Performance Investigation of Pentacene Based Organic Double Gate Field Effect Transistor and its Application as an Ultrasensitive Biosensor
Mohammad Reza Jouharchi
1
(Graduate Student, Department of Electronic, Faculty of Electrical Engineering, Yadegar- e- Imam Khomeini (RAH) Shahr-e-Rey Branch, Islamic Azad University, Tehran, Iran)
Zahra Ahangari
2
(Department of Electronic, Faculty of Electrical Engineering, Yadegar- e- Imam Khomeini (RAH) Shahr-e-Rey Branch, Islamic Azad University, Tehran, Iran)
Farshad Babazadeh
3
(Assistant Professor, Department of Electronic, Faculty of Electrical Engineering, Yadegar- e- Imam Khomeini (RAH) Shahr-e-Rey Branch, Islamic Azad University, Tehran, Iran.)
کلید واژه: Gate Workfunction, Double gate field effect transistor, Nanogap biosensor, Organic transistor, Pentacene,
چکیده مقاله :
In this paper, the electrical performance of double gate organic field effect transistor (DG-OFET) are thoroughly investigated and feasibility of the device as an efficient biosensor is comprehensively assessed. The introduced device provides better gate control over the channel, yielding better charge injection properties from source to channel and providing higher on-state current in comparison with single gate devices. The susceptibility of fundamental electrical parameters with respect to the variation of design parameters is thoroughly calculated. In particular, standard deviation and average value of main electrical parameters signify that metal gate workfunction, channel thickness and gate oxide thickness are fundamental design measures that may modify the device efficiency. The insensitivity of off-state current to the change of channel length and drain bias confirms feasibility of the device in nanoscale regime. Next, a nano cavity is embedded in the gate insulator region for accumulation of biomolecules. The immobilization of molecules with different dielectric constants in the gate insulator hollow alters the gate capacitance and results in the drain current deviation with respect to the air- filled cavity condition. It is shown that by the occupancy of whole volume of the nanogap, a maximum range of on-state current variation can be achieved.
چکیده انگلیسی :
Performance Investigation of Pentacene Based Organic Double Gate Field Effect Transistor and its Application as an Ultrasensitive Biosensor
Abstract:
In this paper, the electrical performance of double gate organic field effect transistor (DG-OFET) are thoroughly investigated and feasibility of the device as an efficient biosensor is comprehensively assessed. The introduced device provides better gate control over the channel, yielding better charge injection properties from source to channel and providing higher on-state current in comparison with single gate devices. The susceptibility of fundamental electrical parameters with respect to the variation of design parameters is thoroughly calculated. In particular, standard deviation and average value of main electrical parameters signify that metal gate workfunction, channel thickness and gate oxide thickness are fundamental design measures that may modify the device efficiency. The insensitivity of off-state current to the change of channel length and drain bias confirms feasibility of the device in nanoscale regime. Next, a nano cavity is embedded in the gate insulator region for accumulation of biomolecules. The immobilization of molecules with different dielectric constants in the gate insulator hollow alters the gate capacitance and results in the drain current deviation with respect to the air- filled cavity condition. It is shown that by the occupancy of whole volume of the nanogap, a maximum range of on-state current variation can be achieved.
Keywords:
Double gate field effect transistor, Gate workfunction, Nanogap biosensor, Organic transistor, Pentacene.
