Next Article in Journal
Fractional Order Complexity Model of the Diffusion Signal Decay in MRI
Previous Article in Journal
Generalized Nonsmooth Exponential-Type Vector Variational-Like Inequalities and Nonsmooth Vector Optimization Problems in Asplund Spaces
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Structure of Normed Simple Annihilator Algebras

by
Sergey V. Ludkowski
Department of Appl. Mathematics, Moscow State Techn. Univ. MIREA, av. Vernadksy 78, Moscow 119454, Russia
Mathematics 2019, 7(4), 347; https://doi.org/10.3390/math7040347
Submission received: 18 February 2019 / Revised: 29 March 2019 / Accepted: 2 April 2019 / Published: 11 April 2019

Abstract

:
This article is devoted to normed simple annihilator algebras. Their structure is investigated in the paper. Maximal families of orthogonal irreducible idempotents of normed simple annihilator algebras are scrutinized. Division subalgebras of annihilator algebras are studied. Realizations of these algebras by operator algebras in Banach spaces are described. For this purpose, quasi finite dimensional operators are investigated.
MSC:
12J05; 16D60; 16D80; 46B28; 46H20

1. Introduction

Algebras and operator algebras over the real field R and the complex field C have found many-sided applications [1,2,3,4]. They compose a large area of mathematics (see, for example, [2,5,6] and references therein). In particular, annihilator algebras play very important roles in structure theory of algebras, decompositions of representations of algebras or groups into irreducible representations, etc. [4,7]. Nevertheless for such algebras over other normed fields little is known. This is caused by their specific features and additional difficulties arising from structure of fields [8,9,10,11,12,13,14,15].
A lot of results in the classical case use the fact that the real field R has the linear ordering compatible with its additive and multiplicative structure and that the complex field C is algebraically closed, norm-complete, locally compact, and is the quadratic extension of R . Besides them there are no other commutative fields with Archimedean multiplicative norms which are complete relative to their norms. However, there are many other normed fields apart from R and C .
It is worth mentioning that the algebraic closure of the field Q p of p-adic numbers is not locally compact. In this paper on algebras X over fields F norms | · | are considered which satisfy the strong triangle inequality | x + y | max ( | x | , | y | ) for each x and y in X. Norms fulfilling the latter condition are also called non-Archimedean norms or ultranorms. Notice that there is not any ordering on an infinite field such as Q p , C p or F p ( t ) compatible with its norm and algebraic structure.
On the other hand, there are fast developing non-Archimedean analysis, functional analysis and representations theory of groups over non-Archimedean fields [14,16,17,18,19,20,21]. This is stimulated not only by mathematical problems, but also their applications in other sciences such as physics, quantum mechanics, quantum field theory, informatics, etc. (see, for example, [22,23,24,25,26,27,28,29] and references therein).
This article is devoted to normed annihilator algebras over non-Archimedean fields. A structure of simple annihilator algebras is studied in the paper. Necessary Notation 1 and Definitions 1–6 are given. Idempotents of algebras and their orthogonality are investigated in Proposition 1. Extensions of algebras are studied in Proposition 2, Theorem 1, and Corollary 1. Maximal families of orthogonal irreducible idempotents of normed simple annihilator algebras are scrutinized. Division subalgebras associated with idempotents are investigated in Theorems 2 and 3. Relations with operator theory and realizations of these algebras by operator algebras are outlined. For this purpose, quasi-finite dimensional operators are studied.
All main results of this paper are quite new and their applications are discussed in the conclusion section.

