Realizations of Hopf algebras of graphs by alphabets
Lo\"ic Foissy (LMPA)

TL;DR
This paper constructs polynomial realizations of Hopf algebras related to graphs and posets using totally quasi-ordered alphabets, providing explicit algebraic embeddings and coproduct structures.
Contribution
It introduces new polynomial realizations of Hopf algebras on graphs and posets via totally quasi-ordered alphabets, with explicit coproduct definitions.
Findings
Polynomial embeddings of graph-related Hopf algebras into polynomial algebras.
Explicit coproduct structures via alphabet doubling and squaring.
Identification of cointeracting bialgebras in the commutative case.
Abstract
We here give polynomial realizations of various Hopf algebras or bialgebras on Feynman graphs, graphs, posets or quasi-posets, that it to say injections of these objects into polynomial algebras generated by an alphabet. The alphabet here considered are totally quasi-ordered. The coproducts are given by doubling the alphabets; a second coproduct is defined by squaring the alphabets, and we obtain cointeracting bialgebras in the commutative case.
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Taxonomy
TopicsAlgebraic structures and combinatorial models · Advanced Topics in Algebra · Advanced Combinatorial Mathematics
Realizations of Hopf algebras of graphs by alphabets
Loïc Foissy
*Fédération de Recherche Mathématique du Nord Pas de Calais FR 2956
Laboratoire de Mathématiques Pures et Appliquées Joseph Liouville
Université du Littoral Côte d’Opale-Centre Universitaire de la Mi-Voix
50, rue Ferdinand Buisson, CS 80699, 62228 Calais Cedex, France
Email: [email protected]*
Abstract
We here give polynomial realizations of various Hopf algebras or bialgebras on Feynman graphs, graphs, posets or quasi-posets, that it to say injections of these objects into polynomial algebras generated by an alphabet. The alphabet here considered are totally quasi-ordered. The coproducts are given by doubling the alphabets; a second coproduct is defined by squaring the alphabets, and we obtain cointeracting bialgebras in the commutative case.
Keywords. Combinatorial Hopf algebras; Feynman graphs; posets
AMS classification. 16T05, 05C25, 06A11
Contents
Introduction
Some combinatorial Hopf algebras admit a polynomial realization, which gives an efficient way to prove the existence of the coproduct and more structures, see [8, 19, 15, 7, 17]. Let us explicit a well-known example. The algebra of quasi-symmetric functions has a basis indexed by compositions, that is to say finite sequences of positive integers.
For any totally ordered alphabet , let us consider the following elements of the ring of formal series generated by :
[TABLE]
This defines a map from to , injective if, and only if, is infinite. This map is an algebra morphism. For example, if , for any totally ordered alphabet :
[TABLE]
and, in :
[TABLE] 2. 2.
If and are totally ordered alphabets, then is too, the elements of being smaller than the elements of . Identifying with a subalgebra of , we define a coproduct on by:
[TABLE]
For example:
[TABLE]
and, in :
[TABLE]
The coassociativity of is easily obtained from the equality . 3. 3.
If and are totally ordered alphabets, then is too, with the lexicographic order. We consider as a subalgebra of , identifying with . We can define a second coproduct on by:
[TABLE]
For example:
[TABLE]
and, in :
[TABLE]
The coassociativity of is easily obtained from the equality . Moreover:
[TABLE]
This implies that in :
[TABLE]
where sends to . This means that the Hopf algebra is a Hopf algebra in the category of right comodules over the bialgebra , the coaction being itself: we call this a pair of bialgebras in cointeraction.
For other examples of such objects and applications, see [16, 18, 10, 9, 11].
