Abstract

Morphotaxy, a process by which a 2D material is chemically modified while retaining its original physical dimensions, is an emerging strategy for synthesizing unconventional materials at the atomically thin limit. Morphotaxy is typically implemented by vapor-phase reactions on mechanically exfoliated or vapor-deposited 2D van der Waals (vdW) materials. Here we report a method for converting solution-processed films of 2D InSe into InI2 and InBr2 using dilute I2 and Br2 solutions, respectively. The converted materials retain the physical dimensions of the original 2D flakes, providing access to non-vdW indium halides in ultrathin form. Liquid-phase exfoliation directly enables this morphotaxial reaction by producing nanosheets with high surface areas and introducing residual polyvinylpyrrolidone that stabilizes the flake morphology and slows the reactivity of I2 and Br2. Overall, this work presents a versatile strategy for achieving atomically thin metal halides and offers mechanistic insights relevant to the morphotaxial halogenation of other solution-processed 2D materials.
Keywords: 2D materials, halogenation, chemical conversion, morphotaxy, solution processing
Over the past two decades, the family of two-dimensional (2D) materials has expanded steadily, enabling access to diverse optical, electronic, and magnetic phenomena.1−3 The vast majority of 2D materials are atomically thin analogues of bulk, layered van der Waals (vdW) crystals, which are obtained either through top-down exfoliation or bottom-up growth processes. Chemical modification, including substitutional doping4 and surface functionalization,5,6 is a powerful strategy for tailoring the physical properties of 2D materials for a wide range of applications. In the extreme case, chemical modification can completely convert a 2D material into a new 2D material of different chemical composition. This class of reactions has recently been described by the term morphotaxy.7 The key attraction of morphotaxy is that the new material retains the shape and dimensions of the original flake or film.7 Morphotaxy allows materials to be accessed in an atomically thin form even if they cannot be exfoliated from a bulk crystal or grown by traditional methods–which can be the case if no bulk analogue exists,8,9 the bulk form does not have a layered crystal structure,10−12 or individual layers in the vdW crystal are difficult to isolate.13 Importantly, morphotaxy not only expands the scope of accessible 2D materials but also facilitates the fabrication of lateral and vertical 2D heterostructures.14−16
Metal chalcogenides have been widely explored as starting materials for morphotaxial transformations. These materials have well-studied methods of preparation and are amenable to a range of chemical reactions including oxidation,14,17 cation exchange,18 chalcogen exchange,15,18 and pnictogen substitution.11,12 However, an underexplored area of morphotaxy research is the halogenation of metal chalcogenides. A large number of emerging 2D materials contain metal–halogen bonds, such as the monolayer ferromagnet CrI3,19−22 the noncolinear antiferromagnet NiI2,23−25 and the antiferromagnetic anisotropic semiconductor CrSBr,26−28 thus motivating the morphotaxial synthesis of additional 2D metal halides. Morphotaxial halogenation of metal chalcogenides has only been reported in two cases–namely, the synthesis of BiTeX (X = Br, Cl) from Bi2Te3 using BiX3 vapor13 and Se-doped InF3 through a high-pressure and high-temperature reaction of InSe and XeF2.10 Therefore, it is of high interest to expand the toolbox of morphotaxial reactions to include a generalized halogenation strategy with a broadened scope of final products and properties.
The majority of reported morphotaxial reactions have been demonstrated using mechanically exfoliated or vapor-deposited starting materials. A key knowledge gap exists in the application of morphotaxy to solution-processed 2D materials, a burgeoning field that enables scalable, low-cost production of printed and flexible electronics and optoelectronics.29−32 Solution-processed films present more chemically complex systems than mechanically exfoliated or vapor-deposited materials since they often contain residual solvents, surfactants, and polymers as well as a large degree of morphological disorder. Due to these challenges, there have been limited demonstrations of morphotaxy using solution-processed 2D materials.10,18 In addition, key mechanistic questions for morphotaxial processes in solution-processed 2D materials have yet to be answered, including the role of organic residues in morphotaxial reactions and whether nanosheets in percolating films can maintain their morphologies following chemical conversion.
Here we report the morphotaxial bromination and iodination of solution-processed InSe films using dilute solutions of I2 and Br2. X-ray photoelectron spectroscopy (XPS), time-of-flight secondary ion mass spectrometry (ToF-SIMS), and energy dispersive X-ray spectroscopy (EDS) confirm that selenium is completely removed in the final material and iodine or bromine are present in an approximate 2:1 atomic ratio with indium. Raman spectroscopy provides further spectroscopic evidence for the identification of these materials as indium dihalides. In addition, atomic force microscopy (AFM) reveals that the shape and dimensions of the original InSe nanosheets are maintained through the reaction. Notably, this morphotaxial synthetic pathway allows the non-vdW materials InI2 and InBr2 to be produced in ultrathin form, although they ultimately become amorphous, as confirmed by transmission electron microscopy (TEM) and selected area electron diffraction (SAED). We also show that residual surface-bound polyvinylpyrrolidone (PVP) from the original solution-based InSe exfoliation plays a key role in mediating the reaction and stabilizing the nanosheet morphology. Furthermore, we demonstrate that In2Se3 can also be used as a starting material for this morphotaxial halogenation reaction. This work provides key mechanistic insights and establishes a morphotaxial halogenation pathway that can likely be generalized to other solution-processed 2D materials.
InSe dispersions were prepared by electrochemical exfoliation using established procedures.33−35 To avoid ambient oxidation of InSe, all procedures were carried out in an inert glovebox atmosphere using anhydrous solvents.36−38 The solution-exfoliated InSe nanosheets were characterized before treatment using AFM, TEM, and XPS. Topographical AFM images show that the exfoliated flakes have an average thickness of ∼2 nm and an average lateral size of ∼700 nm (Figure S1). Transmission electron micrographs show outlines of distinct overlapping flakes (Figure S2a), while SAED of the film shows a 6-fold diffraction pattern consistent with the hexagonal lattice symmetry of InSe (Figure S2b).39 XPS analysis shows In 3d and Se 3d peaks with binding energies matching those reported in literature (Figure 1b).35 Quantification of these peaks gives a Se:In ratio of ∼1.2. Notably, the Se 3d region shows no features in the range of 58–62 eV, indicating that no InSe oxidation occurs during liquid-phase exfoliation and thin film preparation. Significant carbon, nitrogen, and oxygen XPS peaks are observed due to the presence of residual PVP (Figure S3).