2. Normed Annihilator Algebras

To avoid misunderstandings, we first give Definitions and one Notation. Though they follow main lines of that of in [4,7,11,14,30,31], but they also contain some specific ultranormed features. A reader familiar with these sources or the article [32] may skip Notation 1 and Definitions 1–6.
Notation 1.
Assume that F is an infinite field supplied with a multiplicative non-trivial ultranorm | · | F . Assume also that F is non-discrete and Γ F ( 0 , ) = { r R : 0 < r < } , where Γ F : = { | x | F : x F { 0 } } . Henceforward, fields with multiplicative ultranorms are considered, if something other will not be specified.
Let E n ( F ) denote the class containing F and all ultranormed field extensions G of F so that these G are norm-complete and | b | G = | b | F for each b in a given field F. Let also E n denote the class of all infinite non-trivially ultranormed fields F which are norm-complete.
Henceforth, a commutative field is called shortly a field, while a noncommutative field is called a skew field or a division algebra.
Definition 1.
Suppose that c 0 ( α , F ) is a Banach space consisting of all vectors x = ( x j : j α x j F ) subjected to the condition
  • c a r d { j α : | x j | > ϵ } < N 0 for each ϵ > 0
and supplied with the norm
(1) 
| x | = sup j α | x j | ,
where α is a set. For locally convex spaces X and Y over F the family of all linear continuous operators B : X Y will be denoted by L ( X , Y ) . Particularly, for normed spaces X and Y the linear space L ( X , Y ) is also normed
(2) 
| B | : = sup x X { 0 } | B x | / | x | .
For locally convex spaces X and Y over F the space L ( X , Y ) is topologized by a family of semi-norms
(3) 
| B | p , q : = sup x X , p ( x ) > 0 q ( B x ) / p ( x )
for all continuous semi-norms p on X and q on Y.
Speaking about Banach spaces and Banach algebras we stress that a field over which it is defined is ultranorm complete.
Assume that A is an algebra over F, where F E n . It is supposed that an ultranorm
  • | · | A on A satisfies the conditions:
  • | a | A ( Γ F { 0 } ) for each a A , also
  • | a | A = 0 if and only if a = 0 in A,
  • | t a | A = | t | F | a | A for each a A and t F ,
  • | a + b | A max ( | a | A , | b | A ) and
  • | a b | A | a | A | b | A for each a and b in A.
Frequently it is shortly written | · | instead of | · | F or | · | A .
Definition 2.
Assume that F is an infinite field such that F E n and of the characteristic c h a r ( F ) 2 . Assume also that B 2 = B 2 ( F ) is the commutative associative algebra with one generator i 1 such that i 1 2 = 1 and furnished with the involution ( v i 1 ) = v i 1 for each v F . Suppose that A is a subalgebra in L ( X , X ) such that A is also a two-sided B 2 -module, where X = c 0 ( α , F ) is the Banach space over F, α is a set. Then A is called a -algebra if there is
(1) 
a continuous bijective surjective F-linear operator I : A A such that
(2) 
I ( a b ) = ( I b ) ( I a ) and
(3) 
I ( g a ) = ( I a ) g and I ( a g ) = g ( I a )
(4) 
I I a = a
(5) 
( θ ( y ) ) ( a x ) = ( θ ( ( I a ) y ) ) ( x )
for every a and b in A and g B 2 and x and y in X, where θ : X X is the canonical embedding of X into the topological dual space X such that θ ( y ) x = j α y j x j . For the sake of brevity, we can write a instead of I a . The mapping I is called the involution. An element a A is called self-adjoint if a = a .
Definition 3.
For a topological algebra A over a field F and a subset S of A the left annihilator is defined by L ( A , S ) : = { x A : x S = 0 } and the right annihilator by R ( A , S ) : = { x A : S x = 0 } . Shortly they also will be denoted by A l ( S ) : = L ( A , S ) and A r ( S ) : = R ( A , S ) correspondingly.
Definition 4.
An algebra A is called an annihilator algebra if it satisfies conditions (1–3):
(1) 
A l ( A ) = A r ( A ) = 0 and
(2) 
A l ( J r ) 0 and
(3) 
A r ( J l ) 0
for all closed right J r and left J l ideals in A.
Definition 5.
Suppose that w 1 and w 2 are idempotents of an algebra A fulfilling the conditions w 1 w 2 = 0 and w 2 w 1 = 0 . Then they are called orthogonal. A family { w j : j } of idempotents is called orthogonal, if and only if every two distinct of them are orthogonal. It is said that an idempotent p of the algebra A is irreducible, if it cannot be written as the sum of two mutually orthogonal idempotents.