We here give other examples of cointeracting bialgebras coming from the manipulation of alphabets and polynomial realizations. We use here totally quasi-ordered alphabets, that is to say sets with a total transitive reflexive (but not necessarily antisymmetric) relation. The associated algebras are slightly more complicated, see Definition 6. Their different sets of generators allows to polynomially realize Feynman graphs (one set for vertices, one set for internal edges, one set for incoming half-edges and a last one for outgoing half-edges); this gives a family of products on the space generated by isoclasses of Feynman graphs, indexed by a scalar (Theorem 17). If and are two Feynman graphs, is a sum of graphs obtained by gluing together vertices of and ; in particular, if , this is reduced to the disjoint union of and . The trick of doubling the alphabet gives a coproduct , given by ideals (Theorem 19), and the trick of squaring the alphabet gives it a second coproduct ; we obtain in this way a pair of cointeracting bialgebras (Corollary 20). For example, for the following graph:
[TABLE]
we obtain:
[TABLE]
The coproduct is similar to the Connes-Kreimer’s one [2, 3, 4, 6, 5, 1, 16], but slightly different. For example:
[TABLE]
We shall then consider several quotients of , leading to quotient bialgebras of . We obtain in this way a polynomial realization of a Hopf algebra of simple oriented graphs , and then a polynomial realization of the Hopf algebra on quasi-posets of [12, 13, 14, 10]. Restricting to ordered alphabets, instead of quasi-ordered alphabets, we obtain quotients bialgebras, namely based on Feynman graphs with no cycle in Theorem 25 , on simple oriented graphs with no cycle in Theorem 33, and on posets in Theorem 43, obtaining diagrams of Hopf algebras:
[TABLE]
We also show that these Hopf algebra admit noncommutative versions, replacing the algebras by a noncommutative analogue. The last paragraph is devoted to the description of the dual Hopf algebra of posets, using the notion of system of edge between two posets.
1 Operations on alphabets
All the proofs of this section are elementary and left to the reader.
1.1 Quasi-ordered alphabets
Definition 1**.**
A quasi-ordered alphabet is a pair , where is an alphabet and is a total quasi-order on , that is to say a relation on such that:
[TABLE]
If is an order, we shall say that is an ordered alphabet.
Notations 1*.*
Let be a quasi-ordered alphabet. We define an equivalence on X by:
[TABLE]
For all , we shall denote if and not .
1.2 Disjoint union
Proposition 2**.**
Let and be two quasi-ordered alphabets. The set is given a relation :
[TABLE]
Then is a quasi-ordered alphabet.
Remark 1*.*
If and are ordered alphabets, then is also ordered.
Lemma 3**.**
Let be quasi-ordered alphabets.
[TABLE] 2. 2.
Let , and be quasi-ordered alphabets. Then:
[TABLE]
1.3 Product
Proposition 4**.**
Let and be two quasi-ordered alphabets. The set is given a relation in the following way:
[TABLE]
Then is a quasi-ordered alphabet, which we denote by .
Remark 2*.*
If and are ordered alphabets, then is also ordered, and is the lexicographic order.
Lemma 5**.**
Let and be quasi-ordered alphabets.
[TABLE] 2. 2.
Let , and be quasi-ordered alphabets. Then:
[TABLE]
2 Algebras attached to alphabets
2.1 Definition
Definition 6**.**
Let be a quasi-ordered alphabet and let . We put:
[TABLE]
Both of them are given their usual topology of rings of formal series.
Elements of are formal infinite spans of monomials
[TABLE]
where , , with only a finite number of them non-zero. Elements of are formal infinite spans of monomials
[TABLE]
where are elements of , all distinct, , with only a finite number of them non-zero.
2.2 Doubling the alphabets
Proposition 7**.**
Let be two quasi-ordered alphabets. We define a continuous algebra morphism from to or from to by:
[TABLE]
Proof.
In the commutative case, we have to check that for any , . Indeed:
[TABLE]
So is well-defined. The proof in the noncommutative case is similar. ∎
Proposition 8**.**
Let , and be quasi-ordered alphabets. Then:
[TABLE]
seen as morphisms from to , or from to .
Proof.
It is enough to apply these two algebra morphisms on generators. We find:
[TABLE]
When applied to , we find for both of them:
[TABLE]
So these morphisms are equal. ∎
2.3 Squaring the alphabets
Proposition 9**.**
Let be two nonempty quasi-ordered alphabets. There exists a unique continuous algebra morphism from to , or from to such that:
[TABLE]
if, and only if, .
Proof.
In the commutative case, we have to check that for any , . We compute:
[TABLE]
So this holds if, and only if, . The noncommutative case is proved in the same way. ∎
Remark 3*.*
In particular, if , exists if, and only if, or .
Lemma 10**.**
Let and let , and be quasi-ordered alphabets. The following diagrams commute:
[TABLE]
Proof.
As these two maps are algebra morphisms, it is enough to prove that they coincide on generators of or . Let , , .
- •
Both send to .
- •
Both send to .
- •
Both send to .
- •
Both send to
So . ∎
Lemma 11**.**
Let and let , , be quasi-ordered alphabets. The following diagram commutes:
[TABLE]
where:
[TABLE]
Proof.
First step. Let us prove that is an algebra morphism. Let and in .
[TABLE]
As is commutative, .
