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Topos à l'IHES15 / 28
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Eigenvalues and eigenvectorsMaxima and minimaChi-squared distributionMultiplication signVolume (thermodynamics)Set theoryPhysical systemPower (physics)Axiom of choiceElementary arithmeticFinitismusInverse elementSubsetOrbitInsertion lossEnergy levelFamilyArithmetic meanAxiomatic systemDirected graphBeat (acoustics)Stability theoryState of matterGoodness of fitMortality rateMorphismusCategory of beingMultiplicationProcess (computing)1 (number)Matching (graph theory)Object (grammar)Group actionPhysical lawSpecial unitary groupEquivalence relationResultantDecision theoryTheoremAlgebraic structurePhysicalismTranslation (relic)RecursionReliefTheorySlide rulePoint (geometry)MathematicsOcean currentDiagramAreaCycle (graph theory)HalbordnungFunctional (mathematics)Connected spaceExistenceNumerical analysisRight angleFinite element methodNatural numberFinite setUniformer RaumIdentical particlesElement (mathematics)Network topologyPositional notationFreezingSakokuIncidence algebraInclusion mapNuclear spaceAngleLine (geometry)Theory of relativityCausalityAssociative propertyOvalCentralizer and normalizerDivisorThermal radiationGame theoryFamily of setsBinary treePrice indexDependent and independent variablesFrequencyStatistical hypothesis testingConcentricSeries (mathematics)Closed setAtomic numberConnectivity (graph theory)InfinityGrothendieck topologyIdeal (ethics)Variable (mathematics)Water vaporDifferent (Kate Ryan album)Order (biology)Equaliser (mathematics)Basis <Mathematik>Many-sorted logicCommutatorEndomorphismenmonoidKontraktion <Mathematik>First-order logicProof theoryNegative numberBound stateBounded variationQuotientAxiomForestPower setTopostheorieInfinite setMultilaterationSheaf (mathematics)MonoidMereologyLogicAdditionDew pointCartesian coordinate systemPairwise comparisonOperator (mathematics)Boolean algebraFundamental theorem of algebraSinc functionCondition numberLecture/Conference
Transcript: English(auto-generated)
00:17
I think I will skip almost just because of lack of time.
00:25
Here is what I'm supposed to say, and as you see, it's very long, and I won't have time probably to do everything. So I prefer-
00:41
You can take it. Sorry? You can take the time. Oh, well, you will see. So the first paragraph is the behavior of very. If you say, for example, big, very big, very, very big, and you continue, there will be
01:11
what I call a saturation phenomenon, adding one more very won't change the value of what
01:20
you say. And the language is more clever than all of us together because it can even indicate this saturation point. If you want to say very, very up to, you say he's really very big, and that means he's
01:48
very, very, and no need to go, you cannot say he's very, really, very big. Really very big indicates the saturation of very.
02:02
And this I can explain to a six years old, he will understand that, but adding one more very serves to nothing. So I want to see, to model this linguistic phenomenon.
02:25
It's not linguistic because I think it belongs to all languages, in French or ... I want to model this. Of course, the immediate idea is to say, okay, let's call X the set of adjectives
02:56
to which very applies.
03:02
So X is equipped with an endomorphism, which I call T because I'm French, and T is the initial of tre. And this saturation phenomenon will be given by, for all X, there exists an N, number
03:37
N, such that T to the N plus one of X equals T of X, which means T N, sorry, T N of X.
04:00
Okay, that's very pleasant, but has nothing to do with the language. Why? Because if you write this thing, if there is an N, N being well ordered, there will be a smallest N. Nobody will agree on the smallest N. And I didn't put this in the
04:28
data, I just said ... Do you mean the set of fixed points is really very ... Sorry, could you ... The fixed points are really very ... Okay, so certainly this won't work, insets.
04:45
So we might try to see, because insets, the natural numbers are well ordered. Okay, so we might try to say, instead of sets, let's suppose that X is big X, is
05:06
an element of a Grothendieck topos, in that case, N is not well ordered, and this might work. Well even in that case, it doesn't work.