Definition 6.
Let A and B be two Banach algebras over an ultranormed field F, F E n . Let A ^ F B be the completion relative to the projective tensor product topology (see [14,33]) of the tensor product A F B over the field F.
Suppose that B is a Banach algebra over an ultranormed field F, F E n , and x is an element in B. It will be said that x has a left core quasi-inverse y if for each H E n ( F ) an element y B H exists satisfying the equality x + y + y x = 0 , where B H = B ^ F H . Symmetrically a right core quasi-inverse is defined. In particular, if only the field H = F is considered they are called a left quasi-inverse and a right quasi-inverse correspondingly.
Assume that A is a unital Banach algebra over F, where F E n . Suppose also that an element x A has the property: for each field extension G E n ( F ) the left inverse ( 1 + y x ) l 1 exists in A G for each y A G . Then we call x a generalized core nil-degree element. The family of all generalized core nil-degree elements of A is called a core radical and it is denoted by R c ( A ) . By R ( A ) a radical of the algebra A is denoted.
Proposition 1.
Suppose that A is a Banach simple unital annihilator algebra over a field F, F E n , also R c ( A ) = R ( A ) . Then a maximal family of orthogonal irreducible idempotents { w j : j J } exists such that j A w j and j w j A are dense in A.
Proof. 
In view of Proposition 8 in [32] there are irreducible idempotents w j in A. Each right ideal B in A contains a minimal right ideal, consequently, it contains an irreducible idempotent. By virtue of Zorn’s lemma (see [34] or [35]) a maximal orthogonal system { w j : j J } of irreducible idempotents w j exists. Let
C = j A w j
be the sum of all such left ideals. Suppose that c l A C A , where c l K P denotes the closure of a subset P in a topological space K. Then c l A C is a closed left ideal. Therefore, A r ( c l A C ) is the right ideal different from zero. This implies that A r ( c l A C ) contains an irreducible idempotent p orthogonal to each w j . But this is impossible, since the family { w j : j J } is maximal. Thus, it remains that C is dense in A. Similarly, the sum j w j A of all such right ideals is dense in A. □
Proposition 2.
Let F be a field and let { K j : j P } be a family of division algebras such that F is contained in the center Z ( K j ) of K j for each j P , where P is a set. Then a minimal division algebra K exists such that K j K for each j P .
Proof. 
Since K j is a division algebra, then its center Z ( K j ) is a field. We take the tensor product
T = j P K j
of K j as algebras over the field F. Therefore, T is an algebra over F so that T may be noncommutative if at least one of K j is noncommutative. For each K j a natural embedding h j : K j K exists. Moreover, T contains the unit element which can be identified with the unit of the field F.
For each proper left ideal B in T the intersection B j = B h j ( K j ) is a left ideal of K j . In view of Theorem I.9.1 in [7] B j = ( 0 ) , since F T / B and the unit is unique in the associative algebra T / B . Particularly, for a maximal proper left ideal B in T this induces the embedding t h j of K j into the quotient algebra T / B over the field F for each j P , where t : T T / B denotes the quotient F-linear mapping.
Then equations a j x j = b j and y j a j = b j with a j 0 and b j in h j ( K j ) have unique solutions x j and y j in h j ( K j ) for each j P . For an arbitrary a T / B take an element c t 1 ( a ) . Then we deduce that c + B = t 1 ( a ) and consequently, h j ( K j ) t 1 ( a ) = h j ( K j ) { c } , where { c } denotes the singleton in T. At the same time, q u = 0 for some q and u in T implies t ( ( q + B ) ( u + B ) ) = 0 in T / B . Therefore, equations a x = b and y a = b with a 0 and b in T / B have unique solutions x and y in T / B , since B is the proper maximal left ideal in T and h j ( K j ) h i ( K i ) = F for each j i in P. From Theorem 9.2 and Corollary 9.3 in [36] it follows that an embedding of T / B into a unique-division algebra L over F exists. Taking the intersection of all such algebras L one gets a minimal unique-division algebra K over F containing T / B . Thus the embedding of K j into the division algebra K exists for each j P . □
