He identified
the excited electron states in 15 chromophores, or light - absorbing structures, and provided theoretical chemistry insights on the mechanisms by which these molecules take in the light.
Not exact matches
When one of these
excited electrons falls back to its original
state it emits a photon, which in turn stimulates another
electron to emit a photon, and so on.
Instead of relying on light waves emitted by
electrons, it would use radiation emitted when the nucleus is
excited to a high energy
state, and then drops into a lower energy
state.
When a molecule absorbs a photon — the fundamental particle of light —
electrons in the molecular system are promoted from a low - energy (ground)
state to a higher - energy (
excited)
state.
They then exposed the evolving quantum system to a third laser beam to try and
excite the atoms into what is known as a Rydberg
state — a
state in which one of an atom's
electrons is
excited to a very high energy compared with the rest of the atom's
electrons.
OU researchers
excite the Rydberg atom using lasers in a cloud of ground -
state atoms, so the Rydberg
electron can collide with a ground -
state atom and form the molecule.
In an x-ray absorption experiment light
excites a strongly bound core
electron into a conduction band
state.
An
electron which is strongly bound to a Lithium nucleus (green) is
excited into a conduction band
state (red) that interacts with both the Lithium nucleus and Borohydride group.
They also conducted an experiment demonstrating the ability to track changes in a molecule during the transition of an
electron to an
excited state.
A weak UV pulse
excited an outer
electron to a higher
state, followed by a strong infrared pulse creating a field in which the
electron escaped from the molecule due to the tunneling effect.
The first pulse converted the
electron from a conventional, unexcited particle into a wave packet with several different
excited states.
Lasers require an electrical current or another laser to
excite a material's
electrons, which then emit photons as they return to their normal
state.
Evidence for photoinduced
electron transfer from the
excited state of a conducting polymer onto buckminsterfullerene, C60, is reported.
The
electrons travel from their initial
state to the
excited state by two paths rather than one — similar to a forked road leading to the same destination.
Laser light occurs when most of a material's
electrons are in an
excited, or higher, energy
state.
Stacking up two «atomic sandwiches» yields coupled
excited charge
states across the planar interface with the magnetic direction or «spin
state» becoming aligned for a large population of
electrons.
That's because in the
excited state, two
electrons waltz through the molecule, spinning like tops, and only when the
electron spins point in opposite directions does the dance end with the release of a photon.
Rydberg atoms are atoms, in which one single
electron is lifted into a highly
excited state and orbits the nucleus at a very large distance.
Rey says that the strontium atoms in the ground
state can be used to simulate spin - down
electrons, and the
excited atoms, spin - up
electrons.
This challenge requires accurate and efficient methods to compute ground and
excited states, as well as the ability to explicitly treat real - time dynamics of
electrons for systems consisting of hundreds of atoms: TDDFT arguably is the best compromise between accuracy and computational efficiency.
Dr. Martin Head - Gordon is an electronic structure theorist who is known for development of linear scaling methods for performing density functional theory calculations, for new methods for calculating electronic
excited states, and for advances in
electron correlation methods, including the development of widely used density functionals and many -
electron wavefunction theory.
That implies that an
excited electron in a greenhouse gas molecule in the atmosphere can not radiate toward the ground unless it can «find» another
electron on the surface in a ground
state which is capable of absorbing the photon which is to be radiated.