Figure 1.
(a) Schematic representation of the morphotaxial halogenation of InSe. (ODCB = o-dichlorobenzene.) (b) X-ray photoelectron spectroscopy (XPS) of selected elemental peaks for electrochemically exfoliated InSe and morphotaxially converted indium halides. Binding energies are referenced to the SiO2 substrate (Si 2p = 103.5 eV). The spectra are shifted vertically for clarity, and a vertical line is included to assist in comparing the In 3d peak positions. (c) Raman spectra of InSe, c-InI2, and c-InBr2 films. The spectra are shifted vertically for clarity. (d, e) Time-of-flight secondary ion mass spectrometry (ToF-SIMS) of (d) c-InI2 and (e) c-InBr2 collected under negative ion detection mode.
To prepare the halogenated materials, spin-coated films of InSe were treated with dilute solutions of I2 and Br2 at 150 °C under inert atmosphere, as shown in Figure 1a. Following treatment, XPS shows the complete removal of selenium from the films and the appearance of iodine and bromine peaks (Figure 1b). The In 3d peak shifts from 444.6 to 445.3 and 445.8 eV for the I2-treated film and Br2-treated film, respectively. Depth profiling shows that the halogen and indium signals are present throughout the entire ∼100 nm thick film, while no selenium peaks are observed (Figure S5), indicating that our approach is effective in fully converting percolating films of InSe.
Indium forms a variety of halides with iodine and bromine, most notably trihalides, dihalides, and monohalides. The trihalides are commercially available as microcrystalline powders. InI3 adopts a dimeric structure consisting of In2I6 molecules,40 while InBr3 adopts a 2D layered crystal structure.41 The dihalides are isostructural, adopting a mixed-valent In(InX4) structure.42,43 The trihalides and dihalides are difficult to distinguish on the basis of XPS peak positions alone: both InI3 and InI2 show a single In 3d doublet with the 3d5/2 component centered at 445.1 ± 0.1 eV, while InBr3 and InBr2 appear at 445.8 ± 0.1 eV and 445.9 ± 0.1 eV, respectively.44 Therefore, our experimentally observed indium binding energy is consistent with both stoichiometries. The Br 3d and I 3d peak positions also align well with the literature values for both compounds.44
To assess the stoichiometry of the converted films, atomic percentages were calculated based on the XPS peak areas. The ratio of halogen to indium in the films shows a strong depth dependence. Measurements taken at the surface of the films treated with I2 and Br2 show an I:In ratio of 4.4 and a Br:In ratio of 3.6, respectively. However, the ratios fall to 2.2 and 2.3, respectively, after ion beam etching for 30 s (Figure S5). The second set of data more accurately reflects the composition of the converted material, since the surface of the film likely contains excess physisorbed I2 and Br2 that is not removed following the halogenation reaction. The chemical shifts of these species overlap strongly with those of the c-InI2 and c-InBr2, so the individual contributions to the I 3d and Br 3d signals are not resolved in the XPS data. Furthermore, the X:In ratio of approximately 2:1 is corroborated by energy dispersive X-ray spectroscopy (EDS) measurements, as discussed below. These results indicate that the reactions convert InSe to indium dihalides. We therefore denote the chemically converted materials as c-InI2 and c-InBr2.
The chemically converted c-InI2 and c-InBr2 materials, as well as the untreated InSe, were analyzed by Raman spectroscopy. The Raman peak positions of the starting material match those reported for few-layer InSe, with major peaks at 111 cm–1, 210 cm–1, and 233 cm–1 (Figure 1c).45 After halogenation, c-InI2 shows a single strong peak at 138 cm–1, while c-InBr2 shows a single peak at 196 cm–1 (Figure 1c). These features can be assigned to the symmetric stretching modes of InX4– anions, which are present in solid InI2 and InBr2.46−49 For comparison, we also performed Raman spectroscopy on InBr3 and InI3 prepared by mechanical exfoliation of commercially available powders (Figures S6–S8). Mechanically exfoliated InI3 shows several peaks below 200 cm–1, the strongest of which (133 cm–1) corresponds to a symmetrical stretching mode of In2I6 dimers.46 InBr3 shows a major peak at 169 cm–1 as well as smaller peaks at 83 cm–1 and 56 cm–1 in agreement with literature.47,48 These results further support the assignment of the converted material as InX2 rather than InX3. However, the Raman signals for c-InI2 and c-InBr2 are relatively weak compared to the background, and other Raman peaks reported for the dihalides are not observed. These observations suggest that our materials contain the same local structures observed in InI2 and InBr2 (i.e., InX4– ions) but lack the long-range order of those crystal structures. The low crystallinity of the converted films is confirmed by selected area electron diffraction (vide infra). Annealing of the c-InI2 and c-InBr2 samples does not enhance the Raman signal, but instead shows the disappearance of the InX4– peaks above 300 °C (Figure S9). This transition is accompanied by a thinning of the films and a loss of flake morphology (Figure S10), suggesting that the halides are stable up to approximately 200 °C.
Figures 1d and 1e show the mass spectra of c-InI2 and c-InBr2, respectively, obtained using time-of-flight secondary ion mass spectrometry (ToF-SIMS). The spectra show strong halide ion (X–) signals as well as indium halide fragments (InXn–), which are identified by their m/z and isotope peak ratios. The presence of InXn species indicates covalent bonding between indium and halogen atoms in the converted material. Notably, Se– is not observed in either spectrum, corroborating the XPS results. Other indium-containing species such as InOn– or InSen– are also absent.
AFM images of the c-InI2 and c-InBr2 samples show that the flake morphology is retained after conversion to the indium halides. Figures 2a–c show AFM images of drop-casted nanosheets of InSe before and after the reaction with I2 and Br2. The c-InI2 and c-InBr2 films possess clearly defined flakes of comparable size to the original InSe nanosheets. The morphology of the converted nanosheets indicates that the original InSe flakes template the growth of the halides, demonstrating a clear example of morphotaxial conversion.7 Since neither InI2 nor InBr2 has a layered crystal structure, it is not possible to produce ultrathin flakes of these materials by mechanical or liquid-phase exfoliation of the bulk crystals. These InX2 nanosheets are therefore unprecedented non-vdW 2D materials that can only be realized through morphotaxial conversion. Notably, the AFM measurements were performed in air without loss of flake morphology, indicating that the flakes are not highly hygroscopic.