1. Introduction
Recently, a comprehensive study is conducted regarding the application of organic materials. In particular, organic semiconductors provide the merit and benefits of printing on plastic substrates mainly at low temperature via solution-based processes [1-2], facilitating the fabrication of cost-effective extended- area, flexible devices. It is well established that flexible displays [3], field-effect transistors (FETs) [4-6] solar cells [7-8] and light-emitting diodes [9] are among the popular applications of organic materials. However, these materials suffer from low carrier mobility in comparison with silicon based devices [10-13]. By contrast, non-organic materials, mainly silicon, have poor flexibility as well as high temperature fabrication process. Organic Field Effect transistor (OFET) can be considered as one of the critical components of organic integrated circuits with the applications in smart cards, medical implants and sensors. Much the same as traditional metal-oxide semiconductor field effect transistor (MOSFET), OFET contains a conducting channel across the source and drain electrodes, in which the current is modulated by the gate bias. Basically, the arrangement of gate, source and drain electrodes with respect to the organic material and the gate insulator provides different single gate architectures with different electrical performance [14]. In bottom-gate top source/drain contact configuration (BG-TC), the gate insulator is formed above the gate contact and the active organic semiconductor can be deposited by vacuum vapor deposition or solution processing techniques. Next, source/drain contacts are formed above the semiconductor. However, in bottom-gate bottom source/drain contact (BG-BC) architecture, the source and drain electrodes are created below the semiconductor. The BG-BC structure results in higher contact resistance and creates an elevated potential barrier at the source- channel junction. Consequently, low on-state and off-state current are achieved. By contrast, in (BG-TC) design, the bottom gate electrode reduces the contact resistivity and improves the on-state current. High frequency performance of OFET is considered in [15], and an analytical approach is conducted for assessing the threshold voltage of the organic transistor [16].
One of the main challenges of OFET is the low on-state current results from low mobility of carriers. The main target of this paper is designing a novel Double Gate OFET (DG-OFET) structure, aiming towards improving the switching performance of the device and reducing the static power dissipation. The proposed pentacene-based structure takes the advantage of BG-TC and BG-BC structures, providing high on/off current ratio. In this paper, impact of critical design parameters on the electrical performance of the device is comprehensively investigated for optimizing the device performance.
Moreover, statistical analysis is accomplished to calculate sensitivity of device performance based on the variation of critical design parameters. In the first step, all the nominal design parameters are set considered constant and following that, one specific parameter is varied. Next, statistical measures including standard deviation and mean value of each electrical parameter are calculated to elucidate the susceptibility of device performance. By definition, standard deviation is a measurable factor that measures the dispersion of a specific dataset relative to its mean value. If the calculated dataset is scattered further from the average value, a higher standard deviation can be achieved. In addition, feasibility of DG-OFET is assessed as an ultrasensitive is elucidated. Recently, the operation of field effect transistors as label-free biosensors have gained attention, which can electrically detect different biomolecules with high sensitivity. In this paper, a cavity is created in the gate insulator region, which accumulates the biomolecules. Generally, each biomolecule has different permittivity that modifies the gate capacitance (CG) and drain current. The paper is arranged as follows: the simulation setup and device structure are introduced in section two. Next, the electrical performance of double gate organic MOSFET is thoroughly surveyed and impact of design parameter variation on device efficiency are elucidated. Following that, feasibility of the proposed device as an efficient biosensor for detecting biomolecules is clarified. Finally, the paper is outlined in section five.
2. Device structure and Computational models
The schematic and simplified geometry of double gate pentacene based field effect transistor is illustrated in Fig.1 (a). The proposed DG-OFET is a combination of BG-TC, Fig.1(b), and BG-BC, Fig.1(c), OFET structures with two gate electrodes on the top and bottom of the structure. The main benefit of DG-OFET is the coverage of top gate electrode across the device from source to drain, that facilitates reduction of source/drain contact resistance. The initial design parameters are summed up in Table. 1. The width of the device is 1000µm, while in the simulation, the results are scaled to 1µm. The numerical simulations are performed by device simulator, ATLAS [17], and subsequent models are activated for assessing the device performance:
· Carrier mobility models considering the effect of dopant density and impurities on carrier mobility are activated.
· The effect of horizontal and vertical electric field on the mobility of holes are taken into consideration.
· The main current mechanism of organic transistor is based on drift and diffusion of carriers from source to drain in which the gate bias modifies the charge density in the channel. Accordingly, the related models regarding the transport of holes along the device are activated.
· The effect of traps at the gate insulator/ channel interface on the electrical characteristics of the proposed device is activated.
Figure 1: Schematic of (a) DG-OFET (b) BG-TC and (c) BG-BC pentacene based field effect transistor.
