Next Article in Journal
Highly Sensitive and Flexible Capacitive Pressure Sensors Based on Vertical Graphene and Micro-Pyramidal Dielectric Layer
Previous Article in Journal
Raman Spectroscopy Characterization of Multi-Functionalized Liposomes as Drug-Delivery Systems for Neurological Disorders
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Sugar Molecules Detection via C2N Transistor-Based Sensor: First Principles Modeling

1
Department of Electrical and Communication Engineering, College of Engineering, United Arab Emirates University, Al Ain P.O. Box 15551, United Arab Emirates
2
Specialized Rehabilitation Hospital, Abu Dhabi, United Arab Emirates
*
Author to whom correspondence should be addressed.
Nanomaterials 2023, 13(4), 700; https://doi.org/10.3390/nano13040700
Submission received: 5 January 2023 / Revised: 5 February 2023 / Accepted: 8 February 2023 / Published: 11 February 2023

Abstract

:
Real-time detection of sugar molecules is critical for preventing and monitoring diabetes and for food quality evaluation. In this article, a field effect transistor (FET) based on two-dimensional nitrogenated holey graphene (C2N) was designed, developed, and tested to identify the sugar molecules including xylose, fructose, and glucose. Both density functional theory and non-equilibrium Green’s function (DFT + NEGF) were used to study the designed device. Several electronic characteristics were studied, including work function, density of states, electrical current, and transmission spectrum. The proposed sensor is made of a pair of gold electrodes joint through a channel of C2N and a gate was placed underneath the channel. The C2N monolayer distinctive characteristics are promising for glucose sensors to detect blood sugar and for sugar molecules sensors to evaluate food quality. The electronic transport characteristics of the sensor resulted in a unique signature for each of the sugar molecules. This proposed work suggests that the developed C2N transistor-based sensor could detect sugar molecules with high accuracy.

1. Introduction

Carbohydrates are important organic substances for both people and plants because they play a number of crucial roles in growth and development. Glucose and fructose have significant importance since they are important nutrients in people diet. Moreover, xylose levels are measured to check if there is problem with peoples’ ability to absorb nutrients. They can be found naturally in a variety of foods or additives. The detection of these sugar molecules is highly important to evaluate food quality [1,2]. As well, reliable and quick sugar detection during food production and storage is highly important. The detection of glucose, fructose, and xylose can be utilized to assess food quality since they reveal details about a food product’s nutritional value, flavor, and sweetness.
Simple sugars such as glucose are frequently present in fruits, vegetables, and grains. High glucose levels in a food product can be a sign that it is high in carbohydrates and energy, but they can also be a sign that the food is overripe or that it has been processed at high temperatures [3]. Fructose is frequently present in fruits and honey. A food product with high fructose levels may be sweet and have a lot of natural sugars. Fructose content, which is frequently seen in processed foods, can also be an indication that the product has been sweetened with high fructose corn syrup [4]. Dietary carbohydrates contain xylose. Fruits, cereals, bread, and vegetables, including potatoes, peas, and carrots, all include it as part of their sugar composition. Detecting xylose can be used to identify the presence of specific types of fruits or vegetables in a food product. One way to recognize the presence of specific fruits and vegetables in a food product is to look for the sugar xylose, which is frequently present in certain foods. It is possible to identify and confirm the composition of a food product by analyzing the xylose content in a sample.
A large number of people worldwide suffer from diabetes [5,6], and it can lead to significant complications, such as heart attack, kidney failure, and blindness [7,8]. Moreover, glucose metabolism anomalies might lead to various diseases and problems [6,9]. Thus, it is highly crucial to monitor glucose levels and to supervise patients with diabetes. Researchers have developed various types of biosensors to help patients track their glucose concentration without the need to go to the hospital [10].
Blood sugar levels detection is a highly critical research area [11,12]. The two main electrochemical glucose identification methods are non-enzymatic or enzymatic [13]. Enzymatic methods utilize detection elements such as glucose oxidase enzyme (GOx). These methods oxidize glucose and generate compounds that can be detected, such as CO2, O2, or H2O2. When glucose oxidase interacts with enzymatic sensors, it releases oxygen, gluconolactone, and hydrogen. The glucose present on the sensor’s surface oxidizes and is expressed in typical current values. These sensors have high selectivity, however, they still face some challenges, such as: (i) degraded sensitivity with time due to enzymatic leaking; (ii) short life-time and low stability; and (iii) reduction in high overpotentials [14].
Until this time, most of the available blood glucose sensors depend on glucose oxidase (GOx) enzyme-based recognition unit [11,15]. Enzymatic glucose-based sensors have remarkable selectivity and sensitivity; however, they have low detection limits and are not stable with temperatures and humidity variations. Additionally, they require costly enzymes. Currently, research work is being focused on glucose biosensors that are cheaper, non-enzymatic, and sensitive to detect body glucose by using various body fluids, such as saliva, tear, or sweat for the purpose of self-monitoring of diabetes [12].
Various popular techniques can be used to detect glucose such as colorimetric and fluorometric methods [16,17,18,19,20,21]. The main idea behind these methods is using a chemical indicator or a fluorescent probe that changes colour or fluorescence intensity due to the addition of glucose target [21]. These methods are suitable for point-of-care applications as they are relatively simple, easy to use, and cheap. However, they lack the sensitivity of other techniques as the colour change or fluorescence signal can be influenced by other factors, such as temperature, pH, and the presence of other analytes.
One more popular method to detect glucose is paper-based sensors, which is also known as lateral flow assays [22]. Paper-based methods consist of a strip of paper coated with a reagent that is sensitive toward glucose. The targeted glucose sample is added to the strip, and the presence of glucose is identified by the change in colour and fluorescence [22,23]. These devices are popular as they are easy to use, portable, cheap, and simple. However, their signal can be changed due to the presence of other analytes and they are not as sensitive as other techniques [24].
Recently, there has been an increasing interest in electrochemical sensors [25] and biosensors to detect glucose since they provide high selectivity and sensitivity. Other various methods are being explored for the potential of glucose detection such as Raman spectroscopy [26] and mass spectrometry [27].
Electrochemical biosensing is applied extensively to detect biomolecules to diagnose and detect various diseases [28,29]. The biosensing research field has witnessed huge enhancement due to the development of field effect transistors biosensors. These biosensors have shown great performance due to their reliable detection, high sensitivity, and real time monitoring [30]. The sensing mechanism of transistor-based sensors depends on the change in the channel electrical resistance due to molecular addition and adsorption [31,32,33]. These devices have shown effective identification of molecules, ions, bacteria, and several biological entities [28,31,34,35,36,37].
As the biosensor performance relies on its surface to enhance the charge transfer, two-dimensional graphene including functionalized graphene nanomaterial is considered the best selection for glucose sensors. Platinum-functionalized graphene was utilized to detect glucose with a 0.6 M detection limit [38]. Moreover, gold nanoparticles were explored to detect 0.3 μM concentration of glucose [39]. Several nanomaterial biosensors, such as graphene and carbon nanotubes, were used for glucose detection. However, it poses the challenge of potential toxicity [40,41]. Various technologies were studied to design electrochemical reaction sensors based on non-enzymatic glucometers, including carbon-based materials, such as reduced graphene oxide (GO), graphene, metal nanoparticles [42,43], and carbon nanotube (CNT) [44,45].
Carbon nanomaterials doped with nitrogen have better performance in biosensors compared to pristine carbon. Carbon nanomaterials doped with nitrogen are used in biosensors because of their special characteristics that make them suitable for utilization in these kinds of applications [46]. Because the surface to volume ratios of carbon nanomaterials, such as carbon nanotubes and graphene are high, a lot of biomolecules can be adsorbed onto the surface [47]. Nitrogen atom doping of carbon nanomaterials improves their electrical conductivity, increasing their sensitivity for sensing applications [48]. It is possible to create nitrogen-doped carbon nanomaterials by adding nitrogen to carbon nanomaterials. These materials are more stable and have better electrical conductivity than pristine carbon. The electrical conductivity of carbon nanomaterials can be improved by nitrogen atoms acting as electron acceptors, increasing their sensitivity for biosensing applications [49]. Additionally, nitrogen doping can increase the carbon nanostructures’ chemical stability, strengthening their resistance to degradation. Carbon nanomaterials that have been doped with nitrogen are less toxic and more stable in biological settings, which can increase their biocompatibility. Additionally, compared to pristine carbon, nitrogen-doped carbon nanomaterials have demonstrated enhanced stability and biocompatibility, making them appropriate for application in biosensors [50]. Overall, nitrogen-doped carbon nanomaterials are a desirable option for use in biosensors due to their large surface area, electrical conductivity, and biocompatibility [46,48,50].
The novelty of this work is based on using C2N-FET for the first time as a sensor to recognize each of the sugar molecules. To the best of our knowledge, this is the first research that utilizes FET consisting of C2N channel and a pair of gold electrodes to identify glucose, fructose, and xylose molecules.
Within the many carbon nanostructures rich with nitrogen, C2N has been synthesized and computationally studied [51,52]. In this work, first principles modeling was used to study the sensing properties of C2N field effect transistor (FET) for the purpose of non-enzymatic glucose detection. This is the first report that uses C2N FET to detect glucose.
In this research, a field effect transistor based on two-dimensional nitrogenated holey graphene (C2N) was developed, designed, and tested to identify the sugar molecules including xylose, fructose, and glucose. Both density functional theory and non-equilibrium Green’s function (DFT + NEGF) were used to study the designed sensor. Various electronic characteristics were studied such as: work function, density of states, electrical current, and transmission spectrum. The proposed sensor is made of a pair of gold electrodes joint through a channel of C2N and a gate was placed underneath the channel. The C2N monolayer distinctive characteristics are promising for glucose sensors to detect blood sugar. Moreover, the detection of the three types of sugar molecules can be used to evaluate food quality.

