On the finite presentation of operads
Abstract: Operads were introduced to describe compositional structures arising in algebraic topology.
Recently, some researches were interested in using operads in applied mathematics, to model composition
of structures in logic, databases, and dynamical systems. In, we focus on finite presentation of an operad
and its associated algebra. More precisely, we prove the general result stating that if an operad Ohas
a finite presentation, then the associate O-algebra has also a corresponding one. Some application in
physics, especially in wiring diagrams will be discussed.
Key-Words: operad, operad algebra, wiring diagrams, finite presentation, compositionality.
1 Introduction
Operad theory is a field of algebra (more precisely
abstract algebra) used to describe algebraic struc-
ture that models some algebraic properties such
as commutativity, associativity, Lie brackets, . . . .
An operad (or colored operad) is a structure
that consists of a bunch of elements that are
viewed as abstract operations, each one having
a multiple inputs, where inputs are finite ordered
list (possibly zero ones) of elements called colors
in a fixed non-empty finite class S, these oper-
ations are equipped with a specification of how
to compose them in one output (element in S),
and subject to associativity and unity axioms, [1],
these operations are represented by trees which
can be grafted onto each other to represent the
composition. Just like a monoid can be viewed as
a single object category, likewise an operad can
be seen as a single object multicategorie, hence
multicategories are also named as operads, or col-
ored operads, and in case of ambiguity, it can be
identified the class S, then it will be called an
S-colored operad.
An operad-algebras (algebra over on operad)
is a generalization of the notion of a module over
a ring. One can define an operad-algebra as a
concrete realization of the abstract operations of
the operad, in other words, it can be defined as a
set combined with concrete operations on this set
whereby their behaviour is analogous to the ab-
stract operations in the operad : an object com-
bined with operations as defined by the operad,
subject to the composition condition as defined
by the operad, [1]. Operad-algebra is to its as-
sociate operad as group representation is to its
group. They form a category analog of that of
universal algebras. Operads were firstly intro-
duced in algebraic topology in the early of 1970s
by [2], notably to model iterated loop spaces,
and the original definition of operad is due to
J.Peter in his book ”The Geometry of Iterated
Loop Spaces”, and he was the first one to coin
the term operad. Operads are basic in homo-
topy theory, and they have many applications in
many branches of mathematics, [3], [4], such as
string topology, category theory, combinatories
of trees, algebraic deformation theory, homotopi-
cal algebras and vertex operator algebras. Fur-
thermore, operads are essential in mathematical
physics, computer science, biology, and others.
For more details on operads, we refer the inter-
ested reader to, [5], [6].
Here, we focus on two specific operads, that
of wiring diagrams (resp. undirected wiring dia-
grams) denoted through this paper by WD (resp.
UWD). The original definition of wiring diagram
is given by Rupel and Spivak in [7] who observed
that the set of wiring diagrams form an operad
called the operad of wiring diagrams. Wiring di-
agrams are a simplified representation of electri-
cal systems or circuits (graphical language) com-
posed of such operations, each one having a mul-
tiple inputs and multiple outputs, each element
of which is allowed to carry a such value, and
describes how these operations are connected be-
tween them to form a larger one operation more
complicated. Contrary to a wiring diagram, an
undirected wiring diagram is version of wiring di-
agrams that each operation can be seen as a fi-
nite set, which each element is allowed to carry a
value. Mathematically speaking, let Sbe a class,
Received: September 23, 2022. Revised: May 8, 2023. Accepted: May 25, 2023. Published: June 19, 2023.
WSEAS TRANSACTIONS on SYSTEMS
DOI: 10.37394/23202.2023.22.63
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ETTAKI AYOUB1, ELOMARY MOHAMED ABDOU1, MAMOUNI MY ISMAIL2,
1IMII laboratory. Department of Mathematics and Computer Science. FST Settat, MOROCCO
2M@DA research team, Department of Mathematics, CRMEF Rabat, MOROCCO
aS-wiring diagram (we can drop S, and call it a
wiring diagram if Sis clear from the context) in
[1] is given by ψ= (X, Y, DN, v, s) where Yis the
output box of ψand X= (X1, ...., Xn) is a BoxS-
profile with Xithe i-th input box of ψ, (DN, v) is
an S-finite set, and sis the supplier assignment
for ψ. Similarly a S-undirected wiring diagram
(we can drop S, and call it an undirected wiring
diagram if Sis clear from the context) in [1] is
given by ψ= (X, Y, C, f, g) where Yis the output
box of ψand X= (X1, ...., Xn) is a F inS-profile
with Xithe i-th input box of ψ,CF inSthe set
of cables of ψ, and f, g are maps in the cospan di-
agram. More details about the explicit definition
of wiring diagram and undirected wiring diagram
can be found in [1].
In [1], D. Yau established that for each class
S, the collection of S-wiring diagrams is a BoxS-
colored operad denoted WD that has 8 generat-
ing wiring diagrams that they generate the op-
erad WD and 28 elementary generating relations
that they generate together with the associativ-
ity and the unity axioms defined by the operad
WD all the relations in WD , and he also es-
tablished that for each class S, the collection of
S-undirected wiring diagrams is a F inS-colored
operad denoted UWD that has 6 generating undi-
rected wiring diagrams that they generate the op-
erad UWD and 17 elementary generating rela-
tions that they generate together with the asso-
ciativity and the unity axioms defined by the op-
erad UWD all the relations in UWD. Then every
wiring diagram (respectively undirected wiring
diagram) has a presentation in terms of finitely
many generating wiring diagrams (respectively
undirected wiring diagrams) as a finite iterated
operadic composition, diagrams in both WD and
UWD can be built as an operadic composition
of generating diagrams in different ways, so they
can have many different presentations expressed
as a finite iterated operadic composition. Then
the concept of a simplex was crucial to develop
the necessary language to check if two any pre-
sentations of the same diagram are equivalent,
meaning connected by a finite sequence of ele-
mentary equivalences. According to [1] the op-
erad WD (resp UWD ) has a finite presentation
if and only if WD (resp UWD ) satisfies the two
following assertions : the first is that every wiring
diagram (resp. undirected wiring diagram) can
be generated by the generating wiring diagrams
(resp. undirected wiring diagram) as a finite it-
erated operadic composition, and the second is
that if a wiring diagram (resp. undirected wiring
diagram) can be expressed as an operadic com-
position of the generating wiring diagrams (resp.
undirected wiring diagram) in two different ways,
then it can be found a finite sequence of elemen-
tary equivalences from the first operadic compo-
sition to the other one, that’s what it call a finite
presentation theorem for WD (resp. UWD).