Second step. By composition, both and are algebra morphisms: it is enough to prove that they coincide on the generators of or . Let , and .
- •
Both send to and to .
- •
Both send to and to .
- •
Both send to and to .
- •
Both send to
- •
Both send to
- •
Both send to .
Therefore, they are equal. ∎
Remark 4*.*
This does not work for morphisms
[TABLE]
But, if we put , where is the canonical surjection from to , then
[TABLE]
seen as morphisms
[TABLE]
The proof is identical to the one of Lemma 11.
3 Feynman graphs
3.1 Definition
Definition 12**.**
A Feynman graph is given by:
- •
A non-empty, finite set of half-edges, with a map .
- •
A non-empty, finite set of vertices.
- •
An incidence map for half-edges, that is to say an involution .
- •
A source map for half-edges, that is to say a map .
The incidence rule must be respected:
[TABLE]
The set of external half-edges of is:
[TABLE]
The set of Feynman graphs is denoted by .
We shall use graphical representations of Feynman graphs: vertices are represented by , half-edges of type are represented by , half-edges of type by ; the incidence map glues two such half-edges to obtain an oriented internal edge of the Feynman graph . In the sequel, we shall write Feynman graph instead of isoclass of Feynman graphs. We shall also consider ordered Feynman graphs, that is to say Feynman graphs such that the set of vertices is given a total order.
Remark 5*.*
We restraint ourselves to Feynman graphs with a unique type of edges. It is possible to do the same for several type of edges, adding generators to the algebras associated to totally quasi-ordered alphabets.
Example 1*.*
Here are examples of Feynman graphs:
[TABLE]
Definition 13**.**
Let be Feynman graphs and let be a surjective map. We define a Feynman graph in the following way:
- •
.
- •
The set of half-edges of is:
[TABLE]
- •
If , then:
[TABLE]
Roughly speaking, is obtained by identifying the vertices of the disjoint union of Feynman graphs with the same image by , and deleting the loops created in this process. In particular, if , or more generally if is bijective, then is (isomorphic to) the disjoint union .
Remark 6*.*
If are ordered Feynman graphs, then is also ordered: if ,
[TABLE]
We deduce a total order on in this way: for any ,
[TABLE]
Example 2*.*
If and are the Feynman graphs of Example 1 and:
[TABLE]
then:
[TABLE]
We shall use the following particular case:
Definition 14**.**
Let and be Feynman graphs, and an injection. We define an equivalence on by:
[TABLE]
Let be the canonical surjection from to . The Feynman graph is denoted by .
In particular, if , is the disjoint union .
3.2 Monomials and Feynman graphs
Definition 15**.**
Let be a monomial of :
[TABLE]
- (a)
We shall say that is admissible if:
[TABLE] 2. (b)
If is admissible, we attach to a Feynman graph , defined in this way:
- •
The set of vertices of is the set of elements , such that .
- •
*The number of internal edges * \textstyle{i}$$\textstyle{j}
- in is .*
- •
*The number of external edges *
- in is .*
- •
*The number of external edges *
- in is .*
Let be a monomial of :
[TABLE]
We shall say that is admissible if its image in (which is a monomial) is admissible. The Feynman graph attached to the image of in the quotient of is ordered: the set of its vertices is , totally ordered by . This ordered Feynman graph is denoted by .
Example 3*.*
Let , , . In :
[TABLE]
In :
[TABLE]
Lemma 16**.**
Let and be two admissible monomials in or in . We put and be the canonical injection. There exists an admissible monomial , such that in :
[TABLE]
Moreover:
[TABLE]
Proof.
We work in ; the proof for is similar. We put:
[TABLE]
then, as in :
[TABLE]
and . ∎
Theorem 17**.**
Let be a Feynman graph and let a quasi-ordered alphabet. We put:
[TABLE]
Then is a subalgebra of . For any Feynman graphs and :
[TABLE]
Moreover, there exists a quasi-ordered alphabet , such that the elements are linearly independent in . 2. 2.
- (a)
Let be an ordered Feynman graph and let a quasi-ordered alphabet. We put:
[TABLE]
Then is a subalgebra of . For any ordered Feynman graphs and :
[TABLE]
There exists a quasi-ordered alphabet , such that the elements are linearly independent in .
Proof.
- By Lemma 16, is a linear sums of terms , with . It remains to show that all such terms are obtained, which is immediate. So is a subalgebra of .
Let be an infinite set. We give it a relation by:
[TABLE]
making it a quasi-ordered alphabet. Let be a Feynman graph. For any , we define:
- •
is the number of internal edges \textstyle{i}$$\textstyle{j} in .