2. Materials and Methods

The simulation work was produced using the graphical user interface of Virtual Nanolab and the Quantumwise Atomistix Toolkit (QuantumATK 2018.06 developed by Copenhagen, Denmark). United Arab Emirates University High Performance Computing (HPC) was utilized to run ATK-VNL simulations. Seven nodes with a total of 36 processors each have been used for HPC. As a result, 252 processors were used to complete the task.

2.1. Sensor Setup and Configuration

The setup and configuration of the C2N based sensor were conducted and investigated via Quantumwise (ATK-VNL). Figure 1 displays the nanoscale system setup. The left and right gold electrodes, the C2N central area which consists of one layer of C2N, and the gate terminal located beneath the central region make up the C2N metal-semiconductor-metal junction system. The gate is formed of two layers: a metallic layer and a 2.9 Å dielectric layer of SiO2 with a dielectric constant of 3.9. The C2N channel width is 13 Å and length is 28 Å, while the gold electrode length is 10 Å. The system consists of 209 atoms. First-principle electronic transport measurements were generated to detect each of the sugar molecules electronic signature. A, B, and C are indictors for A-, B-, and C-direction as displayed in Figure 1.
Figure 2 shows the atomic structure for each of the sugar molecules: glucose, fructose, and xylose. Due to their unique electronic and chemical structure, each molecule has a distinct electronic signature. Various electronic transport characteristics, including device density of states, transmission spectrum, work function, and electronic current, are generated for the bare C2N transistor and for the transistor with each of the sugar molecules. Figure 3 shows the C2N transistor structures with fructose. The big hollow site shown in Figure 3, which is the most stable site for xylose, fructose, and glucose for the adsorption of each of the sugar molecules [53]. The gate voltage was fixed at 1V, and finite bias voltage was fixed between right and left electrode and ranged from 0 to 1 V.