Theorem 1.
If conditions of Proposition 2 are fulfilled and each K j is a Hausdorff topological division algebra with a topology τ j such that
(i) 
τ j | K i K j = τ i | K i K j
for each i and j in P, then a Hausdorff topology τ on K exists such that an embedding h j : K j K is a homeomorphism of ( K j , τ j ) onto ( h j ( K j ) , τ h j ( K j ) ) for each j P . Moreover, if each K j is normed and
(ii) 
| · | K j | K i K j = | · | K i | K i K j
for each i and j in P, where | · | K j denotes a norm on K j , then K is normed.
Proof. 
We consider on the weak product
S = j P K j
the box product topology, where each s S has the form
s = ( s j : j s j K j , c a r d { j : s j e j } < N 0 ) ,
where e j = 1 denotes the unit element in K j . It induces the corresponding topology a p on the tensor product T, where T is the quotient algebra S / M of S by the submodule M with elements of the form
(1)
( x ) + ( y ) ( z ) with x i + y i = z i for one index i P and with x j = y j = z j for each j i in P;
(2)
( x ) ( y ) with x i = b y i for one index i in P and x j = y j for each j i in P for every b F , ( x ) , ( y ) and ( z ) in S (see also Chapter 3 in [7]). The algebra T is supplied with the multiplication prescribed by the rule
( x ) ( y ) = j P x j y j
for each ( x ) and ( y ) in T. Due to condition ( i ) for each i there exists an algebraic topological embedding of K i into T.
The algebra K over F is obtained as the unique-division algebra K over F containing T / B (see the proof of Proposition 2).
The algebra T is unital, since K j is unital for each j. There exists a neighborhood W j of 1 in K j such that the inversion is continuous on W j for each j. We take
W = j P W j ,
hence W is a neighborhood of 1 in T such that the inversion is continuous on W, since S is supplied with the box topology. Therefore, if B is a left maximal ideal in T, then B is closed in T, since algebraic operations on T are continuous and T is with the continuous inverse on W.
Therefore, the box topology a p on T induces the quotient T 1 -topology b p on T / B , since a p is the Hausdorff topology and B is closed in T. Then we consider a base U of a topology τ on K satisfying the conditions:
(3)
U x = U 0 + x for each x K ,
(4)
U x = x U 1 = U 1 x for each nonzero x in K,
(5)
U 0 ( T / B ) is the base of neighborhoods of zero in the b p topology on T / B , where U x denotes a base of neighborhoods of an element x in K such that U x U ;
(6)
for each E and D in U 0 there exists C U 0 such that C E D ;
(7)
V U 0 V = { 0 } ;
(8)
for each E U 0 there exists D U 0 such that ( D + D ) E and ( D + 1 ) 2 ( E + 1 ) ;
(9)
for each E U 0 there exists D U 0 such that D E and ( D + 1 ) 1 ( E + 1 ) ,
(10)
U | F provides the base of the τ j | F topology on F.
It exists, since F K i and condition ( i ) is fulfilled for each i and j in P and since the b p topology on T / B satisfies analogous to (3–10) conditions due to Theorem 1.3.12 in [37].
Each element of K is obtained from elements of T / B by a finite number of algebraic operations. Therefore, the intersection of all such bases U satisfying conditions (3)–(9) provides a minimal base possessing these properties. In view of Theorem 1.3.12 in [37] this induces a Hausdorff topology τ on K.
From the construction above it follows that τ ( T / B ) = b p , consequently, τ h j ( K j ) is equivalent with the topology τ h j ( K j ) on h j ( K j ) inherited from ( T / B , b p ) for each j P , where h j is the algebraic embedding as in Proposition 2. Therefore h j is the homeomorphism of ( K j , τ j ) onto ( h j ( K j ) , τ h j ( K j ) ) for each j P .
In particular, if K j is normed for each j, then T is normed by | x | = sup j | x j | K j , where | h x | = | h | | x | for each h F and x T . Such normed topology is not stronger than the a p topology. By condition ( i i ) of this theorem norms | · | K j and | · | K i on K i K j are equivalent for each i and j in P, hence there exists an algebraic isometric embedding of K i into T for each i. On the other hand, F K i for each i. This induces the quotient norm on T / B relative to which h j is continuous for each j. Therefore, U 0 and U 1 on K can be chosen countable and such that V + V V for each V U 0 , W W W for each W U 1 . Thus, the minimal division algebra K is normable:
