ZEPTOOLS Technology | From Graphene to Heterostructures: What Exactly Has Changed with Two-Dimensional Materials?


Release time:

2026-01-08

Imagine this: The macroscopic world we’re all familiar with—those sturdy concrete skyscrapers, conductive copper wires, or resilient rubber tires—seems to have properties that were “preordained” from the start. Concrete is strong because cement tightly binds sand and gravel together; rubber is elastic because polymer chains are cross-linked with one another. Yet over the past two decades, the field of materials science has uncovered a startling secret: When we shrink materials down to their absolute smallest scale—down to just a single atomic layer thick—those familiar physical rules we’ve long taken for granted undergo a dramatic transformation.

Imagine this: The macroscopic world we’re all familiar with—the sturdy concrete skyscrapers, the conductive copper wires, or the highly elastic rubber tires—seems to have properties that were “preordained” long ago. Concrete is strong because cement tightly binds sand and gravel together; rubber is elastic because polymer chains are cross-linked with one another. Yet over the past two decades, the field of materials science has uncovered an astonishing secret: When we shrink materials down to their absolute smallest scale—down to just a single atomic layer thick—those familiar physical rules we’ve taken for granted undergo a dramatic transformation.

This is the world of “two-dimensional materials”—a “planar” universe that is only nanometers thick yet brimming with infinite possibilities.

What is “two-dimensional”? A game of scale in the microscopic world.

In our daily lives, most of the objects we come into contact with are three-dimensional. However, at the nanoscale, scientists have reclassified materials based on their size characteristics in all three dimensions. If a material’s three dimensions are all reduced to the nanoscale, it becomes a “zero-dimensional” nanoparticle; if two of its dimensions are nanoscale while the third remains macroscopic, it is classified as a “one-dimensional” nanotube or nanowire; and if only one dimension is compressed to the nanoscale, while the other two dimensions retain their extensive extension, this gives rise to “two-dimensional materials” (2D Materials).

Figure: Classification at the Nanoscale Level

It’s just like a sheet of paper: although it appears incredibly thin in our everyday world, at the atomic scale it’s still “thick.” As for true two-dimensional materials—such as graphene—their “effective thickness” is typically expressed in terms of the interlayer spacing in graphite crystals, which is about 0.34 nanometers. If you were to think of a single-layer graphene as an ultra-thin cling film, you’d need to stack hundreds of thousands of such layers to achieve the thickness of a typical sheet of paper.

Figure 3: Three Typical Nanostructures

Why does becoming “thinner” actually make it stronger?

The reason two-dimensional materials fascinate scientists isn't simply that they become "thinner"—rather, it's the extraordinary properties that emerge once they're reduced to an extreme degree of thinness. At its core, these properties stem from three main factors:

1. Freed from the “weak” van der Waals forces

Take the familiar pencil lead (graphite) as an example: it’s composed of countless layers of graphene stacked on top of one another, with the layers held together by weak van der Waals forces. When you write, a gentle stroke causes the layers to slide past one another and even break apart—this is precisely why graphite feels so soft.

 

The figure shows that graphite (left), with its weak van der Waals forces between layers, is easily broken; in contrast, graphene (right), held together solely by covalent bonds, is exceptionally strong—single-layer graphene is even strong enough to support a soccer ball.
Figure: Structure of Graphite and Physical Demonstration

However, the carbon atoms within a single-layer graphene are strongly bonded to each other via covalent bonds. Once those “loose” interlayer forces are removed, the remaining single-layer structure exhibits astonishing strength.

Experiments show that the intrinsic tensile strength of single-layer graphene is approximately 130 GPa, significantly higher than that of common structural steels. According to theoretical models, a piece of graphene the size of cling film could even withstand the weight of a soccer ball without breaking.

Figure: Schematic diagram of the tensile principle of single-layer graphene

2. Huge “exposure” area

In two-dimensional materials, nearly all atoms are exposed on the surface, giving them an exceptionally high surface-to-volume ratio. This unique property makes these materials extremely sensitive to changes in their surrounding environment. For devices with specific designs, their sensitivity can even approach that of single-molecule detection. As a result, two-dimensional materials emerge as excellent candidates for fabricating ultra-sensitive sensors.