Initial design parameters of DG-OFET
Parameter |
Value |
Channel Length (Lch) | 30µm |
Source and Drain Length | 30µm |
Gate Length (LG) | 90µm |
Thickness of Source/Drain Electrodes | 5nm |
Pentacene Thickness (Tch) | 100nm |
Gate Insulator Thickness (Tox) | 300nm |
Workfunction of Source/ Drain electrodes | 4.9eV |
Gate Workfunction (WFG) | 4.2eV |
Drain-Source Voltage (VDS) | -2V |
Gate Voltage (VGS) | 0:-20V |
3. Results and Discussion
The proposed DG-OFET structure has two gates with similar workfunction value that are designed to be electrically connected. Basically, pentacene based p-channel organic MOSFET operates in the accumulation mode and gate voltage modulates the hole density in the channel. In addition, the related source and drain metal contact workfunction are different from the gate workfunction. Due to the Fermi level energy difference between the source/drain contact and the underlying organic semiconductor, high concentration of holes is induced in the source and drain. The main specification of the suggested structure is the deposition of metal gate contact across the whole length of the device, which can control the hole density in the source, drain and channel regions. In other words, the gate contact assists the hole accumulation in these regions, which as a result, reduces the hole density gradient between source/drain and channel in the on-state.
The hole density distribution in the off-state and on-state are presented along the device from source to drain, depicted in Fig.2. In the absence of gate voltage, the source/drain metal workfunction plays a fundamental role and effectively modulates the source/drain hole concentration. Due to the hole density gradient between channel and source region, a potential barrier is created at the interface, which effectively reduces the off-state leakage current. On the other side, by the increment of gate voltage towards a sufficient negative value, considerable amount of holes is accumulated in the channel. Fig.3 depicts the potential distribution along the device in the off-state and on-state operation. In the off-state, there exists a potential barrier at the source-channel junction, reducing the hole diffusion rate from source into the channel. However, the increment of negative gate bias accumulates holes in the channel, facilitating the transport of carriers towards the drain.
Figure 2: Hole density along the device from source to drain in the off-state and on-state, for VDS=-2V.
Figure 3: Potential along the device from source to drain in the off-state and on-state, for VDS=-2V.
The transfer characteristics (ID-VGS) of DG-OFET are depicted in Fig.4 and the results are compared with BG-TC and BG-BC structures. It is generally accepted that DG-OFET has the capability to attain better gate control over the channel with the added advantage to increase the drain current. In BG-BC single gate structure, the source/drain charge density is modulated by the related contact workfunction and gate voltage merely controls the channel charge concentration. Accordingly, high potential barrier at the source-channel junction results in considerable reduction of off-state current. By contrast, in BG-TC structure, the potential barrier at the source-channel interface is reduced, which can enable better performance as compare to BG-BC structure. The double gate structure takes the advantage of low off-state current of BG-BC structure and improved on-state current of BG-TC device, providing superior performance in terms of on/off current ratio and higher immunity towards short channel effects. The electrical characteristics of the proposed structures are summed up in Table.2.
Figure 4: The transfer characteristics of double gate and single gate organic MOSFET with top and bottom source/ drain configuration, for VDS=-2V.
Table 2
Electrical parameters of three different organic transistors
Structure | Ion (A/µm) | Ioff (A/µm) | Vth(V) | Ion/Ioff |
BG-TC | 6.38E-9 | 1.11E-18 | 1.86 | 5.75E+9 |
BG-BC | 1.28E-9 | 3.09E-19 | 1.91 | 4.14E+9 |
DG-OFET | 1.16E-8 | 4.9E-19 | 1.57 | 2.37E+10 |
The workfunction value of metal gate is an essential design measure that can effectively modify the off-state current and threshold voltage of DG-OFET. The transfer characteristics of the device are illustrated in Fig.5, while the gate workfunction is parametrized. Clearly, the off-state current considerably increases as the gate workfunction enhances towards 5.3eV. The metal gate workfunction value determines the channel flat band potential, which, in turn, affects the charge accumulation in the channel. It is worth mentioning that tuning of metal gate workfunction value is viable for efficient performance of the device.
Figure 5: The transfer characteristics of DG-OFET as a function of gate workfunction, for VDS=-2V.
