Related Experiment Video
Updated: Feb 11, 2026

08:49
Engineering Three-dimensional Epithelial Tissues Embedded within Extracellular Matrix
Published on: July 10, 2016
8.0K
DMRG/FQ: A Polarizable Embedding Approach Combining Density Matrix Renormalization Group and Fluctuating Charges
Matteo Rinaldi1, Chiara Sepali1, Alicia M Kirk1
1Scuola Normale Superiore, Piazza dei Cavalieri 7, Pisa I-56126, Italy.
Journal of Chemical Theory and Computation
|February 10, 2026
Summary
This study introduces a new computational method combining Density Matrix Renormalization Group (DMRG) with a polarizable fluctuating-charge (FQ) force field to simulate electronic excited states in solution, improving accuracy for complex systems.
Area of Science:
- Computational Chemistry
- Quantum Mechanics
- Molecular Dynamics
Background:
- Simulating electronic excited states in solution is challenging due to complex solute-solvent interactions.
- Accurate modeling requires capturing both strong electronic correlation and solvent polarization effects.
Purpose of the Study:
- To develop an integrated multiscale framework for simulating electronic excited states in solution.
- To combine the strengths of Density Matrix Renormalization Group (DMRG) and polarizable fluctuating-charge (FQ) models.
Main Methods:
- Developed a multiscale framework integrating DMRG with a polarizable FQ force field.
- Employed QM/MM embedding with DMRG for electronic structure and FQ for solvent polarization.
- Utilized extensive molecular dynamics sampling for solvated systems.
Main Results:
- Achieved reliable calculations of excitation energies and solvatochromic shifts.
- Demonstrated close agreement between computational results and experimental data.
- Highlighted the crucial role of mutual solute-solvent polarization.
Conclusions:
- The DMRG/FQ approach accurately captures electronic excited states in solution.
- This method is vital for understanding solute-solvent interactions, especially those involving hydrogen bonding.
- The framework provides a robust tool for theoretical chemistry research.
Related Concept Videos
Formal Charges
40.7K
In some cases, there are seemingly more than one valid Lewis structures for molecules and polyatomic ions. The concept of formal charges can be used to help predict the most appropriate Lewis structure when more than one reasonable structure exists.
40.7K
Ions and Ionic Charges
79.3K
In ordinary chemical reactions, the nucleus — which contains the protons and neutrons of each atom and thus identifies the element — remains unchanged. Electrons, however, can be added to atoms by transfer from other atoms, lost by transfer to other atoms, or shared with other atoms. The transfer and sharing of electrons among atoms govern the chemistry of the elements. During the formation of some compounds, atoms gain or lose electrons to form electrically charged particles called...
79.3K
The Extracellular Matrix
89.4K
Overview
89.4K
Atomic Radii and Effective Nuclear Charge
62.3K
The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.
62.3K
Electric Charges
23.1K
From lightning during thunderstorms to electronic devices, the phenomenon of electromagnetism is all around us. The electromagnetic force is one of the four fundamental forces of nature. It has been known to humanity in various forms for thousands of years. For example, the ancient Greek philosopher Thales of Miletus recorded his experiments on static electricity using amber and fur in the sixth century BC.
The English physicist William Gilbert studied the phenomenon of static electricity in...
The English physicist William Gilbert studied the phenomenon of static electricity in...
23.1K
Charge on a Conductor
5.4K
An interesting property of a conductor in static equilibrium is that extra charges on the conductor end up on its outer surface, regardless of where they originate. Consider a hollow metallic conductor with a uniform surface charge density. Since the conductor itself is in electrostatic equilibrium, there should not be any electric field inside the conductor. Now, assume a Gaussian surface enclosing the hollow portion. Applying Gauss's law, the inner surface of the hollow conductor will not...
5.4K