- •
is the number of external edges in .
- •
is the number of external edges in .
Let be an injection: this exists, as is finite and is infinite. We consider:
[TABLE]
Obviously, is admissible and , so is non-zero. As the elements of are all non-zero and their support are disjoint, they are linearly independent.
- Similar proof. ∎
Remark 7*.*
In particular, if :
[TABLE]
3.3 The first coproduct
Definition 18**.**
Let be a Feynman graph, and let .
We define a Feynman graph by the following:
- •
The set of vertices of is .
- •
The set of half-edges of is the set of half-edges such that .
- •
For all half-edge of :
[TABLE] 2. 2.
We shall say that is an ideal of if for all , if and if there is an edge from to in , then . The set of ideals of is denoted by .
Note that if is an ordered Feynman graph, then for any , is also ordered.
Theorem 19**.**
Let be a Feynman graph. For any quasi-ordered alphabets and :
[TABLE]
Proof.
We consider the two following sets:
- •
is the set of triples , where , and are monomials of respectively , and , such that and .
- •
is the set of triples , where is an ideal of , is an admissible monomial of such that , is an admissible monomial of such that .
Let . Let be the set of vertices of belonging to . By Definition of , as , and . Moreover, if and if there is an edge from to in , this means that appears in , so . As , , so : . We define in this way a map:
[TABLE]
It is not difficult to prove that it is a bijection. Hence:
[TABLE]
The proof in is similar. ∎
Corollary 20**.**
Let be the vector space generated by the set of Feynman graphs and let . It is given a Hopf algebra structure: for any Feynman graphs and ,
[TABLE] 2. 2.
Let be the vector space generated by the set of ordered Feynman graphs and let . It is given a Hopf algebra structure by (3)-(4).
Proof.
- For any quasi-ordered alphabet , there is linear map:
[TABLE]
By Theorems 17 and 19, for any quasi-ordered alphabets and , for any :
[TABLE]
Choosing quasi-ordered alphabets , and , such that , and (Proposition 17), we obtain that is an algebra. For all :
[TABLE]
As and are injective, is too, so . Moreover:
[TABLE]
By the injectivity of , is coassociative, so is a bialgebra.
Observe that is filtered by the cardinality of the set of vertices of Feynman graphs, even graded if ; as its components of degree [math] is reduced to , it is connected. Hence, it is a Hopf algebra.
- Similar proof. ∎
3.4 The second coproduct
Definition 21**.**
Let be a Feynman graph, and let be an equivalence on .
We shall say that is -compatible if the following assertions hold:
- •
If is an equivalence class of , then is a connected Feynman graph.
- •
If there is a path in , with , then .
The set of -compatible equivalences will be denoted by . 2. 2.
If are the equivalence classes of , we denote by the disjoint union of the Feynman graphs , . 3. 3.
We denote by the following Feynman graph:
- •
The set of vertices of is .
- •
The half-edges of are the half-edges of such that or not .
- •
For any half-edge of :
[TABLE]
Roughly speaking, is obtained by the deletion in of all the internal edges whose two extremities are not -equivalent, whereas is obtained the deletion in of all the internal edges whose two extremities are -equivalent.
Remark 8*.*
If is ordered, then, as , the Feynman graphs and are also ordered. 2. 2.
The Feynman graph is not the usual contraction of according to a subgraph used by Connes and Kreimer to define a coproduct on Feynman graphs [2, 3, 4, 6, 5, 1, 16], as here all the vertices are conserved.
Notations 2*.*
Let . For any Feynman graph , if are its connected components, we put:
[TABLE]
In particular, .
Proposition 22**.**
Let , be two quasi-ordered alphabets.
We assume that . We consider . For any Feynman graph :
[TABLE] 2. 2.
We consider . For any ordered Feynman graph , in :
[TABLE]
Proof.
- Let be a monomial of , such that . The set of vertices of is denoted by . We define an equivalence on by:
[TABLE]
Let us assume that there is a path in , with . Then, as , in :
[TABLE]
so, in :
[TABLE]
As , we obtain that , and finally:
[TABLE]
Moreover, , with, by Definition of , and . Let be the equivalence which equivalent classes are the connected components of . Then and:
[TABLE]
Moreover, is the unique element of such that (5) holds. Finally, we proved that is a sum of terms , such that there exists , such that is a monomial of and is a monomial of . It is not difficult to see that all these terms are obtained.