The effect of gate length scaling on the electrical performance of DG-OFET is depicted in Fig.6, while the gate length is parametrized from LG=30µm to LG=5µm. The gate length scaling of DG-OFET improves the charge transit time along the channel, yielding higher drive current with insignificant change in the off-state current. It is well established that in DG-OFET architecture, optimization of performance in terms of high on/off current ratio and high frequency operation is highly dependent upon the gate capacitance.
Figure 6: The transfer characteristics of DG-OFET as a function of gate length, for VDS=-2V.
The effect of gate insulator capacitance on the electrical characteristics of the DG-OFET are demonstrated in Fig.7, while the SiO2 thickness is varied from 400nm to 100nm. In particular, the gate capacitance effectively adjusts the potential barrier at the source-channel interface, modifying charge injection properties. Clearly, the drive current is considerably improved as the gate insulator thickness is scaled down to 100nm, yielding an increased gate capacitance due to the accumulated charge in the channel region. By definition, employment of high-k dielectric improves the gate coupling over the channel that eventually allows charge density in the channel to be highly associated with the gate oxide capacitance. The transfer characteristics of the device is illustrated in Fig.8, for different gate oxide materials with dielectric constant ranging from 3.9 (SiO2) to 50 (TiO2). The results demonstrate that the usage of high-k dielectrics as the gate insulator significantly improves the on-state current as well as providing low gate leakage current.
Figure 7: The transfer characteristics of DG-OFET as a function of gate oxide thickness, for VDS=-2V.
Figure 8: The transfer characteristics of DG-OFET as a function of gate insulator permittivity.
Channel thickness is an important design factor that can affect the device efficiency, mainly in nanoscale regime. The results depicted in Fig.9 demonstrate the considerable dependence of DG-OFET performance to the pentacene thickness. In fact, reduction of pentacene thickness up to 50nm results in better gate control over the channel. In this situation, the charge density in the channel is considerably increased, providing higher drive current. By contrast, further reduction of channel thickness below 50nm leads to the increment of threshold voltage and degradation of on-state current. In order to discuss this abnormal behavior in nanoscale regime, two parameters should be taken into consideration: the contact resistance and the carrier mobility. The contact resistivity is expected to scale directly with the pentacene thickness, which may reduce the on-state current. In addition, thin film pentacene is highly disordered and carriers have very low mobility, which signifies the low drain current.
It is well demonstrated that the metal gate workfunction can significantly modify the charge density in the channel. Evidently, to induce considerable amount of holes in the ultra-scaled channel with improved electrical performance, appropriate gate material should be chosen. Figure.10 presents the maximum on-state current as the gate workfunction and channel thickness are varied, providing a comprehensive roadmap for tuning the gate workfunction in different channel thicknesses. It is to be noted that as the channel thickness shrinks down, higher gate workfunction value should be assigned for improving the device performance.
Figure 9: The transfer characteristics of DG-OFET as a function of pentacene thickness, for VDS=-2V.
Figure 10: Maximum on-state current of DG-OFET as a function of pentacene film thickness for different gate workfunction values.
Next, impact of temperature (T) on device performance is assessed and the results are presented in Fig.11. The drain current increases as the temperature reaches to room temperature. However, further increasing of the temperature degrades the carrier mobility and has an adverse effect on device performance. In addition, main analog parameters of the device including transconductance (gm) and current gain are calculated, presented in Fig.12. The cut off frequency of 1MHz is achieved for DG-OFET which provides paves the way for high frequency application of the device. The transconductance can be further improved by employing high-k dielectric materials for the gate insulator.
Figure 11: The transfer characteristics of DG-OFET as a function of temperature, for VDS=-2V.
Figure 12: Analog parameters of DG-OFET including gm and current gain for VDS=-2V.