Figure 2.
(a) Atomic force microscopy (AFM) height image of electrochemically exfoliated InSe nanosheets drop-casted on Si/SiO2. (b, c) AFM images of (b) c-InI2 nanosheets and (c) c-InBr2 nanosheets produced through morphotaxial conversion of InSe. Individual flakes with distinct edges are visible in all three cases. (d) Transmission electron microscopy (TEM) image of c-InI2 nanosheets prepared on a holey SiNx membrane. Inset: Selected area electron diffraction (SAED) pattern showing diffuse rings. (e) Energy dispersive X-ray spectroscopy (EDS) spectrum of c-InI2. (f) UV–vis optical absorbance spectra of InSe, c-InI2, and c-InBr2 films prepared on CaF2 and encapsulated with 30 nm Al2O3 grown by atomic layer deposition.
To further assess the crystallinity and composition of the converted materials, we analyzed a c-InI2 film using TEM and EDS. Despite the relatively thick film, Figure 2d confirms that the film is composed of individual flakes, corroborating the AFM results. Following halogenation, the film shows diffuse rings in SAED, indicating that c-InI2 is amorphous (Figure 2d, inset). The amorphous nature of the flakes likely results from the ultrathin dimensions of the material. In particular, since InI2 is not a layered crystal, surface reconstructions are likely to disrupt the crystalline order of ultrathin flakes. Similar amorphization of non-van der Waals crystals at the 2D limit has been observed in several previous morphotaxy studies,10,11,17 and the mechanism of these reconstructions should be a topic for future studies. EDS measurements of c-InI2 indicate an I:In ratio of ∼2.3, further confirming the dihalide stoichiometry (Figure 2e). Quantification of the EDS spectrum of c-InBr2 similarly gives a Br:In ratio of ∼1.9 (Figure S11).
UV–vis optical absorbance measurements reveal a distinct shift in the optical properties of the films following halogenation. InSe shows absorption maxima at 3.8 and 4.8 eV (Figure 2f), whereas the halogenated materials are significantly blue-shifted. Specifically, c-InI2 absorbs strongly above 6 eV and has peaks at 4.1 and 5.3 eV, while c-InBr2 has a strong peak at 5.9 eV with a shoulder at 5.3 eV. InI2 and InBr2 are predicted to be indirect-gap semiconductors with bandgaps of 1.79 and 2.41 eV, respectively.50 Therefore, it is likely that the observed absorption bands correspond to higher-energy transitions, which are more favorable than absorption at the band edges due to the indirect band gap. The dimensions of the nanosheets may also be one of the contributors to the blue shift compared to bulk InI2 and InBr2, as many materials show band gap widening due to quantum confinement effects at atomically thin dimensions.
We propose the reaction scheme shown in Figure 3a, in which I2 or Br2 oxidizes selenium atoms and substitutes into the crystal lattice, forming selenium halide side products. No selenium-containing species were detected by ToF-SIMS in either the indium halide films or in drop-casted films of the reaction solutions, indicating that these side products likely decompose in solution and/or volatilize during the reaction. We hypothesize that residual PVP plays a key role in moderating the reaction. The presence of residual polymer is evident from the carbon, nitrogen, and oxygen peaks in the XPS spectra (Figure S3). PVP is known to reversibly complex with I2 and Br2, as shown in Figure 3a.51 PVP-I2 is widely used as a topical antiseptic,51,52 while PVP-Br2 has been used as a brominating agent in organic synthesis.53,54 In these applications, the PVP-X2 complex slowly releases I2 or Br2 to produce a more controlled reaction and/or longer-lasting treatment. We thus hypothesize that surface-bound PVP mediates the interaction of I2 and Br2 with the surfaces of the InSe nanosheets. To test this hypothesis, we prepared InSe dispersions and films containing no PVP and exposed them to the same reaction conditions used to produce c-InI2 and c-InBr2. AFM images show that the morphology of the original InSe flakes is completely lost during the reaction (Figure 3b–d). These results indicate that morphotaxial conversion requires a slow and controlled process enabled by the presence of PVP.
Figure 3.
(a) Proposed reaction scheme for the morphotaxial halogenation of InSe. (b–d) AFM micrographs of PVP-free InSe films (b) as prepared and treated with (c) I2 and (d) Br2. (e) Optical micrographs of mechanically exfoliated InSe flakes before and after treatment with I2. Relatively thin flakes (blue/green) are removed, while thicker flakes (orange/brown) shrink in size and change color. (f) ToF-SIMS depth profile of mechanically exfoliated InSe treated with I2. (g) ToF-SIMS depth profile of c-InI2 obtained by iodination of electrochemically exfoliated InSe (with PVP).
To further explore the reaction mechanism, we attempted morphotaxial conversion of mechanically exfoliated InSe flakes. Figures 3e and S12 show InSe flakes prepared by standard Scotch tape methods under inert atmosphere. The thickness of these flakes can be roughly identified by color due to thin-film interference effects.55 Exposure to I2 or Br2 results in the disappearance of thinner flakes and a change in the color and lateral dimensions of thicker flakes, indicating InSe etching. In light of this observation, it is surprising that the flakes in the solution-processed films (∼2 nm thick) are not completely etched, since they are significantly thinner than the mechanically exfoliated flakes (>10 nm thick). These results suggest a dual role for PVP. First, the pyrrolidone groups bind to I2 and Br2 and slow the reaction at the flake surface, enabling controlled substitution of halogens for selenium atoms. Second, the surface-bound polymer provides mechanical support to stabilize the flake structure and prevent the newly formed indium halide from dissolving in solution.
