Logic

Two worlds that both obey the rules

A statement is independent of a list of axioms when there is a structure satisfying the axioms where it holds and another where it fails. That is not a claim about what nobody has managed to prove — it is a proof that nobody can.

Worth reading first: The tree that closes.

For two thousand years the parallel postulate was suspected of being a theorem. The suspicion was reasonable, the effort was enormous, and it was settled by drawing a picture of somewhere it is false.

A line, a point, and many parallelsA disc whose lines are arcs meeting the boundary at right angles, showing several lines through one point that never meet a given line.Pone line, one point off it, and 4 lines through the point that never meet itevery arc here meets the rim at a right angle, and every miss was checked for crossingsinside the disc
Fig. 1 A disc in which “line” means an arc meeting the rim at a right angle. Through the point PP there are several lines that never meet the line at the bottom — the arcs drawn faint are the ones that were checked and do meet it, with the crossing marked. Every arc’s right angle at the rim is asserted as c2=1+ρ2|c|^2 = 1 + ρ^2, and every claimed miss was checked for crossings inside the disc.

Euclid’s fifth postulate says, in the form Playfair gave it, that through a point not on a given line there is exactly one line parallel to it. In the picture there are many. Everything else Euclid asked for still holds.

What the question was

Euclid’s Elements opens with five postulates. Four are short and obvious-sounding: a line can be drawn between any two points, a segment can be extended, a circle can be drawn with any centre and radius, all right angles are equal.

The fifth is not like them. In Euclid’s own phrasing it runs to a paragraph and describes two lines cut by a third, converging on the side where the interior angles add to less than two right angles. It reads like a theorem that has been given up on, and Euclid himself seems to have thought so — he avoids using it for the first twenty-eight propositions.

So the programme was obvious: derive the fifth from the other four. Ptolemy tried, and Proclus, and Ibn al-Haytham, and Omar Khayyam, and Saccheri, and Lambert, and Legendre. Every one produced a proof, and every proof turned out to assume something equivalent to what it was proving — that similar triangles of different sizes exist, that three non-collinear points lie on a circle, that a rectangle exists. Saccheri, in 1733, derived a long list of consequences from its denial hoping to reach an absurdity, found none, and concluded that the results were “repugnant to the nature of a straight line”, which was the only thing left to say.

Saccheri had, without knowing it, developed a large part of hyperbolic geometry.

What settles it

The reason two thousand years of effort produced nothing is that there was nothing to find, and that is what has to be established. An absence of proofs is not an impossibility of proof.

The argument that works has a shape worth stating in general, because it is one of the two or three most useful moves in this field.

A statement SS is independent of a set of axioms AA when there is a structure in which all of AA holds and SS holds, and another in which all of AA holds and SS fails.

That settles it, and the reason is a single observation: a proof is true in every structure where its assumptions are. If SS could be derived from AA, then every structure satisfying AA would satisfy SS. Exhibit one that does not and the derivation cannot exist — not “has not been found”, cannot.

Nothing about this requires knowing anything about proofs. It does not examine derivations, or bound their length, or search. It changes the subject from what can be written down to what is true somewhere, and that is a subject where a single example is conclusive.

The disc, and what its words mean

The structure in the figure is the Poincaré disc, and the whole of it is a decision about what four words mean.

Point means a point strictly inside the unit disc. The rim is not included.

Line means an arc of a circle that meets the rim at right angles — or a diameter, which is the limiting case.

Between and congruent mean what they mean under a distance that blows up towards the rim, so that the arcs have infinite length and the rim is infinitely far away.

Under those readings, Euclid’s first four postulates all hold. Two points determine exactly one such arc; the arcs extend indefinitely because they never reach the rim; circles of any centre and radius exist; all right angles are equal, because angles in this model are the ordinary Euclidean angles between the arcs.

And the fifth fails, visibly and by a lot. Not by one exceptional line but by infinitely many, since any arc through PP that ends on the rim between the base line’s two endpoints misses it.

One line, one point, one parallel — in the planeA straight line and a point beside it, with several lines through the point and only one that never meets it.Pthe same picture in the ordinary plane: one line, one point, and exactly one parallelevery other line through the point was checked and meets the base line somewhere
Fig. 2 The same question in the ordinary plane, for comparison. Exactly one line through PP misses the base line, and every other one meets it at a point the figure computes and marks.

Putting the two side by side is the whole argument in two pictures. Same four postulates, same question, different answers — so the answer is not a consequence of the four.

Why the arcs are checked and not merely drawn

There is a specific way a figure like this can be a lie, and it is worth saying what the drawing does about it.

An arc that is nearly orthogonal to the rim looks exactly like one that is orthogonal. A pair of arcs that miss by a hair looks exactly like a pair that meet. A reader cannot tell, and neither can any check that asks whether the labels are legible or whether the ink stays inside the frame.