In [1], D. Yau used these finite presentations
to describe the WD-algebra and UWD-algebra
in terms of finitely many generating structure
maps and generating axioms corresponding to
the generating wiring diagrams and elementary
relations in their associted operads. His proof
was based on an equivalence between two differ-
ent definitions of O-algebra (where O=WD or
O=UWD). In fact, the WD-algebra (resp. the
UWD-algebra) has 8 generating structure maps
corresponding to the 8 generating wiring dia-
grams, and 28 generating axioms corresponding
to the 28 elementary relations in WD (resp. 6
generating structure maps corresponding to the
6 generating undirected wiring diagrams, and
17 generating axioms corresponding to the 17
elementary relations in UWD). Finally D.Yau
proved that the operad algebra WD-algebra has
a finite presentation corresponding to the one of
WD.
A natural extension, is to investigate the anal-
ogous of D. Yau’s claim for any Ooperad, then
our approach is based on the operad WD (resp.
UWD) which initially invented in Spivak, [7], [8].
This paper deals with an operadic approach to
formulating and proving a more general result
that consider both of these finite presentation
theorems as special cases, our main result stating
that if an operad Ohas a finite presentation, then
the associate O-algebra has also a corresponding
one, a finite presentation of O(resp. O-algebra)
means that the operad O(resp. O-algebra) has a
finite generating set and any two equivalent sim-
plices in O(resp. O-algebra) are connected by
a finite sequence of elementary equivalences in O
(resp. O-algebra). Our results state the following
:
Theorem 1.1. If the operad Ohas a finite gen-
erating set T, then its associated O-algebra, A,
has a corresponding finite generating set Tµ.
That will be sufficient to prove the first part
of our main theorem, to establish the second part
of our theorem, we will define the concept of a
simplex and an elementary equivalence, we will
see that every elementary equivalence is induced
by an elementray relation or an operad associa-
tivity unity equivariance axiom, then we develop
the necessary language that allows us to define
what an elementary relation means, and prove
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the following result :
Theorem 1.2. Let Tbe a finite generating set
for O, and take ζand ξtwo simplices in O. If
|ζ|=|ξ|is an elementary relation in O, then its
corresponding elementary relation in Ais µ|ζ|=
µ|ξ|.
Afterwards, we will show that the operad as-
sociativity unity equivariance axiom in Ohas
a corresponding associativity unity equivariance
axiom in O-algebra, and this together with the
above results permits us to announce the next
result :
Theorem 1.3. If Wthe set of all elementary
equivalences in Tis a strong generating set of O
in T, then its corresponding set Wµof all ele-
mentary equivalences in Tµis a strong generating
set of Ain Tµ.
This last theorem yields the second part of our
main theorem. and that will be sufficient to prove
the following theorem :
Theorem 1.4. If Ohas a finite presentation,
then its associated O-algebra, Ahas a correspond-
ing finite presentation one.
The rest of the paper is broken down as fol-
lows : in section 2 we will summarize the nec-
essary background to prove our results, that will
be proved in section 3. In section 4, we apply see
how our result fits in the cases of both directed
and undirected wiring diagrams operads.
2 Materials
Let Sbe a class, (n, m)N2, and P rof(S) the
class of finite ordered sequences of elements in S.
Elements a= (a1, . . . , an) of P rof (S) of length n
are also called S-profiles.
Definition 2.1. AS-colored operad (O,1,)is
defined as follows:
To any b S and any two S-profiles, a=
(a1, . . . , an)and c= (c1, . . . , cm),(O,1,)is
equipped with
a class Ob
a=Ob
a1, . . . , anwhich ele-
ments are called multimaps;
a bijection
Ob
aσ
O b
where σSn, and = (aσ(1), . . . , aσ(n))
a specific element called the b-colored unit
1b O b
b
a map called the operadic composition iis
defined by
Ob
a× O ai
ci
O b
aic
where aic=
(a1, . . . , ai1, c1, . . . , cm, ai+1, . . . , an).
This is enough to satisfy the associativity, the
unity, and the equivariance axioms.
The best general refernce here is, [1].
Definition 2.2. Let Cbe a collection of mul-
timaps of O, and ψa multimap in O, we say that
ψadmits a presentation in Cif ψcan be expressed
as an iterated operadic composition of multimaps
in C.
For example, consider the collection C=
{ψ1, ψ2, ψ3}, where ψ1, ψ2, ψ3are multimaps in
O.
Suppose ψ O such that ψ= (ψ13ψ2)4ψ3,
then ψhas a presentation in C.
Note that the iterated operadic composition ψ13
(ψ24ψ3) is not necessarily a presentation of ψ
in C, since the equality ψ= (ψ13ψ2)4ψ3=
ψ13(ψ24ψ3) is not assured, for this reason, we
need to define the concept of a simplex later.
Definition 2.3. Let Obe an operad.
1. A set (or collection) Tof multimaps of O
is called a generating set for Oif every
multimap in Ohas a such presentation in
T, meaning that for all ψin Othere ex-
ist ψ1, . . . , ψrin Tsuch that ψcan be de-
composed as an iterated operadic composi-
tion (possibly infinite) of ψ1, . . . , ψr,for some
r1.
2. A set (or collection) Tof multimaps of Ois
called a finite generating set for O, when T
is a finite set (or collection) of mutimaps of
O, and every multimap in Ohas a such pre-
sentation in T, meaning that for all ψin O
there exist ψ1, . . . , ψrin Tsuch that ψcan be
decomposed as a finite iterated operadic com-
position of ψ1, . . . , ψr,for some r1.
The elements of Tare called generating mul-
timaps.
Given an operad O, an algebra over an operad,
or just O-algebra for simplicity, roughly, is a left
module over Owith multiplications parametrized
by O. Formally meaning
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Definition 2.4. Let Obe an operad. An operad-
algebra (shortly O-operad), is a pair (A, µ)
equipped with a class , denoted Ab, for any b S,
called the b-colored entry of A, and the multipli-
cation µis defined to be
Aa=
n
Y
i=1
Aai
µψ
Ab,
called the structure map, where b S, a =
(a1, . . . , an)P rof(S)and ψ O b
a, such
that the associativity, unity, and equivariance ax-
ioms are respected.
Each structure map has one entry of O. The
best general refernce here is, [1].
Simplices:
Let Obe an operad with a finite generating set
T, let nN, we define inductively a n-simplex
ψand its composition |ψ|in Oas follows :
A 1-simplex is a generating multimap, and
its composition |ψ|is defined to be ψitself,
i.e |ψ|=ψ;
An-simplex, for n2 is defined to be a tuple
ψ= (φ, i, ϕ) consists of :
(iN
psimplex φwith p1
qsimplex ϕwith q1
such that p+q=n, and the operadic com-
position |ψ|=|φ| i|ϕ|.
Here, the k-simplices for all 1 kn1
and their compositions are supposed to be
well defined in O.
For simplicity of notation, we also denote a
n-simplex by ψ= (ψ1, . . . , ψn), where the gener-
ating multimaps ψ1, . . . , ψnare ordered in which
they appear in the composition and we write
|ψ|=ψ1i1· · ·in1ψn. Unless otherwise stated a
simplex in Ois a m-simplex in Ofor some m1.
