Related Experiment Video
Updated: Jun 11, 2026

07:36
Fabricating Nanogaps by Nanoskiving
Published on: May 13, 2013
11.1K
Shape-persistent ladder molecules exhibit nanogap-independent conductance in single-molecule junctions
Xiaolin Liu1,2, Hao Yang1,3, Hassan Harb4
1Beckman Institute for Advanced Science and Technology, University of Illinois Urbana-Champaign, Urbana, IL, USA.
Nature Chemistry
|August 26, 2024
Summary
Shape-persistent ladder molecules offer unprecedented control over single-molecule electronic devices. Their unique structure ensures consistent molecular conductance, overcoming challenges posed by dynamic nanoscale junctions.
Area of Science:
- Molecular electronics
- Nanoscale science
- Organic chemistry
Background:
- Precise control of current flow in single molecules is crucial for molecular electronic devices.
- Electron transport in single molecules is highly sensitive to dynamic conformational changes within nanoscale junctions.
Purpose of the Study:
- To develop a strategy for controlling molecular conductance that is independent of junction displacement.
- To investigate the use of shape-persistent molecules for stable electron transport.
Main Methods:
- Synthesis of chemically diverse, charged ladder molecules using a one-pot multicomponent ladderization strategy.
- Measurement of molecular conductance in nanoscale junctions using techniques sensitive to junction displacement.
- Comparison of conductance properties between ladder molecules and non-ladder analogues.
Main Results:
- Ladder molecules exhibited molecular conductance nearly independent of junction displacement (d[log(G/G0)]/dx ≈ -0.1 nm⁻¹).
- Non-ladder analogues showed significantly higher sensitivity to nanogap changes (d[log(G/G0)]/dx ≈ -7 nm⁻¹).
- Ladder molecules demonstrated a narrow distribution of conductance values during dynamic junction manipulation, attributed to their rigid backbone and restricted group rotation.
Conclusions:
- Shape-persistent ladder molecules provide a robust platform for achieving stable, gap-independent molecular conductance.
- The design principles are generalizable, as demonstrated with a butterfly-like molecule.
- This strategy opens new avenues for designing reliable molecular electronic components.
Related Concept Videos
Band Theory
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
Network Covalent Solids
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
Semiconductors
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
P-N junction
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
Metal-Semiconductor Junctions
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Debye–Huckel–Onsager Conductance Equation
The Debye-Hückel-Onsager equation is a cornerstone of physical chemistry, providing a method to determine the molar conductance (Λm) and molar conductance at infinite dilution (Λ°m) for uni-univalent electrolytes.Uni-univalent electrolytes are electrolytes that dissociate in solution to produce one cation with a +1 charge and one anion with a –1 charge per formula unit.This equation addresses two crucial phenomena: the asymmetry effect and the electrophoretic effect. According to this equation,...