The bar chart depicted in Fig.13, demonstrates the sensitivity of essential electrical measures as a function of device design values. Basically, all the design parameters are adjusted to their nominal values and then, one specific parameter is hanged and following that, mean value and standard deviation of selected electrical parameters are calculated. The sensitivity in percentile is calculated as the standard deviation over average value of each electrical parameter for a particular design parameter. Based on statistical analysis, a low sensitivity indicates that the data set are close to the related mean value and variation of a particular design parameter has negligible effect on the electrical efficiency of the device. The results demonstrate that threshold voltage is highly sensitive to the change of metal gate workfunction. Moreover, the main benefit of DG-OFET is the low susceptibility of threshold voltage to the variation of drain bias and gate length shrinkage, which provides application of the device in nanoscale regime. Moreover, regarding off-state current, gate workfunction and pentacene film thickness are substantial parameters that may modify device proficiency. Evidently, gate workfuction considerably affects induced hole density in the channel and modifies the off-state potential barrier at the source-channel interface. Channel thickness is another critical factor that can change the DG-OFET performance in nanoscale regime. Clearly, reduction of channel thickness can effectively modify hole concentration in the channel, source and drain regions. The on-state current is greatly susceptible to drain voltage and effective gate oxide capacitance. Evidently, the drain voltage affects the carrier drift velocity. However, gate oxide capacitance effectively mutates the charge concentration in the channel and the device operation can be further improved by reduction of gate oxide thickness and employment of high-k dielectric materials (HfO2, k=25) as the gate insulator [18]. In addition, channel length scaling can reduce the transit time of carriers, improving the on-state current. Generally, one of the essential application of DG-OFET can be switches, that require high value of on/off current ratio as well as reduced static power dissipation in the off-state operation. The sensitivity analysis reveals that optimum value should be calculated for the gate workfunction and channel thickness in case of improving device switching performance.
Figure 14(a) illustrates the related mean value and variation range of on-state current as a function of different design parameters. Clearly, on-state current faces an outstanding variation while the drain voltage is parametrized. The gate insulator thickness is another factor that affects the gate coupling over the channel, modifying hole concentration in the channel. Moreover, average value as well as variation domain of off-state current with respect to the variation of critical design parameters are illustrated in Fig.14 (b). Clearly, a particular positive aspect of the proposed device is the limited alternation range of off-state current with respect to the channel length scaling and drain bias variation, facilitating application of the nanoscale DG-OFET. However, one of the challenges associated with the application of organic transistor is the high sensitivity of off-state current to the gate workfunction, making it essential to find appropriate material for the gate.
Figure 13: Sensitivity bar chart of related DG-OFET main electrical parameters as a function of essential design measures.
Figure 14: Mean value and variation range of (a) off-state current and (b) on-state current of DG-OFET as a function of main design parameters.
4. Nanogap Biosensor Based on Double Gate Organic Transistor
The schematic of double gate dielectric modulated nanogap DG-OFET is illustrated in Fig.15. The main feature of dielectric modulated DG-OFET involves the embedded hollow in the gate insulator at which certain molecules are collected [19-20]. The fabrication process of the device is fully compatible with the CMOS fabrication process. The gate insulator can be fabricated via atomic layer deposition (ALD) technique, which provides uniform highly resistive dielectric film. Following that, wet etching is used to form the few nanometer nanogap. It is worth to be noted that the upper gate electrode acts like a mask and cannot be etched by hydrofluoric acid (HF) solution (38-40% HF:H2O=1:70). One distinguished feature of the introduced biosensor is the high susceptibility of on-state current to the variation of gate dielectric permittivity, which modifies the gate capacitance. The dielectric layer between the top /bottom gate and the underlying organic material is composed of an air hole in which specified biomolecules are accumulated. In case of storage of biomolecules in the hollow, dielectric constant of the cavity differs from air (k=1) to the specified value of different biomolecules, resulting in the variation of gate capacitance and the drain current. In addition, for simulating absorption of different biomolecules in the nano cavity, the permittivity of the nanogap is changed with respect to the concentrated molecules. The biomolecules which are considered includes protein(k=8), 3-aminoppropyltriethoxysilane (APTES)(k=3.57) and streptavidin(k=2.1) [21]. The size of biomolecules is accounted in the range of deca nanometer for protein and nearly 5nm for streptavidin [22]. In addition, based on experimental results, accumulation of streptavidin within hollow of 10nm length is reported [23]. Accordingly, hollow length of 100nm in vertical direction seems sufficient.
Figure 15: Schematic of the dielectric modulated biosensor in which a hollow is created in the gate insulator.
