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Review

Recent Advances in Electrical Doping of 2D Semiconductor Materials: Methods, Analyses, and Applications

by
Hocheon Yoo
1,2,†,
Keun Heo
3,†,
Md. Hasan Raza Ansari
1,2 and
Seongjae Cho
1,2,*
1
Department of Electronic Engineering, Gachon University, 1342 Seongnamdaero, Sujeong-gu, Seongnam-si, Gyeonggi-do 13120, Korea
2
Graduate School of IT Convergence Engineering, Gachon University, 1342 Seongnamdaero, Sujeong-gu, Seongnam-si, Gyeonggi-do 13120, Korea
3
Department of Semiconductor Science & Technology, Jeonbuk National University, Jeonju-si, Jeollabuk-do 54896, Korea
*
Author to whom correspondence should be addressed.
†
These authors contributed equally to this work.
Nanomaterials 2021, 11(4), 832; https://doi.org/10.3390/nano11040832
Submission received: 20 February 2021 / Revised: 19 March 2021 / Accepted: 22 March 2021 / Published: 24 March 2021
(This article belongs to the Special Issue Two Dimensional Nanomaterials: Energy Conversion and Storage)
Browse Figures
Versions Notes

Abstract

:
Two-dimensional materials have garnered interest from the perspectives of physics, materials, and applied electronics owing to their outstanding physical and chemical properties. Advances in exfoliation and synthesis technologies have enabled preparation and electrical characterization of various atomically thin films of semiconductor transition metal dichalcogenides (TMDs). Their two-dimensional structures and electromagnetic spectra coupled to bandgaps in the visible region indicate their suitability for digital electronics and optoelectronics. To further expand the potential applications of these two-dimensional semiconductor materials, technologies capable of precisely controlling the electrical properties of the material are essential. Doping has been traditionally used to effectively change the electrical and electronic properties of materials through relatively simple processes. To change the electrical properties, substances that can donate or remove electrons are added. Doping of atomically thin two-dimensional semiconductor materials is similar to that used for silicon but has a slightly different mechanism. Three main methods with different characteristics and slightly different principles are generally used. This review presents an overview of various advanced doping techniques based on the substitutional, chemical, and charge transfer molecular doping strategies of graphene and TMDs, which are the representative 2D semiconductor materials.

Graphical Abstract

1. Introduction

Doping is the most common and feasible method used to control the properties of conventional semiconductors. However, 2D materials pose challenges owing to nonconformity to traditional doping techniques, such as ion implantation, which could damage the crystal structures of these materials [1,2,3]. Hence, sophisticated doping techniques are required to preserve the structure and intrinsic properties of 2D materials as well as modulate them according to required applications. Compared to other techniques, such as substitutional, electrical/magnetic field, and strain-effect-induced doping, organic molecular doping methods have numerous advantages. Organic compounds are widely available in natural and synthetic forms; they mostly consist of polymers that are repeated units of monomers. These organic compounds are viable candidates for inducing the required modulations in 2D materials owing to their easy availability and simplicity of doping. The soaking and dipping methods are commonly applied to 2D materials to induce doping effects using organic molecules. Self-assembled monolayers (SAM) play a major part in organic molecule-based doping techniques, which is why most recent organic-molecule-based doping studies have focused on utilizing SAM for doping [4,5]. SAMs were first discovered in 1978 and have since then been extensively used for salinization and surface functionalization of substrates. SAMs are based on silane or thiol coupling agents [6]. However, most recent studies have focused on silane-based SAMs. The dipole moments of end-functional groups in SAMs are normally responsible for inducing n- or p-type doping effects in 2D materials. However, one caveat to the application of SAMs is their hydrophilic nature, which renders the doping effects unstable after few days. Conversely, many organic molecules, such as monoethanolamine (MEA), benzyl viologen (BV), and SAM-thiol, have shown good stability of doping after a few days owing to their hydrophilic nature [6,7]. Nonetheless, organic-molecular-based doping techniques enable enhancement and modulation of the electrical, optical, mechanical, and flexible properties of 2D material-based devices. Using organic molecular doping techniques, many studies have shown unique applications for 2D materials, including photodetectors, photodiodes, p-n junctions, and gas/bio sensors [7,8]. Low-dimensional electronics can be realized even by group-IV atomic membranes, silicene and germane which are considered to be sp2-hybridized layers with honeycomb lattice structures. Thus, the doping techniques can be further extended into those new functional materials with wide applications owing to their higher Si processing compatibility and flexibility. In this work, we have compiled some recent studies that have utilized organic molecules as dopants for 2D materials, with a particular interest in graphene and transition metal dichalcogenides (TMDs) by which numerous device applications have been reported.