05:22
Why? Because as I said, I can explain this to a five years old boy. He knows nothing about ... Sorry, sorry, sorry, I'm speaking English, I'd rather give this talk in French, so you
05:46
will excuse me if my English is sometimes ... So as I said, I can explain this to a five or six years person, and he will understand
06:03
it, or she. But he has no idea at all about natural numbers. He doesn't know what natural numbers are. He doesn't know infinity. This can be said without any use of infinity.
06:26
Therefore, it cannot be done in Grothendieck topos, because in Grothendieck topos, there is a natural numbers object, okay? So all this is elementary language.
06:45
So what can we hope for after that? Maybe nothing, maybe this will fail anyway, but we can try to work in an elementary
07:05
topos without natural numbers object, okay? The five years old knows ... Sorry? The five years old is supposed to know about the elementary topos.
07:20
Well, that was my problem to prepare this talk, because I need ... I shall show how I use them. I need elementary topos, but nothing has been said here about elementary topos,
07:41
and maybe some people don't know what they are or how to use them. So I almost decided to cancel my talk, because I don't like to speak just for my pleasure and with very few persons understanding.
08:04
Note that I say persons. Okay, so I took this as a challenge, and when I finish, you will tell me if the challenge has been met.
08:26
So you don't know about elementary topos, and I don't ... I defined it in my talk, and you were not there. Yes, but I mean, you didn't prove anything about what I ...
08:43
No, it's true. I quoted your Mitchell-Binnabu language and saying that one could use that to ... Okay, but you didn't ... So, but ... No, okay, but people here, just on the basis of your talk, which I like very much,
09:08
could not be able to follow what I say if they don't know how to use the language. So don't panic.
09:22
The language will be the language of set theory. Sorry? The Mitchell-Binnabu language. Yes, okay. I don't like giving names to things. If in the discussion we have the possibility,
09:44
I'll tell you why Mitchell has nothing to do with that. I have proof of what I say. So it's the naive language of set theory.
10:05
The difference with the languages that Olivia presented to us is that it is not a first-order language. It's a higher-order language.
10:21
You can quantify not only on elements, but on subsets. And, for example, the most striking example is one of Peano's axioms, which I will certainly use, namely what characterizes n, many axioms, but the strongest one is that for every
10:52
subset, so I quantify on subsets of n, if 0 is in S, and if Tx or Tn, when n in S,
11:18
if S is stable by T, n in S implies Tn in S, T is usually called successor.
11:30
Then I have all of n. That's the most powerful axiom of Peano's axiom.
11:41
But you see, it requires the possibility to quantify over subsets, okay? There are, and I shall talk about them, other versions of nature numbers. Fried or lauvre, and I shall see how they fit with what I do.
12:09
Okay, now suppose x is equipped with an endomorphism.
12:32
x now is an object of the elementary topos, which you don't know about. Okay, if x is in X, let me first, if S is contained in X, I shall say that S is stable
13:11
if T of S is contained in S. And now, if x is in X, I can take the intersection of all stables of objects,
13:30
which contain x, and this I shall call the orbit of x, okay?
13:44
What is this orbit? It's x, t, x, t, t, x, et cetera, okay?
14:09
So we have the notion of et cetera. Take the orbit. And now, the axiom, which I didn't want to write with sets or with Grothendieck topos,
14:32
or et cetera, or whatnot, is for all x, the orbit of x has a fixed point.
14:46
No need to say anything about natural numbers, okay? So the axiom for vary is an endomorphism such that each orbit has a fixed point.
15:13
If you have objections, you just tell me. I'm confused. Sorry? I am confused. Is this an axiom that you're putting on x?
15:24
No, I say if I want to express the phenomenon of vary as it is in the language, I can express it by saying for all x, the orbit of x. Why do you say for all x?
15:41
You could have one x which has a fixed point. Well, I say vary has the property that very, very, very big is very, very, very, very, very rich stops. Very, very, that's the phenomenon.
16:03
Maybe a source of confusion, Jean, that you wrote capital x, the counter-power looks like... For all little x? An element of x, right? An element of x, small x. Small x, okay, okay. If I have to write everything, I will never finish.
16:26
Yes, please. So you're looking at an object having this, equipped with another model, having this property that all orbit have a fixed point. That's very, has this, I axiomatize very by saying it is an object, very, yes,
16:50
is an endomorphism of an object which has the property that every orbit has a fixed point.