Notably, the present halogenation reactions do not allow full conversion of the mechanically exfoliated flakes. ToF-SIMS depth profiling shows the presence of halides and indium halides on the surface of mechanically exfoliated flakes, but the intensity of these peaks falls significantly below the surface of the material (Figures 3f and S12). Meanwhile, the selenium and indium selenide peaks remain consistently high at all depths, indicating that the majority of the material remains InSe. In comparison, ToF-SIMS depth profiles of c-InI2 and c-InBr2 show significantly lower selenium and indium selenide signals but strong halide and indium halide signals throughout the thickness of the films (Figures 3g and S12). The incomplete conversion of the mechanically exfoliated flakes can be explained by the thickness of the flakes. I2 and Br2 react with the surface of the multilayered flakes and are unable to penetrate into the bulk of the material. In percolating films, however, the reagents can infiltrate through interflake gaps and completely convert the ultrathin nanosheets due to their high surface area. This observation points to a distinct synthetic advantage for solution-processed 2D materials in morphotaxial conversions–namely, a percolating film of ultrathin flakes enables complete chemical conversion even for reactions that cannot penetrate bulk crystals.
To expand the scope of the morphotaxial halogenation process, In2Se3 dispersions were prepared by electrochemical exfoliation and treated with I2 and Br2 using the same conditions as InSe. The as-prepared films show characteristic Raman peaks at 96 cm–1, 168 cm–1, and 208 cm–1, consistent with reported values for In2Se3.34,56 The Raman spectra of the halogenated films match those of c-InI2 and c-InBr2, with major peaks at 138 cm–1 and 196 cm–1, respectively (Figure 4a). As in the case of InSe, the morphology of the individual flakes in the film is retained following conversion (Figures 4b–d). XPS analysis confirms that selenium is replaced with iodine or bromine throughout the full thickness of the films (Figures S13 and S14). These results indicate that solution-phase reactions with I2 and Br2 are applicable to multiple 2D indium selenides and suggest that other 2D metal chalcogenides can be halogenated with this approach.
Figure 4.
(a) Raman spectra of solution processed In2Se3 before and after reaction with I2 and Br2 (532 nm laser excitation). (b) AFM images of solution-processed In2Se3 deposited on Si/SiO2. (c, d) AFM micrographs of (c) c-InI2 and (d) InBr2 derived from the morphotaxial conversion of In2Se3 with I2 and Br2.
In this study, we have shown that liquid-phase exfoliated films of 2D InSe and In2Se3 nanosheets undergo morphotaxial conversion to ultrathin nanosheets of InI2 and InBr2 through a solution-based reaction with I2 or Br2. The reaction achieves complete replacement of Se2– with I– or Br– while maintaining a flake-like morphology. These reactions thus achieve direct bromination and iodination of 2D metal chalcogenides and suggest a versatile pathway to achieving 2D metal halides. Notably, this work identifies key mechanistic considerations for the application of morphotaxy to solution-processed 2D materials. In particular, the residual polymer PVP plays a key role in mediating the substitution reaction and stabilizing the flake morphology. Furthermore, the porous structure of solution-processed percolating films consisting of ultrathin nanosheets enables complete chemical conversion, providing a distinct advantage over mechanically exfoliated flakes where the reaction is confined to the surface.
Compared to other demonstrations of morphotaxy, our pathway is notably more scalable by using solution-based processes to both produce the starting material and achieve the chemical conversion. Dozens of 2D materials have been produced through solution-based processing, providing a variety of starting substrates to test the scope of this reaction in future studies. We anticipate that each system will require slightly different reaction conditions depending on the lattice energy of the starting 2D material and the target halide. For example, a recent study reported no chemical conversion or chalcogen removal after applying the same bromination conditions to WSe2, WS2, MoSe2, and MoTe2.57 While reaction concentration and temperature can be easily adjusted, the identity of the stabilizing polymer provides another variable for controlling the reaction. A variety of polymers can be used to stabilize 2D materials, some of which–including poly(vinyl alcohol) (PVA) and cellulose–are also know to form complexes with iodine.58 The exploration of new 2D material and polymer systems are promising avenues for future research.
Device applications of indium dihalides remain largely unexplored in the existing literature. The versatile synthesis strategy for ultrathin metal halides via morphotaxy presented in this work provides a pathway to advance detailed application studies of these materials. Specifically, we propose that indium dihalides have the potential to serve as scalable solution-processed dielectric materials, which can provide high performance even without crystalline structures. Furthermore, our morphotaxial halogenation approach could facilitate future studies on magnetic 2D metal halides such as CrI3 and NiI2 which are difficult to produce through traditional solution processing methods.
Acknowledgments
This work was primarily supported by the Materials Research Science and Engineering Center of Northwestern University (NSF DMR-2308691). Additional support was provided by the U.S. Department of Commerce, National Institute of Standards and Technology (Award 70NANB19H005) as part of the Center for Hierarchical Materials Design (CHiMaD). M.I.B.U. gratefully acknowledges support from the Northwestern University International Institute for Nanotechnology (IIN) via the IIN Postdoctoral Fellowship. A.F. acknowledges NSF grant DMR-2223922 for support. A.P acknowledges ACS grant DGE-2234667 for support. This work made use of the Keck-II, EPIC, and SPID facilities of Northwestern University’s NUANCE Center, which has received support from the SHyNE Resource (NSF ECCS-2025633), the IIN, and the Northwestern University MRSEC program (NSF DMR-2308691).
Glossary
Abbreviations
- THAB
tetraheptylammonium bromide
- PVP
polyvinylpyrrolidone
- ACN
acetonitrile
- DMF
dimethylformamide
- IPA
isopropyl alcohol
- ODCB
ortho-dichlorobenzene. AFM, atomic force microscopy
- XPS
X-ray photoelectron spectroscopy
- ToF-SIMS
time-of-flight secondary ion mass spectrometry
- TEM
transmission electron microscopy
- SAED
selected area electron diffraction
- EDS
energy dispersive X-ray spectroscopy
Supporting Information Available
The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.nanolett.4c05922.
Additional experimental details and characterization of solution-processed InSe, c-InI2 and c-InBr2 films and mechanically exfoliated InI3 and InBr3 (PDF)
Author Contributions
∇ B.P.K., J.H.L., and M.I.B.U. contributed equally. The manuscript was written through the contributions of all authors. All authors have approved the final version of the manuscript.
The authors declare no competing financial interest.