2. Graphene Doping

2.1. Background

In 2004, Drs. Geim and Novoselov of the University of Manchester, UK, succeeded in exfoliating graphene from bulk graphite using the scotch tape exfoliation method, following which the unique and excellent electrical and mechanical properties of graphene began attracting attention [8,9,10]. Since then, various researchers have actively researched the applications of graphene-based electronic devices. Graphene is a honeycomb-shaped two-dimensional planar carbon allotrope composed of the sp2 bonds of carbon atoms [11]. Graphene is classified as one of the nanostructured carbon allotropes, along with the soccer-ball-like fullerene (C60), columnar carbon nanotubes, and multilayered graphite [12]. Of the four outermost electrons in the carbon atom, three electrons form σ-bonds to produce a hexagonal structure; owing to the long range of π-conjugation of the remaining electron, graphene features excellent physical and electrical properties [13]. Graphene has a 100-fold higher electron mobility than silicon, which is the main raw material for semiconductors, and 100-fold greater electrical conductivity than copper; its tensile strength is more than 200 times that of steel, with excellent elasticity that allows maintenance of the electrical conductivity even if the area is increased or bent by more than 10%. In addition, it has more than twice the thermal conductivity of diamonds [14]. To apply graphene having such excellent properties as a core material in electronic devices, doping is the most effective method as it minimizes physical damage [15,16]. Doping is well known as an effective method to change the electrical properties of a material and is mainly used in technologies involving semiconductors. The basic principle of doping involves adding a material that can donate or remove electrons, thereby changing the electrical properties of the original material. Although the theoretical physical properties of graphene are excellent, in reality, graphene does not have the carrier mobility of theoretical graphene; thus, the surface resistance of the synthesized graphene is relatively high compared to indium tin oxide (ITO) [17]. Thus, it has been noted that electrons and holes are not efficiently transferred in the graphene-based device. To solve this problem, attempts were made to control the work function of graphene and lower its surface resistance by a doping technique mainly used with silicon [18]. In Si-based semiconductor doping technologies, group 3 (boron) or group 5 (nitrogen) ions are used to obtain p- or n-type doped materials or annealed at high temperature with the target material to be doped. However, as graphene is composed of single-layered atoms, it is difficult to apply this method; therefore, new doping technologies must be developed [19,20]. Conventional doping in graphene is similar to that used with silicon technology but proceeds by a different mechanism; this is generally achieved by three main methods, namely substitutional, chemical, and surface charge transfer doping, all of which have distinct characteristics and principles. In particular, doping methods that apply organic molecules or metal particles to the upper surface of graphene by dry deposition to achieve charge transfer have been studied and used in recent years [21]. In general, there are two types of chemical surface modification methods for graphene. One is covalent-bonding technique in which a bond is formed on the surface of graphene and the other is non-covalent-bonding one uses the interaction between graphene and the functional group. First, for the covalent-bonding surface modification method, a functional group is formed at the end of the graphene rather than the surface, and exfoliation is performed by electrostatic repulsion between the functional groups. In this case, as defects are not formed on the surface of graphene, the electrical conductivity of graphene is maintained, and the dispersibility of graphene in a polar organic solvent can be improved due to the electrostatic repulsion. As a result, it becomes easier to manufacture highly conductive composite materials. Second, for the non-covalent-bonding surface modification method, non-covalent functionalization of graphene based on π-π bonding, hydrogen bonding, or interaction among charges reduces defects on the surface of graphene more effectively compared with the covalent functionalization method. Therefore, it has an advantage of not degrading the thermal stability of graphene as well as sustaining the excellent electrical conductivity. On the other hand, there is a drawback in that the dispersibility in a polar organic solvent is reduced compared with the first method. Herein, the characteristics, advantages, and disadvantages of the existing substitution and chemical doping methods are discussed. Furthermore, the basic principles of the organic molecular doping method are examined based on the charge transfer method, with a review of the applications.

2.2. Substitutional Doping

Controlling the number of layers is a predominant way for wide-bandgap modification [22]. Hybrid nanosheets demonstrate the energy-bandgap tunability depending on the number of layers. Practical measurement results based on photoluminescence indicates that the energy bandgap is in the negative relation with the increase in number of layers [22]. Being closely related with doping, the major topic of this work, substitutional doping can be also one of the efficient ways of opening the energy bandgap of graphene, as can be proven by previous theoretical works on B, N, and Bi doping in graphene [23]. Also, the effects of substitutional doping on the materials including the change in electronic properties of graphene were studied by the help of ab initio calculations based on density functional theory (DFT) [24]. When graphene is substituted and doped with other hetero-atoms using chemical vapor deposition (CVD), a graphene lattice is formed via a covalent bond with carbon atoms, and this structure is suitable for device fabrication because it can elicit stable and reproducible electrical properties. Therefore, substitution doping is commonly used in silicon technologies [23,24,25,26]. Since the discovery of graphene, many attempts have been made to replace carbon atoms with boron and nitrogen, which are located to the left and right of carbon in the periodic table. Graphene is a zero-bandgap semimetal and does not have semiconductor characteristics, so it is difficult to use as a transistor. Substitution doping has been reported as a useful method to open the band gap of graphene [12]. Here, boron and nitrogen are the best acceptors and donors as their outermost electrons are trivalent or pentavalent and similar in size to those of carbon. Thus, substituting carbon with graphene using boron and nitrogen, experimental results have been reported on opening the valence and conduction bands [12,23]. There are two main methods of graphene substitution doping, of which the first is substitution during graphene synthesis [12]. CVD is the most common method for synthesizing graphene. Boron (HBO3, H2B6) and nitrogen (NH3) are added when synthesizing through this method (Figure 1a,b) [12,25]. And graphene substituted with boron and nitrogen is synthesized by flowing methane at the same time. The second substitutional doping method involves heat treatment of graphene at high temperatures or slicing plasma while flowing gases containing the substitution elements over the synthesized graphene [24]. If a gas containing boron and nitrogen is flowed while performing strong heat treatment on graphene oxide, the oxide is reduced and replaced, and the degree of doping can be controlled through the intensity of the plasma and the amount of flowing gas (Figure 1c) [27,28]. The doping efficiency and configuration also critically depend on the precursor (s) such as Melamine, polyaniline and polypyrrole (Figure 1d) [24,29,30,31]. However, it has been noted that this doping method can cause structural defects in graphene, which eventually degrade its conductivity and can pose obstacles when applied to electronic devices [32]. One method of compensating for this shortcoming is chemical doping, which is discussed in the next section.