2.2. Computational Method

First-principles method is conducted within the generalized gradient approximation (GGA) exchange correlation function. For the plane-wave basis set, a cut-off energy of 80 Ha is utilized.
A 1 × 1 × 1 k-mesh is used to optimize the structure, while a denser mesh of 2 × 2 × 135 is used for the electronic transport calculations. The systems are optimized till the forces on each atom in the supercell are less than 0.05 eV/Å.
Each of the sugar molecules was optimized separately. Moreover, the gold atoms were optimized before forming the electrodes. Then, the C2N channel was optimized. At the end, the whole sensor with each of the sugar molecules was optimized. 1 × 1 × 1 k-mesh and Monkhorst-Pack grid, a type of uniform grid that is known to provide good convergence, were used for optimization as conducted by previous studies [54].
For the electronic transport characteristics such as IV a denser k-mesh grid was used. Quantumatk website [55] and other articles [56] recommend using 100 along the transport direction which is represented as the C direction in Figure 1. Thomas et al. used 1 × 1 × 100 k-point samplings along the device transport direction to generate the IV calculations [57]. In this work, a 2 × 2 × 135 k-point was utilized.
The electronic transport characteristics are generated by utilizing the density functional theory and non-equilibrium Green’s function (NEGF) approach. The sugar molecules are positioned on the C2N monolayer to investigate the transport characteristics of the C2N monolayer and the sugar molecules. Three areas are included: the left electrode, the right electrode, and the scattering region with each of the sugar molecules. The k-point grid for the electrodes and the scattering region calculation is 2 × 2 × 135.
The computed transmission probability of the electrons with energy (E) is generated, as shown in Equation (1):
    T E = T r Γ R E ξ R Γ L E ξ A E  
Here, Γ L E and Γ R E are the broadening matrix for the left and right electrodes, respectively. ξ A and ξ R refer to the advanced and retarded Green’s function, respectively.
The zero bias conductance is generated with the relation ξ = ξ 0 T E F , where ξ 0 = 2 e 2 / h is the quantum conductance. E and h refer to the electron charge and Planck’s constant, respectively.
The difference of the Fermi functions is used to calculate the integration of T E , V over the energy window f S ,   D E = 1 + exp E E F e V S , D / k B T 1 , which gives the total current displayed in Equation (2):
I = 2 e h d E   T E , V f S E f D E
QuantumATK generates the density of state based on the following equations [58]:
The DeviceDensityOfStates (DDOS) D E is computed via the spectral density matrix σ E = σ L E + σ R E , where L/R refers to the left and right electrodes.
The local density of states (LDOS) is computed as:
D E , r = i j σ i j E i r j r
The basis set orbitals i r are real functions in QuantumATK through the use of solid harmonics.
The device density of state is then obtained by integrating LDOS over all space:
D E = d r D E , r = i j σ i j E S i j
where, S i j = i r j r d r is the overlap matrix. Introducing M i E = j σ i j E S i j , the equation can be written as
D E = i M i E
where M i E is considered as the contribution of DDOS from orbital i. M i E is a spectral Mulliken Population with:
M i = M i E f ( E μ k B T )   d E

3. Results and Discussion

The electrical transport properties were generated for the C2N FET to achieve the practical investigation of the designed C2N FET sensor to specifically detect each of the sugar molecules. Density of states, work function, transmission spectrum, current variation, and current-voltage characteristics were generated for the C2N FET, the C2N FET with the presence of glucose molecule, the C2N FET with the presence of fructose molecule, and for the C2N FET with the presence of xylose molecule.

3.1. Device Density of States (DDOS)

A distinct and significant change in the FET Device DOS have been noticed in the presence of the different sugar molecules. Figure 4 displays a comparison of the DDOS for the bare C2N FET (without any target molecule) and for the C2N FET in the presence of each of the sugar molecules. Figure 4a shows that the bare C2N FET have more energy states than the C2N FET in the presence of glucose molecule, which can be observed at the energy levels of −3.8, −3.6, −3.2, and −2.9 eV. Furthermore, the presence of fructose molecule affected the C2N FET DOS differently, as displayed in Figure 4b, where a new energy spike can be observed at energy level 3.85 eV. Similarly, a significant change in DOS can be noticed in the C2N FET when it is exposed to xylose molecule, as displayed in Figure 4c. Two new energy spikes were noticed at energy levels of 3.7 and 3.9 eV, as shown in Figure 4c.
Figure 5 displays the partial DOS, which reflects a closer look and more detailed information about the effect of each of the sugar molecules on the DDOS. It was noticed that, when a target molecule is added to the device, one unique peak is increased in the DDOS due to glucose (Figure 5a) or fructose (Figure 5b) or xylose (Figure 5c). This indicates that adding each of the sugar molecules results in new electronic states within the energy range of that peak. This may indicate that the sugar molecule is interacting with the C2N channel and modifying its electronic structure. The change in the DDOS is caused by the sugar molecule accepting or donating electrons from the channel material or by forming chemical bonds between the target molecule and the C2N channel.
The DOS of a material is defined as the measure of the number of available electronic states within a certain energy range. The DOS changes due to the presence of various types of molecules since they can introduce defects of impurities into the material, which leads to a change in the electronic structure of the material. As an example, when the material is exposed to a target molecule, the impurities can result in additional energy levels, which can modify the density of states. Moreover, impurities affect electronic states symmetry, which modifies the DOS. Additionally, the mechanical and chemical properties can be changed leading to a change in the DOS. The variation in the DOS depends on the type and concentration of the defects.