17:03
This can be said in the internal language of a topo. Of course. That's why it need. This can be said in the internal language of the topos. Since I have a specialist here, he might tell me what if x doesn't have any element?
17:28
But this is, sorry? I say nothing if x has no elements and I say the orbit of every element stops.
17:41
I say nothing. Because x could be empty and this would be true for the empty. No, it could, even if it's not empty, it can have no global elements. Oh, I'm sorry, x cannot be empty because? No, no, it can be empty. For every, yeah, it can be empty.
18:02
It can be empty. I don't exclude empty. Well, the internal language permits, even if x has no global element, to write this formula. But if you don't like these things quantifying on all x where x is something, an element of
18:36
capital x which has no elements, let me say it in another manner.
18:44
Because it will tell you the power of elementary topos. I shall write, for the time being, I shall write, I shall define a relation which I
19:06
write like this, x smaller than y, if y is in the orbit of x.
19:22
And again, what does that mean when there are no elements? But I can define now something which perhaps might satisfy this is a binary relation. Okay, as a binary relation, it is characterized by, it is the smallest or the intersection
19:57
of all pre-orders on x such that x, this can be proved.
20:32
Okay, at thou, this we can take intersections, etc, etc.
20:41
I could use, and what does it have to do with this? This order relation, because I want to make a remark on the power of topos.
21:01
This is a binary relation on x. A binary relation on x can be viewed as a map from x to the power set of x.
21:26
Okay, and what is this map? It's the map x gives O of x, and now I don't care.
21:41
This is a binary relation well-defined, so now whether x has elements or doesn't have, I don't care. Okay, so I will write as an abbreviation if you want,
22:02
that y in order x O of x is an abbreviation of x smaller than y for this relation. Okay, now I think one more remark, just a side remark.
22:29
To show the power of elementary topos, it has to do with families.
22:44
There are two notions of families, families of sets if you want, or families of anything. A family of sets indexed by i is usually like this,
23:08
and this notion of family you can do for any category, say with pullbacks because you want substitution. There is another notion of family which is the one which is used by this set,
23:25
so I shall call this an implicit family.
23:42
There is another notion of family, namely a family of sets indexed by i is a map from i into sets, or better, it into some sets of sets.
24:05
That's the comprehension scheme which says, well, if I have a map from i into sets, well, the power of topos is that implicit families can always be made explicit.
24:28
Why? If you have this intuitively for each i, you note xi inverse p minus, let's call this p, xi equal p minus one of i,
24:54
and this is a subset of big X.
25:00
So this tells me, this implicit family, I can write it as an explicit family, and this is one of the most fundamental tools of topos. Implicit families can be always made into explicit ones.
25:29
Okay, so orbits and etc, I have to be quick on each thing.
25:48
Orbits and etc, orbits are exactly the notion of etc, of very simple etc. There are more sophisticated etc than this one,
26:02
but I won't have the time to talk about that. All right, so the idea is to study in the topos
26:21
an endomorphism by looking at its orbits. I want to understand properties of an endomorphism. Well, first, look at orbit-wise properties, things which are,
26:43
and then also, how shall I say, see how these orbits fit together. This could be done in sets, it hasn't been done as far as I can see. And many of the things which I will say, not be done systematically,
27:07
many of the things which I will say, I think are new, even in the category of sets. Okay, so I shall call an orbit an object X together with an element X0,
27:49
and an endomorphism T, such that the whole of X is the orbit of X0.
28:07
That's what I call an orbit. So you want to have that O of X0 is X, that's what you want? That the orbit of X0 is X? The orbit of X0 is X.
28:24
I call this an orbit. An abstract orbit. Note that X0 need not be unique or anything. No, it's a generator of the orbit. Well, it's a generator, but maybe there are many now.
28:45
Okay, so you're no longer requiring that every orbit is finite. What properties have such orbits? Are you supposing that the orbit has a fixed point as before?
29:00
No, no, no, I'm talking about orbits in general. I said I want to study an endomorphism by looking, an arbitrary endomorphism, by looking at its orbits and then seeing how the orbits fit together. So the first step is what property can an orbit have?
29:25
First of all, an orbit can be seen as a weak natural numbers object. I shall explain in what sense. Weak.