- Similar proof. ∎
Corollary 23**.**
We define two coproducts on for any Feynman graph by:
[TABLE]
Then and are bialgebras. For any , we define a coaction by:
[TABLE]
If with , or , then is a bialgebra in the category of right -comodules by the coaction , that is to say:
- •
For all , , where:
[TABLE]
- •
.
- •
, where:
[TABLE]
- •
For all , .
Note that . 2. 2.
Similarly, (6) defines a coproduct on , making it a bialgebra on the category of right -comodules.
makes of -comodules,
Proof.
We take or . Hence, . For any quasi-ordered alphabets , , . The proof that , , and are bialgebras is similar to the proof of corollary 20. The only non-trivial remaining assertion to prove is point 3. Let us take alphabets such that , and are injective.
[TABLE]
We conclude by the injectivity of . ∎
3.5 Restriction to ordered alphabets
Let be a Feynman graph. A cycle in is a sequence of vertices , with , all distinct, such that there exist internal edges , with:
[TABLE]
Lemma 24**.**
Let be a Feynman graph. The following conditions are equivalent:
For any ordered alphabet, . 2. 2.
* has a cycle.*
Moreover, there exists an ordered alphabet , such that for any Feynman graph with no cycle, .
Proof.
. Let us assume that has a cycle , with . There exists , all distinct, such that appears in , so . As is an order, , which is a contradiction. So .
. Let us prove that there exists a total order on , such that if there is an edge from to in , then . We proceed by induction on . If , this is obvious. If , as has no cycle, it has a source , that is to say a vertex with no internal incoming edge. The Feynman graph obtained from by deleting and all the attached half-edges has no cycle, so, by the induction hypothesis, the set of its vertices inherits a total order , compatible with the internal edges of . We give a total order by ; as is a source, this order is compatible with the internal edges of .
We take , with its usual order. There exists a monomial of of the form:
[TABLE]
such that : is the number of internal edges between between and , is the number of incoming external edges in , and is the number of external half-edges outgoing from , if is the previously defined order on the set of vertices of . So . ∎
Observe that if has no cycle and , then both and has no cycle. Hence, considering only ordered alphabets, we obtain a Hopf algebra and a bialgebra of Feynman graphs with no cycle:
Theorem 25**.**
Let be the vector space generated by the set of Feynman graphs with no cycle and let .
It is given a Hopf algebra structure: for any Feynman graphs and with no cycle,
[TABLE] 2. 2.
We define a second coproduct by:
[TABLE]
Then is a bialgebra. Moreover, is a bialgebra in the category of -comodules. 3. 3.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to and from to .
Here is its non-commutative version:
Theorem 26**.**
Let be the vector space generated by the set of ordered Feynman graphs with no cycle and let .
It is given a Hopf algebra structure by (7)-(8). 2. 2.
We define a second coproduct by (9). Then is a bialgebra. Moreover, is a bialgebra in the category of -comodules. 3. 3.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to and from to .
Remark 9*.*
There is a canonical injection . This injection is compatible with if, and only if, : indeed, as is the disjoint union, it is compatible with . If , taking G=H=\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 6.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{{{\hbox{\ellipsed@{6.0pt}{6.0pt}}}}\hbox{\kern-6.0pt\raise 0.0pt\hbox{\hbox{\kern 6.0pt\raise 0.0pt\hbox{\textstyle{}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 36.24512pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{{{\hbox{\ellipsed@{6.0pt}{6.0pt}}}}\hbox{\kern 36.24512pt\raise 0.0pt\hbox{\hbox{\kern 6.0pt\raise 0.0pt\hbox{\textstyle{}}}}}}\ignorespaces}}}}\ignorespaces:
- •
In :
[TABLE]
- •
In :
[TABLE]
However, is compatible with and .
4 Quotients of Feynman graphs
4.1 Simple oriented graphs
Let be a quasi-ordered alphabet. We consider the following quotients of and :
[TABLE]
Elements of are formal spans of monomials
[TABLE]
where the , with only a finite number of them non-zero. Elements of are formal spans of monomials
[TABLE]
where are elements of , all distinct, , with only a finite number of them non-zero. The canonical surjections from to or form to are both denoted by .
Proposition 27**.**
Let be two quasi-ordered alphabets, and , such that .
There exist unique algebra morphisms and , such that the following diagrams commute:
[TABLE]
They are given in the following way: if , ,
[TABLE] 2. 2.
The same assertions hold if one replaces and by and everywhere.
Proof.
