The primary aim of this proposal is to integrate a comprehensive understanding of the topological character of 2D-MOFs with deep learning techniques to stimulate discovery of new 2D-MOF structures. and open new horizons for research at the forefront of science and technology. Below we provide details of the proposed methodologies, and the corresponding work-plans:
4.1. Fundamental Understanding of Topological Character:
Identifying and designing optimized 2D-MOF structures with an experimentally realizable topological signature is a challenging and non-trivial task with huge technological implications. We propose to develop and apply high-end computational methods based on multi-scale electronic structure calculations (DFT and tight-binding) coupled with high-resolution spin-dependent STM and Fourier transform STS (FT-STS) simulations to enable a fundamental understanding of the magnetization states in 2D-MOF systems. The electronic structure calculations involving computation of orbital charge densities (LUMO and HOMO states), relaxed molecular structures, local density of states (LDOS), and projected density of states (PDOS) will establish crucial knowledge by investigating how the interaction between a particular 2D-MOF and a surface govern the atomic-scale morphology, electronic coupling, and charge transfer mechanisms. The analysis of STM images and FT-STS maps will provide an exquisitely detailed insight into the momentum or k-space properties of the material and allow the resolution of electronic scattering properties of 2D-MOF systems. The development in this work can be divided into four steps:
STEP 1 – SUBSTRATE SURFACE ENGINEERING: The choice of substrate surface (see for examples in
Figure 3) plays a crucial role in governing the overall structural, symmetry, chemical, electronic and magnetic properties of 2D-MOFs. Most theoretical studies so far are based on stand-alone MOF structures; however, the topological character of a 2D-MOF structure may alter or completely disappear after interaction with the substrate surface. In this step, we propose to fill this gap of knowledge by establishing an accurate understanding of the entire 2D-MOF/substrate system. Secondly, noble metal surfaces (such as Ag, Cu, etc.) have been the overwhelming choice in the reported studies for on-surface synthesis of 2D-MOFs [
20,
21,
22]. Recently, a few experimental studies have explored novel 2D material surfaces such as graphene [
28] as a promising weakly interacting substrate, but incisive theoretical guidance to this end is still lacking. Another highly interesting but emerging avenue is hybrid interfaces formed by coupling of MOFs with 2D topological insulators (TI) such as Bi
2Te
3 [
37] and Bi
2Se
3 [
29]. These novel systems can provide efficient ways to engineer the Dirac point and offer opportunities to tune spin dependent transport properties of the substrate for novel spintronic applications, and for designing new 2D magnetic materials. This step proposes to strive to understand and explore ways to design and engineer 2D-MOF/substrate combinations to preserve the topological character. An important innovation here is to focus on technologically relevant novel surfaces such as silicon and novel 2D TIs as a 2D-MOF support platform, which is expected to open new avenues for future technologies for example in quantum computing [
26,
27].
STEP 2 – UNDERSTANDING ELECTRONIC PROPERTIES: A comprehensive understanding of the spin-dependent band structures should be performed through DFT and tight-binding calculations, where the presence of electronic states in the bulk bandgap and spin-momentum locking would demonstrate a topological phase. A particular focus can be given to the investigation of the spin-orbit coupling (SOC) mediated gap opening mechanism. An important innovation here will be to systematically examine the role of SOC tunability on the topological character based on combinations of metal atoms and ligands, as well as the external effects such as strain and electric fields.
STEP 3 – SPIN TEXTURE OF TOPOLOGICAL EDGE STATES: In this step, high-resolution spin-polarized STM images and STS maps (such as shown in
Figure 4) will be computed, which will provide a direct access to understand the magnetization states of 2D-MOF systems. Due to correlation between momentum and spin of such states, the investigation of local spin texture will reveal topological character. The spin-polarized FT-STS may offer a unique pathway to resolve electronic scattering properties of the 2D-MOF systems as a function of spin and hence provide direct insights into the possible local spin-momentum locking mechanism. The comprehensive STM simulator developed recently [
39] which considers a detailed description of the STM tip state will allow the computation of functionalized tips going beyond the traditional bare metallic tips, providing another degree of freedom to gain insight into the electronic and spin properties of MOFs.
