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Metals are special, because they have no energy gap at all.
This two-way interaction arises because the energy gap in either direction is similar.
Fears of a future energy gap could, of course, turn out to be unfounded.
For silver, the energy gap widens and it becomes silvery.
This has nothing to do with energy efficiency or plugging the energy gap.
The range of the energy gap is from 0.5 to 0.6 eV.
But that narrows, rather than erases, the energy gap.
It is a semiconductor with a large energy gap of around 3 eV.
A semiconductor has an energy gap within which no electron can move or exist with that energy.
The energy gap is just too large.
It displays an inverted band structure, and the optical energy gap, e, is less than 0.
Energy levels from quantum states in two different shells will be separated by a relatively large energy gap.
The junction is thin, and the electric field is large enough that electrons jump the energy gap.
The energy gap in a semiconductor under the influence of pressure or magnetic field slightly varies and thus does not deserve any consideration.
The emitted photon in some sense measures the energy gap, because it carries all the information about the energy.
This exponential behavior is one of the pieces of evidence for the existence of the energy gap.
Exceptions to Kasha's rule arise when there are large energy gaps between excited states.
There is a decent energy gap between the two states, meaning a good ΔH.
This is what leads to the different coloring of different materials - they all have different energy gaps.
As a result the energy gap is reduced, and the frequency required to achieve resonance is also reduced.
The energy gap is labeled Δ, which varies according to the number and nature of the ligands.
This wavelength of the emitted photon of light corresponds to the energy gap between these two states.
If the energy perfectly matches the energy gap between states of an atom, the photon can be absorbed quite easily.
For linear polyenes, the energy gap is given as:
It is left with one unused electron that sits in an isolated energy level in the middle of the energy gap.