Supplementary Material
References
- Sangwan V. K.; Hersam M. C. Electronic Transport in Two-Dimensional Materials. Annu. Rev. Phys. Chem. 2018, 69 (1), 299–325. 10.1146/annurev-physchem-050317-021353. [DOI] [PubMed] [Google Scholar]
- Novoselov K. S.; Mishchenko A.; Carvalho A.; Castro Neto A. H. 2D Materials and van der Waals Heterostructures. Science 2016, 353 (6298), aac9439 10.1126/science.aac9439. [DOI] [PubMed] [Google Scholar]
- Gish J. T.; Lebedev D.; Song T. W.; Sangwan V. K.; Hersam M. C. Van der Waals Opto-spintronics. Nat. Electron. 2024, 7 (5), 336–347. 10.1038/s41928-024-01167-3. [DOI] [Google Scholar]
- Loh L.; Zhang Z.; Bosman M.; Eda G. Substitutional Doping in 2D Transition Metal Dichalcogenides. Nano Res. 2021, 14 (6), 1668–1681. 10.1007/s12274-020-3013-4. [DOI] [Google Scholar]
- Zhao Y.; Gobbi M.; Hueso L. E.; Samorì P. Molecular Approach to Engineer Two-Dimensional Devices for CMOS and beyond-CMOS Applications. Chem. Rev. 2022, 122 (1), 50–131. 10.1021/acs.chemrev.1c00497. [DOI] [PubMed] [Google Scholar]
- Jariwala D.; Marks T. J.; Hersam M. C. Mixed-Dimensional van der Waals Heterostructures. Nat. Mater. 2017, 16 (2), 170–181. 10.1038/nmat4703. [DOI] [PubMed] [Google Scholar]
- Lam D.; Lebedev D.; Hersam M. C. Morphotaxy of Layered van der Waals Materials. ACS Nano 2022, 16 (5), 7144–7167. 10.1021/acsnano.2c00243. [DOI] [PubMed] [Google Scholar]
- Lu A.-Y.; Zhu H.; Xiao J.; Chuu C.-P.; Han Y.; Chiu M.-H.; Cheng C.-C.; Yang C.-W.; Wei K.-H.; Yang Y.; Wang Y.; Sokaras D.; Nordlund D.; Yang P.; Muller D. A.; Chou M.-Y.; Zhang X.; Li L.-J. Janus Monolayers of Transition Metal Dichalcogenides. Nat. Nanotechnol. 2017, 12 (8), 744–749. 10.1038/nnano.2017.100. [DOI] [PubMed] [Google Scholar]
- Zhang J.; Jia S.; Kholmanov I.; Dong L.; Er D.; Chen W.; Guo H.; Jin Z.; Shenoy V. B.; Shi L.; Lou J. Janus Monolayer Transition-Metal Dichalcogenides. ACS Nano 2017, 11 (8), 8192–8198. 10.1021/acsnano.7b03186. [DOI] [PubMed] [Google Scholar]
- Sreepal V.; Yagmurcukardes M.; Vasu K. S.; Kelly D. J.; Taylor S. F. R.; Kravets V. G.; Kudrynskyi Z.; Kovalyuk Z. D.; Patanè A.; Grigorenko A. N.; Haigh S. J.; Hardacre C.; Eaves L.; Sahin H.; Geim A. K.; Peeters F. M.; Nair R. R. Two-Dimensional Covalent Crystals by Chemical Conversion of Thin van der Waals Materials. Nano Lett. 2019, 19 (9), 6475–6481. 10.1021/acs.nanolett.9b02700. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Wang W.; Qi J.; Zhai L.; Ma C.; Ke C.; Zhai W.; Wu Z.; Bao K.; Yao Y.; Li S.; Chen B.; Repaka D. V. M.; Zhang X.; Ye R.; Lai Z.; Luo G.; Chen Y.; He Q. Preparation of 2D Molybdenum Phosphide via Surface-Confined Atomic Substitution. Adv. Mater. 2022, 34 (35), 2203220. 10.1002/adma.202203220. [DOI] [PubMed] [Google Scholar]
- Cao J.; Li T.; Gao H.; Lin Y.; Wang X.; Wang H.; Palacios T.; Ling X. Realization of 2D Crystalline Metal Nitrides via Selective Atomic Substitution. Sci. Adv. 2020, 6 (2), eaax8784 10.1126/sciadv.aax8784. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Hajra D.; Sailus R.; Blei M.; Yumigeta K.; Shen Y.; Tongay S. Epitaxial Synthesis of Highly Oriented 2D Janus Rashba Semiconductor BiTeCl and BiTeBr Layers. ACS Nano 2020, 14 (11), 15626–15632. 10.1021/acsnano.0c06434. [DOI] [PubMed] [Google Scholar]
- Ho P.-H.; Chang Y.-R.; Chu Y.-C.; Li M.-K.; Tsai C.-A.; Wang W.-H.; Ho C.-H.; Chen C.-W.; Chiu P.-W. High-Mobility InSe Transistors: The Role of Surface Oxides. ACS Nano 2017, 11 (7), 7362–7370. 10.1021/acsnano.7b03531. [DOI] [PubMed] [Google Scholar]
- Feng W.; Zheng W.; Chen X.; Liu G.; Cao W.; Hu P. Solid-State Reaction Synthesis of a InSe/CuInSe2 Lateral p–n Heterojunction and Application in High Performance Optoelectronic Devices. Chem. Mater. 2015, 27 (3), 983–989. 10.1021/cm504268j. [DOI] [Google Scholar]
- Li T.; Cao J.; Gao H.; Wang Z.; Geiwitz M.; Burch K. S.; Ling X. Epitaxial Atomic Substitution for MoS2–MoN Heterostructure Synthesis. ACS Appl. Mater. Interfaces 2022, 14 (51), 57144–57152. 10.1021/acsami.2c16425. [DOI] [PubMed] [Google Scholar]
- Cui Q.; Sakhdari M.; Chamlagain B.; Chuang H.-J.; Liu Y.; Cheng M. M.-C.; Zhou Z.; Chen P.-Y. Ultrathin and Atomically Flat Transition-Metal Oxide: Promising Building Blocks for Metal–Insulator Electronics. ACS Appl. Mater. Interfaces 2016, 8 (50), 34552–34558. 10.1021/acsami.6b11302. [DOI] [PubMed] [Google Scholar]