Moreover we say that a simplex ψis a presenta-
tion of |ψ|, and the set of all presentations of ψ
in O, denoted by
ψ={Ψsimplex in O/|Ψ|=ψ}.
For example, we can consider for some
i, j, k, l Nthe case of a 5-simplex in Owhich is
an iterated operadic composition in the operad
Oof the form:
(((ψ1iψ2)jψ3)kψ4)lψ5,shortly
((((ψ1, i, ψ2), j, ψ3), k, ψ4), l, ψ5)
((ψ1i(ψ2jψ3)) kψ4)lψ5,shortly
(((ψ1, i, (ψ2, j, ψ3)), k, ψ4), l, ψ5)
(ψ1i((ψ2jψ3)kψ4)) lψ5,shortly
((ψ1, i, ((ψ2, j, ψ3), k, ψ4)), l, ψ5)
(ψ1i(ψ2j(ψ3kψ4))) lψ5,shortly
((((ψ1, i, ψ2), j, ψ3), k, ψ4), l, ψ5)
((ψ1iψ2)j(ψ3kψ4)) lψ5,shortly
(((ψ1, i, ψ2), j, (ψ3, k, ψ4)), l, ψ5)
ψ1i(ψ2j(ψ3k(ψ4lψ5))),shortly
(ψ1, i, (ψ2, j, (ψ3, k, (ψ4, l, ψ5))))
ψ1i(ψ2j((ψ3kψ4)lψ5)),shortly
(ψ1, i, (ψ2, j, ((ψ3, k, ψ4), l, ψ5)))
ψ1i((ψ2j(ψ3kψ4)) lψ5),shortly
(ψ1, i, ((ψ2, j, (ψ3, k, ψ4)), l, ψ5))
ψ1i(((ψ2jψ3)kψ4)lψ5),shortly
(ψ1, i, (((ψ2, j, ψ3), k, ψ4), l, ψ5))
ψ1i((ψ2jψ3)k(ψ4lψ5)),shortly
(ψ1, i, ((ψ2, j, ψ3), k, (ψ4, l, ψ5)))
(ψ1iψ2)j((ψ3kψ4)lψ5),shortly
((ψ1, i, ψ2), j, ((ψ3, k, ψ4), l, ψ5))
(ψ1iψ2)j(ψ3k(ψ4lψ5)),shortly
((ψ1, i, ψ2), j, (ψ3, k, (ψ4, l, ψ5)))
((ψ1iψ2)jψ3)k(ψ4lψ5),shortly
(((ψ1, i, ψ2), j, ψ3), k, (ψ4, l, ψ5))
(ψ1i(ψ2jψ3)) k(ψ4lψ5),shortly
((ψ1, i, (ψ2, j, ψ3)), k, (ψ4, l, ψ5)).
In our example, for ψ= (((ψ1iψ2)j
ψ3)kψ4)lψ5,there exists a 5-simplex Ψ =
((((ψ1, i, ψ2), j, ψ3), k, ψ4), l, ψ5) (shortly Ψ =
(ψ1, ψ2, ψ3, ψ4, ψ5)) whose composition is ψ=
|Ψ|= (((ψ1iψ2)jψ3)kψ4)lψ5,then
the 5-simplex Ψ is a presentation of ψ=|Ψ|,
but neither ((((ψ1, j, ψ2), i, ψ3), k, ψ4), l, ψ5) nor
(((ψ1, i, (ψ2, j, ψ3)), k, ψ4), l, ψ5) is not necessarily
a presentation of ψ.
Definition 2.5. Two simplices ψand ϕare said
to be equivalent in O, whenever their composi-
tions |ψ|and |ϕ|are equal in O.
A sub-simplex b
ψof ψis defined to be itself
if ψis a 1-simplex, since otherwise ψ= (φ, i, ϕ)
is defined as above, hence a sub-simplex of ψis
defined to be either a sub-simplex of φ, or of ϕ,
or ψitself, and we write b
ψψ.
Once again in our example, for ψ=
(ψ1i(ψ2jψ3))k(ψ4lψ5),both ψ1i(ψ2jψ3) =
(ψ1, i, (ψ2, j, ψ3)), ψ2jψ3= (ψ2, j, ψ3),or
ψ4lψ5= (ψ4, l, ψ5) are sub-simplices of
ψ, however, both ψ1iψ2= (ψ1, i, ψ2) and
ψ3k(ψ4lψ5)=(ψ3, k, (ψ4, l, ψ5)) are not.
In what follows, we will see how two such sim-
plices that are presentations of the same mul-
timap can be related, more precisely we develop
the precise concept that will allow us to be able to
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replace (or substitue) a sub-simplex of a simplex
by another one.
Definition 2.6. Given a n-simplex ψin Owith
ψ= (ψ1, ...., ψn)and k < n. A relaxed k-moves
of ψis the given of some 1k, kk; 1
snkand a (nk+k”)-simplex ϕsuch that
:
1. ψj=ϕjfor all 1js1,
2. ψj=ϕjk+kfor all s+kjn,
3. |ζ|=|ξ|, for ζ= (ψs, ...., ψs+k1)a sub-
simplex of ψ, and ξ= (ϕs, ...., ϕs+k1)a
sub-simplex of ϕsuch that
Remarks.
Firstly it is worth to point out the compat-
ibility with the operadic composition iof
ψs+k=ϕs+k,
a relaxed k-moves of ψ, is finally a l-simplex
ϕ, where l=nk+k such that nk+1
ln+k1. Since k < n then 2 l2n2,
for s= 1, we obtain ζ= (ψ1, ...., ψk), ξ=
(ϕs, ...., ϕk) and ψj=ϕjk+kfor all 1+k
jn,
if k= 1, then ϕis a n-simplex, such that
ψj=ϕjfor all 1 jn,
one may consider k=n, but in this case we
should have k< k and k< k,
ak-relaxed moves is a substitution of a k-
simplex (kk) with k”-simplex (kk),
but keeping fixed the operadic composition
into which they are substituted.
Definition 2.7. Under the same hypotheses of
the previous definition, we say that ψand ϕare
equivalent by a relaxed k-moves.
Vocabulary.
Let Obe an operad with a finite generating set
T, then :
every multimap in Ohas a decomposition (or
presentation) in T, then there exists a sim-
plex ψin Twhich is a presenation of this
multimap. The above equality relation
|ζ|=|ξ|
is either an operad associativity or unity or
an equivariance axiom, otherwise is called an
elementary relation,
an elementary sub-simplex ˆ
ψof ψis a sub-
simplex of one of two following forms:
ˆ
ψis one side (either left or right) of a
specified elementary relation,
ˆ
ψis one side (either left or right) of a
specified operad associativity or unity
or equivariance axiom involving only the
generating multimaps.