Immediate verifications. ∎
Definition 28**.**
Let be a Feynman graph. We denote by the simple oriented graph obtained by the following procedure:
Delete all the external edges of . 2. 2.
Delete the loops, that is to say internal edges with two identical extremities. 3. 3.
If has several edges from to , where , keep only one edge from to in .
Lemma 29**.**
Let and be two Feynman graphs. The following conditions are equivalent:
* for any quasi-ordered alphabet .* 2. 2.
.
Proof.
. Let be a quasi-ordered alphabet. As , we can assume that . We denote by the set of pairs such that there is an edge from to in and in , with . There exist non-zero scalars , , for , and scalars , , , , , , and a set of injections from to such that:
[TABLE]
Their image under are both equal to:
[TABLE]
. Let us choose an alphabet , such that and are non-zero. Let be a monomial of :
[TABLE]
Then:
[TABLE]
where if and [math] otherwise. This monomial appears in , so there is a monomial in , of the form:
[TABLE]
with, if , if, and only if, if, and only if, . This implies that . ∎
For any simple graph , we denote and , where is any Feynman graph such that (for example, ). These elements, if they are all non-zero, form a basis of a subalgebra of or . We obtain a quotient of and based on simple graphs. To sum up:
Theorem 30**.**
Let be the vector space generated by the set of simple graphs and let .
It is given a Hopf algebra structure: for any simple graphs and ,
[TABLE] 2. 2.
We define a second coproduct by:
[TABLE]
Then is a bialgebra. Moreover, is a bialgebra in the category of -comodules. 3. 3.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to and from to .
It has a non-commutative version:
Theorem 31**.**
Let be the vector space generated by the set of ordered simple graphs and let .
It is given a Hopf algebra structure by (10)-(11). 2. 2.
We define a second coproduct by (12). Then is a bialgebra. Moreover, is a bialgebra in the category of -comodules. 3. 3.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to and from to .
Remark 10*.*
As simple graphs are Feynman graphs, there is a canonical injection . It is compatible with if, and only if, . Indeed, the disjoint union product is compatible with . If , taking G=H=\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 6.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{{{\hbox{\ellipsed@{6.0pt}{6.0pt}}}}\hbox{\kern-6.0pt\raise 0.0pt\hbox{\hbox{\kern 6.0pt\raise 0.0pt\hbox{\textstyle{}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 75.77625pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{{{\hbox{\ellipsed@{6.0pt}{6.0pt}}}}\hbox{\kern 75.77625pt\raise 0.0pt\hbox{\hbox{\kern 6.0pt\raise 0.0pt\hbox{\textstyle{}}}}}}\ignorespaces}}}}\ignorespaces:
[TABLE]
Hence, is not compatible with . Moreover, is not compatible with and . For example, if G=\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 6.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{{{\hbox{\ellipsed@{6.0pt}{6.0pt}}}}\hbox{\kern-6.0pt\raise 0.0pt\hbox{\hbox{\kern 6.0pt\raise 0.0pt\hbox{\textstyle{}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 75.77625pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{{{\hbox{\ellipsed@{6.0pt}{6.0pt}}}}\hbox{\kern 75.77625pt\raise 0.0pt\hbox{\hbox{\kern 6.0pt\raise 0.0pt\hbox{\textstyle{}}}}}}\ignorespaces}}}}\ignorespaces:
[TABLE]
4.2 Simple graphs with no cycle
Lemma 32**.**
Let be a simple graph. The following conditions are equivalent:
For any ordered alphabet, . 2. 2.
* has a cycle.*
Moreover, there exists an ordered alphabet , such that for any simple graph with no cycle, .
Proof.
Similar to the proof of Lemma 24. ∎
Consequently, we obtain Hopf algebras structures on simple graphs with no cycle:
Theorem 33**.**
Let be the vector space generated by the set of simple graphs with no cycle and let . It is given a Hopf algebra structure: for any simple graphs with no cycle and ,
[TABLE]
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to .
Here is its non-commutative version:
Theorem 34**.**
Let be the vector space generated by the set of ordered simple graphs with no cycle and let . It is given a Hopf algebra structure by (13)-(14). Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to and from to .
4.3 quasiposets
Let be a quasi-ordered alphabet. We consider the following quotients of and :
[TABLE]
The canonical surjection from to and from to are both denoted by .
Definition 35**.**
Let be a simple oriented graph, which set of vertices is denoted by . We define a quasi-order on , by:
[TABLE]
Note that any quasi-poset, that is to say any pair , where is a finite set and is a quasi-order on , can be obtained in this way: consider the arrow diagram of , which is a simple graph such that .