29:50
As I said before, there are many notions equivalent of NNO. There are the L'Hauvre definition, there are the Fried definition,
30:06
which some people may not know, but I will recall it, and there is the Peyamu definition. Let's see, let's compare with L'Hauvre's definition.
30:20
If this is an orbit, and if I have any object Y equipped with Y zero, and translations I will always call T, okay, if this is an orbit,
30:44
there is at most one F making this diagram commutative. So in L'Hauvre there is one and one F, I said it's weak NNO,
31:04
replaced there exists one and one S, is there exists at most one. So this shows how it is a weak NNO in the sense of L'Hauvre.
31:25
In the sense of Peyamu, it is said that natural numbers satisfy
31:42
the most important axiom of Peyamu, the fifth of recursion, and you add zero is not a successor, let's call S the image of T, S for successor.
32:03
Zero is not a successor, and the map T is monic, and the big recursion axiom.
32:23
Well, an orbit, and also that everything is either zero or a successor. In an orbit, what do we have from Peyamu's axiom? We have the big axiom, recursion axiom, but we also have that X zero union
32:56
S by S, I said, is all of X.
33:02
Another way of saying is that in an orbit, all the elements are either X zero or successors, there are no other elements. So it's again a weak- By S you mean the image of the operator T? Sorry?
33:20
You mean the image of the operator T? Yes, S I called the image of T, S meaning the successor elements. So again, we see that we have weakened a little bit, well, a big bit, but nevertheless,
33:47
we have weakened the definition of natural numbers of Peyamu. Yes? Because this reminds me of the very first construction- Can you speak louder? Sorry, sorry, yes. This reminds me of the construction of Debeke in the beginning with an infinite set and you get a natural-
34:05
No, no, I mentioned Fried, I mentioned Peyamu, and I mentioned Lovier. I'm not talking about Moore, otherwise I will be here tomorrow. What I mean is if you have zero is not in S, you have a monoid such as zero is not in S-
34:24
In an orbit, zero can be in S. In an orbit, zero can be in S, okay? Well, since you are mentioning this, I anticipate on something which I was
34:44
going to say anyway, namely this. Suppose I don't even have to talk about orbits.
35:02
Suppose I have an endomorphism. I shall say that an element x is cyclic if T of x is in the orbit of x.
35:34
What does that mean? Start with x, write T x, T T x, T T T T T x, sometimes you come back to x.
35:42
x is in the orbit. x is cyclic if, sorry, x is in the orbit of T x.
36:06
That means, I want to understand with that, that means start with x, write T x, T T x, T T x, and you find x. That's correct for cyclic, okay?
36:25
And let's add one more thing. I shall say that T is acyclic if, not if it doesn't have any cycle.
36:51
No, this negation doesn't work at all. A is acyclic if and only if, that's my definition,
37:01
every cycle, cyclic element is fixed, is a fixed point.
37:23
I start with x and then it's just at the very first step, I finish. This is acyclic. What about what?
37:40
That if it has a fixed point. Well, then it's x is not, if it has a fixed point, every fixed point is cyclic. But acyclic means that the only cyclic elements are the fixed points.
38:06
That's my definition. Okay, let's call, let's call C of x the object of cyclic elements.
38:20
Let's call fix x the object of fixed elements. This one is very easy to describe, no need of higher order. It's just fix x is the equalizer of the identity and T.
38:42
But cyclic elements, you cannot define in a category unless it is a topos or topos-like. We have always this inclusion and to say that T is acyclic is this equality.
39:13
Okay, let me just, I know everything but I might forget a few elementary things.
39:53
Now, first theorem is that an orbit is acyclic if and only if the pre-order relation
40:10
on the orbit is an order relation. Okay, have to be proved, it's not difficult, I'll come to a difficult question a little bit later.
40:27
For example, the natural numbers if they exist are acyclic.
40:40
Okay, because the order relation induced by successor is an order relation. Well, again we shall see, I said orbits are weak natural numbers.
41:04
Let me give another example. If is an orbit, then it is a monoid with one generator and such monoids are commutative.
41:39
So, when you prove that the natural numbers is a commutative monoid for addition etc.
