent Company. The buffer solution was phosphate buffer (6 mM, pH 7.4). The water was purified using a Millipore filtration system.
The arrays of ZNA are characterized by field emission scanning electron microscopy (FESEM, Hitachi, S-4300). The field emission properties of ZNA are measured using a two-parallel-plate configuration in a homemade vacuum chamber at a base pressure of ~1.0×10−6 Pa at room temperature. The sample is attached to one of stainless-steel plates as cathode with the other plate as anode. The distance between the electrodes is 300 μm. A direct current voltage sweeping from 0 to 5,000 V was applied to the sample at a step of 50 V. The emission current is monitored using a Keithley 6485 picoammeter.
Synthesis of ZNA and Glucose Sensors
ZNA were directly grown on a Si (100) wafer with an area of 4 cm2 by a multi-step hydrothermal process . The Si (100) wafer (4 cm2) is equably cut as 16 pieces of same area (0.5×0.5 cm2) samples. The samples for measurement of field emission were then prepared as follow: the films of Si (100) wafers deposited with ZNA were immersed in 2 mL Eppendorf cups with 10 μL of glucose oxidase (GOx) (10 U μL−1) and 1 mL of PBS buffer solution, respectively. Then the β-d-(+) glucose with different concentrations (from 1 nM to 50 μM) was added into the solution and incubated for 30 min at room temperature. After incubation, the samples were washed by pure water for three times. The samples were desiccated via vacuum for field emission measurement.
Results and Discussion
The properties of ZnO nanostructures are significantly influenced by surface adsorptions, which have been attracting great attention because the surface absorptions sometime disturb the fluorescence, field emission, and field effect transistors [30, 31, 32]. In general, the changes of properties caused by surface energy band bending, induced by surface adsorptions. As shown in Fig. 4, GOx specifically catalyzes the oxidation of β-d-(+)-glucose into gluconate and H2O2. H2O2 and ZnO to form ZnO(OH)x on the surface of ZnO nanorods , which depletes the electrons on the ZnO nanorods and yields oxygen ions (O−, O2−, or O2−) . Leading to the electrons on the ZnO nanorods are trapped by the adsorbed oxygen molecules, and the surface depletion region of ZnO nanorods can be formed, making resistance increase. While the H2O2 is raised with the increase of glucose, more electrons are captured by the oxygen molecules at the nanorod surface. Thus, the surface depletion region is widened and the carrier density in the ZnO nanorod is decreased even more. At the same time, gluconolactone can be absorbed strongly on the surface of ZnO nanorods by hydrogen bonding with ZnO(OH)x, which induces the surface passivation to block the electrons emission of ZnO nanorods under electronic field. The surface passivation increases to completely deplete the electrons emission of ZnO nanorods with the increase of ZnO(OH)x on the surface of ZnO nanorods. The result indicates that field emission properties were not observed on the ZNA at the glucose concentration ≥500 nM.
In summary, we demonstrated a new glucose sensor based on the field emitter of ZNA. The results showed that a wide range of glucose concentrations from 1 nM to 50 μM is easily detected, which exhibits ultra-sensitivity for glucose detection. The experimental LOD of glucose concentration is 1 nM, which is lower than previous reported glucose sensor based on EST, FST, and SPR. The new glucose sensor shows the potential to detect low levels of glucose in biological system.
This work was supported by the National Nature Science Foundation of China (10874187 and 20873155) and the National Basic Research 973 Program of China.