| x + y | K max ( | x | K , | y | K ) and
| x y | K | x | K | y | K
for each x and y in K. □
Corollary 1.
If conditions of Theorem 1 are satisfied, then a completion K ˜ of K relative to a left uniformity l τ induced by τ exists such that K ˜ is a division algebra. Moreover, if condition ( i i ) of Theorem 1 is fulfilled, then K ˜ is the Banach division algebra.
Proof. 
Consider on the multiplicative group K of nonzero elements of K the left uniformity l τ induced by τ . In view of §8.1.17 and Theorem 8.3.10 in [34] and conditions ( 3 , 4 ) (see the proof of Theorem 1) the completion K ˜ of K relative to l τ is the unique-division algebra over F.
If in addition Condition ( i i ) of Theorem 1 is fulfilled, then we take K ˜ as the completion of K relative to its norm. □
Theorem 2.
Let A be a simple unital annihilator Banach algebra over a normed field F, F E n , with R c ( A ) = R ( A ) , and let { w j } be a maximal orthogonal system of irreducible idempotents in it. Then a Banach division algebra G exists such that w j A w j G for each irreducible idempotent w j in A, also
i , j w i A w j   i s   d e n s e   i n   A .
Proof. 
Suppose that { w j } is a maximal orthogonal system of irreducible idempotents in the algebra A. For a chosen idempotent w i one gets the two-sided non-nil ideal A w i A . Since A is simple, then c l A ( A w i A ) = A , where c l A S denotes the closure of a subset S in A. Therefore, w j A w i A w j ( 0 ) for each j. Moreover, this implies that w j A w i A w j w j A w j = G j w j , where G j is a division algebra over F according to Theorem 9 in [32].
Consider the algebra A j : = A G j = A ^ F G j obtained from A by extension. For each j elements x j and y j in A j exist such that w j x j w i y j w j = w j . We put w j , i = w j x j w i and w i , j = w i y j w j and w j , k = w j , i w i , k . Therefore, the elements w j , i and w i , j belong to A j and w j , j = w j , since w i 2 = w i . Then we infer that
w j 1 , k 1 w k 1 , k 2 = w j 1 x j 1 w i w i y k 1 w k 1 w k 1 x k 1 w i w i y k 2 w k 2
= w j 1 x j 1 w i ( y k 1 w k 1 x k 1 w i ) y k 2 w k 2 and
w j 1 , k 2 = w j 1 , i w i , k 2 = w j 1 x j 1 w i w i y k 2 w k 2
= w j 1 x j 1 w i y k 2 w k 2 .
Notice that this construction implies that w i , j w j , i w i A w i = G i w i and consequently, w i , j w j , i = b w i for a scalar b = b i , j G i . The multiplication of both sides of the latter equality on the left by w j , i and on the right by w i , j leads to
w j , i w i , j w j , i w i , j = w j 2 = b w j , i w i , j = b w j 2 ,
consequently, w j = b w j and hence b = 1 . Therefore, we deduce that
w j 1 , k 1 w k 1 , k 2 = w j 1 , i w i , k 1 w k 1 , i w i , k 2 = w j 1 , i w i w i , k 2 = w j 1 , k 2 ,
since w j , i w i = w j , i , w i w i , j = w i , j . Then we infer that
w j 1 , k 1 w j 2 , k 2 = w j 1 , i w i , k 1 w j 2 , i w i , k 2 and
w i , k 1 w j 2 , i = w i y k 1 w k 1 w j 2 x k 2 w i , consequently ,
( 1 ) w j 1 , k 1 w j 2 , k 2 = 0 and
( 2 ) w k 1 w j 2 = 0
for each k 1 j 2 , also
( 3 ) w j 1 , k 1 w k 1 , k 2 = w j 1 , k 2
for every j 1 , k 1 , k 2 .
Thus, the set w j A w k is composed of elements which are multiples of the element w j , k , consequently, w j x w k , j w j A w j = G j w j , where the division algebra G j is over the field F according to Theorem 9 in [32]. Therefore, a scalar b G j exists such that w j x w k , j = b w j . Multiplying on the right by w j , k and using identity ( 3 ) we infer that w j x w k = b w j , k , where b = b ( j , k , x ) G j . This implies that
j , k w j A w k = : B A ,
where B is an algebra over F.
By virtue of Theorem 1 and Corollary 1 a Banach division algebra G exists such that G j G for each j, since G j is the algebra over F for each j, also since A is the Banach algebra.
We put A G = A ^ F G , that is A G is the right G-module and the algebra over F. Thus, this provides the inclusion
j w j A w j = : E A G .
On the other hand, w j A w j A as the algebra over F for each j, since w j A for each j. Please note that the sum of all w j A w k contains the F-linear span Y of the set ( j w j A ) ( k A w k ) . The multiplication and addition are continuous on A, hence Y is dense in the F-linear span X of ( j w j A ) A , since k A w k is dense in A. In its turn X is dense in the F-linear span V of A 2 , since j w j A is dense in A. Therefore, E is dense in A, since V is the two-sided ideal in A which is necessarily dense in A. □