41:47
and has a generator, that's true for any orbit. So, many things one proves for natural numbers are true for orbits or other,
42:04
for example, for acyclic orbits, then you have a total order.
42:26
I rush, the fourth thing is killing the cycles.
42:42
It's passing to the associated field, the associated order. How do you do that? If you have a pre-order relation, you can take the associated order. So, let's write x equivalent to y if x smaller than y and y smaller than x.
43:27
And let's write x doubly equivalent to y if x and y belong to the same cycle.
43:49
These things are almost the same. When is x equivalent to y if and only if x equal y or x and y are acyclic.
44:19
This relation is symmetric transitive, not necessarily reflexive because
44:33
x and x need not be cocyclic and yet they are equal.
44:44
Okay, so we can take the quotient of x by this equivalence relation.
45:12
This quotient is now t respects this equivalence relation.
45:26
So, factors as an endomorphism of this. However, this is an order relation.
45:45
The pre-order becomes an order relation on x. And the orbits now, each orbit of x gives an orbit here,
46:00
but now the orbits are ordered. Therefore, this is acyclic. So, what we have done is just by identifying two points which are in the same cycle,
46:24
we have replaced the whole cycle by a fixed point. And this says what? Let's call by, to have notation, t of e,
46:48
the category of objects equipped with an endomorphism. Let's call a of e, the subcategory of this formed only with acyclic thing.
47:11
What I have just proved is contract an adjoint by just killing the cycle.
47:23
Killing means reducing them to a single element. And in particular, if every orbit of t of x has a cycle,
47:42
then for the associated acyclic object, every orbit will have a fixed point and we will be in the situation of varying.
48:04
Now, there are many more things to say, but I have to take only a tiny bit of each paragraph if I want to respect the time. So, what comes next?
48:26
There is a difficult theorem which says the following. This one is really, the other ones are little exercises, each one takes maybe 10 lines at most provided you give them in the correct order.
48:51
But here is a difficult theorem.
49:06
An orbit is finite if and only if it has a cyclic element.
49:43
That's a fact. I'm sorry, I don't want to annoy you, but just for the purpose of the talk, can you tell how you define finite?
50:03
Finite is Kuratowski finite. There is a notion of finite, but again, if you don't know elementary toposus, think of finite as finite. I want to speak things that people can understand.
50:29
Sorry? I'm not saying anything about axiom of choice.
50:42
In an elementary topos, one defines Kuratowski finite elements, which in the case of sets are just the finite elements. In the case of Grotnik toposus, they are a bit more complicated.
51:02
But think of them as finite. That's all I can do. It would be good for the purpose of your talk, that if someone writes down the notions of Kuratowski finite on the blackboard.
51:21
Maybe you don't want to do it, but Olivia is ready. I don't care. Provided she doesn't take on my time of talk.
51:41
Well, it is in a sense, first it is difficult, but it has some philosophical connotations.
52:07
That means that this abstract definition of finiteness, or even in set, the definition of finiteness has something to do with orbits, with et cetera.
52:24
Finite has something to do with et cetera. Orbits are axiomatization of et cetera.
52:47
So I just don't take your time off. You are. So the idea is this, is that one can describe using our logic the collections of finite subset of a power set.
53:04
Because what you have are the singleton. The singleton is a singleton map. This is given. And finite subset are generated by finite union of singletons. So you take the smallest joint subnatus.
53:20
I mean, sub-object of P is closed under union, and which contain the singleton. And if you do that, you get all the kuratowski finite subset of X. The kuratowski finite subset of X is something which is contained in the smallest.
53:42
And X would be kuratowski finite if X itself is contained in the smallest. OK. Well, let me say I don't like your definition. I shall give an equivalent definition.
54:02
No, no, why? It's not your definition. By the way, it's not your definition. It's the definition where you find. OK, so I shall give another definition, which will perhaps make it more intuitive
54:24
why there is something between orbits and finiteness. Instead of saying that this is a joint sublattice,
54:47
that means we can suffice to say that it's stable by the following operation. If S is in power set of X and X in X,
55:10
then it's stable by not taking the union of two things,
55:25
taking the union of one thing and a singleton. You obtain all of X by iterating the process of taking the union of X and the singleton.
55:43
What does it have to do with et cetera? Well, I didn't want to talk about this, but the et cetera I mentioned is a very simple one. There are more complicated et cetera.
