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Writer's pictureTriple Helix

How Rubber Bands Inspired a Generation of Quantum Optimizers

Image Citation: [1]


Written by Simon Nirenberg ‘28

Edited by Parsa Lajmiri ‘26


Sometimes, simple solutions can be incredibly effective. Such is the case for the Nudged Elastic Band (NEB), a method of computationally modeling chemical reactions and phase transitions.


The PES and MEP

Chemical reactions are like journeys through mountainous landscapes with peaks and valleys. Molecules move from one stable state (like a valley) to another, often over a high-energy barrier (like a mountain pass) that separates reactants from products. This landscape, called the Potential Energy Surface (PES), represents the energy of the system in all its possible configurations. The path the system traces along the landscape is called the Minimum-Energy Pathway (MEP). Mapping the MEP is crucial in drug design, materials science, catalysis, and more. However, doing so is easier said than done. Though it is called a ”Surface,” the PES is often far more than 2 dimensions; its dimensionality depends on the number of parameters that uniquely describe the system [2]. This number is often on the order of the number of atoms in the system, meaning the PES can rapidly grow to dozens of dimensions even for “simple” reactions. Beyond this, there can be many thousands of plausible paths from reactant to product to distinguish between. NEB offers a relatively low-cost computational solution to this problem.


The Elegant Simplicity of NEB

Imagine stretching a rubber band between two points on a hilly path. The band naturally curves, tracing a path that connects the start and end points while bending around obstacles in between, behavior that strikingly resembles how molecules behave on energy landscapes. This is the essence of NEB: a digital “rubber band” between points on a potential energy surface, shaped by forces that act in tandem to reveal the most efficient path from reactants to products.


In NEB, we create a series of images—snapshots of the intermediate system configuration—between the initial and final states. Each image feels two forces: a “spring force” and a force from the Potential Energy Surface (PES). The spring force holds each image in place relative to its neighbors, like tension in the rubber band, ensuring they stay evenly spaced along the path. At the same time, the PES force pushes each image along the gradient of the PES. The “nudged” part of the name refers to a way NEB restricts this PES force. NEB allows each image to feel only the PES force perpendicular to the path, preventing images from simply sliding downhill and getting stuck in energy valleys, a common issue in energy mapping. This nudging keeps images anchored to a uniform path while still following energy gradients. By iteratively running this “physics” simulation, NEB eventually converges to reveal a smooth MEP [2].


Figure 1: Left: A diagram displaying a 2-D PES and its corresponding MEP, with the transition state colored green. Right: a top-down view of this PES showing the initial interpolated path from reactant to product, along with the initial NEB and PES forces on a particular image, directing the path toward the MEP [3].


CI-NEB

In the context of the MEP, the highest-energy point, known as the saddle point, represents the “mountain pass” that molecules must cross. This point is particularly important because it provides both the transition state structure and the activation energy for the reaction, which are crucial for understanding the dynamics and thermodynamics of the reaction respectively. While regular NEB gets close to the saddle point, finding it exactly often requires additional optimization. To address this problem, quantum chemists developed Climbing-Image NEB (CI-NEB), a variant of NEB that allows the highest-energy image to “climb” upward, ignoring the spring force and letting the PES force act directly.

CI-NEB is a small but significant improvement over NEB: by letting the highest-energy image climb independently, CI-NEB pinpoints the saddle point without extra steps, providing an even better picture of the true reaction path [4]. When it comes to modeling cases like surface catalysis and crystal defect migration, where even minor differences in the activation energy lead to massive behavior changes at the macroscopic scale, this improvement can be remarkably powerful.


Limitations

Despite its elegance, NEB has limitations, especially on complex or rugged energy landscapes. The method can struggle with sharp turns or plateaus on the potential energy surface, which often cause it to bend away from the true MEP (akin to a rubber band getting caught on a corner). Convergence issues may also arise in strongly sloping regions, leading to uneven spacing of images and risking missed transition states. The accuracy of NEB can also depend heavily on the initial setup: poorly spaced starting images can slow convergence or lead to incorrect paths. Additionally, energy optimization is limited by the accuracy of the energy calculator used [2]. Despite these challenges, NEB remains a foundational tool for reaction pathfinding, acting as an excellent low-cost starting point for more advanced methods.


Conclusions

With only two basic forces—spring tension and perpendicular nudging—NEB methods provide an elegant solution to a complex problem, illustrating how physics-inspired intuition can make sense of the molecular world. This simple but powerful insight has brought these methods to the forefront of computational science, where they play an indispensable part in the design of new quantum materials, enzymes, and pharmaceuticals, pushing the boundaries of human ingenuity.


References

  1. Rubber Division, ACS. Rubber Band Contest for Young Inventors [Internet]. Akron (OH): Akron Global Polymer Academy, The University of Akron. Available from: https://www.rubber.org

  2. Jónsson H, Mills G, Jacobsen KW. Nudged elastic band method for finding minimum energy paths of transitions. In: Berne BJ, Ciccotti G, Coker DF, editors. Classical and Quantum Dynamics in Condensed Phase Simulations: World Scientific; 1998. p. 385-404.

  3. Cordier P. Nudged Elastic Band. RheoMan - Multiscale Modelling of Mantle Rheology [Internet]. Lille (FR): Unité Matériaux et Transformations, Université Lille 1. Available from: http://www.rheoman.eu/

  4. Henkelman G, Uberuaga BP, Jónsson H. A climbing image nudged elastic band method for finding saddle points and minimum energy paths. The Journal of Chemical Physics. 2000 Dec 8;113(22):9901–4.


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