2.3. Chemical Doping

In implementing an electronic device based on a graphene electrode, adjusting the band energy is important to achieve power efficiency and reliability of the device [18]. However, it is difficult to find a material with the desired energy band that also has appropriate conductivity. Therefore, it is more suitable to change the work function by simple surface or chemical treatment. Even in silicon-based device technologies, research on changing the properties using chemical dopants has been underway for more than a decade. Many researchers have developed various doping techniques to effectively control the electrical and optical properties of the carbon-based target material. Doping methods using chemical substances have been widely studied because they do not change the mechanical and chemical properties of the target substance and can easily control the electrical properties [26,33]. Controlling the work functions of carbon materials and improving their electrical properties using chemical doping methods has also been investigated. Doping of graphene using chemicals has been studied continuously through theoretical and experimental methods, and the work function of graphene can be changed to p-type or n-type depending on the chemicals used (Figure 2a) [11]. For example, gold chloride, which is commonly used for doping organic conductors, is the most well-known material for doping graphene; it is a p-type dopant that can increase the work function of graphene and lower its surface resistance (Figure 2b) [34]. Gold chloride dissolves in nitromethane and dissociates into gold trivalent cations and chlorine ions; the reaction by which the gold trivalent cations remove electrons from graphene and reduce to gold nanoparticles occurs spontaneously on the surface of graphene because of the negative Gibbs free energy [16]. Similarly, it has been reported that graphene’s work function and surface resistance can be lowered using metal chlorides with high work functions and negative Gibbs free energies [34]. The work function of graphene is known to be about 4.2–4.4 eV and may increase to 4.7–5.1 eV depending on the concentration of the gold chloride doping solution; further, the surface resistance varies depending on the method of synthesis but may be lowered to 150 Ω/sq after doping [35,36,37]. As stable, complementary dopants of graphene, poly (ethylene imine) and diazonium salts were investigated [33]. The carrier transport properties in graphene devices doped with these molecules exhibit asymmetries in electron–hole conductances; while maintaining the conductance of one carrier, the conductance of the other carrier decreases. As shown in the Figure 2c, the simulation results suggest that the origin of this asymmetry is the imbalanced carrier injection from the graphene electrode caused by misalignment of the neutrality points. In addition, the conductivity of graphene increases rapidly when steam is applied to the surface of graphene with strong acids, such as nitric acid and hydrogenated iodine. Methods to control the work function by changing the electrical properties of graphene using materials such as bis (trifluoromthanesulfonyl) amide (TFSA) and poly (ethylene imine) (PEI) have been published [26,38,39,40]. As an effective electron dopant and a stable encapsulating layer, SU-8 photoresist can be used to achieve highly stable n-type graphene nano-meshes. The chemically stable n-type electro-chemical characteristics of the SU-8-doped graphene were evaluated in air using Raman spectra, electrical transport properties, and electronic band structures [41,42].
The SU-8 doping causes minimum damage to the hexagonal carbon lattice structure of the graphene layer and is completely reversible by removal of the uncross-linked SU-8 resist, shown in Figure 2d. In conclusion, the chemical doping method is able to effectively control the fermi-level of graphene with a chemical substance with electronegativity, which has a large gap with carbon, and can be the main technical basis for the charge transfer method described in the following section.

2.4. Charge Transfer Method (Molecular Doping)

As mentioned above, the Fermi level of graphene could be easily modulated through chemical doping, but more sophisticated technologies are required to create the band gap. The last of the main doping methods for graphene involve surface charge transfer using an organic molecular polymer material. Doping can be performed by exchange of electrons between semiconductor and dopants adsorbed on the semiconductor surface in case of surface transfer doping technique. For this reason, this technique is also called as adsorbate-induced doping. In general, the surface transfer doping does not ruin the atomic arrangement of graphene and has high process repeatability [26]. As noted previously, doped graphene for various electrical properties could be obtained through direct synthesis and post treatments. Among those post treatment methods, wet doping methods can be performed using acid, metal chloride treatment, and organic molecular material coatings on the graphene surface using dip, spin coating, etc. [16]. When a molecule capable of causing charge transfer is applied to the surface of graphene or a thin doping film is deposited, charge transfer occurs spontaneously owing to the difference in electronegativity from the carbon constituting graphene. This mechanism has been widely introduced as an effective method for doping graphene. Theoretically, as shown in Figure 3a,b, DFT was employed in order to investigate changes in the electronic structure and vibrational property of graphene when aromatic molecules such as aniline and nitrobenzene are adsorbed [21]. The simulation results explicitly reveal the importance of dynamic corrections to phonon frequency of molecular-doped graphene, which have been previously proven to be crucial for electrochemical and substitutional doping with either B or N. These findings clearly contrast between the electrochemical and molecular doping methods of graphene and have merits such as controllability of the dopant, scalability, and ease of use over the direct synthesis methods. Using this method, it is possible to functionalize graphene by effectively controlling its band gap, thereby increasing applicability to various types of electronic devices. To implement the organic molecular doping method described herein, methods of doping at room temperature using chemicals having high or low electronegativities compared to carbon have been attempted [43,44]. Depending on whether number of electrons is insufficiently small or large enough on the graphene surface, the type of graphene is determined to be either p-type or n-type by accepting or repelling the electrons from the surface. The charge transfer takes place by the combinational determination by the graphene Fermi level, the highest occupied molecular orbital (HOMO), and the lowest unoccupied molecular orbital (LUMO) levels of the species adsorbed on the graphene surface. If the HOMO level of the adsorbent on graphene is higher than the graphene Fermi level, the adsorbent becomes a donor that transfers electrons to graphene. Conversely, when the LUMO of the adsorbent is higher than the Fermi level of graphene, charge transfer is allowed to take place from the graphene layer to the adsorbent which acts as the acceptor. Previous literature addresses that ammonium group (NH4) can be an ideal candidate for molecular doping [45]. The group meets the requirements, in the quantitative manner, for stable physisorption and efficient doping in graphene. The ammonium groups usually demonstrate relatively large physisorption energies more than 1 eV and effectively transform graphene into an n-type material. Also, the ammonium radicals show relatively large binding energies around 1.55 eV, compared with other small molecules, when they are physiosorbed on the graphene surface (Figure 3c). Tunability of molecular doping in an electrical matter was investigated in a back-gated field-effect transistors by Singh et al. (Figure 3d) [46]. The amount of charge transfer doping showed a monotonic decrease for one of the representative p-type dopants, gaseous dopant NO2, when the back-gate voltage increased in the negative direction. On the other hand, it showed a monotonic increase when n-type gaseous dopant NH3 was employed. The series of results strongly support that utilization of the principle of adsorption-driven doping technique can be expected for controlling the sensitivity and selectivity in molecular detector applications. For graphene, tetrafluoro-tetracyanoquinodimethane (F4-TCNQ) and fluoropolymer (CYTOP) are well known as adsorbents that cause active surface charges [44,47,48]. F4-TCNQ is a very strong electronic acceptor, and recently, the results of increasing the work function to 5.24 eV in graphene doping using this acceptor was reported [44]. The transfer of charge from F4-TCNQ to graphene is caused by the cyano functional groups, which are part of the structure of F4-TCNQ. This functional group is a structure in which electrons are insufficient and serve to strongly pull electrons from graphene. Owing to this, graphene provides electrons to F4-TCNQ, thereby forming a depletion layer and achieving p-type doping [47,48]. In the case of CYTOP, it replaces PMMA, which is mainly used to transfer graphene and has advantages where graphene doping can proceed simultaneously with transfer. This polymer support layer is a type of fluorine compound and can be easily structurally bonded to the carbon of graphene to cause p-type doping by bonding through a simple annealing process. Owing to the insulating characteristics of CYTOP, charge transfer cannot naturally occur between CYTOP and graphene. However, it has been reported that owing to the differences in electrostatic attraction, a dipole moment between graphene and CYTOP causes p-type doping of graphene [49,50]. That is, when a molecule capable of causing charge transfer is applied on graphene or a structure formed through deposition, charge transfer may occur spontaneously by the difference in electronegativity with carbon constituting graphene. Based on these advantages, organic molecular doping is expected to be the most effective method for doping graphene without an additional annealing process.