Lemma 36**.**
Let be a quasi-ordered alphabet. For any simple graphs , , the following conditions are equivalent:
* for any quasi-ordered alphabet .* 2. 2.
The quasi-posets and are isomorphic.
Proof.
We define a congruence on the set of monomials of by . Then two monomials of have the same image under if, and only if, they are congruent. At the level of graphs, this gives that for any quasi-ordered alphabet , if, and only if, one can go from to by a sequence of transformations:
[TABLE]
that is to say if, and only if, and are isomorphic. ∎
Proposition 37**.**
Let be two quasi-ordered alphabets. There exists a unique algebra morphism such that the following diagram commutes:
[TABLE] 2. 2.
The same assertion hold, after replacing and by and everywhere.
Proof.
- If , in :
[TABLE]
So is defined from to .
- Similar proof. ∎
Remark 11*.*
Unfortunately, this does not work for , except if is a totally ordered alphabet.
For any quasi-poset , we denote and , where is any simple graph such that , for example the arrow graph or the Hasse graph of . These elements, if all non-zero, are a basis of a subalgebra of or . We obtain a quotient of and based on quasi-posets. We shall need the following definitions to describe it:
Definition 38**.**
Let be two quasi-posets, and be an injective map. We consider the quotient, already used in Definition 14:
[TABLE]
We define a relation on by:
[TABLE]
The transitive closure of is denoted by , and is a quasi-poset.
Note that if and are ordered quasi-posets, then is also an ordered quasi-poset.
Definition 39**.**
Let be a quasi-poset and let .
We denote by the quasi-poset . Note that if is a poset, is too. 2. 2.
We shall say that is an ideal (or an open set) of if:
[TABLE]
The set of ideals of is denoted by .
Theorem 40**.**
Let be the vector space generated by the set of quasi-posets and let .
It is given a Hopf algebra structure: for any quasi-posets ,
[TABLE] 2. 2.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to .
Here is its non-commutative version:
Theorem 41**.**
Let be the vector space generated by the set of ordered quasi-posets and let .
It is given a Hopf algebra structure by (15)-(16). 2. 2.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to .
The Hopf algebras and are introduced and studied in [12, 13, 14, 10].
4.4 Posets
Lemma 42**.**
Let be a quasi-poset. The following conditions are equivalent:
For any ordered alphabet , . 2. 2.
* is a poset.*
Moreover, there exists an ordered alphabet , such that for any poset , .
Proof.
Similar to the proof of Lemma 24. ∎
Consequently, we obtain a Hopf algebra structure on posets.
Theorem 43**.**
Let be the vector space generated by the set of posets and let .
It is given a Hopf algebra structure: for any posets and ,
[TABLE] 2. 2.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to .
Here is its non-commutative version:
Theorem 44**.**
Let be the vector space generated by the set of ordered posets and let .
It is given a Hopf algebra structure by (17)-(18). 2. 2.
Let us consider the map:
[TABLE]
It is a Hopf algebra morphism from to .
Remark 12*.*
Using Remark 11, we could use totally ordered alphabets to define a second coproduct on . We would obtain the coproduct given for any poset of order by:
[TABLE]
which is coassocative, with a right counit but no left counit.
4.5 Dual product
We now describe the dual product of on . We identify and its graded dual through the symmetric pairing defined for any pair of posets by:
[TABLE]
where is the number of automorphisms of .
Proposition 45**.**
Let us define a coproduct on in the following way: If is a poset, denoting by its connected components,
[TABLE]
Then is coassociative and counitary, and for any :
[TABLE]
Proof.
The coassociativity of is immediate. Its counit is the map defined by for any poset . Let , , be three posets. Let us denote by the different isoclasses of connected components of , and . There exist , , , such that:
[TABLE]
Moreover:
[TABLE]
Hence:
[TABLE]
Moreover:
[TABLE]
Finally, . ∎
Definition 46**.**
Let and . We denote by the set of subsets of . A system of edges from to is a map such that:
For any , such that , then for any , , we do not have . 2. 2.
For any , for any , then if, and only if, .
Proposition 47**.**
Let , be two posets and be a system of edges from to . We define an order on in the following way:
- •
For any , if .
- •
For any , if .
- •
For any , , if there exists , , such that and .
This poset is denoted by . Moreover, is an ideal of and the edges of the Hasse graph of are:
- •
The edges of the Hasse graph of ,
- •
The edges of the Hasse graph of ,
- •
The edges , with and .
