🔬 ◆ Frontier — not yet benchmarked Ch.15 Materials & Nanotechnology

Molecular Electronics

Molecular Electronics — Single-Molecule Transport · Nanoelectronics

Compute with single molecules — predict and design the quantum conductance of a molecule wired between two electrodes.

📋 The problem

If single molecules could act as wires and transistors, electronics could shrink to the molecular scale. Predicting and designing the quantum conductance of a molecule wired between two electrodes is the central challenge.

🧗 Why it's a grand challenge

Transport depends on quantum interference, level alignment and the molecule–electrode contact — all sensitive and hard to measure; DFT+NEGF is expensive and approximate.

🧮 Governing model

G = (2e²/h)·T(E_F);   T(E) = Tr[Γ_L G^r Γ_R G^a]  (NEGF)

Coherent quantum transport through a molecular junction: Landauer conductance G=(2e²/h)·T(E_F) with the transmission T(E) from non-equilibrium Green's functions (NEGF) of the molecule+leads.

Current best: DFT+NEGF transport + break-junction conductance measurements

🧭 Possible approaches

  • ML / graph surrogates of NEGF transport
  • Inverse design for target conductance / rectification
  • Models of contact geometry and corona effects

🎯 Build the benchmark

Predict single-molecule conductance from structure (≲ 0.3 dex error); inverse-design for a target conductance.

Metric: conductance_logerr — log10 conductance error (lower better)

Datasets to start from: Single-molecule break-junction corpus, DFT+NEGF transmission set

☆ Build the benchmark — earn PWM →

🤖 Build an AI agent to solve it

An agent that designs molecular junctions for a target electrical behavior and predicts conductance.

Once a benchmark exists, an AI4Science agent can iterate solutions against it — every verified solution earns PWM.

⚛ View the machine-readable principle (L1-934) → ← All grand hard problems

This is a frontier framing page — an open problem, not yet benchmarked or verified, unlike PWM's mature computational-imaging benchmarks.