3. TMD Doping

3.1. Background

TMD doping techniques are classified in two ways: (i) atom-substitutional doping [51,52,53,54,55,56,57,58,59] and (ii) molecular doping. Substitutional doping replaces transition-metal (or chalcogen) atoms with dopants and has the merit of not damaging the crystal structure. However, control of the relative amounts of the different atoms is still challenging. As a result, accurate doping control for TMD materials doped with substitutional doping techniques has not yet been reported. Meanwhile, in molecular doping, the doping technique is divided into two mechanisms: (i) charge transfer from the dopant molecules to the TMDs and (ii) dipole effects of dopant molecules. TMDs are doped by transferring carriers directly from the dopant molecule to the TMD by the potential difference of the dopant molecule and the TMD. The dipole effect of the molecular dopant also provides electrical doping of TMDs. A typical feature of TMDs is the Schottky barrier (SB) of TMD–metal junctions. The SB prevents charge injection from the contact electrode to TMDs, which limits the electrical performance, including the effective charge carrier mobility and subthreshold swing. Additional dipole effects in the molecular dopant modify the energy structure of the TMD; hence, the SB width at the TMD and metal interface can be modulated by the dipole moment of the molecular dopant. In particular, in the case of SAMs, forming a junction with the TMD surface and the alignment structure of the monolayer has an effective dipole effect. Furthermore, SAMs adjust the dipole direction (i.e., negative or positive dipole) and intensity depending on their functional group. However, both (i) atom-substitutional doping and (ii) molecular doping techniques have several limitations, including environmental and operational stability of the doping effect, off-current increase, and difficulty of accurate doping control. This section describes the features, advantages and disadvantages of recently reported substitution and molecular doping methods on TMDs. In addition, the fundamental principles of the organic molecular doping process are described, and its application to photodetectors, complementary circuits, and neuromorphic devices are reviewed.

3.2. Substitutional Doping

Much efforts have been made to dope TMDs to precisely control their electrical properties, and intrinsic semiconductors are becoming more important. One approach is to produce doped TMDs by substitution of (i) transition metal [51,52,53,54,55,56,57,58,59] or (ii) chalcogen atoms [60,61,62,63,64,65,66] within the TMD lattice. In TMD composed of transition metal (M) interposed between two chalcogen (X) atomic layers, substitutional doping of TMD is realized through replacement of the transition metal atom (e.g., Mo or W) or chalcogen atom (e.g., S, Se, or Te) with another atom. This doping approach forms a new chemical bond, which provides higher doping effect stability when compared to charge transfer doping. Using the in-situ synthesis doping process of the acceptor Niobium (Nb), substitutionally Nb-doped WSe2 can be fabricated (Figure 4a) [51,55,56,58]. The doping process substituted by Nb enables reducing the contact resistance for hole charge carriers, and as a result, high-performance p-type operation as high as 116 cm2V−1s−1 with an on/off ratio of 106 was obtained (Figure 4b) [51]. Besides, there are successful cases of substitutional doping based on various transition metal atoms, such as iron (Fe), rhenium (Re), and vanadium (V), achieving Fe-doped WS2, Re-doped MoS2, and in-plane heterostructures, such as V-doped WxMo1−xS2−MoxW1−xS2 by liquid-phase precursor-assisted synthesis (Figure 4c) [59].
Recently, the n-doping effect in WS2 was reported for Sn-substituted Snx-W1-x-S2 through post-growth substitution [57]. In addition to transition metal substitution, the chalcogen atom can be substituted with chlorine (Cl) [62,64], nitrogen (N) [60,63], or oxygen (O) [61,65]. Cl substitution doping by remote inductively coupled plasma (ICP) allowed MoS2 to be n-doped with a Fermi level shift close to the conduction band (Figure 5a) [64]. Electron irradiation beam (e-beam) causes atom sputtering to create a sulfur vacancy, which enables post-synthesis doping [66]. Another technique to produce chalcogen-atom-substituted doping is dipping in 1,2-dichloroethane (DCE) solution, resulting in a reduction of the SB width with electrical n-doping effects (Figure 5b) [62]. The Cl-doping enables the contact resistances of WS2 and MoS2 to decrease to 0.7 kΩ·μm and 0.5 kΩ·μm, respectively. Meanwhile, p-doping effects can be obtained by substitution with N atoms on chalcogen vacancies. Atomic nitrogen treatment by plasma-confinement plate induced p-type behaviors of nitrogen-doped WS2 from the baseline n-type WS2, which enabled complementary device operation of WS2 (Figure 5c) [63]. In addition to atomic substitutions, hydrogenated MoS2-TM (Co, Ni and Cu) can be obtained through the adsorbed O2 with the formation of OOH radical (Figure 5d) [61]. Thus, it is important to form accurately controlled vacancies in TMDs where the dopants are implanted.