3.2. Work Function

The C2N FET response to each of the sugar molecules is investigated by calculating the work function displayed in Figure 6. The calculated work function value for the C2N FET is 5.92 eV; for the C2N FET with glucose, it is 6.08 eV; for the C2N FET with fructose, it is 6.05 eV; and for the C2N FET with xylose, it is 6.106.
Figure 6 shows an increment in the work function for the C2N FET with each of the sugar molecules in comparison to the bare C2N FET. This increment indicates that the adsorption of each of the sugar molecules leads to a decrement in the electron mobility. The work function increment is caused by the cloud charge transfers from the C2N channel toward the sugar molecules. The study’s findings are in line with previous research work [53].
The increment in the work function of C2N due to presence of each of the sugar molecules is believed to be associated with changes in the electronic characteristics of the C2N material due to the interaction between each of the target molecules and the C2N surface [53]. The energy needed to remove an electron from the surface can increase when the target molecule accepts electrons from the C2N material, increasing the work function.
Moreover, it is expected that the movement of charge carriers from the C2N material to the sugar molecules leads to a decrement in the density near Fermi level. Thus, the Fermi level shifts to higher energies leading to an increment in the work function.

3.3. Transmission Spectrum

Figure 7 shows the transmission spectra T(E) for the C2N FET with and without each of the sugar molecules (glucose, fructose, and xylose) at different biases: (a) V = 0 V, (b) V = 0.2 V, and V= 0.4 V. The figure shows the changes in transmission spectrum when different sugar molecules are added at a varying applied voltage. The transmission spectrum has a low value in the energy range [0.4, 0.9] eV because of the energy window within the band gap of the semiconducting C2N channel.

3.4. Current-Voltage

The current vs. voltage characteristics for the C2N FET sensor and for each of the sugar molecules adsorbed via the C2N FET sensor are shown in Figure 8. A fixed 1 V gate potential was used while the Vds was set to 0.2, 0.4, 0.6, 0.8, and 1 V. Figure 8 shows the current voltage curves for C2N FET at 0.2, 0.4, 0.6, 0.8, 1 V before and after the addition of each of the sugar molecules. The variation in current reading with the addition of sugar molecules indicates successful detection. The adsorbed target molecule interacts with the C2N-FET and changes its conductivity by changing the carriers’ concentration. C2N is a semiconducting nanomaterial, which has a nonlinear resistance, resulting in a nonlinear IV curve, as shown in Figure 8.
The current of the C2N-FET differs noticeably for each sugar molecule. The size, electrical state, and way that each sugar molecule interacts with the C2N-FET channel are all unique. When the gate potential was fixed at 1 V and the bias voltage among the left and right electrodes was fixed at 0.4 V, the created sensor produced the best results. The best sensitivity was achieved by setting the bias voltage at 0.4 V, as shown in Figure 8. This work is a proof of concept that the developed C2N-FET can be utilized to detect the different types of sugar molecules.
The sensor showed the best sensitivity at 0.4 V bias voltage. Figure 9 shows the sensor’s response (change in current), where the highest variation in the electrical signal was due to glucose molecule adsorption. These results show that the device has high selectivity for glucose and results in a distinct electrical current for each of the sugar molecules. The current variation is due to the change in the charge and the electrical potential after introducing the target molecules which alters the charge carriers’ density. Thus, the sensor conductivity and current change.
This work is a proof of concept that the modeled and studied C2N FET can be utilized as a sensor for sugar molecules detection, such as glucose, fructose, and xylose. This research indicates that each of the sugar molecules have a unique electronic signature that can be identified via the designed C2N FET.
After employing the computational methods to detect each of the sugar molecules, the results of the sensor can be utilized to identify the performance in real-time applications. Such computational methods provide valuable results, such as how each of the sugar molecules will interact with the sensor. These results can be utilized to optimize the sensor design and performance in terms of stability, sensitivity, and selectivity. Moreover, the used computational method provides insights into the electronic transport characteristics of the system due to each of the sugar molecules. These electronic properties include electron density, work function, transmission spectrum, and current–voltage measurements. These results can be utilized to understand how the target molecule interacts with the sensor and affects the sensor’s performance.
After the validation of the sensor via computational methods, the sensor can be designed, fabricated, and tested in real-time applications. Then, the sensor’s performance can be evaluated by comparing the computational expectations with the experimental findings.
In this work, C2N FET was utilized to detect each one of the sugar molecules separately, where each one of them resulted in a unique electronic signature and unique variation in current indicating the possibility of detecting each of them in real-time applications. The highest sensitivity was toward glucose molecule, which can be used to monitor and control diabetes.
The addition of a mixture of two or three sugar molecules is also expected to result in a specific variation in current and a unique electronic signature, since each sugar molecule interacts with the C2N channel and modifies its electronic properties in a unique way.
In general, the employed computational method results in valuable information about the performance of the designed sensor. However, computational methods do not show the limit of detection of the sensor in real-time applications. The limit of detection can only be identified by experiment by measuring the response of the fabricated sensor toward various concentration of the target analyte.
Combining both computational method with experimental data can be used to overcome the limitations of such technology. This comparison leads to identifying the potential sources of error and uncertainty. It is worth mentioning that the employment of computational methods enables researchers to suggest future directions to study to enhance the sensor’s performance and then test it experimentally.
Introducing structure variables, such as surface roughness, pores, and alien molecules to a sensor, will result in a significant effect on its electronic properties and performance.
In terms of work function, the existence of surface roughness or defects lead to a shift in the work function. Moreover, surface roughness can also affect the amount of charge that can be stored on the device, which affects its sensitivity.
In terms of density of states, impurities and defects can generate localized states within the bandgap of the sensor, which can modify electrical current and the conductivity of the device. Moreover, surface roughness and pores can affect the DOS by creating additional pathways for charge carriers to pass through.
In terms of current, impurities and defects work as scattering centers for the charge carriers, which might lead to a reduction in the device mobility and current. Introducing structure variables impact the electronic properties and performance of a sensor, affecting its work function, density of states, and current.

4. Conclusions

Real-time identification of the different sugar molecules is essential for monitoring and preventing diabetes and to evaluate food quality. In this research, a field effect transistor based on two-dimensional nitrogenated holey graphene (C2N) was designed, developed, and tested to identify the sugar molecules, including xylose, fructose, and glucose. To investigate the characteristics of this device, non-equilibrium Green’s function and density functional theory (NEGF + DFT) were utilized. Various electronic properties were studied, including density of states, work function, transmission spectrum, and electrical current. The proposed sensor consists of a pair of gold electrodes connected via a channel of C2N and a gate. The electronic characteristics of the C2N FET changed because of the adsorption of the target molecules. The measurable variations in the electronic characteristics with each sugar molecule validate the potential of the C2N FET sensor in detecting sugar molecules. The C2N monolayer distinctive characteristics are promising for glucose sensors to detect blood sugar.