Figure: Schematic diagram illustrating the working principle of a two-dimensional material sensor, highlighting its enormous exposed surface area, which enables ultra-sensitive detection of environmental molecules.

3. The “cage” effect of electrons

In bulk materials, electrons can move freely in three-dimensional space; however, when the material is compressed to two dimensions, electrons become confined to a single plane. Quantum confinement and interlayer coupling jointly reshape the material’s band structure, weakening its original characteristics.

A classic example is molybdenum disulfide (MoS₂): in its bulk form, it is an indirect-bandgap semiconductor with very low luminescence efficiency. However, when it is reduced to a single layer, it transforms into a direct-bandgap semiconductor and can emit bright fluorescence in the visible-light range.

Figure: Comparison of the band structures between monolayer and bulk MoS₂

The “star member” of the two-dimensional materials family

Since graphene was discovered in 2004, the family of two-dimensional materials has grown rapidly, each possessing its own unique characteristics:

1. Graphene: It is the undisputed king of electrical and thermal conductivity, boasting a Fermi velocity that’s about one-third the speed of light. It’s both transparent and remarkably tough, absorbing only around 2% of visible light. Although its lack of a band gap (giving it semi-metallic properties) currently limits its direct application in logic circuits, it nonetheless remains a cornerstone in the fields of electronics, energy materials, and composite materials.

The figure shows that both graphene (left) and hexagonal boron nitride (right) are two-dimensional materials. Although both possess a hexagonal lattice structure, their physical properties are strikingly different: graphene is an excellent electrical conductor, whereas hexagonal boron nitride is a wide-bandgap insulator.

2. Transition Metal Dichalcogenides (TMDCs): Most single-layer TMDCs, such as MoS₂ and WS₂, are direct-bandgap semiconductors, making them highly suitable for fabricating transistors, photodetectors, and light-emitting devices. They exhibit a typical MX₂ structure, in which a layer of transition-metal atoms is sandwiched between two layers of chalcogen atoms.

Figure: MoS₂ (left) and WTe₂ (right). Both are two-dimensional transition metal dichalcogenides. MoS₂ most commonly adopts the 2H phase, which is semiconducting, whereas WTe₂ tends to adopt the 1T phase, which is metallic.

3. Black phosphorus (Phosphorene): After being exfoliated into a single layer, black phosphorus is referred to as "black phosphorene." Its structure, resembling a crumpled honeycomb, gives rise to unique anisotropic properties. The band gap of black phosphorus can be tuned by varying the number of layers—from approximately 0.3 eV (in bulk) to about 1.5 eV (in the monolayer), covering a crucial spectral range from visible light to mid-infrared.

Graphene phosphide (also known as two-dimensional black phosphorus) is a two-dimensional semiconductor that is considered a highly promising material for transistors.

4. Xenes Family: Following the example of graphene, scientists have also synthesized silicene, germanene, and stanene. These materials typically require special substrates and inert environments to remain stable, yet they show great potential in cutting-edge fields such as topological electronics.

The figures show that silicene (left), germanene (middle), and stanene (right) all possess a corrugated hexagonal lattice structure.

Building the future like “building with blocks”: Manipulation and Assembly

Understanding the properties of materials is just the first step. The most fascinating aspect of two-dimensional materials is that we can stack different materials like building blocks to create “van der Waals heterostructures.”

For example, we can use graphene as the electrode, boron nitride as the insulating layer, and sandwich a layer of MoS₂ in between as the light-emitting layer. Such a structure doesn't exist in nature, but we can achieve it artificially.

Figure: Schematic diagram of the construction of a van der Waals heterostructure based on two-dimensional materials.

However, this “building-block” approach is by no means easy. Researchers are working with thin films that are only atomic-layer thick and must perform gripping, alignment, and bonding at the micrometer scale. To accomplish these tasks, they rely on sophisticated micro-manipulation platforms.