So the figures do the arithmetic. A circle centred at cc with radius ρρ is orthogonal to the unit circle exactly when c2=1+ρ2|c|^2 = 1 + ρ^2, and every arc drawn asserts that identity to within 10810^{-8} before it is emitted. Every arc claimed to be parallel has its intersections with the base line computed — a circle-circle intersection, solved exactly — and the figure refuses to draw unless the intersection set inside the disc is empty. The arcs that do meet are drawn differently and their crossings are marked, so the picture states which claim it is making about each one.

That is what makes this a figure rather than an illustration. It is checking the property the essay is about, on the instance it draws, every time it is drawn.

What a model is, said generally

The disc is a particular thing and the notion behind it is not, so it is worth stating the general version once.

A set of axioms is a set of sentences in some vocabulary — words like point, line, lies on. The sentences do not mean anything by themselves; they are strings with a grammar. A model supplies the meanings: a collection of things to be the points, a collection to be the lines, a relation to be lies on, and so on for every word in the vocabulary. Once that is supplied, every sentence in the vocabulary becomes true or false, and the model satisfies the axioms when all of them come out true.

Two consequences follow immediately and both are the whole of this essay.

A proof is a syntactic object and truth-in-a-model is not. A derivation is a finite arrangement of symbols obeying rules; whether a sentence holds in a model is a question about a structure. The bridge between them is soundness: what is derivable from AA holds in every model of AA. That single sentence is what turns a picture into an impossibility proof.

The vocabulary means nothing until a model says so. Hilbert’s remark that one should be able to say “tables, chairs and beer mugs” in place of “points, lines and planes” is exactly this: the axioms constrain the relations between the words and are silent about what the words are. The disc takes line to mean an arc, and nothing in Euclid’s first four postulates objects, because none of them says what a line is.

That second point is the one that took longest to be accepted, and it is the real content of the nineteenth century’s change of view. Before it, geometry was about space and the axioms were attempts to describe it, so a geometry in which the fifth postulate failed was a description of something false. After it, the axioms are a specification and anything meeting the specification is a model, so a second model is not a rival account of space but a demonstration about the specification.

One line, one point, one parallel — in the planeA straight line and a point beside it, with several lines through the point and only one that never meets it.Pthe same picture in the ordinary plane: one line, one point, and exactly one parallelevery other line through the point was checked and meets the base line somewhere
Fig. 3 Seven lines through the point in the ordinary plane. Six of them meet the base line — the meeting point of each is computed and marked where it falls inside the frame — and exactly one does not. The figure asserts that count rather than drawing it: exactly one of the seven has no crossing.

Angles, and how different this place is

A triangle whose angles come to 67.6 degreesA triangle in the disc model with sides drawn as arcs, and its three angles measured from the tangents.20.8°20.8°26.0°angles 20.8° + 20.8° + 26.0° = 67.6°, against 180° in the planethe shortfall is 112.4°, and in this model that number is the triangle's area
Fig. 4 A triangle in the disc, with its angles measured from the tangents to the three arcs. They come to less than a straight angle, and the figure computes the shortfall.

The disc is not a small perturbation of the plane. Triangles there have angles adding to less than 180°180°, always, and the shortfall is not an error term — it is the triangle’s area.

That last identity deserves its own sentence, because it has no Euclidean analogue at all. In the plane, area and angle sum are independent: a triangle can have any area and its angles always come to 180°180°. Here the angle sum determines the area completely, so there is no such thing as a large triangle with nearly Euclidean angles, and similar triangles of different sizes do not exist. Two triangles with the same angles are congruent.

A triangle whose angles come to 148.8 degreesA triangle in the disc model with sides drawn as arcs, and its three angles measured from the tangents.46.9°46.9°54.9°angles 46.9° + 46.9° + 54.9° = 148.8°, against 180° in the planethe shortfall is 31.2°, and in this model that number is the triangle's area
Fig. 5 A smaller triangle in the same disc. The angles are much closer to adding to 180°180° — the shortfall has shrunk with the area, exactly as the identity says it must.

Comparing the two triangles explains why nobody noticed for two thousand years. Small figures in this geometry look Euclidean, and the departure grows with size. If the universe, or the page being worked on, is a small patch, the fifth postulate is true to any precision that can be measured, and every consequence of it holds to the same precision. The difference is real and it is invisible locally.

A triangle whose angles come to 34.0 degreesA triangle in the disc model with sides drawn as arcs, and its three angles measured from the tangents.9.8°9.8°14.4°angles 9.8° + 9.8° + 14.4° = 34.0°, against 180° in the planethe shortfall is 146.0°, and in this model that number is the triangle's area
Fig. 6 A larger triangle again, pushed further towards the rim. The angles have shrunk further and the shortfall has grown with the area, which is the identity working rather than a coincidence of the drawing.

What “the axioms are consistent” actually means here

There is a subtlety in this argument that is worth not glossing over, because it is where the modern subject begins.