Author Contributions

Conceptualization, A.W., F.A., S.A. and M.H.; methodology, A.W., F.A., S.A. and M.H.; software, A.W. and F.A.; validation, A.W., F.A., S.A. and M.H.; formal analysis, A.W., F.A., S.A. and M.H.; investigation, A.W., F.A., S.A. and M.H.; resources, A.W., F.A., S.A. and M.H.; writing—original draft preparation, A.W., F.A. and S.A.; writing—review and editing, A.W., F.A., S.A. and M.H.; visualization, A.W., F.A., S.A. and M.H.; supervision, F.A.; project administration, F.A.; funding acquisition, F.A. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Informed Consent Statement

Not applicable.

Data Availability Statement

All data generated or analyzed during this study are included in this published article.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Liu, K.; Wang, X.; Luo, B.; Wang, C.; Hou, P.; Dong, H.; Li, A.; Zhao, C. Enzyme-Free Electrochemical Sensors for In Situ Quantification of Reducing Sugars Based on Carboxylated Graphene–Carboxylated Multiwalled Carbon Nanotubes–Gold Nanoparticle–Modified Electrode. Front. Plant Sci. 2022, 13. [Google Scholar] [CrossRef] [PubMed]
  2. Crespo-Rosa, J.R.; Foca, G.; Ulrici, A.; Pigani, L.; Zanfrognini, B.; Cubillana-Aguilera, L.; Palacios-Santander, J.M.; Zanardi, C. Simultaneous Detection of Glucose and Fructose in Synthetic Musts by Multivariate Analysis of Silica-Based Amperometric Sensor Signals. Sensors 2021, 21, 4190. [Google Scholar] [CrossRef] [PubMed]
  3. Rippe, J.M.; Angelopoulos, T.J. Sugars and Health Controversies: What Does the Science Say? Adv. Nutr. 2015, 6, 493S–503S. [Google Scholar] [CrossRef]
  4. Rippe, J.M.; Angelopoulos, T.J. Sucrose, High-Fructose Corn Syrup, and Fructose, Their Metabolism and Potential Health Effects: What do We Really Know? Adv. Nutr. 2013, 4, 236–245. [Google Scholar] [CrossRef]
  5. Association, A.D. Diagnosis and Classification of Diabetes Mellitus. Diabetes Care 2010, 33, S62–S69. [Google Scholar] [CrossRef]
  6. Sehit, E.; Altintas, Z. Significance of nanomaterials in electrochemical glucose sensors: An updated review (2016–2020). Biosens. Bioelectron. 2020, 159, 112165. [Google Scholar] [CrossRef]
  7. Gregg, E.W.; Sattar, N.; Ali, M.K. The changing face of diabetes complications. Lancet Diabetes Endocrinol. 2016, 4, 537–547. [Google Scholar] [CrossRef]
  8. Nathan, D.M. Long-Term Complications of Diabetes Mellitus. N. Engl. J. Med. 1993, 328, 1676–1685. [Google Scholar] [CrossRef]
  9. Lee, A.K.; Warren, B.; Lee, C.J.; McEvoy, J.W.; Matsushita, K.; Huang, E.S.; Sharrett, A.R.; Coresh, J.; Selvin, E. The Association of Severe Hypoglycemia with Incident Cardiovascular Events and Mortality in Adults with Type 2 Diabetes. Diabetes Care 2017, 41, 104–111. [Google Scholar] [CrossRef]
  10. Gubala, V.; Harris, L.F.; Ricco, A.J.; Tan, M.X.; Williams, D.E. Point of Care Diagnostics: Status and Future. Anal. Chem. 2012, 84, 487–515. [Google Scholar] [CrossRef]
  11. Mani, V.; Devasenathipathy, R.; Chen, S.-M.; Wang, S.-F.; Devi, P.; Tai, Y. Electrodeposition of copper nanoparticles using pectin scaffold at graphene nanosheets for electrochemical sensing of glucose and hydrogen peroxide. Electrochim. Acta 2015, 176, 804–810. [Google Scholar] [CrossRef]
  12. Dong, X.-C.; Xu, H.; Wang, X.-W.; Huang, Y.-X.; Chan-Park, M.B.; Zhang, H.; Wang, L.-H.; Huang, W.; Chen, P. 3D Graphene–Cobalt Oxide Electrode for High-Performance Supercapacitor and Enzymeless Glucose Detection. ACS Nano 2012, 6, 3206–3213. [Google Scholar] [CrossRef]
  13. State, S.; Enache, L.-B.; Potorac, P.; Prodana, M.; Enachescu, M. Synthesis of Copper Nanostructures for Non-Enzymatic Glucose Sensors via Direct-Current Magnetron Sputtering. Nanomaterials 2022, 12, 4144. [Google Scholar] [CrossRef]
  14. Sakr, M.A.; Elgammal, K.; Delin, A.; Serry, M. Performance-Enhanced Non-Enzymatic Glucose Sensor Based on Graphene-Heterostructure. Sensors 2020, 20, 145. [Google Scholar] [CrossRef]
  15. Sternberg, R.; Barrau, M.-B.; Gangiotti, L.; Thévenot, D.R.; Bindra, D.S.; Wilson, G.S.; Velho, G.; Froguel, P.; Reach, G. Study and development of multilayer needle-type enzyme-based glucose microsensors. Biosensors 1989, 4, 27–40. [Google Scholar] [CrossRef]
  16. Huang, Z.; Zheng, L.; Feng, F.; Chen, Y.; Wang, Z.; Lin, Z.; Lin, X.; Weng, S. A Simple and Effective Colorimetric Assay for Glucose Based on MnO2 Nanosheets. Sensors 2018, 18, 2525. [Google Scholar] [CrossRef]
  17. Wang, C.; Li, J.; Tan, R.; Wang, Q.; Zhang, Z. Colorimetric method for glucose detection with enhanced signal intensity using ZnFe2O4–carbon nanotube–glucose oxidase composite material. Analyst 2019, 144, 1831–1839. [Google Scholar] [CrossRef]