56:02
For example, suppose we have X equipped with a family of endomorphisms, not just one.
56:21
The et cetera will consist in taking something, taking something, the orbits are obtained by taking something and Ti, any i of that something,
56:48
not just this is a kind of multiple et cetera. Well, the power set of X has this structure.
57:07
Namely, if X equals the power set of i,
57:21
it has this structure by taking Ti of a subset with i in i equal the subset union i.
58:02
So what's a finite object? Or more generally, we look at the orbits in the sense which I will not define of this Ti. The orbits are all the finites of objects of i.
58:24
Saying that i is finite is that... Okay. Okay. We have one definition so that you can explain your theorem now. No, the theorem is this.
58:41
An orbit is finite if and only if it has a cyclic element and that's a difficult theorem. How can you see this? Because I want you to see, to have a vague idea of what's going on, but it's not trivial.
59:02
Suppose you have a computer and a repetitive process start with one thing, take Ti of that thing and then Ti Ti, et cetera, et cetera. And suppose you give the...
59:25
I know nothing about computer science, by the way. So don't... And suppose you give him the only instruction, start with some X,
59:41
do repeat the computation and stop when you find something you have already... a result you have already met. And it stops. Which means Tx, et cetera, has a cycle.
01:00:02
Well, it will stop certainly in a finite number, in a finite time. Conversely, if it stopped in a finite time, that means that it has met a cyclic element. That is very vague, but that's how it is, except that in that case it's finite in
01:00:25
the usual sense of set theory, whereas k-finite has been defined by you now or by other persons, but the point is that this finiteness, for example, doesn't have some properties one
01:00:52
might expect of finite. For example, a sub-object of a finite object need not be finite. We all believe that the subset of the finite set is finite.
01:01:06
Of course, because we live, in set theory, in a Boolean topos, I'm not supposing it's Boolean. Here is another very strange, and to me it was surprising, result.
01:01:33
Here it is.
01:01:49
Suppose x is smaller than y. We can, that is y is in the orbit of x, we can define the closed interval x, y as
01:02:12
being all the z, which were between x and y.
01:02:22
Now the following are equivalent, for all these intervals are finite, is equivalent to all the xx are finite.
01:02:53
This can be proved. But this equivalence, this equivalence is not true in general.
01:03:02
It is true if and only if the topos is Boolean. Now here we get an if and only if the structure, the whole structure of the topos is determined by this.
01:03:22
And of course, if t is acyclic, these two equivalent conditions are satisfied. But if they are not acyclic, the topos has to be Boolean. Let's say also something, acyclic means maybe there is no fixed point.
01:03:49
If there is a fixed point, okay, it's acyclic, but maybe there isn't. For example, for the natural numbers, there is no fixed point. However, every interval of the natural numbers, closed interval, is finite.
01:04:08
We know that for the natural numbers, but we know it now for every acyclic orbit. Not only the thing which goes all the way, the orbit which goes all the way to the fixed
01:04:24
point, if there is a fixed point, is finite, but all the intervals are finite. But the surprising thing is that Booleanness is needed, unless you assume the orbits, the
01:04:43
thing is acyclic, Booleanness is needed in general for this equivalence. So, again, some properties of et cetera imply properties of the whole topos.
01:05:04
Now, seven is connected components. In this case, I shall give an idea of the proof, because I like it and because
01:05:24
it doesn't take a long time. We have this order relation. So it's a category.
01:05:42
So we can talk about the connected components. When are two objects, two elements, x and y, I shall put another equivalence thing,
01:06:05
in the same connected components? The answer is very simple. Namely, they are in the same connected component if the orbit of x and the orbit of y has
01:06:29
a common element.
01:06:42
I shall give a proof. It's not so obvious, unless I miss something. Well, this relation is obviously reflexive and symmetric, remains to show that it is transitive.
01:07:11
Usually, to get the connected component, you have to make zigzags like this. But here that says just one zigzag is enough.
01:07:25
Why? Suppose x, y, there is an element u in the orbit of x, and there is an element v here
01:07:50
in the orbit of z intersect the orbit. But these, u and v, are both in the orbit of y.