Definition 7.
Let X be a Banach space over a field F, F E n , such that X also has the structure of a right G-module, where G is a division algebra over F. An operator s L ( X , X ) will be called (right) quasi-finite dimensional if its range s ( X ) is contained in a finite direct sum x 1 G x n G embedded into X and such that s is right G-linear, that is s ( x b ) = ( s x ) b for each x X and b G , where x 1 ,…, x n are nonzero vectors belonging to X.
Theorem 3.
Let A be a simple unital annihilator Banach algebra over a normed field F, F E n , with R c ( A ) = R ( A ) . Then a Banach division algebra G exists such that A G : = A ^ F G has an embedding T into the algebra L ( X , X ) , where X is a Banach space over F and a right G-module, such that
(1) 
T ( A G ) contains all (right) quasi-finite dimensional operators so that T ( A G ) is a Banach subalgebra in L ( X , X ) and
(2) 
a dense subalgebra B in A G exists whose image T ( B ) consists of quasi-finite dimensional operators.
Proof. 
Let a Banach division algebra G be provided by Theorem 2. Then w i A w i = G i G for each i and hence w i A G w i = G , since G is the division algebra over F.
We denote A G by A shortly. Then c l A ( A w i A x ) ( 0 ) for each x 0 , consequently, A w i A x ( 0 ) and hence
( 3 ) w i A x ( 0 )
for each x 0 in A.
Next we consider a left regular representation of the algebra A by operators L x for each x A , where L x y : = x y for each y A . From property ( 3 ) it follows that the left regular representation A x L x is the F-linear isomorphism. On the other hand, G j A and G j G and G j G = G G j = G for each j. The operator L x is right G-linear for each x A , that is L x ( y b ) = ( L x y ) b for each y A and b G , since A and G are associative algebras over the field F, also A has the structure of the right G-module.
In view of Formulas ( 2 , 3 ) in the proof of Theorem 2 the operator L w k , i maps the one-dimensional over G right module w i A w j into w k A w j , also L w j , k w l A w i = ( 0 ) for k l . Since the sum j w i A w j is dense in w i A , then L w k , i w i A w j is the one-dimensional over G right module. Therefore, the operator L x is quasi-finite dimensional for each x in B, where
B : = j , k w j A w k .
Suppose now that V is a one-dimensional operator in w i A over G and b w i A is an element such that b A 0 . Therefore, w i A = G b N ( V ) , where
N ( V ) : = { x w i A : V x = 0 }
Assume that L ( A , N ( V ) ) = ( 0 ) . This implies that L ( A , N ( V ) A ) = L ( A , N ( V ) ) = ( 0 ) , since the closed right G-module M N ( V ) A generated by N ( V ) A has the natural embedding ψ into A and ψ M N ( V ) A is a right ideal in A. Therefore, this leads to the equality A = ψ M N ( V ) A . On the other hand, N ( V ) = w i N ( V ) , consequently,
M w i N ( V ) w i A = w i A .
Then the identity w i A w i = w i G would imply that N ( V ) = w i A providing the contradiction. This implies that L ( A , N ( V ) ) ( 0 ) .
We take now x 0 in L ( A , N ( V ) ) . Let x b = 0 , hence w i A x = M G b N ( V ) x = ( 0 ) contradicting Property ( 3 ) , consequently, x b 0 and hence x b A is a non-null right ideal in A. Then x b A = w i A , since w i A is the minimal right ideal in A and x b A w i A . Thus, an element y A exists fulfilling the condition y x b = V b . This implies that the operators V and L y x coincide on G b . Mention that L y x N ( V ) = ( 0 ) = V N ( V ) , since x L ( A , N ( V ) ) , hence L y x = V . Thus, all right G-linear one-dimensional over G operators are among L x , where x A .
Assume that A is a Banach algebra, then G provided by Theorem 2 is also a Banach division algebra over F. By the continuity of the multiplication in A we deduce that w i A is a closed F-linear subspace in A, consequently, | L x | | x | for each x A , since
| L x y | = | x y | | x | | y |
for each y A . Therefore A x L x is the continuous isomorphism into L ( X , X ) and each L x is the limit relative to the operator norm topology of quasi-finite dimensional operators L x n with x n B for each n N . □