Suppose that we have a n-simplex ψ(for
some integer n2) in Owhich is a
presentation of the multimap |ψ|in O,
and ζis a sub-simplex of ψsuch that
|ζ|=|ξ|, where ξis a simplex in O, then
the relation |ζ|=|ξ|is either an elemen-
tary relation or an operad associativity
or unity or equivariance axiom involving
only the generating multimaps, hence,
one can obtain a relaxed k-moves of the
simplex ψby substituting the elemen-
tary sub-simplex ζby the other one ξ,
two simplicies ψand ϕare called to be el-
ementarily equivalent in O, if ψand ϕare
equivalent by a relaxed k-moves (for some in-
teger k2), then we write ψk
ϕ(if there is
no confusion, we can drop kand write ψϕ)
and call this an elementary equivalence in O,
in other words an eleelementary equivalence
is a subsitution of a elementary sub-simplex
of one side by the other one,
two simplicies ψand ϕare said to be con-
nected by a finite sequence of elementary
equivalences in Oif and only if there exist
some simplices ψ1, ...., ψrin Osuch that ψ1
k1
. . . kr1
ψr, and ψk
ψ1
k1
. . . kr1
ψr
kr
ϕfor
some integers k, k1, . . . , kr2.
Denotations. Let Obe an operad with a finite
generating set T. Let ψbe an n-simplex in Ofor
some integer n2.
The set of all relaxed k-moves of ψin Tis
denoted by Wk
ψ,
The set of all relaxed k-moves for all k
{2, . . . , n 1}is
Wn
ψ:=
n1
[
k=2
Wk
ψ,
and this is the set of all relaxed n-moves of
ψin T. In other words, Wn
ψis the set of all
elementary equvalences of ψ.
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The set of all relaxed n-moves in Tis denoted
by W, where
W:= [
ψ∈O
Wn
ψ
In other words, Wis the set of all elementary
equivalences in T.
Definition 2.8. Let Obe an operad with a finite
generating set T, and Wthe set of all its ele-
mentary equivalences. We say that Wis a strong
generating set for Oin Tif any two equivalent
simplices in Tare connected by a finite sequence
of elementary equivalences in W. Roughly speak-
ing, Wis the set that generate all relations in
O.
Finally, one may understand that a multimap
can be built by using the generating multimaps in
two ways different thanks to a finite sequence of
steps connecting them such that each step is re-
lated to the next one by replacing an elementary
sub-simplex of one side (either left or right) of a
specified elementary relation or a specified operad
associativity/unity/equivariance axiom involving
only the generating multimaps with the elemen-
tary sub-simplex of the other side.
3 Results and proofs
In this section we will present and prove our re-
sults related the finite presentations of an operad
and its associate algebra. Firstly let us recall
what that means. In all the remainder of this
paper, let (O,1,) be an S-colored operad and
(A, µ) the associated O-algebra.
Definition 3.1. We say that O(respectively O-
algebra A) has a finite presentation if O(respec-
tively O-algebra A) satisfies the two following as-
sertions :
1. O(respectively O-algebra A) has a finite gen-
erating set,
2. any two simplices in O(respectively O-
algebra A) that are presentation of the same
multimap (respectively structure map) are
connected by a finite sequence of elementary
equivalences.
Our first result states the following :
Theorem 3.1. If the operad Ohas a finite gen-
erating set, then the associated O-algebra A, has
a corresponding finite generating set.
Proof. Let T={ψ1, . . . , ψd}be a finite generat-
ing set for Owhere dN.Then every multimap
ψin Ohas a presentation in Tof the form
ψ=ψl1i1· · · ik1ψlk,
where lr, k Nfor all integers 1 rk,
and ψl1, . . . , ψlkin T(note that some of the ψlr
may be repeated). It follows that there exists
al-simplex (ψl1, . . . , ψlk) in O(especially in T)
whose composition is ψ. Then the structure map
µψin O-algebra Aassociated to the multimap
ψin Ois µψ=µψl1i1···◦ik1ψlk, applying the
associativity axiom of the O-algebra A, we get
µψ=µψl1i1· · · ik1µψlk.Then µψhas a pre-
sentation in the set Tµ={µψ1, . . . , µψd}. Since ψ
is an arbitrary element in O, then this is true for
all ψin O, so each structure map µψin Ahas a
presentation in Tµ, then Tµis a finite generating
set for A.
Definition 3.2. The structure maps of Tµare
called generating structure maps.
Lemma 3.1. Let n2, and ψ1, . . . , ψnbe some
multimaps in O. If (ψ1, . . . , ψn)is a n-simplex
in O, then its corresponding n-simplex in Ais
(µψ1, . . . , µψn).
Proof. We will lead an induction proof. For
n= 1, a 1-simplex ψin Ois a generating mul-
timap, and its composition is itself |ψ|=ψ, since
ψis a generating multimap in O, then by the
previous theorem, its associated structure maps
µψin Ais a generating structure map, hence
the corresponding 1-simplex of ψin Ais the 1-
simplex µψ, and its composition is defined as itself
|µψ|=µ|ψ|=µψ, in other words, one can define
the 1-simplices in Aas the generating structure
maps.
For n= 2, a 2-simplex is an iterated operadic
composition in Oof the form ψ= (ψ1, i, ψ2)
for some integer i1, and its composition is
|ψ|=ψ1iψ2, consider ψ1 O b
a1, . . . , an, and
ψ2 O ai
c1, . . . , cm, are two generating mul-
timaps in O, then by the operadic composition
idefined by O, we can assert that ψ1iψ2
Ob
aic, then its associated structure map is
defined by
µψ=µψ1iψ2:=
i1
Y
k=1
Aai×
m
Y
j=1
Acj×
n
Y
k=i+1
Aai
µψ
Ab
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Follows, [1], the associativity axiom in Astates
that
µψ=µψ1iψ2=µψ1iµψ2
where µψ1and µψ2are generating structures maps
in A(1-simplices) corresponding to the generat-
ing multimaps (1-simplices) ψ1and ψ2respec-
tively in O. Hence, the corresponding 2-simplex
of ψin Ais µψ= (µψ1, i, µψ2) for some integer
i1, and its composition is defined in Aas
|µψ|=µ|ψ|=µψ1iψ2=µψ1iµψ2
Then the statement holds for n= 2.
Assume that the statement holds for any given
integer p, q n, and let ψ= (ψ1, . . . , ψn+1) be a
(n+ 1)-simplex, then ψis an iterated operadic
composition in Oof the form ψ= (ϕ, i, φ) for
some integer i1, where ϕis a p-simplex for
some integer p1, and φis a q-simplex for some
integer q1 such that p+q=n+ 1, with-
out loss of generality we can suppose that ϕ=
(ψ1, . . . , ψr) and φ= (ψr+1, . . . , ψn+1) then by in-
duction on n, the corresponding p-simplex of ϕin
Ais µϕ= (µψ1, . . . , µψr), its composition |µϕ|=
µ|ϕ|=µψ1i1· · · ir1µψr, and the corresponding
q-simplex of φin Ais µφ= (µψr+1 , . . . , µψn+1 ), its
composition |µφ|=µ|φ|=µψr+1 ir+1 · · ·inµψn+1 ,
by definition of the (n+1)-simplex ψ, the next op-
eradic composition |ψ|=|ϕ| i|φ|is well defined
in O, then µ|ψ|=µ|ϕ|◦i|φ|, and by the associativ-
ity axiom in A, we get
|µψ|=µ|ψ|=µ|ϕ|◦i|φ|=µ|ϕ|i1µ|φ|
Hence the n+ 1-simplex in Acorresponding the
n+ 1-simplex ψ= (ψ1, . . . , ψn+1) in Ois µψ=
(µψ1, . . . , µψn+1 ).