STEP 4 – LONG-RANGE ROBUST MAGETIC ORDERING IN 2D-MOFs: Step 4 proposes to investigate long-range magnetic ordering in 2D-MOF structures. Elucidating such magnetic properties can be important for understanding possible nontrivial topological electronic properties of these systems, since the latter can result from magnetic phenomena but also be the cause of well-defined spin structure. The presence of such spin structure in 2D materials provides an ideal platform for the realization of 2D magnets, which is presently a central focus of the research due to its huge technological relevance for novel applications including in sensing and hard-disk data storage. 2D-MOF structures can be engineered to implement 2D magnets by the selection of metal ions and the selection of structural morphologies [
43]. However, the demonstration of robust magnetism in 2D-MOFs is still an open question and requires a rigorous and systematic theoretical understanding of the origin of ferromagnetic/anti-ferromagnetic character. The computational tools developed in Steps 1-3 above can be applied to develop a fundamental understanding of the magnetic signature in 2D-MOF materials, with the aim of identifying suitable building blocks (metal ions, molecular ligands) and the structural morphologies for the realization of long-range robust ferromagnetic character.
At the completion of the above four steps, we anticipate that: (i) The established knowledge will fill a critical gap on the fundamental understanding of structural, electronic and magnetic properties of 2D-MOFs, particularly their interaction with technologically relevant substrates. (ii) New experiments will be proposed to target optimized 2D-MOF and surface combinations for realization of topological quantum states in organic materials. (iii) The comprehensive understanding of the long-range magnetic order in 2D-MOFs will uncover novel structural symmetries for realization of 2D magnets.
4.2. Machine-Learning Framework:
This is the most ambitious part of our vision, in which we propose to formulate a machine learning (ML) framework with the capability of high-throughput screening of a large number of 2D-MOFs to identify structures that host topological phases at a fraction of the computational cost compared to the traditional full-scale quantum mechanical (DFT or tight-binding) simulations. So far, computer learning techniques have scarcely been applied to the design of topological materials [
44], with no effort targeted towards 2D-MOFs. The progress is further hindered due to the limited availability of data on the electronic and spin properties of 2D-MOFs from experiments and theory. Therefore, to address the grand challenge of discovering the first experimentally viable topological 2D-MOF, a systematic development is needed.
One of the key reasons behind the immense technological interests in 2D-MOFs is the availability of a large number of building units (metal atoms and organic molecule ligands), as well as numerous possibilities for on-surface atomic-scale engineering of their morphology and symmetry by exploiting supramolecular chemistry [
17]. This offers rich opportunities to design a variety of functionalized materials, targeting a wide range of applications. Despite large number of possibilities to form MOFs, only a handful of structures are currently predicted to host topological states, with experimental demonstration still elusive. The enormous design possibilities for 2D-MOFs present a challenging combinatorial design problem that can be addressed by exploiting the efficiency of deep learning techniques, which is the goal here. A detailed flow chart diagram is illustrated in
Figure 5, which lays out our vision to deliver an all-inclusive theoretical framework with the capability of highly accurate prediction, and design, of 2D-MOFs hosting topological character. The idea underpinning the proposed tool is based on transfer learning approach in which the understanding of the correlation of structural features and fundamental material parameters with topological character is developed (4.1) and integrated this knowledge with artificial intelligence techniques such as by supervised training of a deep-learning neural network. The work in this subsection is divided in following three Steps:
STEP 1 – LEARNING AND TRAINING: In the context of topological character, a thorough and quantitative structure-property relationship (QSPR) study will be conducted by carefully establishing a correlation between the electronic and spin properties of 2D-MOFs with their composition, structure, and symmetry. The analysis and results from subsection 4.1 above will provide crucial data to the learning process. We propose to identify a list of material descriptors describing the building block units (metal atoms and molecular ligands), the role of spin-orbit coupling to create bandgap at Dirac points, and the symmetry arising from the connectivity of metal and organic molecules leading to the desired linear dispersion relation at the Dirac points in the electronic band-structure. To enable accurate and fast learning, the QSPR analysis will be conducted by employing a variety of advanced algorithms such as linear regression analysis, decision tree regression, and non-linear support vector machines [
45]. The detailed insights obtained by QSPR will train an artificial neural network (NN) for high-throughput screening and computer-aided design of topological 2D-MOFs.