3. Conclusions

The results obtained in this article can be used for further investigations of normed algebras and operator algebras on non-Archimedean Banach spaces, their cohomologies, spectral theory of operators, non-Archimedean functional analysis, the representation theory of groups, algebraic geometry, PDEs, applications in the sciences, etc. Other possible applications are in mathematical coding theory and its technical implementations [38,39,40], because frequently codes are based on binary systems and algebras over non-Archimedean fields. Idempotents and decompositions of operator algebras can be used for an analysis and a classification of flows of information [22,41] and a solution of related PDEs [27,42].
In particular, Propositions 1 and 2, Theorems 2 and 3 can be used for studies of invariant subspaces of operator algebras in ultranormed spaces. They also can be used for studies of decompositions of totally disconnected topological groups representations by operators in ultranormed spaces into irreducible representations. Moreover, their relations with division algebras can be scrutinized with the help of Proposition 2 and Theorems 1 and 2.
It is worth mentioning that it also can serve for advances in non-Archimedean quantum field theory and quantum mechanics, because they are based on algebras and operator algebras over ultranormed fields [23,24,28,29].

Funding

This research received no external funding.

Conflicts of Interest

The author declares no conflict of interest.

References

  1. Dixmier, J. C-Algebras; North-Holland Publishing Company: Amsterdam, The Netherlands, 2011. [Google Scholar]
  2. Dunford, N.; Schwartz, J.C. Linear Operators; John Wiley and Sons, Inc.: New York, NY, USA, 1966. [Google Scholar]
  3. Fell, J.M.G.; Doran, R.S. Representations of -Algebras, Locally Compact Groups, and Banach -Algebraic Bundles; Acad. Press: Boston, MA, USA, 1988; Volume 1–2. [Google Scholar]
  4. Naimark, M.A. Normed Rings; Nauka: Moscow, Russia, 1968. [Google Scholar]
  5. Beckenstein, E.; Narici, L.; Suffel, C. Topological Algebras; North-Holland Publishing Company: Amsterdam, The Netherlands, 1977. [Google Scholar]
  6. Kadison, R.V.; Ringrose, J.R. Fundamentals of the Theory of Operator Algebras; Academic Press: New York, NY, USA, 1983. [Google Scholar]
  7. Bourbaki, N. “Algèbre” Ch. 1–3; Springer: Berlin, Germany, 2007. [Google Scholar]
  8. Amice, Y. Interpolation p-Adique. Bull. Soc. Math. Fr. 1964, 92, 117–180. [Google Scholar] [CrossRef]
  9. Diarra, B.; Ludkovsky, S.V. Spectral integration and spectral theory for non-archimedean Banach spaces. Int. J. Math. Math. Sci. 2002, 31, 421–442. [Google Scholar]
  10. Escassut, A. Analytic Elements in p-Adic Analysis; World Scientific: Singapore, 1995. [Google Scholar]
  11. Escassut, A. Ultrametric Banach Algebras; World Scientific: Hackensack, NJ, USA, 2003. [Google Scholar]
  12. Kersten, I. Brauergruppen von Körpern; Friedr. Vieweg and Sons: Braunschweig, Germany, 1990. [Google Scholar]
  13. Ludkowski, S.V. Non-archimedean antiderivations and calculus of operators with local spectra. Far East J. Math. Sci. 2016, 99, 455–489. [Google Scholar]
  14. Van Rooij, A.C.M. Non-Archimedean Functional Analysis; Marcel Dekker Inc.: New York, NY, USA, 1978. [Google Scholar]
  15. Weil, A. Basic Number Theory; Springer: Berlin, Germany, 1973. [Google Scholar]
  16. Diarra, B. On reducibility of ultrametric almost periodic linear representations. Glasgow Math. J. 1995, 37, 83–98. [Google Scholar] [CrossRef]
  17. Ludkovsky, S.V. Quasi-Invariant and Pseudo-Differentiable Measures in Banach Spaces; Nova Science Publishers, Inc.: New York, NY, USA, 2008. [Google Scholar]
  18. Ludkovsky, S.V. Stochastic Processes in Non-Archimedean Banach Spaces, Manifolds and Topological Groups; Nova Science Publishers, Inc.: New York, NY, USA, 2010. [Google Scholar]
  19. Robert, A. Representations p-adiques irréductibles de sous-groupes ouverts de SL2(Zp). C. R. Acad. Sci. Paris Sér. I Math. 1984, 298, 237–240. [Google Scholar]