The transfer characteristics of nanogap DG-OFET is illustrated in Fig.16 as the drain current is calculated before and after the absorption of different biomolecules. It is evident that the drain current improves as the permittivity of the nanogap is enhanced. The drain voltage is considered as VDS=-0.05V for increasing the sensitivity of biosensor. It is well established that variation of nanogap permittivity leads to the modulation of gate capacitance and as a consequence, a considerable variation of drain current is achieved. It is essential to survey sensitivity of DG-OFET based biosensor upon the percentage of nano cavity capacity filled by molecules. The on-state current versus the occupancy of the hollow is illustrated in Fig.17 for different molecules. It is evident that on-state current increases as the higher percentage of the hole is filled with immobilized biomolecules. In particular, the gate capacitance can be calculated as follows:
(1)
(2)
In which, 
is the capacitance of cavity that is accumulated by molecules, 
is the related capacity of the air-filled cavity,
shows the gate oxide capacitance, 
denotes the vacuum permittivity and 
represents relative permittivity of the biomolecule (air). Moreover, 
represents the thickness of nanogap that is filled by biomolecule (air). Evidently, the increment of filled cavity results in the dominant role of , improving the gate coupling over the channel.
Figure 16: Transfer characteristic of dielectric modulated biosensor as a function of permittivity of the absorbed biomolecule. The drain current in the case of air-filled nanogap is presented for comparison.
Figure 17: On-state current of DG-OFET versus volume of the hollow that is filled by biomolecules with different dielectric permittivity.
Basically, the charge of the absorbed biomolecules can effectively modulate the charge density in the channel. The effect of neutral, positive and negative charge density are comprehensively assessed and the results are illustrated in the bar chart of Fig.18. Negatively charged biomolecules as well as dielectric constant of biomolecules can significantly modulate the channel hole density and as a consequence, can modify the maximum on-state current. Clearly, negatively charged absorbed molecules attract holes to the surface of the channel and amplifies the gate electric field. Accordingly, the sensitivity of the biosensor can be comprehensively improved. However, on the other side, molecules with positive charge repel holes from the surface and reduces the current, degrading the performance of the biosensor.
.
Figure 18: On-state current bar chart of dielectric modulated biosensor for neutral, positively and negatively charged biomolecules. The drain current in the case of air-filled nanogap is presented for comparison.
5. Conclusion
In summary, electrical performance of double gate organic field effect transistor is comprehensively investigated. The double gate structure provides superior efficiency in terms of on-state current and on/off current ratio. Sensitivity analysis reveals that gate workfunction and gate insulator thickness are substantial design measures that may modify the performance of DG-OFET. In addition, scaling of pentacene film thickness results in the enhancement of source/drain contact resistance and reduction of carrier mobility, degrading the device performance. It is well established that metal gate workfunction engineering is essential for optimizing the efficiency of the device. The low susceptibility of off-state current to the drain voltage variation and gate length scaling is a key advantage for the application of proposed structure in nanoscale regime. Next, the cavity embedded in the gate insulator of organic transistor provides the feasibility of this device as an efficient dielectric modulated biosensor. It is worth notifying that for achieving the highest sensitivity after the accumulation of molecules, maximum volume of the hollow should be filled by the biomolecules.
6. References
[1] Eslamian M. Inorganic and organic solution-processed thin film devices. Nano-micro letters. 2017 Jan 1;9(1):3.
[2] Sberna PM, Trifunovic M, Ishihara R. Solution-based fabrication of polycrystalline Si thin-film transistors from recycled polysilanes. ACS sustainable chemistry & engineering. 2017 Jun 14;5(7):5642-5.
[3] Yin D, Chen ZY, Jiang NR, Liu YF, Bi YG, Zhang XL, Han W, Feng J, Sun HB. Highly transparent and flexible fabric-based organic light emitting devices for unnoticeable wearable displays. Organic Electronics. 2020 Jan 1;76:105494.
[4] Zenitani H, Maiti TK, Hayashi T, Tanimoto Y, Sato K, Chen L, Kikuchihara H, Miura-Mattausch M, Mattausch HJ. Analysis of printed organic MOSFET characteristics with a focus on the temperature dependence. Japanese Journal of Applied Physics. 2016 Mar 15;55(4S):04EL05.