STEP 2 – HIGH-THROUGHPUT SCREENING AND PREDICTION: Based on the large number of building block units (metal atoms and organic molecular ligands), we propose to establish a comprehensive database of hypothetical 2D-MOF structures. For this purpose, the publicly available databases of 2D-MOF structures can be consulted [
9,
10]. The carefully trained and benchmarked deep learning neural network from the Step 1 above will perform a high-throughput screening of the large databases of hypothetical 2D-MOF structures and identify candidate 2D-MOF materials with the predicted topological character. Subsequently, the shortlisted 2D-MOFs will be rigorously studied by performing detailed DFT and TB simulations to confirm the presence of the desired topological and magnetic properties. The successful completion of this step will identify optimized combinations of 2D organic materials and substrate surfaces and propose new measurements to be carried out by the experimental teams.
STEP 3 – INVERSE DESIGN OF 2D-MOFs: The Steps 1 and 2 aim to identify topological 2D-MOFs via high-throughput screening of the large databases of pre-defined 2D-MOF structures; however, the ambitious goal of Step 3 here is to perform bottom-up designing of new 2D-MOF structures hosting topological states by exploiting inverse-design methods [
11]. The idea is based on starting from a selection of metal atoms and molecular ligands and iteratively form different possible structures to target the desired band structure and magnetic properties. The existing literature has primarily focused on the hexagonal symmetries [
13,
14,
15,
16], but the square symmetry has recently revealed the presence of surprisingly robust magnetic character [
43]. The ML framework will explore novel and unexplored symmetries for 2D-MOFs, which could be the key to search for the next breakthrough topological material. To systematically pursue this task, advanced Monte Carlo algorithms such as simulated annealing can be implemented in conjunction with quantum simulations to design optimized 2D-MOF structures.
4.3. Exact Atom Characterisation Technique (EACT):
The subsections 4.1 and 4.2 above focus on theoretically predicting candidate 2D-MOF/surface combinations hosting topological electronic states. In experiments the adsorption of 2D-MOFs on surfaces leads to significant changes in their physical structures, which in-turn strongly impact the presence of topological character. Therefore, it is crucial to understand the post-adsorption structural details of 2D-MOFs with atomic-level resolution.
For 2D-MOF structures, non-contact AFM (nc-AFM) [
28,
29] and functionalized STM imaging [
46,
47] scans are widely used to determine their structural details. The resulting images provide good resolution in in-plane directions, but present, at best, very limited information along the out-of-plane direction. In practice, the molecular adsorption leads to atom displacements along both in-plane and out-of-plane directions (see
Figure 6). The objective of this subsection is to propose a new imaging technique prototype, hereafter labelled as exact atom characterization technique (EACT), to pinpoint the exact atomic positions
in-situ via STM. The technique will be scalable to large-scale 2D-MOF structures and will enable an unprecedented understanding of the adsorption-induced conformational distortions. The critical knowledge obtained from EACT will allow engineering of electronic and spin properties of 2D-MOFs with exquisite precision.