Then the statement holds for n+ 1.
Corollary 3.1. Let b
ψbe a sub-simplex of the
n-simplex ψin O, then the corresponding sub-
simplex of b
ψin Ais µb
ψ.
Proof. Given a n-simplex ψin Ofor an integer
n1, then its corresponding n-simplex in Ais
µψ. Once again we will lead an induction proof ;
for n= 1, ψis a 1-simplex, then ψis a generating
multimap, and a sub-simplex of ψis defined to be
itself b
ψ=ψ, then the corresponding sub-simplex
of b
ψ=ψin Ais µb
ψ=µψthat is a generat-
ing structure map. Then the statement holds for
n= 1.
Suppose that the statement holds for any integers
p, q 1, and ψis a n+ 1-simplex for an integer
n1, then according to the definition of a sim-
plex ψcan be written as the form ψ= (ϕ, i, φ)
for some integer i1, with ϕis p-simplex and
φis q-simplex such that p+q=n+ 1, and the
operadic composition in O,|ψ|=|ϕ|i|φ|, then a
sub-simplex b
ψof ψis defined to be a sub-simplex
of either ϕ, or of φ, or ψitself, hence, if b
ψis
a sub-simple of either ϕ, or of φ, by induction
on n, the corresponding sub-simplex of b
ψin A
is µb
ψwhich is a sub-simplex of either µϕ, or of
µφ, otherwise, if b
ψis defined to be ψitself, then
the corresponding sub-simplex of b
ψ=ψin A,
is the corresponding simplex of ψin Awhich is
µb
ψ=µψ.
Then the statement holds for n+ 1.
Corollary 3.2. Let ψand ϕbe two simplices in
O, then ψand ϕare equivalent in Oif and only
if their associated simplices µψand µϕare equiv-
alent in A. More presicely
|ψ|=|ϕ|⇔|µψ|=|µϕ|
Proof. Suppose ψ= (ψ1, . . . , ψr) and ϕ=
(ϕ1, . . . , ϕs) are two simplices in Ofor some inte-
gers r, s 1 such that |ψ|=|ϕ|.
Then ther exist i1,...ir1, j1, . . . , js1Nsuch
that |ψ|=ψ1i1· · · ir1ψr, and |ϕ|=ϕ1j1
· · · js1ϕs, since the corresponding simplex of
ψin Ais µψ= (µψ1, . . . , µψr) with composition
|µψ|=µ|ψ|=µψ1i1· · · ir1µψr, and the corre-
sponding simplex of ϕin Ais µϕ= (µϕ1, . . . , µϕs)
with composition |µϕ|=µ|ϕ|=µϕ1j1· · ·js1µϕs,
then the relation |ψ|=|ϕ|implies
|µψ|=µ|ψ|=µψ1i1···◦ir1µψr=µϕ1j1···◦js1µϕs=µ|ϕ|=|µϕ|
Conversely, we know that the construction of a
simplex in Arequires the existence of a simplex
in O. Let ψand ϕbe two simplices in Oand
their associated simplices respectively µψand µϕ
are equivalent in A, i.e |µψ|=µ|ψ|=µ|ϕ|=
|µϕ|, since each structure map has one entry in
O, let it be for example Oa
b1, . . . , bmwith
(a, b) S × P rof (S) for some mN, then
|ψ|,|ϕ| O a
b1, . . . , bm, therefore they have the
same structure map, hence |ψ|=|ϕ|, so ψand ϕ
are two simplices equivalent in O. This finishes
the proof.
Our second lemma corresponding to the k-
moves states that
Lemma 3.2. Given a n-simplex ψin Owith ψ=
(ψ1, . . . , ψn), for any k < n, and any ϕ Wk
ψ,
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one have
µϕ Wk
µψ
in other words, if ψand ϕare equivalent by a
relaxed k-moves in O, then µψand µϕare equiv-
alent by a relaxed k-moves in O-Algebra A.
In fact
ϕ Wk
ψµϕ Wk
µψ
Proof. Let ϕ Wk
ψ, then there exist 1 k, k
k , 1snk, and (nk+k”)-simplex ϕ
with
1. ψj=ϕjfor all 1 js1,
2. ψj=ϕjk+kfor all s+kjn,
3. ζ= (ψs, . . . , ψs+k1) is a sub-simplex of ψ,
and ξ= (ϕs, . . . , ϕs+k1) is a sub-simplex
of ϕsuch that |ζ|=|ξ|, which is compatible
with the operadic composition iof ψs+k=
ϕs+k.
We conclude by the Lemma 3.1 and the Corollary
3.2
1. µψj=µϕjfor all 1 js1,
2. µψj=µϕjk+kfor all s+kjn,
3. µζ= (µψs, . . . , µψs+k1) is a sub-simplex of
µψ, and µξ=µϕs, . . . , µϕs+k1is a sub-
simplex of µϕsuch that µ|ζ|=µ|ξ|, which is
compatible with the operadic composition i
of µψs+k=µϕs+k.
Then µψand µϕare equivalent by a relaxed k-
moves in O-Algebra A.
As a direct consequence, now we can announce
the following :
Theorem 3.2. Under the same hypotheses of
Definition 2.6, consider ζand ξtwo simplices in
Osuch that |ζ|=|ξ|is an elementary relation in
O, then its corresponding elementary relation in
Ais µ|ζ|=µ|ξ|.
Proof. Let |ζ|=|ξ|be an elementary relation
in O, then ζand ξare two simplices that are
equivalent in O, by the Corollary 3.2, their cor-
responding simplices in Aare equivalent, hence
|µζ|=µ|ζ|=µ|ξ|=|µξ|, and the previous Lemma
3.2 provides that this relation is an elementary
relation in Awhich is the corresponding of the
elementary relation |ζ|=|ξ|in O.
Remarks
For the operad WD (resp. UWD) , we
know from the finite presentation theorem
in Chapter 5, in [1] (resp. in Chapter
10, in [1]) that one may substitute a sub-
simplex within a simplex presentation by an-
other, only by allowing substitution of an el-
ementary sub-simplex of one side of an el-
ementary relation or an operad associativ-
ity/unity/equivariance axiom involving only
generating wiring diagrams by the elemen-
tary sub-simplex of the other side,
in theorems 3.2, we saw that each elementary
relation in Ohas a corresponding elementary
relation in A. Now we will prove the cor-
responding associativity/unity/equivariance
axiom for generating multimaps in A.