01:08:06
And we have seen that in an orbit, the pre-order is a total pre-order. So we have either u in the orbit of v, or v in the orbit of u.
01:08:21
But that's trivial to check that it is transitive. Okay, so pi zero is, here is one more thing, one more application of the orbits.
01:08:45
Suppose we have x equipped with an endomorphism. I want to talk about t, t composed with t, t composed with, etc.
01:09:06
Well, you look at x, the x, and it is equipped with an endomorphism that's called t blank.
01:09:23
For each f, take t, well, composed with f, so it can take the orbit of the identity. And the orbit of the identity is exactly what we want. So we have not only a level of elements, but of functions.
01:09:47
For example, suppose you want to, suppose you say, okay, with nature numbers, I can write for all x there exists an n, such that tn plus one of x equals tn of x.
01:10:20
But suppose I want to say something more, namely, not for all x there exists an n, but there exists an n for all x, which is good enough for all x. So you see, I'm writing formulas as if there were nature numbers, but there isn't.
01:10:47
How do you say this? That means the orbit of t has a fixed point. And this will give you a uniformity of t in x to the power x.
01:11:05
For all x? Such that for all x, this holds. I want to be able to say that this fixed point, there is a uniformity, a uniform bound.
01:11:25
So you see that this notion of etc. covers many, many, many things, even when there is no nature numbers object, and you want to do as if there was one.
01:11:45
So this orbit, the orbit of the identity along t, I shall call it the leading orbit. And what property does it have? This, for every x, the leading orbit maps subjectively on the orbit of x.
01:12:09
Take the evaluation. If you have f in the orbit of t, in the leading orbit,
01:12:37
then for each x, evaluate f at x,
01:12:43
and this is a mapping of this into of little x. And we know that such mappings are unique, and we know they are subjective.
01:13:04
So every orbit of any element is a quotient of this leading orbit. For example, if this leading orbit has a fixed point, then all orbits have a fixed point.
01:13:26
Now, I will finish with just one more remark. Important one.
01:13:41
I have said that very has the property that each orbit has a fixed point. Okay? I claim that this is a very important notion, mathematical notion.
01:14:03
What does it mean? That t is such for all x has a fixed point.
01:14:40
I call such an x and t rooted forest.
01:15:02
Why? Each connected component is a rooted tree, which means all the orbits are finite, have a fixed point, et cetera, et cetera. That's the correct definition of a tree.
01:15:22
So it's important. This says that very is a rooted forest. I think I have...
01:15:52
Do we have any questions? So during the lecture, it was mentioned about...
01:16:02
If you will please speak louder, I don't... I'm hard of hearing. Okay. So you mentioned the definitions of natural number objects in a topos. You mentioned the names of rain, lauvir, and piano. Is it possible to give the three definitions precisely?
01:16:25
So I want to know the three definitions of... An elementary topos? Well, I suppose it is an elementary topos. I'm not sure, I'm not sure. The section of the piano in the topos. No, no.
01:16:40
The section of the piano in the topos is the section of the piano that everyone knows. Okay. This is the section of the natural number.
01:17:02
Lauvir is a small part of the endomorphism S
01:17:21
and an element zero. What is universal for this to be there?
01:17:45
And for the orbit that I mentioned, it is not existence, but unicity. If it exists, it is unicity. Or otherwise, existence is unicity. The section of the piano is not.
01:18:06
Zero is not a successor. The successor is a mono. And you, zero, are a successor. This is the three elements.
01:18:21
We know that I regard the successor and the element zero.
01:18:41
That is a sub. Zero is not a successor, because it is a one. And that means that you are a successor. And that means that the successor is a mono, because in a sub it is a mono. That means everything. And what happens next?
01:19:01
There is the fact that, as I said before, that the ground is connected. So what is this? We are saying that we are not connected.
01:19:20
What we are saying is that the co-egalizator is exactly the same as the ground is connected.
01:19:40
Everything is connected. Very good. Because every element can be connected with the point of the orbit. Then what happens next? This is Friday.
01:20:02
I leave the room. For now, I have already spoken to a number of people. It is not the first time. There is a paragraph that I did not mention, but it is very good in the discussion.
01:20:20
Now, a plea for the language. A plea for the language. And it is very good. It is already a plea for the language.