3.3. Molecular Doping

Compared to substitutional doping techniques, molecular doping has several advantages: low-cost processing and large area coverage. By simply coating or depositing a film that provides a doping effect, the electrical properties of the TMDs, such as effective mobility, threshold voltage, and subthreshold swing, can be adjusted. This approach enables forming a heterostructure of the doping film and the TMD, in which the electrical or optical characteristics of the TMDs can be enhanced by (i) charge transfer from the dopant molecules to TMDs [62,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92] or (ii) dipole effects of the dopant molecules of the doping film [4,5,6,7,93,94,95]. The energy band structure of MoS2 could be controlled through molecular doping from the deposited tetrathiafulvalene and dimethyl-phenylenediamine molecules as donors and tetracyanoethylene (TCNE) and tetracyanoquinodimethane (TCNQ) as acceptors (Figure 6a,b) [72,88]. Solution-coating of polyethyleneimine (PEI) showed effective doping on device characteristics by reducing the contact resistance; accordingly, effective mobility was improved by 1.6 times (Figure 6c) [68,85]. However, (i) charge transfer effects from dopant molecules could be easily degenerated as this doping approach is fundamentally a reaction by physical adsorption rather than doping by chemical bonding. For example, in MoS2 and WSe2, the charge transfer doping with enhanced electrical properties was achieved with potassium [75], but the doping effect was not stable in air (Figure 6d). Thus, air-stability in molecular doping has been considered as an important developmental aspect. Benzyl viologen (BV) provided air-stable n-doping effects on MoS2, and as a result, a subthreshold swing of 77 mV/decade and high sheet electron density of 1.2 × 1013 cm−2 were obtained in ambient air. Triphenylphosphine (PPh3) was used as a dopant with controllable non-degenerate doping, which provided robust doping of MoS2 for 14 days in ambient air (Figure 6e,f) [2,88]. By controlling the ratio of the two dopants: tris(pentafluorophenyl)borane (BCF), containing electron-withdrawing fluorine, and tritolylborane (TTB), containing electron donor methyl groups, the operation behaviors of TMDs were controlled from ambipolar to unipolar switching characteristics (Figure 6g) [2,88].
The doping effect by (ii) dipole of dopant molecules showed non-degenerated effects. The SAM treatment of octadecyltrichlorosilane (OTS) caused a positive dipole moment at the WSe2-OTS interface, enabling the p-doping phenomenon (Figure 7a,b) [4,6]. On the other hand, the SAM treatment of (3-aminopropyl) trimethoxysilane (APTMS) caused a negative dipole moment, turning out the n-doping of rhenium diselenide (ReSe2) [90,96]. Because the SAM materials are aligned to form a junction on the surface of the TMDs, the interface dipole is effectively provided [97,98,99,100,101]. Oxide dopantsof transition metal oxides (TMO) also provide non-degenerated doping effects on TMDs [71]. TiO2 and MoO3 form interface dipole, enabling n- and p-doping of MoS2, respectively, non-degenerately. Poly-(diketopyrrolopyrrol-eterthiophene) (PDPP3T) as a polymer semiconductor exhibited a high doping effect on multilayer MoSe2 and MoS2, leading to significant improvements in the on-current (≈×2000 higher) (Figure 7c,d) [93,94]. Polymer chains in PDPP3T assist alignment with directionality in junction structure with TMDs, providing effective charge transfer and dipole effects. To provide high-stable doping effects, a two-step functionalization doping scheme was developed. The two-step n-doping process based on oxygen plasma treatment and Al2O3 deposition allowed MoSe2 transistors to operate as unipolar n-doped behavior, and the negative bias illumination stress (nbis) test for 7200 s and the environmental stability test for 21 days showed unchanged stable doping effect (Figure 7e) [91]. Although the molecular doping techniques have been intensively studied for control of the TMD devices, uniformity and controllability still remain as challenging issues.

3.4. Applications

The electrical properties can be controlled through TMD doping, and various applications of photodetectors [84,86], complementary circuits [73,74], and neuromorphic devices [89] have been actively demonstrated. As the doping techniques modulate the energy band of TMDs, not only electrical properties but also optical properties can be improved through doping [4,7,84,86,89,90,94,96]. Higher photoresponsivity and temporal photoresponse performance could be achieved by the surface charge transfer doping. Another application is to build complementary circuits by selective doping of TMDs [73,74,80,81,94]. Pristine TMD devices suffer from ambipolar characteristics, normally-on operation due to VTH shift, and contact resistance, which limit implementation to complementary circuits. High DC voltage gain of the complementary inverter as high as ~170 V/V was obtained by p-type MoSe2 transistor and the PDPP3T-doped n-type MoS2 transistor (Figure 8a,b) [94]. Recently emerging applications are neuromorphic devices such as synaptic transistors and artificial neurons [102]. SB barrier modulation by defect doping and 1T′ (metal) phase transition by lithium-ion intercalation enabled MoS2 to operate as a synaptic memristor behavior. Neuromorphic phototransistors were demonstrated by using charge transfer effects in perovskite and MoS2 hybrid structure, which emulated human sensory adaptation (Figure 8c) [89]. Furthermore, the improvement of sensing properties can be achieved by the doping methods in 2D materials [102,103,104,105,106,107,108,109]. As an example, Au nanoparticles on MoS2 induced n-doping effects, which significantly enhanced chemical sensing properties with respect to various volatile organic compounds (Figure 8d) [109]. Another emerging application based on the doping process in 2D materials is found in nanomechanics [110,111,112,113]. To make high performance nanogenerators with larger output power, formation of surface charges or control of work functions of 2D materials is crucial. Graphene quantum dots were n-doped with nitrogen, providing high photoluminescence (PL) quantum efficiency above than 90% [110]. Also, negatively-charged graphene surface had an ion-dipole interaction with the positive charged in the polyvinylidenefluoride (PVDF), which resulted in enhanced triboelectric nanogenerator (Figure 8e). Furthermore, AuCl3-doped crumpled graphene enabled the triboelectric nanogenerator to operate with higher performance of output voltage and current = 80.6 V and 11.9 μA/cm2 at the doping level of 1.2 mg/mL [111]. Because doping technique can substantially control the electronic structure of a TMD, various doping processes can be applied according to the requirements for specific device application (Table 1).