  18. Wu, X.; Yin, J.; Liu, J.; Gu, Y.; Wang, S.; Wang, J. Colorimetric detection of glucose based on the binding specificity of a synthetic cyclic peptide. Analyst 2020, 145, 7234–7241. [Google Scholar] [CrossRef]
  19. Klonoff, D. Overview of Fluorescence Glucose Sensing: A Technology with a Bright Future. J. Diabetes Sci. Technol. 2012, 6, 1242–1250. [Google Scholar] [CrossRef]
  20. Gao, J.; Zhou, J.; Qu, X. Fluorometric Method for Quantitative Determination of Glucose and Its Application to Human Serum. Anal. Sci. 2005, 21, 409–412. [Google Scholar] [CrossRef]
  21. Wang, C.; Tan, R.; Li, L.; Liu, D. Dual-Modal Colorimetric and Fluorometric Method for Glucose Detection Using MnO2 Sheets and Carbon Quantum Dots. Chem. Res. Chin. Univ. 2019, 35, 767–774. [Google Scholar] [CrossRef]
  22. Ilacas, G.C.; Basa, A.; Nelms, K.J.; Sosa, J.D.; Liu, Y.; Gomez, F.A. Paper-based microfluidic devices for glucose assays employing a metal-organic framework (MOF). Anal. Chim. Acta 2019, 1055, 74–80. [Google Scholar] [CrossRef]
  23. Hou, Y.; Lv, C.-C.; Guo, Y.-L.; Ma, X.-H.; Liu, W.; Jin, Y.; Li, B.-X.; Yang, M.; Yao, S.-Y. Recent Advances and Applications in Paper-Based Devices for Point-of-Care Testing. J. Anal. Test. 2022, 6, 247–273. [Google Scholar] [CrossRef] [PubMed]
  24. Kasetsirikul, S.; Shiddiky, M.; Nguyen, N.-T. Challenges and perspectives in the development of paper-based lateral flow assays. Microfluid. Nanofluidics 2020, 24, 17. [Google Scholar] [CrossRef]
  25. Heller, A.; Feldman, B. Electrochemical Glucose Sensors and Their Applications in Diabetes Management. Chem. Rev. 2008, 108, 2482–2505. [Google Scholar] [CrossRef] [PubMed]
  26. Scholtes-Timmerman, M.J.; Bijlsma, S.; Fokkert, M.J.; Slingerland, R.; van Veen, S.J.F. Raman Spectroscopy as a Promising Tool for Noninvasive Point-of-Care Glucose Monitoring. J. Diabetes Sci. Technol. 2014, 8, 974–979. [Google Scholar] [CrossRef] [PubMed]
  27. Wahjudi, P.N.; Patterson, M.E.; Lim, S.; Yee, J.K.; Mao, C.S.; Lee, W.N.P. Measurement of glucose and fructose in clinical samples using gas chromatography/mass spectrometry. Clin. Biochem. 2010, 43, 198–207. [Google Scholar] [CrossRef]
  28. Wu, G.; Dai, Z.; Tang, X.; Lin, Z.; Lo, P.K.; Meyyappan, M.; Lai, K.W.C. Biosensing: Graphene Field-Effect Transistors for the Sensitive and Selective Detection of Escherichia coli Using Pyrene-Tagged DNA Aptamer (Adv. Healthcare Mater. 19/2017). Adv. Healthc. Mater. 2017, 6, 1700736. [Google Scholar] [CrossRef]
  29. Piccinini, E.; Bliem, C.; Reiner-Rozman, C.; Battaglini, F.; Azzaroni, O.; Knoll, W. Enzyme-polyelectrolyte multilayer assemblies on reduced graphene oxide field-effect transistors for biosensing applications. Biosens. Bioelectron. 2017, 92, 661–667. [Google Scholar] [CrossRef]
  30. Fu, W.; Jiang, L.; van Geest, E.P.; Lima, L.M.C.; Schneider, G.F. Sensing at the Surface of Graphene Field-Effect Transistors. Adv. Mater. 2017, 29, 1603610. [Google Scholar] [CrossRef]
  31. Zhan, B.; Li, C.; Yang, J.; Jenkins, G.; Huang, W.; Dong, X. Graphene Field-Effect Transistor and Its Application for Electronic Sensing. Small 2014, 10, 4042–4065. [Google Scholar] [CrossRef]
  32. Fenoy, G.; Marmisollé, W.; Azzaroni, O.; Knoll, W. Acetylcholine biosensor based on the electrochemical functionalization of graphene field-effect transistors. Biosens. Bioelectron. 2019, 148, 111796. [Google Scholar] [CrossRef]
  33. Wasfi, A.; Awwad, F.; Gelovani, J.G.; Qamhieh, N.; Ayesh, A.I. COVID-19 Detection via Silicon Nanowire Field-Effect Transistor: Setup and Modeling of Its Function. Nanomaterials 2022, 12, 2638. [Google Scholar] [CrossRef]
  34. Zhang, X.; Jing, Q.; Ao, S.; Schneider, G.F.; Kireev, D.; Zhang, Z.; Fu, W. Ultrasensitive Field-Effect Biosensors Enabled by the Unique Electronic Properties of Graphene. Small 2020, 16, 1902820. [Google Scholar] [CrossRef]
  35. Tan, X.; Yang, M.; Zhu, L.; Gunathilaka, G.; Zhou, Z.; Chen, P.Y.; Zhang, Y.; Cheng, M.M.C. Ultrasensitive and Selective Bacteria Sensors Based on Functionalized Graphene Transistors. IEEE Sens. J. 2022, 22, 5514–5520. [Google Scholar] [CrossRef]
  36. Verhulst, A.S.; Ruić, D.; Willems, K.; Dorpe, P.V. Boosting the Sensitivity of the Nanopore Field-Effect Transistor to Translocating Single Molecules. IEEE Sens. J. 2022, 22, 5732–5742. [Google Scholar] [CrossRef]
  37. Cherik, I.C.; Mohammadi, S. Dielectric Modulated Doping-Less Tunnel Field-Effect Transistor, a Novel Biosensor Based on Cladding Layer Concept. IEEE Sens. J. 2022, 22, 10308–10314. [Google Scholar] [CrossRef]
