Related Experiment Video
Updated: Oct 17, 2025

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
13.0K
Quantum-state-dependent decay rates of electrostatically trapped Rydberg NO molecules
1Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK. s.hogan@ucl.ac.uk.
Physical Chemistry Chemical Physics : PCCP
|October 6, 2021
Summary
Researchers prepared nitric oxide (NO) molecules in long-lived Rydberg-Stark states and decelerated them to rest. They observed decay rates influenced by intramolecular interactions, offering insights into Rydberg state dynamics.
Area of Science:
- Physical Chemistry
- Molecular Physics
- Quantum Mechanics
Background:
- Nitric oxide (NO) molecules are crucial in various chemical and physical processes.
- Understanding the behavior of molecules in excited states is fundamental to molecular physics.
- Long-lived Rydberg states offer a unique platform for studying molecular interactions and dynamics.
Purpose of the Study:
- To prepare nitric oxide (NO) molecules in long-lived Rydberg-Stark states.
- To decelerate these excited NO molecules to rest using a transmission-line Rydberg-Stark decelerator.
- To investigate the decay dynamics of these trapped Rydberg states and identify factors influencing their lifetimes.
Main Methods:
- Resonance-enhanced two-colour two-photon excitation was used to prepare NO in Rydberg-Stark states.
- A transmission-line Rydberg-Stark decelerator operated at 30 K was employed to slow down and trap the molecules.
- In situ detection via pulsed electric field ionization and measurements of decay rates were performed for principal quantum numbers n = 32–50.
Main Results:
- NO molecules were successfully prepared in long-lived Rydberg-Stark states and decelerated to rest.
- Measured decay times ranged from 200 μs to 400 μs, generally decreasing with increasing principal quantum number (n).
- Deviations from the general trend were observed, attributed to rotational and vibrational channel interactions influencing decay rates.
Conclusions:
- Weak intramolecular interactions, specifically rotational and vibrational channel interactions, play a significant role in the slow decay of long-lived Rydberg states in NO.
- The study provides new insights into the complex dynamics governing the stability and decay of excited molecular states.
- These findings contribute to a deeper understanding of quantum phenomena in molecular systems.
Related Concept Videos
Deactivation Processes: Jablonski Diagram
1.1K
Luminescence, the emission of light by a substance that has absorbed energy, is a process that involves the interaction of molecules with light. The energy-level diagram, or Jablonski diagram, is a graphical representation of these interactions, illustrating the various states and transitions a molecule can undergo. In a typical Jablonski diagram, the lowest horizontal line represents the ground-state energy of the molecule, which is usually a singlet state. This state represents the energies...
1.1K
The Quantum-Mechanical Model of an Atom
53.3K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
53.3K
The Bohr Model
75.1K
Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as...
75.1K
The de Broglie Wavelength
30.6K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
30.6K
Atomic Nuclei: Nuclear Relaxation Processes
774
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
774
Molecular Spectroscopy: Absorption and Emission
3.7K
Molecules possess discrete energy levels called quantum states. Unlike atoms, which have simpler energy levels, molecules possess additional rotational and vibrational energy levels. Each energy level is separated by an energy gap, with the gaps between adjacent electronic, vibrational, and rotational levels varying significantly. The three types of energy levels in a diatomic molecule are shown in Figure 1.
3.7K