4. Conclusions and Outlook

In this review, we have provided an overview of important recent researches on doping strategies covering substitutional, chemical and molecular methods for graphene and advanced two-dimensional semiconducting materials. Owing to the atomically thin nature and dangling-bond free surface, two-dimensional semiconducting materials are regarded as a strong candidate for the viable channel materials that can prevent short-channel effects. To further expand the potential applications of these two-dimensional semiconductor materials, technologies capable of precisely controlling the electrical properties of the material are essential. Recently, there is a continuous demand for the development of doping techniques for these two-dimensional semiconducting materials that can improve device performance by precisely controlling the carrier concentration. Doping has been traditionally used to effectively change the electrical and electronic properties of materials through relatively simple processes. To change the electrical properties, substances that can donate or remove electrons are added. Doping of atomically thin two-dimensional semiconductor materials is similar to that used for silicon but has a slightly different mechanism. When it comes to doping techniques accompanying doping-induced bandgap modification, the strain effects should be considered doubtlessly. One of the most recent articles reveals that bandgap engineering can be expected in the TMD semiconductor materials [22], which can be substantially carried out in doping process simultaneously in some cases. At the same time, the interfacial status should be recursively studied in this doping-induced bandgap modulation scenario because the increase in instability of the interface states results in the degradation of carrier mobilities and unwanted memory effects which threaten ideal transistor characteristics. While more advanced doping techniques with higher reliability and process repeatability are developed, these two practical concerns can be more delved into than ever toward integrated circuit and system-level applications of the graphene and TMD semiconductor materials. This review presented an overview of recent advanced doping techniques covering substitutional, chemical and molecular methods of graphene and TMDs, which are the representative 2D semiconductor materials.

Funding

This research was supported by the Ministry of Trade, Industry and Energy of Korea (MOTIE) with the Korean Semiconductor Research Consortium (KSRC) through the program for development of future semiconductor devices (Grant No. 10080513) and also supported in part by the National Research Foundation of Korea (NRF) Grant funded by the Ministry of Science and ICT of Korea (MSIT) (Grant No. NRF-2020R1A2C1101647).