  38. Wu, H.; Wang, J.; Kang, X.; Wang, C.; Wang, D.; Liu, J.; Aksay, I.A.; Lin, Y. Glucose biosensor based on immobilization of glucose oxidase in platinum nanoparticles/graphene/chitosan nanocomposite film. Talanta 2009, 80, 403–406. [Google Scholar] [CrossRef] [PubMed]
  39. Mishra, A.K.; Jarwal, D.K.; Mukherjee, B.; Kumar, A.; Ratan, S.; Tripathy, M.R.; Jit, S. Au nanoparticles modified CuO nanowire electrode based non-enzymatic glucose detection with improved linearity. Sci. Rep. 2020, 10, 11451. [Google Scholar] [CrossRef]
  40. Taguchi, M.; Ptitsyn, A.; McLamore, E.S.; Claussen, J.C. Nanomaterial-mediated Biosensors for Monitoring Glucose. J. Diabetes Sci. Technol. 2014, 8, 403–411. [Google Scholar] [CrossRef]
  41. Kwak, Y.H.; Choi, D.S.; Kim, Y.N.; Kim, H.; Yoon, D.H.; Ahn, S.-S.; Yang, J.-W.; Yang, W.S.; Seo, S. Flexible glucose sensor using CVD-grown graphene-based field effect transistor. Biosens. Bioelectron. 2012, 37, 82–87. [Google Scholar] [CrossRef] [PubMed]
  42. Scandurra, A.; Ruffino, F.; Sanzaro, S.; Grimaldi, M.G. Laser and thermal dewetting of gold layer onto graphene paper for non-enzymatic electrochemical detection of glucose and fructose. Sens. Actuators B Chem. 2019, 301, 127113. [Google Scholar] [CrossRef]
  43. Juſík, T.; Podešva, P.; Farka, Z.; Kováſ, D.; Skládal, P.; Foret, F. Nanostructured gold deposited in gelatin template applied for electrochemical assay of glucose in serum. Electrochim. Acta 2016, 188, 277–285. [Google Scholar] [CrossRef]
  44. Kwon, S.-Y.; Kwen, H.-D.; Choi, S.-H. Fabrication of Nonenzymatic Glucose Sensors Based on Multiwalled Carbon Nanotubes with Bimetallic Pt-M (M = Ru and Sn) Catalysts by Radiolytic Deposition. J. Sens. 2012, 2012, 784167. [Google Scholar] [CrossRef]
  45. Tortorich, R.P.; Shamkhalichenar, H.; Choi, J.-W. Inkjet-Printed and Paper-Based Electrochemical Sensors. Appl. Sci. 2018, 8, 288. [Google Scholar] [CrossRef]
  46. Hwang, H.S.; Jeong, J.W.; Kim, Y.A.; Chang, M. Carbon Nanomaterials as Versatile Platforms for Biosensing Applications. Micromachines 2020, 11, 814. [Google Scholar] [CrossRef]
  47. Rauti, R.; Musto, M.; Bosi, S.; Prato, M.; Ballerini, L. Properties and behavior of carbon nanomaterials when interfacing neuronal cells: How far have we come? Carbon 2019, 143, 430–446. [Google Scholar] [CrossRef]
  48. Lobov, I.A.; Davletkildeev, N.A.; Nesov, S.N.; Sokolov, D.V.; Korusenko, P.M. Effect of Nitrogen Atoms in the CNT Structure on the Gas Sensing Properties of PANI/CNT Composite. Appl. Sci. 2022, 12, 7169. [Google Scholar] [CrossRef]
  49. Dandu, N.K.; Chandaluri, C.G.; Ramesh, K.; Saritha, D.; Mahender Reddy, N.; Ramesh, G.V. Chapter 11—Carbon nanomaterials: Application as sensors for diagnostics. In Advanced Nanomaterials for Point of Care Diagnosis and Therapy; Dave, S., Das, J., Ghosh, S., Eds.; Elsevier: Amsterdam, The Netherlands, 2022; pp. 211–248. [Google Scholar]
  50. Yang, C.; Denno, M.E.; Pyakurel, P.; Venton, B.J. Recent trends in carbon nanomaterial-based electrochemical sensors for biomolecules: A review. Anal. Chim. Acta 2015, 887, 17–37. [Google Scholar] [CrossRef]
  51. Xu, B.; Xiang, H.; Wei, Q.; Liu, J.Q.; Xia, Y.D.; Yin, J.; Liu, Z.G. Two-dimensional graphene-like C2N: An experimentally available porous membrane for hydrogen purification. Phys. Chem. Chem. Phys. 2015, 17, 15115–15118. [Google Scholar] [CrossRef]
  52. Hussain, T.; Sajjad, M.; Singh, D.; Bae, H.; Lee, H.; Larsson, J.A.; Ahuja, R.; Karton, A. Sensing of volatile organic compounds on two-dimensional nitrogenated holey graphene, graphdiyne, and their heterostructure. Carbon 2020, 163, 213–223. [Google Scholar] [CrossRef]
  53. Panigrahi, P.; Sajjad, M.; Singh, D.; Hussain, T.; Andreas Larsson, J.; Ahuja, R.; Singh, N. Two-dimensional Nitrogenated Holey Graphene (C2N) monolayer based glucose sensor for diabetes mellitus. Appl. Surf. Sci. 2022, 573, 151579. [Google Scholar] [CrossRef]
  54. Chang, P.-H.; Liu, H.; Nikolić, B.K. First-principles versus semi-empirical modeling of global and local electronic transport properties of graphene nanopore-based sensors for DNA sequencing. J. Comput. Electron. 2014, 13, 847–856. [Google Scholar] [CrossRef]
  55. QuantumATK. Why Are So Many k-Points Needed in the Transport Direction in a Device Calculation? Available online: https://docs.quantumatk.com/tutorials/transport_kpoints/transport_kpoints.html (accessed on 29 January 2023).
  56. Kaur, J.; Kumar, R.; Vohra, R.; Sawhney, R.S. Density functional theory investigations on the interaction of uracil with borospherene. Bull. Mater. Sci. 2022, 45, 22. [Google Scholar] [CrossRef]