The disc shows that the fifth postulate does not follow from the other four provided the disc exists — that is, provided the ordinary plane, out of which it is built, is itself consistent. Everything in the model is made of ordinary Euclidean circles and ordinary real numbers.

So what has been proved is a relative statement: if Euclidean geometry is consistent, so is the geometry that denies the fifth postulate. Beltrami and Klein made exactly this point in the 1860s, and it is the reason the discovery of hyperbolic geometry became a proof rather than remaining a curiosity. Lobachevsky and Bolyai had developed the geometry and could not rule out that a contradiction lay a thousand theorems further on; the model rules it out, by showing that any contradiction there would produce one here.

Nothing in this method ever gives an absolute consistency proof, and by a later result nothing else does either. What it gives is a network: this system is consistent if that one is. That is less than was wanted in 1900 and it is what is available, and it has turned out to be enough for almost everything.

The move, and where else it goes

Once the pattern is visible it is everywhere.

Independence in set theory. The continuum hypothesis and the axiom of choice are both independent of the usual axioms, and both were settled the same way: Gödel built a structure in 1940 where they hold, Cohen built structures in 1963 where they fail. Cohen’s method — forcing — is enormously harder than drawing a disc, and it is doing the identical job.

Independence in arithmetic. Goodstein’s theorem is true and not provable from the usual axioms of arithmetic, and the proof of the second half is a model-theoretic argument of the same family.

Ordinary mathematics, all the time. The reason a group theorist knows commutativity is not a consequence of the group axioms is that there is a non-abelian group. Nobody calls that an independence proof, and it is one, with the same logic behind it.

A line, a point, and many parallelsA disc whose lines are arcs meeting the boundary at right angles, showing several lines through one point that never meet a given line.Pone line, one point off it, and 3 lines through the point that never meet itevery arc here meets the rim at a right angle, and every miss was checked for crossingsinside the disc
Fig. 7 The same construction with the outside point moved. The count of parallels changes with the placement and the conclusion does not — which is the point: the postulate fails at every point of this model, not at a special one.

The dates, which are the interesting part

The chronology is worth having because it separates three things that are usually run together.

1829 and 1832. Lobachevsky and Bolyai independently publish developments of the geometry in which the fifth postulate fails. Gauss had reached the same results earlier and did not publish, by his own account because he feared “the outcry of the Boeotians”. What all three had was a body of theorems — an extensive, coherent, non-contradictory-looking subject — and no way to be sure a contradiction was not waiting a thousand theorems further on.

1868. Beltrami exhibits a model. Now the geometry is not merely undisturbed so far; it is as consistent as the ordinary plane, and the two-thousand-year question is closed. Klein and Poincaré give further models over the following fifteen years, of which the disc here is the best known.

The forty-year gap between the two is the gap this essay is about. Developing the geometry was the creative work and it did not settle the question. Building the model was, mathematically, much less: a translation exercise, taking each word to an arc or a distance and checking four postulates. And it settled it completely.

That ordering — the hard creative work first, the decisive small argument afterwards, and the small argument being the one that closes the question — is common enough in this field to be worth expecting. It is the same shape as Cook’s construction for rule 110, fifteen years after the conjecture, and it recurs whenever the thing to be established is an impossibility rather than a fact.

The habit worth taking

The transferable part is not the disc. It is the change of question.

When a statement resists proof, there are two things it could mean, and they feel identical from the inside: the proof is hard, or the proof does not exist. No amount of further searching distinguishes them, because both look like failing to find a proof.

What distinguishes them is looking somewhere else entirely. Stop asking whether the statement follows and start asking whether it is true in everything the axioms describe. That question is answered by construction rather than by search, and one construction is conclusive where two thousand years of searching was not.

The lesson, stated as a habit: if a proof will not come, try to build a counterexample to the whole idea of a proof. The two are not alternatives; they are the two possible answers to one question, and only one of them can be established by working harder.

There is a last thing this episode changed, and it is larger than the geometry. Before 1868 an axiom was understood as a self-evident truth about a subject that existed independently of it, and a second geometry was therefore an absurdity — space cannot be two ways at once. Afterwards an axiom is a constraint, a system is whatever satisfies its constraints, and having several models is the ordinary condition rather than a scandal. Every axiom system in modern mathematics is read the second way: the group axioms describe groups, plural, and nobody asks which one is the real one.

That change of reading is what made the rest of this field possible. Asking whether a sentence is provable from a system, rather than whether it is true, requires the system to be an object one can stand outside of and compare things against — and the disc is the first place anybody did that convincingly.

What links here

Computed from the collection, not written here: the essays that point at this one.

Reads more easily once this is understood

Essays that name this one as worth reading first.

Named objects

A dashed tag is an object no other essay names yet.

AxiomConsistencyGeodesicIndependenceInterpretationModelParallel postulateRelative consistency