Proposition 3.1. The associativity axiom holds
in A(for the definition see 2.11 and 2.12 in [1]).
Proof. For some integers n2, m, l 1, and
1i<jnwhere |c|=n,|b|=m, and |a|=l.
Let f O d
c,g O ci
a, and h O cj
b, be
some generating multimaps in O, then the hori-
zontal associativity in Ostates that
(fjh)ig= (fig)j1+lh
the corresponding equality in Aof this equality
is given by
µ(fjh)ig=µ(fig)j1+lh
by the associativity axiom in A, we obtain
(µfjµh)iµg= (µfiµg)j1+lµh
Since f, g and hare generating multimaps in O,
then µf,µg, and µhare generating structure
maps in Acorresponding respectively to f, g and
h. Hence the last equality is the corresponding
associativity of the horizontal associativity in A.
Suppose now n, m 1, 1 in, and 1
jm.
Let f O d
c,g O ci
b, and h O bj
a,
are some generating multimaps in O, then the
vertical associativity in Ostates that
fi(gjh)=(fig)i1+jh
the corresponding equality in Aof this equality
is given by
µfi(gjh)=µ(fig)i1+jh
by the associativity axiom in A, we have
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µfi(µgjµh)=(µfiµg)i1+jµh
where µf,µg, and µhare generating structure
maps in A, corresponding respectively to the gen-
erating multimaps f, g and hin O. Then the last
equality is the corresponding associativity of the
vertical associativity in A.
Remark: By the operad associativity in O, we
mean both the horizontal and the vertical asso-
ciativity, and by the O-operad associativity in A,
we mean their corresponding in A.
Proposition 3.2. The unity axiom holds in A
(for the definition see 2.13 and 2.14 in [1]).
Proof. Let f O d
cbe a generating multimap,
1d O d
dand 1dthe d-colored unit in O, and
1ci O ci
cithe ci-colored unit in O.
The left unity in Ostates 1d1f=f. Then,
the corresponding equality in Aof this equality
is given by
µ1d1f=µf
by associtivity axiom in A, we get
µ1d1µf=µf
On the other hand, the right unity in Ostates
that
fi1ci=f.
the corresponding equality in Aof this equality
is given by
µfi1ci=µf
Once again, the associtivity axiom in A, assert
µfiµ1ci=µf
where µfis a generating structure map corre-
sponding to the generating multimap fin O, and
µ1ci,µ1dare the identity maps in Acorrespond-
ing respectively to the ci-colored and d-colored
unit in O. Then the corresponding unity axiom
in Aholds.
Proposition 3.3. The equivariance axiom holds
in A(for the definition see 2.15 in [1]).
Proof. For some integers n, m 1 and 1 in
where |c|=n,|b|=m,σSn, and τSm.
Let f O d
c, and g O cσ(i)
b, be generating
multimaps in O, then the equivariance axiom in
Ostates
fσigτ= (fσ(i)g)σiτ
the corresponding equality in Aof this equality
is given by
µfσigτ=µ(fσ(i)g)σiτ
by the associativity axiom in A, we obtain
µfσiµgτ=µ(fσ(i)g)σiτ
where fσ O d
,gτ O cσ(i)
and (fσ(i)
g)σiτ O d
(cσ(i)b)(σiτ).
Since f, g are generating multimap in O, then fσ,
gτare too, hence µfσ,µgτare generating struc-
ture maps in Acorresponding respectively to the
generating multimaps fσ,gτin O.
Then the last equality is the equivariance axiom
in Acorresponding to the equivariance axiom in
O.
Vocabulary.
Let Obe an operad equipped with a finite gener-
ating set T, and Athe O-algebra equipped with
the corresponding finite generating set Tµ.
every structure map in Ahas a presentation
in Tµ, then there exists a simplex in Tµwhich
is presentation of this structure map. The
equality relation defined in the Theorem 3.1
|µζ|=µ|ζ|=µ|ξ|=|µξ|
is either an O-operad associativity or unity
or an equivariance axiom, or an elementary
relation in A,
an elementary sub-simplex µb
ψof µψis a sub-
simplex of one of two following forms:
µb
ψis one side (either left or right) of a
specified elementary relation in A,
µˆ
ψis one side (either left or right) of a
specified O-operad associativity or unity
or equivariance axiom involving only the
generating sturture maps.
Suppose that we have a n-simplex µψ
(for some integer n2) in Awhich is
a presentation of the structure map |µψ|
in A, and µζis a sub-simplex of µψsuch
that |µζ|=|µξ|, where µξis a simplex
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in A, then the relation |µζ|=|µξ|is ei-
ther an elementary relation in Aor an O-
operad associativity or unity or equivari-
ance axiom involving only the generat-
ing structur maps, hence, one can obtain
a relaxed k-moves of the simplex µψby
substituting the elementary sub-simplex
µζby the other one µξ,
two simplicies µψand µϕare called to be el-
ementarily equivalent in A, if µψand µϕare
equivalent by a relaxed k-moves (for some
integer k2), then we write µψ
k
µϕ(if
there is no confusion, we can drop kand write
µψµϕ) and call this an elementary equiv-
alence in A, in other words an elementary
equivalence is a subsitution of a elementary
sub-simplex of one side by the other one.
two simplicies µψand µϕare said to be
connected by a finite sequence of elementary
equivalences in Aif and only if there exist
some simplicies µψ1, . . . , µψrin Asuch that
µψ1
k1
. . . kr1
µψr, and µψ
k
µψ1
k1
. . . kr1
µψr
kr
µϕfor some integers k, k1, . . . , kr2.
Denotations. Let Obe an operad with a finite
generating set Tand Aits associated O-algebra
with the corresponding finite generating set Tµ.
Let ψbe an n-simplex in Oand µψits corre-
sponding n-simplex in A.
The set of all relaxed k-moves of µψin Tµis
denoted by Wk
µψ,
The set of all relaxed k-moves for all k
{2, . . . , n 1}is
Wn
µψ:=
n1
[
k=2
Wk
µψ,
and this is the set of all relaxed n-moves of
µψin Tµ. In other words, Wn
µψis the set of
all elementary equvalences of µψin A.
The set of all relaxed n-moves in Tµis de-
noted by Wµ, where
Wµ:= [
µψ∈A
Wn
µψ
In other words, Wµis the set of all elementary
equivalences in Tµ.
Lemma 3.3. Let ψand ϕbe two simplices ele-
mentarily equivalent in O, then their correspond-
ing simplices µψand µϕare elementarily equiva-
lent in A. In other words
ψϕµψµϕ
Proof. Let ψand ϕbe two simplices elementarily
equivalent in O, then ψand ϕare equivalent by
a relaxed k-moves, then ϕ Wk
ψ, by the Lemma
3.2, we get µϕ Wk
µψ, where µψand µϕare the
corresponding simplices of ψand ϕrespectively in
A, in other words, µψand µϕare equivalent by a
relaxed k-moves in A, then they are elementarily
equivalent in A.