  20. van Rooij, A.C.M.; Schikhof, W.H. Groups representations in non-archimedean Banach spaces. Bull. Soc. Math. Fr. Mem. 1974, 39–40, 329–340. [Google Scholar] [CrossRef]
  21. Schikhof, W.H. Ultrametric Calculus; Cambridge University Press: Cambridge, MA, USA, 1984. [Google Scholar]
  22. Anashin, V. Automata finitness criterion in terms of van der Put series of automata functions. p-Adic Numbers Ultrametric Anal. Appl. 2012, 4, 151–160. [Google Scholar] [CrossRef]
  23. Aref’eva, I.Y. Holographic relation between p-adic effective action and string field theory. Proc. Steklov Inst. Math. 2014, 285, 26–29. [Google Scholar] [CrossRef]
  24. Aref’eva, I.Y.; Dragovich, B.; Frampton, P.H.; Volovich, I.V. Wave functions of the universe and p-adic gravity. Int. J. Mod. Phys. 1991, 6, 4341–4358. [Google Scholar] [CrossRef]
  25. Dragovich, B. On measurements, numbers and p-adic mathematical physics. p-Adic Numbers Ultrametric Anal. Appl. 2012, 4, 102–108. [Google Scholar] [CrossRef]
  26. Isham, C.J. Topological and global aspects of quantum theory. In Relativity, Groups and Topology II; Stora, R., De Witt, B.S., Eds.; Elsevier Sci. Publ.: Amsterdam, The Netherlands, 1984. [Google Scholar]
  27. Revuzhenko, A.F. Mathematical Analysis of Non-Archimedean Variable Functions. In Specialized Mathematical Apparatus for Stuctural Geo-Environment Level Description; Nauka: Novosibirsk, Russia, 2012. [Google Scholar]
  28. Viswanathan, K.S. Colliding gravitational plane waves and black hole creation. p-Adic Numbers Ultrametric Anal. Appl. 2012, 4, 143–150. [Google Scholar] [CrossRef]
  29. Vladimirov, V.S.; Volovich, I.V.; Zelenov, E.I. p-adic Analysis and Mathematical Physics; Nauka: Moscow, Russia, 1994. [Google Scholar]
  30. Bourbaki, N. Première Partie. Les Structures Fondamentales de L’analyse. XI. Livre II. Algèbre. Ch. IV. Polynomes et Fractions Rationnelles. Ch. V. Corps Commutatifs; Hermann: Paris, France, 1950. [Google Scholar]
  31. Bourbaki, N. “Algèbre commutative” Ch. 1–7; Hermann: Paris, France, 1988. [Google Scholar]
  32. Ludkowski, S.V. Normed dual algebras. Mathematics 2019, 7, 174. [Google Scholar] [CrossRef]
  33. van der Put, M.; van Tiel, J. Espaces nucléaires non-archimédiens. Indag. Math. 1967, 29, 556–561. [Google Scholar]
  34. Engelking, R. General Topology; Mir: Moscow, Russia, 1986. [Google Scholar]
  35. Kunen, K. Set Theory; North-Holland Publishing Co.: Amsterdam, The Netherlands, 1980. [Google Scholar]
  36. Neumann, B.H. Embedding non-associative rings in division rings. Proc. Lond. Math. Soc. 1951, 1, 241–256. [Google Scholar] [CrossRef]
  37. Arhangel’skii, A.; Tkachenko, M. Topological Groups and Related Structures; Atlantis Press: Amsterdam, The Netherlands, 2008. [Google Scholar]
  38. Blahut, R.E. Algebraic Codes for Data Transmission; Cambridge University Press: Cambridge, MA, USA, 2003. [Google Scholar]
  39. Magomedov, S.G. Assessment of the impact of confounding factors in the performance information security. Russ. Technol. J. 2017, 5, 47–56. [Google Scholar]
  40. Shum, K.P.; Ren, X.; Wang, Y. Semigroups on semilattice and the constructions of generalized cryptogroups. Southeast Asian Bull. Math. 2014, 38, 719–730. [Google Scholar]
  41. Sigov, A.S.; Andrianova, E.G.; Zhukov, D.O.; Zykov, S.V.; Tarasov, I.E. Quantum informatics: Overview of the main achievements. Russ. Technol. J. 2019, 7, 5–37. [Google Scholar]
  42. Zaikin, B.A.; Bogadarov, A.Y.; Kotov, A.F.; Poponov, P.V. Evaluation of coordinates of air target in a two-position range measurement radar. Russ. Technol. J. 2016, 4, 65–72. [Google Scholar]

Share and Cite

MDPI and ACS Style

Ludkowski, S.V. Structure of Normed Simple Annihilator Algebras. Mathematics 2019, 7, 347. https://doi.org/10.3390/math7040347

AMA Style

Ludkowski SV. Structure of Normed Simple Annihilator Algebras. Mathematics. 2019; 7(4):347. https://doi.org/10.3390/math7040347

Chicago/Turabian Style

Ludkowski, Sergey V. 2019. "Structure of Normed Simple Annihilator Algebras" Mathematics 7, no. 4: 347. https://doi.org/10.3390/math7040347

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop