Molecular Geometry & Bonding
what the shape decides
Concept

Satellite — where it appears

A line in a photoelectron spectrum that no one-electron picture accounts for, produced when removing an electron leaves the ion excited. Its intensity is weight borrowed from the fundamental line for the same orbital, so a strong satellite means a weakened fundamental rather than an extra electron somewhere.

Named by 4 essays across 2 fields — each of them below, with the objects they name alongside it.

The boundary belongs to the gap, not to the repulsion. The repulsion at which a satellite stops being tellable from a fundamental by intensity, against the system's own one-electron gap. Four systems: ring of 6, gap 2.000, boundary 8; chain of 4, gap 1.236, boundary 4; chain of 6, gap 0.890, boundary 2; ring of 4, gap 0.000, boundary 0.25. The three with a gap order exactly with it, and the ring of four — whose half-filled ground state is degenerate and whose gap is zero — has no boundary at all: its contrast is one at every repulsion, so its satellites are never distinguishable and there is nothing for a boundary to separate.

The boundary belongs to the gap

A satellite stops being tellable from a fundamental somewhere, and it can be located on one ring at one filling. Four systems put it at repulsions of 2, 4 and 8 — ordering exactly with each one's own one-electron gap and not with its band width — and the fourth, whose gap is zero, has no boundary at all: its satellites are indistinguishable at every repulsion including none.

spectra · Photoelectron The contrast at three fillings, and the floor two of them reach. The intensity contrast on a ring of 6 against the on-site repulsion, at three fillings. At two electrons it settles on a number well above the factor of two the test needs. At half filling it falls through two and lands on exactly one from U = 64 upward — and every point where it reads exactly one is a point where the cut between fundamental and satellite falls between two lines of identical weight. Those are drawn hollow.

A ratio of exactly one is a tie

Does the intensity contrast fall below two at half filling? It does — it falls to exactly one. But one is the floor of a ratio between two ranked quantities, and it is reached here because the cut between fundamental and satellite lands between two lines of identical weight. The guard installed to catch that case tests the wrong degeneracy, and the guard installed to license the extrapolation cannot tell an exact answer from a divergent one.

spectra · Photoelectron The same three fillings, on a ring and on a chain. The intensity contrast against the on-site repulsion at two, four and six electrons, for both geometries. Two of the ring's three curves flatten onto exactly one and stay there — the hollow marks, where the rank cut falls between two degenerate lines. The chain's corresponding curve approaches the same value from above without reaching it, because a chain of six has no exactly degenerate removal lines at any repulsion at all.

The number the tie got right

On a ring of six the contrast at half filling comes out exactly one, and the one is an artefact — the rank cut had landed between two lines of identical weight, so the ratio was a quantity divided by itself. The chain of six has no such pair anywhere, at any repulsion, at any filling. Its contrast at half filling converges to one anyway.

spectra · Photoelectron Six removal lines, each smooth, and the contrast is whichever two sit at the cut. The weight of each of the six strongest removal lines of the half-filled chain of six, followed from U = 16 upward by continuity in energy and labelled by the energy it tends to. Every line is monotone from U = 19. The contrast is the third strongest over the fourth, so it changes whenever two lines exchange those ranks: at U = 28.92 the line tending to +0.45 overtakes the one tending to −1.80 and the two weights are equal, and at U = 157 the fourth and fifth exchange. Lines at ±E, drawn in one colour, converge to one weight.

The limit of one is a parity

A half-filled chain of six has no degenerate removal lines, and its intensity contrast still goes to one — after dipping near U = 32 and rising again to U = 128. Followed line by line, every removal line is smooth and monotone; the dip is an exact tie between two lines at U = 28.916, and the rise ends where two satellites change places. At large repulsion the lines pair up at ±E with equal weights, so the contrast goes to one exactly when the cut falls inside a pair. On a chain of four it does not, and the limit is 1.3125.

wrong · Photoelectron

Named alongside it

The objects these essays reach for when they reach for this one.

DegeneracyExact diagonalisationHubbard modelPhotoelectron spectroscopyMany-electron wavefunctionsOn-site repulsionSpectral weightIonisation energyKoopmans theoremBand widthConventionElectron correlation

All concepts