Keywords
orthogonality, norm derivatives, ϼ_*-orthogonality.
This article is included in the Fallujah Multidisciplinary Science and Innovation gateway.
Orthogonality is an important concept in normed spaces, and many generalizations of this concept have been proposed. In this paper, we introduce a new concept of orthogonality in normed spaces, denoted by ϼ LM -orthogonality, which is related to ϼ ∗ -orthogonality. The fundamental properties of this new concept are systematically analyzed, including symmetry, non-negativity, scalar homogeneity, linear independence of orthogonal vectors, the Cauchy–Schwarz type inequality, the zero property, and other characteristics. We also explain the relationship between this new definition and some other well-known types of orthogonality.
orthogonality, norm derivatives, ϼ_*-orthogonality.
In an inner product space , two vectors are said to be orthogonal, denoted by if and only if . In spaces whose norm is induced by an inner product, the notion of orthogonality admits a natural and uniquely determined form. Extending this concept to more general normed spaces enable a deeper investigation of their geometric and analytical interrelations, thus offering a broader framework to generalize classical Euclidean ideas to abstract mathematical settings.
Consider as a real normed vector space whose dimension is not less than two, there exist several notions of orthogonality, among which the definition introduced by (Birkhoff–James) is one of the most prominent. If , define ⇔ , (t ) see.1
In 1986, Amir in2 defined the norm derivatives using two functionals, be functionals, as follows:
A mapping was introduced by MiliĆiĆ in3 as follows: . But M. Nur and H. Gunawan in4 defined an orthogonality relation based on norm derivatives by , Also Zamani and Moslehian in5 defined an orthogonality functional by (ṡ, ) = λ + (1- λ) ∀ λ R, and ṡ is - orthogonality to denoted by the notions of -orthogonality is introduced in6 as: 0. Recall that is smooth at if and only if for all
These functionals extend the concept of the inner product to a normed space, and many geometric properties will be reformulated in the normed space using the concept of the norm derivative. Now we shall address some important theorem that we will need in this research.
6Suppose ( , ‖·‖) represents a real normed vector space, then
(i) (t ṡ, ) = (ṡ, t )= (ṡ, ) for all ṡ, ∈ and all t ∈ R.
(ii) | | for all ṡ, .
(iii) For all vectors except the zero vector, ṡ, ∈ , if , then ṡ and are independent in the linear sense.
(iv) (ṡ, t ṡ + ) = +2t ṡ, ) + (ṡ, ) for all ṡ, and all t ∈ R.
For more information about other orthogonalities you can see.7–10
This section is devoted to introducing a new form of orthogonality by using -orthogonality as follows:
Suppose ( , ‖·‖) represents a real normed vector space then , the functional which defines as , We say that ṡ is - orthogonality to , we denoted by ṡ if .
Suppose ( , ‖·‖) represents a real normed vector space. Then
(a) We have = since 0 then 0, implies 0.
(b) From definition of -orthogonality we have = = = 0
In the same way, we prove .
(c) From definition of -orthogonality and -orthogonality we get =
Thus = 0 or = 0
By theorem 1.1 (iii) for all nonzero vectors ṡ, , if , then ṡ and are linearly independent.
Hence, whether = 0 or = 0 it follows that ṡ and are linearly independent.
If come from inner product space then = .
Suppose represents a real normed vector space and let , ∈ .
Obvious
The converse of (a), (b) and (c) of theorem 3.1 are not true. For example, take and if in the space =
But = 0
Hence ṡ but the others are not.
The converse of (d), (e) and (f ) of theorem 3.1 are not true. For example, take ṡ = (2,0,0) and = (1,1,0) if = + in the space X = , then
But = 0
Hence ṡ but the others are not.
Consider the real normed space = with the norm = where ,
we have = and =
Thus = (1) = 1
= = -1
= (1) = 1
= = -1
We have = therefore = = 0,
Since implies = = 0,
Also = λ + (1- λ) ) = λ + (1- λ) (1)= 1-2λ put λ = then
But = = = 1 0
Hence , and
Consider the real normed space = with the norm = max { } where , . Then for every we have
We have = therefore = = 0 and = = =
Hence , and
From example 3.4 and example 3.5 it follows that the orthogonalities, , , and are generally incomparable.
If X is smooth then but not equal to .
This study is entirely theoretical and does not rely on any experimental or external datasets. Therefore, no data are available in connection with this research.
This article is a purely theoretical study in functional analysis and does not involve clinical trials, animal studies, observational studies, or qualitative research. Therefore, standard reporting guidelines such as CONSORT, ARRIVE, STROBE, or COREQ/SRQR do not directly apply. Standard practices for presenting theoretical mathematical results have been followed, including clear definitions, theorems, proofs, and logical consistency.
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