Proof.
Note that if , we cannot have and .
is obviously reflexive. If and , then both and belong to , or both belong to . Hence, and , or and . In both cases, , so is antisymmetric. Let us assume that and . Four cases hold.
. Then , so . 2. 2.
. There exist , , such that and . So . 3. 3.
. There exist , , such that and . So . 4. 4.
. Then , so .
Hence, is an order.
Let be an edge of the Hasse graph of , that is to say:
- •
.
- •
If , then .
Three cases are possible.
. As , is an edge of the Hasse graph of . 2. 2.
. As , is an edge of the Hasse graph of . 3. 3.
. Then there exists , , such that and . By definition, so . As is an edge, and , so .
Conversely:
- •
Let be an edge of the Hasse graph of . If , necessarily as , so , which implies .
- •
Similarly, if is an edge of the Hasse graph of , then it is an edge of the Hasse graph of .
- •
If and , then . If , two cases are possible.
If , there exists , , such that , . So . As is an edge, and . 2. 2.
Similarly, if , .
Obviously, is an ideal of . ∎
Lemma 48**.**
Let be three posets. We consider the two following sets:
- •
* is the set of triple , where is an ideal of , is an isomorphism from to and is an isomorphism from to .*
- •
* is the set of pairs , where is a system of edges from to and is an isomorphism from to .*
Then and are in bijection.
Proof.
We shortly denote and .
First step. Let defined by , with:
- •
is defined by and .
- •
For any , is the set of such that is an edge of the Hasse graph of .
Let us prove that is well-defined.
Let , , , such that and . Then , , and are edges of the Hasse graph of . We obtain:
[TABLE]
This contradicts that is an edge of the Hasse graph of .
Let , , with . Then . As is an edge, , so . We proved that is a system of edges from to .
By the preceding lemma, the image by of the edges of are the edges of , so is an isomorphism. We proved that is well-defined.
Second step. Let defined by , where:
- •
.
- •
and .
By the preceding lemma, is well-defined.
Last step. Let . We put and . Then , and similarly, . So .
Let . We put and . For any , :
[TABLE]
Therefore, . Moreover, for , , so . Hence, . ∎
Theorem 49**.**
We define a product on in the following way: for any posets ,
[TABLE]
Then is a Hopf algebra. Moreover, for any :
[TABLE]
Proof.
Let be posets. By the preceding lemma:
[TABLE]
As is non degenerate and is a Hopf algebra, dually is a Hopf algebra.
Let . For any :
[TABLE]
We conclude by the non degeneracy of . ∎
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] A. Connes and D. Kreimer, From local perturbation theory to Hopf- and Lie-algebras of Feynman graphs , Mathematical physics in mathematics and physics (Siena, 2000), Fields Inst. Commun., vol. 30, Amer. Math. Soc., Providence, RI, 2001, pp. 105–114.
- 2[2] Alain Connes and Dirk Kreimer, Hopf algebras, renormalization and noncommutative geometry , Comm. Math. Phys. 199 (1998), no. 1, 203–242.
- 3[3] , Renormalization in quantum field theory and the Riemann-Hilbert problem , J. High Energy Phys. (1999), no. 9, Paper 24, 8.
- 4[4] , Renormalization in quantum field theory and the Riemann-Hilbert problem. I. The Hopf algebra structure of graphs and the main theorem , Comm. Math. Phys. 210 (2000), no. 1, 249–273.
- 5[5] , From local perturbation theory to Hopf and Lie algebras of Feynman graphs , Lett. Math. Phys. 56 (2001), no. 1, 3–15, Euro Conférence Moshé Flato 2000, Part I (Dijon).
- 6[6] , Renormalization in quantum field theory and the Riemann-Hilbert problem. II. The β 𝛽 \beta -function, diffeomorphisms and the renormalization group , Comm. Math. Phys. 216 (2001), no. 1, 215–241.
- 7[7] G. H. E. Duchamp, J.-G. Luque, J.-C. Novelli, C. Tollu, and F. Toumazet, Hopf algebras of diagrams , Internat. J. Algebra Comput. 21 (2011), no. 6, 889–911.
- 8[8] Gérard H. E. Duchamp, Florent Hivert, Jean-Christophe Novelli, and Jean-Yves Thibon, Noncommutative symmetric functions VII: free quasi-symmetric functions revisited , Ann. Comb. 15 (2011), no. 4, 655–673.