Theorem 3.3. Let ψand ϕbe two simplices con-
nected by a finite sequence of elementary equiva-
lences in O, then their corresponding simplices
µψand µϕare connected by a finite sequence
of elementary equivalences in A. More precisely
if ψ1, . . . , ψris a finite sequence of elementary
equivalences in O, for an integer r1such that
ψψ1 · · · ψrϕ
Then
µψµψ1 · · · µψrµϕ
where µψ1, . . . , µψris the corresponding finite se-
quence of elementary equivalences of ψ1, . . . , ψr
in A.
Proof. Let ψand ϕbe two simplices connected
by a finite sequence of elementary equivalences in
O, then there exist simplices ψ1, . . . , ψrsuch that
ψψ1 · · · ψrϕ, since ψψ1, then
the Lemma 3.3 assert that µψµψ1, similraly
µψ1µψ2, . . . , µψrµϕ.
Hence
µψµψ1 · · · µψrµϕ
Lemma 3.4. Let Obe an operad and Aits asso-
ciated algebra, let Tbe a finite generating set for
O, and Tµits corresponding finite generating set
of A, if Wthe set of all elementary equivalences
in Tis a strong generating set of Oin T, then
Wµthe set of all elementary equivalences in Tµis
a strong generating set of Ain Tµ.
Proof. Let µψ= (µψ1, . . . , µψr) and µϕ=
(µϕ1, . . . , µϕs) be two simplices in Tµfor some
integers r, s 1 that are equivalent, then their
composition are equal in A, i.e |µψ|=|µϕ|,
the Corollary 3.2 assert that the two simplices
ψ= (ψ1, . . . , ψr) and ϕ= (ϕ1, . . . , ϕs) are equiva-
lent in O, i.e |ψ|=|ϕ|, since Wis a strong gener-
ating set of Oin T, then ψand ϕare connected
by a finite sequence of elementary equivalences in
W, then there exist φ1, . . . , φlfor an integer l1
such that ψφ1 · · · φlϕ, by the previous
Lemma 3.3, we get µψµφ1 · · · µφlµϕ,
where µφ1, . . . , µφlis a finite sequence of ele-
mentary equivalences in Wµ. This finishes the
proof.
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As we have collected all necessary tools, we can
now formulate and prove our following main the-
orem :
Theorem 3.4. Suppose that Ohas a finite pre-
sentation, then Ahas a corresponding finite pre-
sentation one.
Proof. Firstly, we have to prove that every struc-
ture map can be expressed as a finite iter-
ated operadic composition in terms of generating
structue maps in A.
Indeed, let µψbe a simplex in Afor a fixed
simplex ψin Owhose composition is µ|ψ|, let
T={ψ1, . . . , ψd}be a finite generating set for
Owhere dN, then there exist ψ1, . . . , ψl T
for lNsucht that ψ= (ψ1, . . . , ψl) and
|ψ|=ψ1i1· · ·◦il1ψlfo some integers ı1, . . . , il11
By Theorem 3.1, the corresponding finite gen-
erating set of Tin Ais Tµ={µψ1, . . . , µψd},
and by Lemma 3.1 the corresponding l-simplex
of (ψ1, . . . , ψl) in Ais (µψ1, . . . , µψl) whose com-
position is given by
|µψ|=µ|ψ|=µψ1i1···◦il1ψl=µψ1i1· · · il1µψl
Since this is true for every structure map in A,
then every structure map can be expressed as a
finite iterated operadic composition in terms of
generating structue maps in Tµwhich is a finite
generating set of A.
Secondly, it remains to prove that if a struc-
ture map can be operadically generated by the
generating structure maps in two different ways,
then there exists a finite sequence of elementary
equivalences in Wµfrom the first iterated op-
eradic composition to the other one.
Let µ|φ|be a structure map in A, for a fixed |φ|
in Owhich is generated by the generating struc-
ture maps in two different ways, then there exist
two simplices in O,ψ= (ψ1, . . . , ψr) in which the
composition is |ψ|and ϕ= (ϕ1, . . . , ϕs) in which
the composition is |ϕ|for some integers r, s 1
such that
µ|φ|=µ|ψ|=µ|ϕ|
By the corollary 3.2, we get |ψ|=|ϕ|, then ψ
and ϕare equivalent in T, since Wis a strong
generating set for Oin T, then there exist a finite
sequence of elementary equivalences φ1, . . . , φm
in W, such that ψφ1 · · · φmϕfor
some integer m1,the Theorem 3.3 assert that
µψand µϕare connected by a finite sequence of
elementary equivalences in Wµ
µψµφ1 · · · µφmµϕ
By the Lemma 3.4, Wµis a strong generating set
of Ain Tµ, hence µψand µϕare connected by
finite sequence of elementary equivalences in Wµ.
This fineshes the proof
Our approach’s advantage that it allow us
to get a finite presentation of the O-algebra
Adirectly out of the finite presentation of the
operad O.
Unfortunately, we wanted to prove that any
multimap (resp. structure map) in the Ooperad
with a finite generating set has a stratified pre-
sentation which is a simplex presentation where
the same generating multimaps within the sim-
plex must appear in a consecutive serie, for ex-
ample, suppose Oan operad with the finite gen-
erating set T= (ψ1, ψ2, ψ3), consider the follow-
ing 9-simplex (ψ1, ψ2, ψ3, ψ1, ψ3, ψ2, ψ3, ψ1, ψ3)
then the stratified 9-simplex is given by
(ψ1, ψ1, ψ1, ψ2, ψ2, ψ3, ψ3, ψ3, ψ3). D.Yau had
proved that every wiring diagram in WD (resp.
undirected wiring diagram in UWD) has a strat-
ified presentation (see Theorem 5.11 and 10.12 in
[1]), but we couldn’t prove that for a such simplex
in O.
4 Applications
As an application of our main theorem, we will
consider the operad of wiring diagrams, denoted
WD, and that of undirected wiring diagrams, de-
noted UWD. We suppose here that the reader is
familiar with the basic tools, vocabulary of the
operad of wiring diagrams (directed or not) and
its structure. If not, we recommend, [1]. Let
us recall that a multimap in WD (respectively
in UWD) is called a wiring diagram (respec-
tively undirected wiring diagram), and a gener-
ating multimap in WD (respectively in UWD) is
called a generating wiring diagram (respectively
a generating undirected wiring diagram). In fact,
D. Yau has especially proved that both WD and
UWD have a finite presentation (Theorem 5.22 in
[1], for WD), (Theorem 10.19 in [1], for UWD).