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. (a) Schematic illustration of the chemical vapor deposition (CVD) deposition of B-G on Cu foils by using phenylboronic acid (adapted from [23] with permission from Journal of Materials Chemistry A). (b) Experimental setup commonly used for CVD graphene doping (adapted from [25] with permission from Chemical Society Reviews). (c) Schematic diagram of the possible mechanism of nitrogen incorporation in CNWs by NH3 and N2 plasma post-treatment respectively (adapted from [24] with permission from Nano-Micro Letters). (d) N-doped graphene derived from polypyrrole [25] (adapted from [25] with permission from Chemical Society Reviews).
Figure 1. (a) Schematic illustration of the chemical vapor deposition (CVD) deposition of B-G on Cu foils by using phenylboronic acid (adapted from [23] with permission from Journal of Materials Chemistry A). (b) Experimental setup commonly used for CVD graphene doping (adapted from [25] with permission from Chemical Society Reviews). (c) Schematic diagram of the possible mechanism of nitrogen incorporation in CNWs by NH3 and N2 plasma post-treatment respectively (adapted from [24] with permission from Nano-Micro Letters). (d) N-doped graphene derived from polypyrrole [25] (adapted from [25] with permission from Chemical Society Reviews).
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Figure 2. (a) Schematic band structures of graphene (adapted from [11] with permission from Insciences Journals). (b) Sheet resistance measurements of few-layer graphene (FLG) samples made before and after doping with different AuCl3 concentrations (adapted from [34] with permission from Applied Surface Science). (c) Non-equilibrium Green’s function (NEGF)-based simulations comparing three types of graphene channel potentials (adapted from [33] with permission from Nano Letters). (d) Schematic of an n-type graphene transistor with SU-8 as an n-type dopant and self-encapsulation. Upper diagram described basic chemical compounds of SU-8 and the chemical reaction for generating photo-acid upon UV exposure (adapted from [41] with permission from Applied Physics Letters).
Figure 2. (a) Schematic band structures of graphene (adapted from [11] with permission from Insciences Journals). (b) Sheet resistance measurements of few-layer graphene (FLG) samples made before and after doping with different AuCl3 concentrations (adapted from [34] with permission from Applied Surface Science). (c) Non-equilibrium Green’s function (NEGF)-based simulations comparing three types of graphene channel potentials (adapted from [33] with permission from Nano Letters). (d) Schematic of an n-type graphene transistor with SU-8 as an n-type dopant and self-encapsulation. Upper diagram described basic chemical compounds of SU-8 and the chemical reaction for generating photo-acid upon UV exposure (adapted from [41] with permission from Applied Physics Letters).
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Nanomaterials 11 00832 g003 550
Figure 3. (a) Electronic structure of the pristine single-layer graphene, aniline-adsorbed graphene, and nitrobenzene-adsorbed graphene (adapted from [21] with permission from Physical Review B). (b) Top view of the lowest-energy configurations of the molecules adsorbed on graphene (adapted from [21] with permission from Physical Review B). (c) Electronic density of states (DOS) for graphene with no impurities (shaded area) and with a physiosorbed NH4 group (black solid line) (top). N–H complex: H atom trapped at a substitutional N dopant site of graphene (bottom left). A NH3 molecule physiosorbed over a N–H complex (C: gray; N: light gray (cyan)); H: white spheres (bottom right) (adapted from [45] with permission from Physical Review B). (d) Current-voltage transfer characteristics of aback-gated CVD graphene field-effect transistor (FET) in air and in the presence of NO2 and NH3. Inset shows the percentage conductance changes of CVD grown multi-layer graphene (MLG) with the flow of 20 ppm NO2 and 550 ppm NH3 (top). Energy-band diagrams showing shift in Fermi level in back-gated graphene sensor as a result of gate bias and NO2 adsorption (bottom) (adapted from [46] with permission from Applied Physics Letters). (e) Molecular structure of F4-TCNQ. Bond lengths are in Å and angles in degrees (left). Molecule of F4-TCNQ on top of graphene (right) (adapted from [48] with permission from Journal of Physics: Condensed Matter).
Figure 3. (a) Electronic structure of the pristine single-layer graphene, aniline-adsorbed graphene, and nitrobenzene-adsorbed graphene (adapted from [21] with permission from Physical Review B). (b) Top view of the lowest-energy configurations of the molecules adsorbed on graphene (adapted from [21] with permission from Physical Review B). (c) Electronic density of states (DOS) for graphene with no impurities (shaded area) and with a physiosorbed NH4 group (black solid line) (top). N–H complex: H atom trapped at a substitutional N dopant site of graphene (bottom left). A NH3 molecule physiosorbed over a N–H complex (C: gray; N: light gray (cyan)); H: white spheres (bottom right) (adapted from [45] with permission from Physical Review B). (d) Current-voltage transfer characteristics of aback-gated CVD graphene field-effect transistor (FET) in air and in the presence of NO2 and NH3. Inset shows the percentage conductance changes of CVD grown multi-layer graphene (MLG) with the flow of 20 ppm NO2 and 550 ppm NH3 (top). Energy-band diagrams showing shift in Fermi level in back-gated graphene sensor as a result of gate bias and NO2 adsorption (bottom) (adapted from [46] with permission from Applied Physics Letters). (e) Molecular structure of F4-TCNQ. Bond lengths are in Å and angles in degrees (left). Molecule of F4-TCNQ on top of graphene (right) (adapted from [48] with permission from Journal of Physics: Condensed Matter).
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Figure 4. (a) Nb-doped WSe2 monolayer for DFT calculations (adapted from [51] with permission from Royal Society of Chemistry). (b) Schematic of monolayer NbxW1−xS2 and transfer characteristics of the monolayer (black line is NbxW1−xS2, red line is WS2) (adapted from [55] with permission from ACS publications). (c) Experimental and simulated STEM images and line scans of Re and Mo dopants; the dots in the line scans represent experimental results, whereas the solid lines represent simulated results (adapted from [59] with permission from ACS publications).
Figure 4. (a) Nb-doped WSe2 monolayer for DFT calculations (adapted from [51] with permission from Royal Society of Chemistry). (b) Schematic of monolayer NbxW1−xS2 and transfer characteristics of the monolayer (black line is NbxW1−xS2, red line is WS2) (adapted from [55] with permission from ACS publications). (c) Experimental and simulated STEM images and line scans of Re and Mo dopants; the dots in the line scans represent experimental results, whereas the solid lines represent simulated results (adapted from [59] with permission from ACS publications).
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Figure 5. (a) Change in band structure for adsorption of chlorine atom on S vacancy of MoS2 (adapted from [64] with permission from Royal Society of Chemistry). (b) Transfer length method (TLM) resistances of Cl-doped WS2 and MoS2 and schematic band diagram of metal-transition metal dichalcogenide (TMD) contacts with and without chloride doping (adapted from [62] with permission from ACS publications). (c) Transfer characteristics at VDS = 1 V for pristine WS2 and N-WS2 transistors (adapted from [63] with permission from ACS publications). (d) Geometric structure and charge density difference for intermediate OOH adsorption on the hydrogenated MoS2-TM (Co, Ni and Cu) system; the gray, red, violet, pink, green, blue, and yellow spheres represent H, O, Co, Ni, Cu, Mo and S atoms, respectively (adapted from [61] with permission from Elsevier).
Figure 5. (a) Change in band structure for adsorption of chlorine atom on S vacancy of MoS2 (adapted from [64] with permission from Royal Society of Chemistry). (b) Transfer length method (TLM) resistances of Cl-doped WS2 and MoS2 and schematic band diagram of metal-transition metal dichalcogenide (TMD) contacts with and without chloride doping (adapted from [62] with permission from ACS publications). (c) Transfer characteristics at VDS = 1 V for pristine WS2 and N-WS2 transistors (adapted from [63] with permission from ACS publications). (d) Geometric structure and charge density difference for intermediate OOH adsorption on the hydrogenated MoS2-TM (Co, Ni and Cu) system; the gray, red, violet, pink, green, blue, and yellow spheres represent H, O, Co, Ni, Cu, Mo and S atoms, respectively (adapted from [61] with permission from Elsevier).