Take ZEPTOOLS Technology’s two-dimensional material transfer stage as an example: it integrates imaging, heating, adsorption, and multi-axis collaborative functions, making it an essential tool for laboratories to fabricate van der Waals heterostructures.

Its design reflects a profound understanding of microfabrication processes:

Distinctive appearance with strong visual identity: The device features a design that combines modularity with engineering principles. Its overall layout is open and logically clear, making it easy to quickly identify and get started with in the laboratory. 
Supporting the preparation of multilayer heterogeneous structures: The transfer stage supports a series of critical steps—including picking, aligning, bonding, and releasing two-dimensional materials—and can be used to fabricate multilayer van der Waals heterostructures. 
Modular design, easy to operate and visually intuitive: The system consists of modules for imaging, displacement, heating, adsorption, and others. Each module can be understood independently and can also work collaboratively to complete the process. 
Combines high-precision control capability with broad compatibility: The transfer stage features precise, stable, and repeatable displacement capabilities in motion control, making it suitable for microscale alignment requirements during the transfer of two-dimensional materials.

 

Figure: ZEPTOOLS Technology’s 2D Material Transfer Stage

It is precisely thanks to these sophisticated tools that two-dimensional materials research has evolved from the initial rough attempts of “peeling off films with tape” to an engineering era focused on building complex quantum devices.

The future is here: Application prospects of two-dimensional materials

When we can prepare and precisely manipulate these ultra-thin materials, the doors to the future will be opened.

Faster chips: Field-effect transistors (FETs) based on TMDCs or black phosphorus boast high on/off ratios and carrier mobilities. Their ultra-thin channels can effectively suppress short-channel effects, making them promising candidates for post-silicon-era chips. 
Ultra-sensitive sensor: Leveraging the enormous surface area and high sensitivity of two-dimensional materials, it is possible to construct sensors that approach single-molecule detection, suitable for environmental monitoring and medical diagnostics. 
Super Battery: Graphene’s high conductivity and large surface area make it an ideal material for battery electrodes. In certain electrochemical systems, some metallic phases of MoS₂ even exhibit specific capacitances higher than those of graphene. 
Flexible Electronics: Two-dimensional materials are ultra-thin and flexible, with layers that can slide past one another, making them prime candidates for foldable screens, flexible circuits, and wearable electronic devices.

Figure: Applications Based on Two-Dimensional Materials

From the very first roll of tape to today’s sophisticated transfer stages; from that fleeting glimpse of graphene to the vast family of two-dimensional materials, we are witnessing a revolution in materials science.

In this “flat” world, rules are rewritten and imagination is unleashed.

Although there are still many engineering challenges to scaling up the production of these atomically thin layers, we’ve already reached the threshold of a new era and are poised to embrace a future that’s thinner, stronger, and smarter.

Reference materials 
1. Ossila. “2D Materials: An Introduction to Two-Dimensional Materials.” Ossila, 2025. 
2. Nanowerk. “Nanoparticle Types, Properties, and Uses.” Nanowerk, 2025. 
3. Sabhadiya, Jignesh. “What is Graphite?—Definition, Types, and Uses.” Mech Daily, 2 Apr. 2024. 
4. Ma Jiang et al. “The Influence of Defect Location on the Tensile Deformation of Single-Layer Graphene.” Computational Physics 35.04 (2018): 475–480. 
5. Liu, De-Sheng et al. “Tailored performance of layered transition metal dichalcogenides via integration with low-dimensional nanostructures.” RSC Advances 20 (2017): 11987–11997. 
6. Suhail, Atif, and I. Lahiri. “Two-Dimensional Hexagonal Boron Nitride and Borophenes.” 2020. 0. 
7. Fei Cai. “Contact Resistance Parallel Model for Edge-Contacted 2D Material Back-Gate FET.” Electronics 65, no. 1 (2020). 
8. Miaosen Hu. “Sensitivity Enhancement of 2D Material-Based Surface Plasmon Resonance Sensor with an Al-Ni Bimetallic Structure.” Sensors 23, no. 3 (2023).