In the chapter 3 in [1] D. Yau described the
set
TWD ={ϵ, δ, τ, θ, λ, σ, σ, ω}
of 8 wiring diagrams which is a finite generating
set for the operad WD. In the chapter 8 in [1] he
had described the set
TUWD =nϵ, ω, τf, θ(X,Y ), λ(X,x±), σ(X,x1,x2)o
of 6 undirected wiring diagrams which is a finite
generating set for the operad UWD. Then ev-
ery wiring diagram (resp. undirected wiring dia-
gram) has a presentation in TWD (resp. TUWD)
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as a finite iterated operadic composition. That is
the first assumption of our theorem.
For the wirings diagrams, in the chapter 3 in
[1] D. Yau described 28 elementary relations in
TWD, and in the chapter 5 in [1] he had proved
that any two equivalent simplices in WD are ei-
ther equal or are connected by a finite sequence
of elementary equivalences where each elemen-
tary equivalence is induced by either one of the
28 elementary relations or an operad associativ-
ity/unity/equivariance axiom for the generating
wiring diagrams. Following our denotations, the
set WWD of all elementary equivalences in TWD
is a strong generating set of WD. That is the
second assumption of our theorem.
Hence, by our main theorem 3.4, the WD-algebra
has a corresponding finite presentation.
By using our approach in Theorem 3.1, the cor-
reseponding finite generating set for the WD-
algebra is given by
TWD
µ={µϵ, µδ, µτ, µθ, µλ, µσ, µσ, µω}.
which elements are called the generating struc-
ture maps corresponding to the 8 generating
wiring diagrams. Then every structure map can
be obtained from finitely many generating struc-
ture maps via some iterated operadic composi-
tions. These generating structure maps are ex-
actly those defined by D. Yau (see definition 6.9
in [1]). For example the first generating wiring
diagram in WD is the empty wiring diagram
ϵ WD (see Definition 3.1 in [1]), then
its corresponding generating structure map in the
WD-algebra is defined to be µϵ: A(see
Definition 6.9 in [1]).
In other hand, by applying Theorem 3.2 to
the operad WD, we find that every elementary
relation in WD has a corresponding elementary
relations in the WD-algebra. Then every one
of the 28 elementary relations in WD (see def-
inition 3.43 in [1]) has a corresponding elemen-
tary relation in the associated WD-algebra that
are exactly the generating axioms defined by D.
Yau (see definition 6.9 in [1]). For example,
the first elementary relation in WD (see propo-
sition 3.15 in [1]) says that if τb,a WD a
b
and τc,b WD b
care two consecutive name
changes, then they can be composed into one
name change τc,a WD a
c, i.e
τb,a τc,b =τc,a
By using our Theorem 3.2, its corresponding ele-
mentary relation in WD is given by
µτb,a µτc,b =µτc,a
where µτx,y := Ax Ay.
This last equality is exactly the first generating
axiom in WD-algebra defined by D.Yau (see def-
inition 6.9 in [1]). The corresponding operad as-
sociativity, unity and equivariance axiom can be
obtained immediately from the propositions 3.1,
3.2 and 3.3.
In [1] D.Yau had proved that (Theorem 5.22)
any two equivalent simplices in WD are either
equal or are connected by a finite sequence of ele-
mentary equivalences in WD which each elemen-
tary equivalence is induced by either one of the
28 elementary equivalences or an operad associa-
tivity/unity/equivariance axiom for the generat-
ing wiring diagrams in WD, hence, by our The-
orem 3.3 any two equivalent simplices in WD-
algebra are either equal or are connected by a fi-
nite sequence of elementary equivalences in WD-
algebra, which each elementary equivalence in
WD-algebra is induced by either one of the 28
generating axioms or an WD-algebra operad as-
sociativity/unity/equivariance axiom for the gen-
erating structures maps. Following our denota-
tions, the set WWD
µof all elementary equivalences
in TWD
µis a strong generating set of WD-algebra.
Then, WD-algebra has a finite presentation.
The same can be done for the operad UWD,
of undirected wiring diagrams by considering its
finite generating set
T=nϵ, ω, τf, θ(X,Y ), λ(X,x±), σ(X,x1,x2)o,
whose corresponding finite generating set for the
WD-algebra is
Tµ=nµϵ, µω, µτf, µθ(X,Y ), µλ(X,x±), µσ(X,x1,x2)o.
and the elementary relations in UWD is given by
D. Yau (see definition 8.26 in [1] ), and their cor-
responding elementary relations in UWD-algebra
that are called by D. Yau generating axioms (see
definition 11.1 in [1]).
For more application, the reader can see the op-
erad of normal wiring diagrams and strict wiring
diagrams and their algebras.
5 Future Work
As an extension of our study, we will try to in-
vestigate our result and discribe the operad with
two inputs and one output, a such operad is of
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the form OZ
X Y , where X, Y, Z S.
Let ψbe a multimap in OZ
X Y , by the i-
composition in OZ
X Y , we can decompose ψ
as follows :
OZ
I× O I
I I× O I
X× O I
Y
(1;Id;Id)
O Z
I I× O I
X× O I
Y
(1;Id)
O Z
X I× O I
Y2
O C
X Y
Here, Iis a specific element in S.
For a specific elements X, Y and Zin S, we will
try to find a finite generating set Tfor this op-
erad.
By putting
ψZ O Z
I
ψI O I
I I
ψX O I
X
We obtain
ψ= ((ψZ1ψI)1ψX)2ψY
By the associativity axiom in O, we get also
ψ= ((ψZ1ψI)2ψY)1ψX
ψ=ψZ1((ψI1ψX)2ψY)
ψ=ψZ1((ψI2ψY)1ψX)
ψ= (ψZ1(ψI1ψX)) 2ψY
ψ= (ψZ1(ψI2ψY)) 1ψX
These equalities give all the presentation possible
of ψ, then there is 6 simplices, in fact, six
4-simplices that can be a presentation of ψ.
from these equalities, we check the following
elementary relations in OZ
X Y :
(ψZ1ψI)1ψX=ψZ1(ψI1ψX)
(ψZ1ψI)2ψY=ψZ1(ψI2ψY)
(ψI1ψX)2ψY= (ψI2ψY)1ψX
The six 4-simplices are :
ψ1= (((ψZ,1, ψI),1, ψX),2, ψY)
ψ2= (((ψZ,1, ψI),2, ψY),1, ψX)
ψ3= (ψZ,1,((ψI,1, ψX),2, ψY))
ψ4= (ψZ,1,((ψI,2, ψY),1, ψX))
ψ5= ((ψZ,1,(ψI,1, ψX)),2, ψY)
ψ6= ((ψZ,1,(ψI,2, ψY)),1, ψX)
References:
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[7] Rupel, D., Spivak, D.I., The operad of tem-
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[10] Yau, D., and Johnson, M.W., A Foundation
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Volume 22, 2023
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Ettaki Ayoub, Elomary Mohamed Abdou,
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E-ISSN: 2224-2678
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Volume 22, 2023