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Figure 6. (a,b) Charge transfer between molecular donors (tetracyanoethylene (TCNE) and tetracyanoquinodimethane (TCNQ)) and MoS2 with sulfur vacancies. Total density of states (DOS) (black) and local density of state (LDOS) of the molecule (red) (adapted from [72] with permission from ACS publications). (c) Transfer characteristics of pristine and poly (ethylene imine) (PEI)-doped multilayer MoS2 transistors (adapted from [85] with permission from John Wiley and Sons). (d) Schematic of a top-gated few-layer WSe2 transistor with chemically n-doped source/drain contacts by K exposure [75]. (e) Transfer characteristics of a 3-layer WSe2 device (L∼6.2 μm) as a function of K exposure time (adapted from [75] with permission from ACS publications). (f) Descriptive diagram for n-doping mechanism of PPh3 at the PPh3/WSe2 interface (adapted from [84] with permission from John Wiley and Sons). (g) Extracted field-effect mobility ratio (μFE ratio = μFE_PPh3/μFE_Control) at VGS = VTH (adapted from [84] with permission from John Wiley and Sons). (h) Transfer characteristics of MoS2 device on a semi-log scale with gradually decreasing ratios of TPB/BCF (VDS = 0.1 V) (adapted from [83] with permission from Royal Society of Chemistry).
Figure 6. (a,b) Charge transfer between molecular donors (tetracyanoethylene (TCNE) and tetracyanoquinodimethane (TCNQ)) and MoS2 with sulfur vacancies. Total density of states (DOS) (black) and local density of state (LDOS) of the molecule (red) (adapted from [72] with permission from ACS publications). (c) Transfer characteristics of pristine and poly (ethylene imine) (PEI)-doped multilayer MoS2 transistors (adapted from [85] with permission from John Wiley and Sons). (d) Schematic of a top-gated few-layer WSe2 transistor with chemically n-doped source/drain contacts by K exposure [75]. (e) Transfer characteristics of a 3-layer WSe2 device (L∼6.2 μm) as a function of K exposure time (adapted from [75] with permission from ACS publications). (f) Descriptive diagram for n-doping mechanism of PPh3 at the PPh3/WSe2 interface (adapted from [84] with permission from John Wiley and Sons). (g) Extracted field-effect mobility ratio (μFE ratio = μFE_PPh3/μFE_Control) at VGS = VTH (adapted from [84] with permission from John Wiley and Sons). (h) Transfer characteristics of MoS2 device on a semi-log scale with gradually decreasing ratios of TPB/BCF (VDS = 0.1 V) (adapted from [83] with permission from Royal Society of Chemistry).
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Nanomaterials 11 00832 g007 550
Figure 7. (a) Schematic of back-gated transistor fabricated on octadecyltrichlorosilane (OTS)-doped WSe2 and energy band diagrams of Pt-WSe2-Pt junctions (adapted from [79] with permission from ACS publications). (b) Transfer characteristics of transistors fabricated on (black) undoped and (red) 1.2% OTS-doped WSe2 devices (adapted from [79] with permission from ACS publications). (c) Schematic of PDPP3T-doped MoSe2 transistor (adapted from [93] with permission from John Wiley and Sons). (d) Transfer characteristics of PDPP3T-doped MoSe2 as a function of annealing temperature (adapted from [93] with permission from John Wiley and Sons). (e) Comparison of shifts in VTH derived from NBIS test results (adapted from [91] with permission from John Wiley and Sons).
Figure 7. (a) Schematic of back-gated transistor fabricated on octadecyltrichlorosilane (OTS)-doped WSe2 and energy band diagrams of Pt-WSe2-Pt junctions (adapted from [79] with permission from ACS publications). (b) Transfer characteristics of transistors fabricated on (black) undoped and (red) 1.2% OTS-doped WSe2 devices (adapted from [79] with permission from ACS publications). (c) Schematic of PDPP3T-doped MoSe2 transistor (adapted from [93] with permission from John Wiley and Sons). (d) Transfer characteristics of PDPP3T-doped MoSe2 as a function of annealing temperature (adapted from [93] with permission from John Wiley and Sons). (e) Comparison of shifts in VTH derived from NBIS test results (adapted from [91] with permission from John Wiley and Sons).
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Figure 8. (a) Schematic of complementary metal-oxide-semiconductor (CMOS) inverter using doped-MoS2 and MoSe2 transistors (adapted from [94] with permission from ACS publications). (b) Transfer curves of CMOS inverter using doped-MoS2 and MoSe2 transistors (adapted from [94] with permission from ACS publications). (c) Sensory adaptation of the eye and CsPb(Br0.5I0.5)3−MoS2 phototransistor (adapted from [89] with permission from ACS publications). (d) Real-time resistances of pristine MoS2 and Au-doped MoS2 sensors exposed to various VOCs (adapted from [109] with permission from ACS publications). (e) Triboelectric nanogenerator using n-doped graphene quantum dots and polyvinylidenefluoride (PVDF) (adapted from [110] with permission from Elsevier).
Figure 8. (a) Schematic of complementary metal-oxide-semiconductor (CMOS) inverter using doped-MoS2 and MoSe2 transistors (adapted from [94] with permission from ACS publications). (b) Transfer curves of CMOS inverter using doped-MoS2 and MoSe2 transistors (adapted from [94] with permission from ACS publications). (c) Sensory adaptation of the eye and CsPb(Br0.5I0.5)3−MoS2 phototransistor (adapted from [89] with permission from ACS publications). (d) Real-time resistances of pristine MoS2 and Au-doped MoS2 sensors exposed to various VOCs (adapted from [109] with permission from ACS publications). (e) Triboelectric nanogenerator using n-doped graphene quantum dots and polyvinylidenefluoride (PVDF) (adapted from [110] with permission from Elsevier).
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Table
Table 1. Comparison among TMD doping techniques with respect to doping process temperature, features, and applications.
Table 1. Comparison among TMD doping techniques with respect to doping process temperature, features, and applications.
CategoryTMDDopantDoping Process
Temperature (°C)		FeaturesDevice and
Application		Ref.
Substitutional dopingWS2Nb800–830
(doping in synthesis)		Supply of Nb/
Lattice Strain		Transistor [55,56]
Substitutional dopingMoS2Nb/Re750
(doping in synthesis)		Supply of Nb and ReTransistor[58]
Substitutional dopingMoS2/
WS2		Fe, Re, and V700–800
(doping in synthesis)		Liquid-phase precursor-assistN/A[59]
Substitutional dopingMoS2N~200
(doping in synthesis)		Hydrothermal methodSupercapacitor[60]
Molecular
doping		MoS2Benzyl viologenRoom
temperature		Air-stable dopingTransistor[2]
Molecular
doping		MoS2/
WS2		ClRoom
temperature		Using 1, 2 dichloroethane (DCE)Transistor[62]
Molecular
doping		MoS2ClN/ACl in remote
plasma		Transistor[64]
Molecular
doping		MoS2Oleylamine300Contact resistance analysisTransistor[69]
Molecular
doping		WSe2TriphenylphosphineN/ACharge transfer dopingTransistor/
photodetector		[84]
Molecular
doping		MoS2PolyethylenimineRoom
temperature		Charge injectionTransistor/
photodetector		[85]
Molecular
doping		MoS2CsPb(Br1–xIx)3 perovskite100Phase segregation effectSensory adaptive photodetector[89]
Molecular
doping		MoSe2,
MoS2		PDPP3T300Schottky barrier modulationPhotodetector/
CMOS inverter		[93,94]
Molecular
doping		MoS2Au nanoparticleRoom
temperature		Charge transfer dopingVOCs sensor[109]
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Yoo, H.; Heo, K.; Ansari, M.H.R.; Cho, S. Recent Advances in Electrical Doping of 2D Semiconductor Materials: Methods, Analyses, and Applications. Nanomaterials 2021, 11, 832. https://doi.org/10.3390/nano11040832

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Yoo H, Heo K, Ansari MHR, Cho S. Recent Advances in Electrical Doping of 2D Semiconductor Materials: Methods, Analyses, and Applications. Nanomaterials. 2021; 11(4):832. https://doi.org/10.3390/nano11040832

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Yoo, Hocheon, Keun Heo, Md. Hasan Raza Ansari, and Seongjae Cho. 2021. "Recent Advances in Electrical Doping of 2D Semiconductor Materials: Methods, Analyses, and Applications" Nanomaterials 11, no. 4: 832. https://doi.org/10.3390/nano11040832

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