[5] Yasin M, Tauqeer T, Rahman HU, Karimov KS, San SE, Tunc AV. Polymer–fullerene bulk heterojunction-based strain-sensitive flexible organic field-effect transistor. Arabian Journal for Science and Engineering. 2015 Jan 1;40(1):257-62.
[6] Hupman MA, Hill IG, Syme A. Preliminary characterization of the response of an organic field effect transistor to ionizing radiation. Radiation Measurements. 2018 Nov 1;118:31-5.
[7] Liu J, Chen S, Qian D, Gautam B, Yang G, Zhao J, Bergqvist J, Zhang F, Ma W, Ade H, Inganäs O. Fast charge separation in a non-fullerene organic solar cell with a small driving force. Nature Energy. 2016 Jul;1(7):16089.
[8] Li W, Ye L, Li S, Yao H, Ade H, Hou J. A High‐Efficiency Organic Solar Cell Enabled by the Strong Intramolecular Electron Push–Pull Effect of the Nonfullerene Acceptor. Advanced Materials. 2018 Apr;30(16):1707170.
[9] Rana R, Mehra R. Investigation of Organic LED Materials Using a Transparent Cathode for Improved Efficiency. Journal of Electronic Materials. 2019 Apr:1-9.
[10] Kokil A, Yang K, Kumar J. Techniques for characterization of charge carrier mobility in organic semiconductors. Journal of polymer science part b: polymer physics. 2012 Aug 1;50(15):1130-44.
[11] Asthana PK, Goswami Y, Basak S, Rahi SB, Ghosh B. Improved performance of a junctionless tunnel field effect transistor with a Si and SiGe heterostructure for ultra low power applications. RSC Advances. 2015;5(60):48779-85.
[12] Astana PK, Ghosh B, Rahi SB, Goswami Y. Optimal design for a high performance H-JLTFET using HfO 2 as a gate dielectric for ultra low power applications. RSC Advances. 2014;4(43):22803-7.
[13] Iino H, Usui T, Hanna JI. Liquid crystals for organic thin-film transistors. Nature communications. 2015 Apr 10;6:6828.
[14] Ogier SD, Matsui H, Feng L, Simms M, Mashayekhi M, Carrabina J, Terés L, Tokito S. Uniform, high performance, solution processed organic thin-film transistors integrated in 1 MHz frequency ring oscillators. Organic Electronics. 2018 Mar 1;54:40-7.
[15] Cortes-Ordonez H, Jacob S, Mohamed F, Ghibaudo G, Iniguez B. Analysis and Compact Modeling of Gate Capacitance in Organic Thin-Film Transistors. IEEE Transactions on Electron Devices. 2019 Apr 3;66(5):2370-4.
[16] ATLAS User Manual, Santa Clara, USA: Silvaco International, 2015.
[17] Vargas-Bernal R. Advances in computational modeling of electronic devices based on graphene. IEEE Journal on Emerging and Selected Topics in Circuits and Systems. 2015 Feb 5;5(1):109-16.
[18] Kumar A, Tripathi MM, Chaujar R. Ultralow-power dielectric-modulated nanogap-embedded sub-20-nm TGRC-MOSFET for biosensing applications. Journal of Computational Electronics. 2018 Dec 1;17(4):1807-15.
[19] Ahangari Z. Performance assessment of dual material gate dielectric modulated nanowire junctionless MOSFET for ultrasensitive detection of biomolecules. RSC Advances. 2016;6(92):89185-91.
[20] Kim S, Baek D, Kim JY, Choi SJ, Seol ML, Choi YK. A transistor-based biosensor for the extraction of physical properties from biomolecules. Applied Physics Letters. 2012 Aug 13;101(7):073703.
[21] Jang DY, Kim YP, Kim HS, Ko Park SH, Choi SY, Choi YK. Sublithographic vertical gold nanogap for label-free electrical detection of protein-ligand binding. Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures Processing, Measurement, and Phenomena. 2007 Mar 22;25(2):443-7.
[22] Kim S, Kim JY, Ahn JH, Park TJ, Lee SY, Choi YK. A charge pumping technique to identify biomolecular charge polarity using a nanogap embedded biotransistor. Applied Physics Letters. 2010 Aug 16;97(7):073702.