- Chen H.; Chen Z.; Ge B.; Chi Z.; Chen H.; Wu H.; Cao C.; Duan X. General Strategy for Two-Dimensional Transition Metal Dichalcogenides by Ion Exchange. Chem. Mater. 2017, 29 (23), 10019–10026. 10.1021/acs.chemmater.7b03523. [DOI] [Google Scholar]
- Huang B.; Clark G.; Navarro-Moratalla E.; Klein D. R.; Cheng R.; Seyler K. L.; Zhong D.; Schmidgall E.; McGuire M. A.; Cobden D. H.; Yao W.; Xiao D.; Jarillo-Herrero P.; Xu X. Layer-Dependent Ferromagnetism in a van der Waals Crystal Down to the Monolayer Limit. Nature 2017, 546 (7657), 270–273. 10.1038/nature22391. [DOI] [PubMed] [Google Scholar]
- Huang B.; Clark G.; Klein D. R.; MacNeill D.; Navarro-Moratalla E.; Seyler K. L.; Wilson N.; McGuire M. A.; Cobden D. H.; Xiao D.; Yao W.; Jarillo-Herrero P.; Xu X. Electrical Control of 2D Magnetism in Bilayer CrI3. Nat. Nanotechnol. 2018, 13 (7), 544–548. 10.1038/s41565-018-0121-3. [DOI] [PubMed] [Google Scholar]
- Jiang S.; Li L.; Wang Z.; Mak K. F.; Shan J. Controlling Magnetism in 2D CrI3 by Electrostatic Doping. Nat. Nanotechnol. 2018, 13 (7), 549–553. 10.1038/s41565-018-0135-x. [DOI] [PubMed] [Google Scholar]
- Jiang S.; Shan J.; Mak K. F. Electric-Field Switching of Two-Dimensional van der Waals Magnets. Nat. Mater. 2018, 17 (5), 406–410. 10.1038/s41563-018-0040-6. [DOI] [PubMed] [Google Scholar]
- Song Q.; Occhialini C. A.; Ergeçen E.; Ilyas B.; Amoroso D.; Barone P.; Kapeghian J.; Watanabe K.; Taniguchi T.; Botana A. S.; Picozzi S.; Gedik N.; Comin R. Evidence for a Single-Layer van der Waals Multiferroic. Nature 2022, 602 (7898), 601–605. 10.1038/s41586-021-04337-x. [DOI] [PubMed] [Google Scholar]
- Lebedev D.; Gish J. T.; Garvey E. S.; Stanev T. K.; Choi J.; Georgopoulos L.; Song T. W.; Park H. Y.; Watanabe K.; Taniguchi T.; Stern N. P.; Sangwan V. K.; Hersam M. C. Electrical Interrogation of Thickness-Dependent Multiferroic Phase Transitions in the 2D Antiferromagnetic Semiconductor NiI2. Adv. Funct. Mater. 2023, 33 (12), 2212568. 10.1002/adfm.202212568. [DOI] [Google Scholar]
- Lebedev D.; Gish J. T.; Garvey E. S.; Song T. W.; Zhou Q.; Wang L.; Watanabe K.; Taniguchi T.; Chan M. K.; Darancet P.; Stern N. P.; Sangwan V. K.; Hersam M. C. Photocurrent Spectroscopy of Dark Magnetic Excitons in 2D Multiferroic NiI2. Adv. Sci. 2024, 11 (38), 2407862. 10.1002/advs.202407862. [DOI] [PMC free article] [PubMed] [Google Scholar]
- Telford E. J.; Dismukes A. H.; Lee K.; Cheng M.; Wieteska A.; Bartholomew A. K.; Chen Y.-S.; Xu X.; Pasupathy A. N.; Zhu X.; Dean C. R.; Roy X. Layered Antiferromagnetism Induces Large Negative Magnetoresistance in the van der Waals Semiconductor CrSBr. Adv. Mater. 2020, 32 (37), 2003240. 10.1002/adma.202003240. [DOI] [PubMed] [Google Scholar]
- Wilson N. P.; Lee K.; Cenker J.; Xie K.; Dismukes A. H.; Telford E. J.; Fonseca J.; Sivakumar S.; Dean C.; Cao T.; Roy X.; Xu X.; Zhu X. Interlayer Electronic Coupling on Demand in a 2D Magnetic Semiconductor. Nat. Mater. 2021, 20 (12), 1657–1662. 10.1038/s41563-021-01070-8. [DOI] [PubMed] [Google Scholar]
- Wu F.; Gutiérrez-Lezama I.; López-Paz S. A.; Gibertini M.; Watanabe K.; Taniguchi T.; von Rohr F. O.; Ubrig N.; Morpurgo A. F. Quasi-1D Electronic Transport in a 2D Magnetic Semiconductor. Adv. Mater. 2022, 34 (16), 2109759. 10.1002/adma.202109759. [DOI] [PubMed] [Google Scholar]
- Hu G.; Kang J.; Ng L. W. T.; Zhu X.; Howe R. C. T.; Jones C. G.; Hersam M. C.; Hasan T. Functional Inks and Printing of Two-Dimensional Materials. Chem. Soc. Rev. 2018, 47 (9), 3265–3300. 10.1039/C8CS00084K. [DOI] [PubMed] [Google Scholar]
- Dai Y.; He Q.; Huang Y.; Duan X.; Lin Z. Solution-Processable and Printable Two-Dimensional Transition Metal Dichalcogenide Inks. Chem. Rev. 2024, 124 (9), 5795–5845. 10.1021/acs.chemrev.3c00791. [DOI] [PubMed] [Google Scholar]
- Finocchio G.; Incorvia J. A. C.; Friedman J. S.; Yang Q.; Giordano A.; Grollier J.; Yang H.; Ciubotaru F.; Chumak A. V.; Naeemi A. J.; Cotofana S. D.; Tomasello R.; Panagopoulos C.; Carpentieri M.; Lin P.; Pan G.; Yang J. J.; Todri-Sanial A.; Boschetto G.; Makasheva K.; Sangwan V. K.; Trivedi A. R.; Hersam M. C.; Camsari K. Y.; McMahon P. L.; Datta S.; Koiller B.; Aguilar G. H.; Temporão G. P.; Rodrigues D. R.; Sunada S.; Everschor-Sitte K.; Tatsumura K.; Goto H.; Puliafito V.; Åkerman J.; Takesue H.; Ventra M. D.; Pershin Y. V.; Mukhopadhyay S.; Roy K.; Ting Wang I.; Kang W.; Zhu Y.; Kaushik B. K.; Hasler J.; Ganguly S.; Ghosh A. W.; Levy W.; Roychowdhury V.; Bandyopadhyay S. Roadmap for Unconventional Computing with Nanotechnology. Nano Futures 2024, 8 (1), 012001 10.1088/2399-1984/ad299a. [DOI] [Google Scholar]
- Pecunia V.; Petti L.; Andrews J.; Ollearo R.; Gelinck G. H.; Nasrollahi B.; Jailani J. M.; Li N.; Kim J. H.; Ng T. N.; Feng H.; Chen Z.; Guo Y.; Shen L.; Lhuillier E.; Kuo L.; Sangwan V. K.; Hersam M. C.; Fraboni B.; Basirico L.; Ciavatti A.; Wu H.; Niu G.; Tang J.; Yang G.; Kim D.; Dremann D.; Jurchescu O. D.; Bederak D.; Shugla A.; Costa P.; Perinka N.; Lanceros-Mendez S.; Chortos A.; Khuje S.; Yu J.; Ren S.; Mascia A.; Concas M.; Cosseddu P.; Young R. J.; Yokota T.; Somoya T.; Jeon S. J.; Zhaon N.; Li Y.; Shukla D.; Wu S.; Zhu Y.; Takei K.; Huang Y.; Spiece J.; Gehring P.; Persaud K.; Llobet E.; Krik S.; Vasquez S.; Aurora Costa Angeli M.; Lugli P.; Fabbri B.; Spagnoli E.; Rossi A.; Occhipinti L. G.; Tang C.; Yi W.; Ravenscroft D.; Kandukuri T. R.; Ul Abideen Z.; Azimi Z.; Tricoli A.; Rivadeneyra A.; Rojas S.; Gaiardo A.; Valt M.; Galstyan V.; Zappa D.; Comini E.; Noel V.; Mattana G.; Piro B.; Strand E.; Bihar E.; Whiting G. L.; Shkodra B.; Petrelli M.; Moro G.; Raucci A.; Miglione A.; Cinti S.; Casson A. J.; Wang Z.; Bird D.; Batchelor J. C.; Xing L.; Johnson L. S. J.; Alwatter A. A.; Kyndiah A.; Viola F. A.; Caironi M.; Albarghouthi F. M.; Smith B. N.; Franklin A. D.; Pal A.; Banerjee K.; Johnson Z. T.; Claussen J. C.; Moudgil A.; Leong W. L. Roadmap on Printable Electronic Materials for Next-Generation Sensors. Nano Futures 2024, 8, 032001 10.1088/2399-1984/ad36ff. [DOI] [Google Scholar]
- Lin Z.; Liu Y.; Halim U.; Ding M.; Liu Y.; Wang Y.; Jia C.; Chen P.; Duan X.; Wang C.; Song F.; Li M.; Wan C.; Huang Y.; Duan X. Solution-Processable 2D Semiconductors for High-Performance Large-Area Electronics. Nature 2018, 562 (7726), 254–258. 10.1038/s41586-018-0574-4. [DOI] [PubMed] [Google Scholar]
- Lin Z.; Wan Z.; Song F.; Huang B.; Jia C.; Qian Q.; Kang J. S.; Wu Y.; Yan X.; Peng L.; Wan C.; Zhou J.; Sofer Z.; Shakir I.; Almutairi Z.; Tolbert S.; Pan X.; Hu Y.; Huang Y.; Duan X. High-Yield Exfoliation of 2D Semiconductor Monolayers and Reassembly of Organic/Inorganic Artificial Superlattices. Chem. 2021, 7 (7), 1887–1902. 10.1016/j.chempr.2021.03.022. [DOI] [Google Scholar]
- Li P.; Hao Q.; Liu J.; Qi D.; Gan H.; Zhu J.; Liu F.; Zheng Z.; Zhang W. Flexible Photodetectors Based on All-Solution-Processed Cu Electrodes and InSe Nanoflakes with High Stabilities. Adv. Funct. Mater. 2022, 32 (10), 2108261. 10.1002/adfm.202108261. [DOI] [Google Scholar]
- Bandurin D. A.; Tyurnina A. V.; Yu G. L.; Mishchenko A.; Zólyomi V.; Morozov S. V.; Kumar R. K.; Gorbachev R. V.; Kudrynskyi Z. R.; Pezzini S.; Kovalyuk Z. D.; Zeitler U.; Novoselov K. S.; Patanè A.; Eaves L.; Grigorieva I. V.; Fal’ko V. I.; Geim A. K.; Cao Y. High Electron Mobility, Quantum Hall Effect and Anomalous Optical Response in Atomically Thin InSe. Nat. Nanotechnol. 2017, 12 (3), 223–227. 10.1038/nnano.2016.242. [DOI] [PubMed] [Google Scholar]
- Shi L.; Zhou Q.; Zhao Y.; Ouyang Y.; Ling C.; Li Q.; Wang J. Oxidation Mechanism and Protection Strategy of Ultrathin Indium Selenide: Insight from Theory. J. Phys. Chem. Lett. 2017, 8 (18), 4368–4373. 10.1021/acs.jpclett.7b02059. [DOI] [PubMed] [Google Scholar]
- Kang J.; Wells S. A.; Sangwan V. K.; Lam D.; Liu X.; Luxa J.; Sofer Z.; Hersam M. C. Solution-Based Processing of Optoelectronically Active Indium Selenide. Adv. Mater. 2018, 30 (38), 1802990. 10.1002/adma.201802990. [DOI] [PubMed] [Google Scholar]
- Muschinsky W. P.; Pawlenko N. M. Investigation of the GaSe-InSe System. Kris. Technol. 1969, 4 (2), K5–K7. [Google Scholar]
- Forrester J. D.; Zalkin A.; Templeton D. H. Crystal and Molecular Structure of Indium(III) Iodide (In2I6). Inorg. Chem. 1964, 3 (1), 63–67. 10.1021/ic50011a013. [DOI] [Google Scholar]
- Staffel T.; Meyer G. In5Br7, the Second Mixed-Valence In(I)—In(II) Bromide: In2[In2Br6]Br. With an Appendix on a Structure Refinement of InBr3. Z. Anorg. Allg. Chem. 1988, 563 (1), 27–37. 10.1002/zaac.19885630105. [DOI] [Google Scholar]
- Khan M. A.; Tuck D. G. The Crystal Structure of Indium Diiodide, Indium(I) Tetraiodoindate(III), In[InI4]. Inorg. Chim. Acta 1985, 97 (1), 73–76. 10.1016/S0020-1693(00)87992-X. [DOI] [Google Scholar]
- Staffel T.; Meyer G. The Mono-, Sesqui-, and Dibromides of Indium: InBr, In2Br3, and InBr2. Z. Anorg. Allg. Chem. 1987, 552 (9), 113–122. 10.1002/zaac.19875520913. [DOI] [Google Scholar]
- Freeland B. H.; Habeeb J. J.; Tuck D. G. Coordination Compounds of Indium. Part XXXIII. X-Ray Photoelectron Spectroscopy of Neutral and Anionic Indium Halide Species. Can. J. Chem. 1977, 55 (9), 1527–1532. 10.1139/v77-213. [DOI] [Google Scholar]
- Molas M. R.; Tyurnina A. V.; Zólyomi V.; Ott A. K.; Terry D. J.; Hamer M. J.; Yelgel C.; Babiński A.; Nasibulin A. G.; Ferrari A. C.; Fal’ko V. I.; Gorbachev R. Raman Spectroscopy of GaSe and InSe Post-transition Metal Chalcogenides Layers. Faraday Discuss. 2021, 227 (0), 163–170. 10.1039/D0FD00007H. [DOI] [PubMed] [Google Scholar]
- Ichikawa K.; Fukushi K. Raman spectra of InI, InI2 and InI3. Correlation between Structure and Thermodynamic Properties of Fused InxI1–x Mixtures. J Chem. Soc. Faraday Trans. 1980, 76 (0), 291–301. 10.1039/f19807600291. [DOI] [Google Scholar]
- Davies J. E.; Waterworth L. G.; Worrall I. J. Studies of the Constitution of Indium Bromides. Journal of Inorganic and Nuclear Chemistry 1974, 36 (4), 805–807. 10.1016/0022-1902(74)80816-X. [DOI] [Google Scholar]
- Bues W.; Akhras Z.; Okon G. Ramanspektren von Indium(III)-Halogeniden im Kristallinen Zustand und in der Schmelze. Z. Anorg. Allg. Chem. 1976, 425 (3), 193–199. 10.1002/zaac.19764250302. [DOI] [Google Scholar]
- Waterworth L.; Worrall I. J. Metal-Metal Bonds in Lower Valent Indium Compounds. Inorg. Nucl. Chem. Lett. 1972, 8 (2), 123–125. 10.1016/0020-1650(72)80096-5. [DOI] [Google Scholar]
- Munro J. M.; Latimer K.; Horton M. K.; Dwaraknath S.; Persson K. A. An Improved Symmetry-Based Approach to Reciprocal Space Path Selection in Band Structure Calculations. npj Comput. Mater. 2020, 6 (1), 112. 10.1038/s41524-020-00383-7. [DOI] [Google Scholar]
- Siggia S. The Chemistry of Polyvinylpyrrolidone-Iodine. J. Am. Pharm. Assoc. Sci. Ed. 1957, 46 (3), 201–204. 10.1002/jps.3030460317. [DOI] [PubMed] [Google Scholar]
- Jalil A.; Matuszczak B.; Nguyen Le N.-M.; Mahmood A.; Laffleur F.; Bernkop-Schnürch A. Synthesis and Characterization of Thiolated PVP–Iodine Complexes: Key to Highly Mucoadhesive Antimicrobial Gels. Mol. Pharmaceutics 2018, 15 (8), 3527–3534. 10.1021/acs.molpharmaceut.8b00503. [DOI] [PubMed] [Google Scholar]
- Lakouraj M. M.; Tajbakhsh M.; Mokhtary M. Poly(vinylpyrrolidone)-Bromine Complex; a Mild and Efficient Reagent for Selective Bromination of Alkenes and Oxidation of Alcohols. J. Chem. Res. 2005, 2005 (8), 481–483. 10.3184/030823405774663246. [DOI] [Google Scholar]
- Mokhtary M.; Lakouraj M. M. Polyvinylpolypyrrolidone–Bromine Complex: Mild and Efficient Polymeric Reagent for Bromination of Activated Aromatic Compounds. Chin. Chem. Lett. 2011, 22 (1), 13–17. 10.1016/j.cclet.2010.06.002. [DOI] [Google Scholar]
- Puebla S.; Li H.; Zhang H.; Castellanos-Gomez A. Apparent Colors of 2D Materials. Adv. Photon. Res. 2022, 3 (4), 2100221. 10.1002/adpr.202100221. [DOI] [Google Scholar]
- Balakrishnan N.; Staddon C. R.; Smith E. F.; Stec J.; Gay D.; Mudd G. W.; Makarovsky O.; Kudrynskyi Z. R.; Kovalyuk Z. D.; Eaves L.; Patanè A.; Beton P. H. Quantum Confinement and Photoresponsivity of β-In2Se3 Nanosheets Grown by Physical Vapour Transport. 2D Mater. 2016, 3 (2), 025030 10.1088/2053-1583/3/2/025030. [DOI] [Google Scholar]
- Zou T.; Kim H.-J.; Kim S.; Liu A.; Choi M.-Y.; Jung H.; Zhu H.; You I.; Reo Y.; Lee W.-J.; Kim Y.-S.; Kim C.-J.; Noh Y.-Y. High-Performance Solution-Processed 2D P-Type WSe2 Transistors and Circuits through Molecular Doping. Adv. Mater. 2023, 35 (7), 2208934. 10.1002/adma.202208934. [DOI] [PubMed] [Google Scholar]
- Moulay S. Molecular Iodine/Polymer Complexes. J. Polym. Eng. 2013, 33 (5), 389–443. 10.1515/polyeng-2012-0122. [DOI] [Google Scholar]
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