Recently, the dipole field originating from an NV-diamond has been proposed for atomic-scale imaging of 3D molecules [
48]. Unlike NV-diamond, silicon (Si) offers a highly clean and a very well-understood surface. Moreover, it has been demonstrated that phosphorus (P) atoms can be fabricated and characterized in Si via STM lithography with single-atom level precision [
39,
49]. Coupled with very long coherence times of P nuclear and electron spins [
50], the phosphorus-silicon (Si:P) system offers a highly promising platform for dipolar field imaging of 2D-MOFs. Indeed, a subsequent study has proposed Si:P platform for the imaging of 3-D molecules [
53]. Here we propose to exploit the dipole field from electronic wave function confined on a phosphorus donor fabricated about 2-3 nm below the Si surface as a magnetic probe and interact with the dipole fields of the on-surface nuclei in the target 2D-MOFs (
Figure 7). The dipole-dipole interaction will be controlled by an external magnetic field, which could be applied via spin-polarized STM tips [
51]. A quantum protocol will be designed to effectively read-out the exact atomic locations of the nuclei spins in the target 2D-MOFs. The recently developed protocol [
53] will provide a strong foundation for the formulation of EACT technique being proposed here. The development here can be achieved by completing the following three Steps:
STEP 1 – ELECTRONIC STRUCTURE OF Si:P:2D-MOF SYSTEM: We propose to establish a detailed understanding of the electron wave function and the resulting dipole field in a complete Si:P:2D-MOF system – a highly challenging problem which has not been done previously to the best of our knowledge. This non-trivial semiconductor/organic-material system cannot be understood through traditional DFT simulations, since the Si:P wave function has a very large spatial distribution which require simulations of over several million atoms [
54,
55,
56,
57]. Our earlier work has established an atomistic tight-binding model, which has in the past provided an excellent understanding of the Si:P electron wave functions [
39,
54,
55,
56,
57]. This tight-binding method can be coupled with DFT theory to establish a new self-consistent DFTB method capable of investigating Si:P:2D-MOF electronic structure and providing an exact shape and orientation of the dipole-dipole field above the silicon surface. This will significantly advance our knowledge of silicon/organic material interfaces, a technologically relevant material.
A second important task in this Step is to examine the extent and the gradient of dipole fields as a function of the orientations of the applied magnetic fields, which will dictate the volume and resolution of imaging of atoms inside the target 2D-MOFs. We propose to optimize these parameters through a careful analysis of the dipole fields originating from the engineered placement of P atom arrays underneath the Si surface. The strength of the dipole field can be tuned by increasing number of closely spaced P atoms, thereby enhancing the confinement of wave function.
STEP 2 – QUANTUM PROTOCOL: At the heart of the proposed EACT technique is a quantum detection protocol which will enable readout of the atom types and positions in the target 2D-MOF structure. A highly cumbersome protocol was proposed for NV-based bio-molecular imaging [
48], which can be drastically simplified by leveraging from the very long coherence times of both electron and nuclear spins on P atom in Si [
53]. This can also provide additional flexibility in terms of detection and storage of the target nuclear spin information. The protocol will utilize already published pulse sequence [
58] for decoupling of spins in the target 2D-MOF. At first the electron spin of P atom will interact with the MOF nuclei spins and acquire phase associated with the entire spin environment. This information will then be transferred to the nuclear spin of P atom, with very long coherence time. The external magnetic field will selectively rotate the target nuclear spins, which controllably interact with the Si:P electronic spin and transfer the information about their type and location. A measurement protocol will read the encoded information in Si:P and determine the target spin locations with high fidelity.
STEP 3 – ANALYSIS AND BENCHMARKING: The goal of the established EACT technique is to enable highly accurate structural analysis of 2D-MOF structures by bridging the gap between DFT based theoretical relaxations and experimental measurements. In this Step we propose to directly compare EACT results with the atomic details (atom positions, bond lengths and orientations, etc.) of theoretically relaxed 2D-MOFs. In particular, it is proposed to investigate 2D-MOF structures which have been experimentally assembled and structurally characterized via nc-AFM to further facilitate a high-level benchmarking of the existing theoretical and experimental methods.
At the conclusion of the above three Steps in subsection 4.3, we anticipate that: (i) a rigorous understanding of 2D-MOF structural properties resulting from the interaction between MOF and surface will be achieved, (ii) significant advancement of knowledge by bridging the gap between 3D DFT relaxations and 2D nc-AFM images, (iii) a prototype of a new imaging technique will be developed with clear pathway towards experimental implementations.