  57. Thomas, S.; Kumar, V.; Roy, D.R.; Zaeem, M.A. Two-Dimensional Boron–Phosphorus Monolayer for Reversible NO2 Gas Sensing. ACS Appl. Nano Mater. 2020, 3, 10073–10081. [Google Scholar] [CrossRef]
  58. QuantumATK. Device Density of State. Available online: https://docs.quantumatk.com/manual/Types/DeviceDensityOfStates/DeviceDensityOfStates.html (accessed on 29 January 2023).
Figure 1. C2N-FET sensor designed by ATK-VNL. (a) Schematic representation of the C2N-FET device. (b) Cross-sectional view of the C2N-FET device. The built sensor consists of two gold electrodes, a monolayer C2N channel and a gate underneath the channel. Color code: hydrogen—white, nitrogen—blue, gold—yellow, and carbon—gray.
Figure 1. C2N-FET sensor designed by ATK-VNL. (a) Schematic representation of the C2N-FET device. (b) Cross-sectional view of the C2N-FET device. The built sensor consists of two gold electrodes, a monolayer C2N channel and a gate underneath the channel. Color code: hydrogen—white, nitrogen—blue, gold—yellow, and carbon—gray.
Nanomaterials 13 00700 g001
Figure 2. Atomic structure of each of the sugar molecules: glucose (a), fructose (b), and xylose (c). Color code: oxygen—red, carbon—gray, and hydrogen—white.
Figure 2. Atomic structure of each of the sugar molecules: glucose (a), fructose (b), and xylose (c). Color code: oxygen—red, carbon—gray, and hydrogen—white.
Nanomaterials 13 00700 g002
Figure 3. (a) Schematic diagram of the C2N-FET sensor with fructose. (b) Cross-sectional view of the C2N-FET sensor with fructose.
Figure 3. (a) Schematic diagram of the C2N-FET sensor with fructose. (b) Cross-sectional view of the C2N-FET sensor with fructose.
Nanomaterials 13 00700 g003
Figure 4. Change in device density of states (DOS) of simulated C2N FET in presence of (a) glucose molecule; (b) fructose molecule; and (c) xylose molecule.
Figure 4. Change in device density of states (DOS) of simulated C2N FET in presence of (a) glucose molecule; (b) fructose molecule; and (c) xylose molecule.
Nanomaterials 13 00700 g004aNanomaterials 13 00700 g004b
Figure 5. Total and partial density of states (DOS) of C2N FET in presence of (a) glucose molecule, (b) fructose molecule, and (c) xylose molecule.
Figure 5. Total and partial density of states (DOS) of C2N FET in presence of (a) glucose molecule, (b) fructose molecule, and (c) xylose molecule.
Nanomaterials 13 00700 g005aNanomaterials 13 00700 g005b
Figure 6. Work function of: C2N FET; C2N FET with the presence of glucose molecule; C2N FET with the presence of fructose molecule; and C2N FET with the presence of xylose molecule.
Figure 6. Work function of: C2N FET; C2N FET with the presence of glucose molecule; C2N FET with the presence of fructose molecule; and C2N FET with the presence of xylose molecule.
Nanomaterials 13 00700 g006
Figure 7. Transmission spectra T(E) for C2N-FET sensor with three different sugar molecules (a) bias voltage = 0 V, (b) bias voltage = 0.2 V, and (c) bias voltage = 0.4 V.
Figure 7. Transmission spectra T(E) for C2N-FET sensor with three different sugar molecules (a) bias voltage = 0 V, (b) bias voltage = 0.2 V, and (c) bias voltage = 0.4 V.
Nanomaterials 13 00700 g007
Figure 8. Current–voltage characteristics vs bias for the C2N FET (orange), for the C2N FET with glucose (blue), for the C2N FET with xylose (red), and for the C2N FET with fructose (green).
Figure 8. Current–voltage characteristics vs bias for the C2N FET (orange), for the C2N FET with glucose (blue), for the C2N FET with xylose (red), and for the C2N FET with fructose (green).
Nanomaterials 13 00700 g008
Figure 9. Variation in electrical drain current for the various types of sugar molecules.
Figure 9. Variation in electrical drain current for the various types of sugar molecules.
Nanomaterials 13 00700 g009
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Wasfi, A.; Awwad, S.; Hussein, M.; Awwad, F. Sugar Molecules Detection via C2N Transistor-Based Sensor: First Principles Modeling. Nanomaterials 2023, 13, 700. https://doi.org/10.3390/nano13040700

AMA Style

Wasfi A, Awwad S, Hussein M, Awwad F. Sugar Molecules Detection via C2N Transistor-Based Sensor: First Principles Modeling. Nanomaterials. 2023; 13(4):700. https://doi.org/10.3390/nano13040700

Chicago/Turabian Style

Wasfi, Asma, Sarah Awwad, Mousa Hussein, and Falah Awwad. 2023. "Sugar Molecules Detection via C2N Transistor-Based Sensor: First Principles Modeling" Nanomaterials 13, no. 4: 700. https://doi.org/10.3390/nano13040700

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop