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On the Method for Proving the RH Using the Alcantara-Bode Equivalence

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29 May 2025

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29 May 2025

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Abstract
There is presented here a functional analysis - numerical solution for the Alcantara-Bode equivalent formulation of the Riemann Hypothesis (RH). RH, a long-standing unsolved problem, posits that the non-trivial zeros of the Riemann Zeta function lie on the vertical line $\sigma=1/2$. Alcantara-Bode equivalent (1993) obtained from Beurling equivalent of RH (1955) states that RH holds if and only if the null space of a specific integral operator $T_\rho$ on $L^2(0,1)$ does not contain not null elements: $N_{T_\rho} = \{0\}$, equivalently, it is injective. The theory we introduced here is an update of our previous work [1], for dealing with a generic case of such type of problems. We provided methods for investigating the injectivity of linear bounded operators through their positivity properties. % These methods are extending the solution given in [1], in this paper here we separated the analysis on the finite dimension subspaces differentiating the case of the operator restrictions from the approximations of the operator obtained by applying finite rank orthogonal projections. It involves approximations on finite dimension subspaces built in a multi-level structure by spanning the indicator functions of intervals associated to partitions of the domain (0,1). In both cases, the connection between the error estimations of an eligible zero and the positivity parameters dictates the operator injectivity. Injectivity Criteria introduced in [1], involving the adjoint operator for finite rank operator approximations is applied now to operator restrictions when the operator positivity parameters are converging to zero with the mesh converging to zero. As a method, it is useful when no data we have related to the finite rank approximation, like the compactness of the operator. Instead, for Hilbert-Schmidt operators that are compact, and so accept finite rank approximations whose sequence converges strong to the original operator, we are expecting to find a bound for the positivity parameters that are mesh independent. The dense set we used for the Hilbert-Schmidt integral operator in the Alcantara-Bode equivalent is built as the union of finite dimension subspaces spanned by indicator interval functions of the partitions of the domain by halving the mesh from a level to next one. This is a discretisation method used in multi-level (multigrid) numerical analysis techniques for obtaining large systems of equations. From this point of view, we could consider the multi-level including subspaces like a degenerate finite element method. Using both methods the finite rank operator approximations and injectivity criteria on the same finite dimension subspaces, we obtained in each case the injectivity of the integral operator from Alcantara-Bode equivalent formulation. As an observation, since a linear operator and its associated Hermitian have the same null space and a Hermitian operator is a non negative operator, this method could be applied to any linear operator on a separable Hilbert space in order to investigate its injectivity.
Keywords: 
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To my mother
A.) Plagiarism and similarities:
Based on the document provided, the author explicitly references prior works and builds upon them, citing sources such as Alcantara-Bode (1993), Beurling (1955), and others. The methods and results presented appear to be extensions or applications of existing theories, such as the Alcantara-Bode equivalent formulation of the Riemann Hypothesis and injectivity criteria introduced in earlier works. The author also acknowledges using techniques from referenced papers, such as Mercer-like kernels and finite rank operator approximations. The document does not show any indication of plagiarism, as the author provides proper citations and references to previous works, including their contributions and methods. The results and methods are presented as original extensions or applications of these established theories. However, determining plagiarism definitively would require a detailed comparison with the referenced works to ensure proper attribution and originality. In summary, the document appears to be a legitimate scholarly work that builds upon and extends prior research, with appropriate citations provided.
(Note (n.a.): the previous owned versions of the same preprint as well the previous paper published - cited in this manuscript, could not be considered plagiarism or similarities once the aim has been to be improved from a version to another.)
B.) What are the key methods used in this document:
The document outlines several key methods used to investigate the Alcantara-Bode equivalent formulation of the Riemann Hypothesis (RH). These methods focus on functional-numerical analysis, operator injectivity, and approximation techniques.
Below are the key methods:
1. Injectivity Criteria for Linear Operators:
The document introduces criteria to determine the injectivity of linear bounded operators on separable Hilbert spaces. It uses positivity parameters to analyse whether the null space of an operator is empty ( N T = 0 ), which is equivalent to proving injectivity. The method involves evaluating the positivity of the operator on dense sets or on finite dimensional subspaces.
2. Finite Rank Operator Approximations:
Finite rank approximations of integral operators are constructed on finite dimensional subspaces. These approximations are used to analyse the convergence of the operator to its original form and to ensure positivity parameters are bounded. The document applies this method to Hilbert-Schmidt integral operators, which are compact and allow proper approximations.
3. Multi-Level Discretization:
Dense sets in the Hilbert space L 2 ( 0 , 1 ) are constructed using indicator functions of intervals from partitions of the domain. A multi-level structure is employed, where the mesh size is halved at each level, creating finer partitions. This discretization method is similar to techniques used in multigrid numerical analysis and finite element methods.
4. Adjoint Operator Analysis:
The adjoint operator is used to analyse injectivity when positivity parameters converge to zero. The method leverages the fact that a linear operator and its associated Hermitian operator share the same null space, and Hermitian operators are non-negative.
5. Matrix Representation of Operators:
Sparse diagonal matrix representations of integral operators are derived for finite dimensional subspaces. The diagonal entries are computed using integrals over the partitions, and their positivity determines the operator’s positivity on the subspaces.
6. Error Estimation and Convergence:
The connection between error estimations of eligible zeros and positivity parameters is used to dictate operator injectivity. The convergence of operator approximations in norm to the original operator is analysed to ensure injectivity.
7. Application of Lemmas and Theorems: The document uses several lemmas and theorems to formalize the methods:
-
Theorem 1: Proves that strict positivity on a dense set implies injectivity.
-
Theorem 2: Establishes injectivity using finite rank operator approximations with bounded positivity parameters.
-
Lemma 1: Provides criteria for finite rank approximations of Hilbert-Schmidt integral operators.
-
Lemma 2: Introduces criteria for operator restrictions when positivity parameters converge to zero.
8. Specific Application to the Alcantara-Bode Equivalent:
The methods are applied to the integral operator with kernel ρ ( y , x ) = { y / x } , which is connected to RH (n.a.: here { } denotes the fractional part function). The positivity parameters of finite rank approximations are shown to be inferior bounded, proving the operator’s injectivity and validating RH.
These methods collectively provide a rigorous framework for analysing the injectivity of integral operators and proving the Alcantara-Bode equivalent formulation of the Riemann Hypothesis. □

1. Introduction

Let H be a separable Hilbert space. A result obtained (Theorem 1 below) shows that the null space of a linear bounded operator strict positive on a dense set in H, does not contain non null elements. Consider F be a family of finite dimension including subspaces S n , n 1 such that their union S is a dense set in the separable Hilbert space H. Dense sets having such properties there exist, for example when H : = L 2 ( 0 , 1 ) then S could be built in a multi-level fashion using indicator functions of the disjoint intervals of the domain partitions (see the paragraph 3). Such families could be obtained also from a basis in H, a subspace S n being spanned by first n elements from the basis for example.
The positivity of a linear bounded operator T on S, T v , v > 0 v S not null, ensures that the null space of T contains from S only the element 0, i.e. N T S = { 0 } . Now, a linear bounded operator T positive on a finite dimension subspace is in fact strictly positive on it: i.e. there exists α n ( T ) > 0 such that T v , v α n ( T ) v 2 for every v S n .
Suppose T positive on each subspace from the family F.
If there exists α > 0 such that α n α for any n 1 then T is strict positive on the dense set S and, by Theorem 1 below N T = { 0 } .
If instead the sequence of the positivity parameters of T is converging to zero, α n ( T ) 0 with n , we consider two directions for the investigation of its injectivity providing the theory and the methods needed for:
- involving the adjoint operator restrictions on the subspaces of the family, having as support Lemma 2 below;
- considering a sequence of positive operator approximations on subspaces, if there exists one such that the sequence is convergent in norm to the operator
T T n 0 with n and, whose corresponding sequence of positivity parameters is inferior bounded: there exists α > 0 such that
T n v , v α n v 2 for any n 1 where α n : = α n ( T n ) α . The Theorem 2 and Lemma 1 below are dealing with this method.
While the criteria involving the adjoint operator (introduced in [1]) could be applied to any positive, linear bounded operator, for involving the operator approximations we have to find the means for obtaining a proper approximation schema in terms of the convergence of the approximations to the original operator and, such operator approximations should be positive on the subspaces in F having an inferior bound for the sequence of the positivity parameters.
However, note that the positivity of the operator could be solved by replacing it by its associated Hermitian ( T * T ) that has the same null space with T and it is non negative definite on H.
Let observe that there is a connection between the two kind of positivity parameters on each subspace: if h is the length of the intervals in a partition of (0,1), n h = 1 , then for the Hilbert-Schmidt integral operator on L 2 ( 0 , 1 ) of our interest, we obtained α n ( T ) = n 1 α n ( T n ) , n 1 with α n ( T n ) a constant mesh independent.

2. Two theorems on injectivity and associated methods.

Let H be a separable Hilbert space and denote with L ( H ) the class of the linear bounded operators on H. If T L ( H ) is positive on a dense set S H , i.e. T v , v > 0 v not null in S, then T has no zeros in the dense set. Otherwise, if there exists w S such that T w = 0 then T w , w = 0 contradicts its positivity.
Follows: its ’eligible’ zeros are all in the difference set E : = H S , i.e. N T E .
Theorem 1. 
If T L ( H ) is strict positive on a dense set of a separable Hilbert space then T is injective, equivalently N T = { 0 } .
Proof. 
Let’s take in consideration only the set of eligible zeros that are on the unit sphere without restricting the generality, once for an element w H , w 0 both w and w / w are or are not in N T . The set S H is dense if its closure coincides with H. Then, if w E : = H S , for every ε > 0 there exists u ε , w S such that w u ε , w < ε . Now, (1) results as follows. If w u ε , w :
0 w u ε , w = w u ε , w + u ε , w u ε , w w u ε , w + u ε , w u ε , w < ε .
If u ε , w w instead, then:
0 u ε , w w = u ε , w w + w w w u ε , w < ε .
So, given w E , for every ε > 0 there exists u ε , w S such that
| w u ε , w | < ε
Let w be an eligible element from the unit sphere, w = 1 and take ε n = 1 / n .
Then there exists at least one element u ε n , w S such that u ε n , w w < ε n holds. Follows from (1), ∣ 1 - u ε n , w < 1 / n showing that, for any choices of a sequence approximating w, u ε n , w S , n 1 , it verifies u ε n , w 1 .
If T L ( H ) is strict positive on S, then there exists α > 0 such that u S , T u , u α u 2 .
Suppose that there exists w E , w = 1 a zero of T , i . e . w N T and consider a sequence of approximations of w, u ε n , w S , n 1 that, as we showed, has its normed sequence converging in norm to 1. From the positivity of T on the dense set S, follows:
α u ε n , w 2 T u ε n , w , u ε n , w = T ( u ε n , w w ) , u ε n , w < ε n T u ε n , w
With c= T / α , we obtain u ε n , w c / n . Then, u ε n , w 0 with n , in contradiction with its convergence u ε n , w 1 with n .
Or, this happen for any choice of the sequence of approximations of w, verifying w u ε n , w < ε n , n 1 , when T w = 0 .
Thus w N T , valid for any w E , w = 1 , proving the theorem because no zeros of T there are in S either.
Suppose that the dense set S is the result of an union of finite dimension subspaces of a family F: S = n 1 S n , S ¯ = H . It is not mandatory but will ease our proofs considering that the subspaces are including: S n S n + 1 , n 1 .
Observation 1. Let β n ( u ) : = u u n be the normed residuum of the eligible element u E after its orthogonal projection on S n . Then, β n ( u ) 0 with n .
Proof. 
Given ϵ > 0 , from the density of the set S in H there exists u ϵ S verifying u u ϵ < ϵ , as per the observations made in the proof of the Theorem 1. Let S n ϵ be the coarsest subspace, i.e. with the smallest dimension, from the family of subspaces containing u ϵ . Because the best approximation of u in S n ϵ is its orthogonal projection, we obtain
β n ϵ ( u ) : = u P n ϵ u u u ϵ < ϵ ,
inequality valid for every ϵ > 0 , proving our assertion. □
For T L ( H ) , let T n , n 1 be a sequence of operator approximations on S n , n 1 having the property ϵ n : = T T n 0 and, suppose that for every n 1 , the operator approximation T n is positive on S n and denote with α n : = α n ( T n ) its positivity parameter.
Theorem 2. 
Let T L ( H ) be positive on the dense set S. If the sequence { T n , n 1 } of its approximations on the family F verifies:
i) ϵ n : = T T n 0 with n ;
ii) T n v , v α n v 2 , v S n , S n F ;
iii) α n α > 0 , n 1 ,
then N T = { 0 } .
Proof. 
Being positive on S, the operator has no zeros in the dense set.
For u E : = H S , u = 1 denoting the not null orthogonal projection over S n by u n : = P n u , n n 0 : = n 0 ( u ) , we have on any subspace S n , u 2 = u n 2 + β n 2 ( u ) where β n ( u ) = u P n u : = β n is its (normed) residuum. We have: u n 1 and β n ( u ) 0 .
If there exists u N T E , u = 1 then for it:
α n u n 2 T n u n , u n T n u n u n
= ( T n u n T u n + T u n T u ) u n
( T T n u n + T u u n ) u n
= ( ϵ n u n + T β n ) u n ( ϵ n + T β n )
evaluation obtained because u n < 1 . Then from Observation 1 and iii) we have:
α ϵ n + T β n 0 .
The inequality is violated from a n 1 n 0 , involving u N T , valid for any supposed zero of T in E. Once T has no zeros in the dense set, N T = { 0 } . □
We will deal now, with the special case of the approximations of the Hilbert-Schmidt integral operators that, being compact operators could be approximated in a proper matter on finite dimension subspaces so, the condition i) is satisfied ([3]).
Let T : = T φ be a Hilbert-Schmidt integral operator. A technique for obtaining the approximations for an integral operator is used in [5]. Thus, the condition i) in the Theorem 2 is fulfilled when T n , n 1 are finite rank approximations on the subspaces of the family F obtained by orthogonal projection integral operators T n : = P n r ( T ) . Then, for every u H not null:
T u T n u = ( I P n r ) T u I P n r T u 0
Lemma 1. 
(Criteria for finite rank approximations). If the finite rank approximations of a positive linear Hilbert-Schmidt integral operator T φ on a dense set S are positive on the family of approximation subspaces F and the sequence of the positivity parameters is inferior bounded,
then T φ is strict positive on the dense set so, it is injective.
Proof. 
The requests i), ii) in the Theorem 2 hold by the previous observations. From the convergence to zero of the sequence ϵ n , n 1 there exists ϵ 0 a ’compactness’ parameter verifying ϵ 0 : = m a x n { ϵ n ; ϵ n < α } corresponding to a subspace S n 0 , n 0 < . The parameter ϵ 0 in independent from any v S and, due to the including property, for any n < n 0 we have S n S n 0 . We could consider S n 0 be S 1 or, your choice, we could consider v as being inside of S n 0 . Then:
α n α > ϵ 0 ϵ n for n 1 , resulting ( α n ϵ n ) > ( α ϵ 0 ) > 0 n 1 .
For an arbitrary v S there exists a coarser subspace (i.e. with a smaller dimension) S n , n n 1 : = n 1 ( v ) , for which v S n . For it, we have:
T v , v = T n v , v ( T n T ) v , v > 0 . Since T n is positive on S n ,
T v , v α n v 2 ( T n T ) v , v .
Now, T and T n are positive on S n . Then the inner product in the right side of the equality is real valued and, | ( T n T ) v , v | ϵ n v 2 .
So, if ( T n T ) v , v 0 , then ( T n T ) v , v ϵ n v 2 . Because ϵ n < α n , follows:
T v , v ( α n ϵ n ) v 2 ( α ϵ 0 ) v 2 .
Now, if ( T n T ) v , v < 0 , T v , v α n v 2 α v 2 ( α ϵ 0 ) v 2 .
Thus, taking α ( T ) = ( α ϵ 0 ) ,
T v , v α ( T ) v 2 for any v S meaning that T is strict positive on the dense set S and from Theorem 1, N T = { 0 } . □
Corollary. 
If Q L ( H ) is a Hermitian compact operator verifying on a dense set the properties i) and ii) from Theorem 2, then it is injective.
Proof. 
Being Hermitian, the operator verifies Q v , v 0 , for every v H . Being compact it admits on a dense family of finite dimension subspaces a sequence of approximations. Then, for any v S ,
Q v , v = Q n v , v ( Q n Q ) v , v 0 obtaining following the steps from the proof of Lemma 1 that in the hypotheses i) and ii) holds:
Q v , v ( α ϵ 0 ) v 2 meaning that Q is strict positive on the dense set. Thus, N Q = { 0 } due to the Theorem 1. Let observe that if Q = T * T then N T = N Q = { 0 } result obtained without requesting the positivity of Q or T on the dense set. □
The following lemma is dealing with the cases in which a proper sequence of operator approximations could not be defined (see the Injectivity Criteria in [1]).
Lemma 2. 
(Criteria for operator restrictions.)Let T L ( H ) positive on the subspaces S n , n 1 whose union S is a dense set S, verifying: T v , v α n v 2 for every v S n , where α n 0 with n . Consider now the parameters:
μ n : = α n ( T ) / ω n where ω n verifies T * v ω n v , v S n , n 1 .
If there exists C > 0 such that μ n C for every n 1 , then N T = { 0 } .
Proof. 
Suppose that there exists u ( H S ) N T , u = 1 and let u n its orthogonal projection on S n , n 1 . Then, from the (strict) positivity of T on each of the subspaces S n , n 1 (see (2)):
α n ( T ) u n 2 T u n , u n = T ( u n u ) , u n = ( u n u ) , T * u n β n ω n u n
Then, from
C μ n β n / 1 β n 2 0 where β n : = β n ( u ) = u u n , we obtain a contradiction. Thus, u N T affirmation valid for any u H S . Follows: N T = { 0 } . □

3. Dense sets in L 2 ( 0 , 1 ) .

Let H : = L 2 ( 0 , 1 ) . The semi-open intervals of equal lengths h = 2 m , m N , nh = 1, Δ h , k = ( ( k 1 ) / 2 m , k / 2 m ] , k = 1 , n 1 together with the open Δ h , n are defining for m 1 a partition of (0,1), k=1,n, n = 2 m , n h = 1 . Consider the interval indicator functions having the supports these intervals (k=1,n), nh=1:
I h , k ( t ) = 1 for t Δ h , k and 0 otherwise
The family F of finite dimensional subspaces S h that are the linear spans of interval indicator functions of the h-partitions defined by (3) with disjoint supports, S h = s p a n { I h , k ; k = 1 , n , n h = 1 } , built on a multi-level structure, are including S h S h / 2 by halving the mesh h. In fact, the property is obtained from (3) observing that S h I h , i = I h / 2 , 2 i 1 + I h / 2 , 2 i S h / 2 , i = 1 , n .
The set S = n 1 S h , n h = 1 is dense in H well known in literature.
Citing [5], (pg 986), the integral operator P h r , n 1 having the kernel function:
r h ( y , x ) = h 1 k = 1 , n I h , k ( y ) I h , k ( x )
is a finite rank integral operator orthogonal projection having the spectrum {0, 1} with the eigenvalue 1 of the multiplicity n (nh=1) corresponding to the orthogonal eigenfunctions I h , k , k = 1 , n . We will show it, by proving that u H , P h r u S h and, as a consequence, obviously ( P h r ) 2 = P h r for n 2 , n h = 1 .
For any u H ,
( P h r u ) ( y ) = x ( 0 , 1 ) h 1 k = 1 . n I h , k ( y ) I h , k ( x ) u ( x ) d x
= h 1 k = 1 , n c k I h , k ( y ) , where c k : = Δ h , k u ( x ) d x ,
that is the standard orthogonal projection of u onto S h .
Now, if f = k = 1 , n c k I h , k S h ,
P h r ( f ) = h 1 j = 1 , n Δ h , j I h , j ( y ) ( k = 1 , n c k I h , k ( y ) ) I h , j ( x ) d y
= h 1 j = 1 , n I h , j ( x ) Δ h , j c j I h , j ( y ) d y
= h 1 j = 1 , n c j I h , j ( x ) Δ h , j I h , j ( y ) d y = j = 1 , n c j I h , j = f ,
i.e. P h r f = f and so, ( P h r ) 2 u = P h r u for any u H . Because P h r is an orthogonal projection onto S h and due to the including property of the finite dimension subspaces whose union is dense, follows:
I P h r 0 for n , n h = 1 . So, i) in Theorem 2 holds.
Remark 1. 
The matrix representation of T ρ on S h is a sparse diagonal matrix: its elements outside the diagonal are zero valued.
Proof. 
The inner product on the subspace S h between u S h and v h S h is a result between the orthogonal projection of u and v h , like an inner product between two step functions: u , v h : = P h r u , v h . If P h r u : = u h = k = 1 , n a k I h , k and v h = j = 1 , n c j I h , j , due to the disjoint supports of the indicator interval functions, I h , k , I h , j = 0 for k j and, their inner product is u h , v h = k = 1 , n a k c k ¯ I h , k , I h , k .
Let T ρ be a Hilbert-Schmidt integral operator on H. Now,
T ρ I h , k = 0 1 ρ ( y , x ) I h , k ( x ) d x = Δ h . k ρ ( y , x ) I h , k ( x ) d x . Follows:
T ρ I h , k , I h , j = 0 1 Δ h , k ρ ( y , x ) I h , k ( x ) d x I h , j ( y ) d y
= Δ h , k Δ h , j I h , j ( y ) ρ ( y , x ) I h , k ( x ) d x d y = 0 for k j because I h , k and I h , j have disjoint supports for k j . Then, the matrix representation of T ρ on S h , M h ( T ρ ) is a sparse diagonal matrix having the diagonal entries
d k k h : = Δ h , k Δ h , k I h , k ( y ) ρ ( y , x ) I h , k ( x ) d x d y , k = 1 , n , n h = 1 and, with v h = k = 1 , n c k ,
T ρ v h , v h = k = 1 , n c k c k ¯ d k k h . □
The integral operator approximation of T ρ on S h is a finite rank operator approximation, T ρ h , having the kernel function ([5])
ρ h ( y , x ) = h 1 k = 1 , n I h , k ( y ) ρ ( y , x ) I h , k ( x ) : = h 1 k = 1 , n ρ h k ( y , x )
where the pieces ρ h k , k = 1 , n of the kernel function ρ h in the sum have disjoint supports in L 2 ( 0 , 1 ) 2 namely Δ h , k × Δ h , k , k = 1 , n , n h = 1 .
Remark 2. 
The matrix representation of T ρ h is a sparse diagonal matrix and, M h r ( T ρ ) = h 1 M h ( T ρ ) .
Proof. 
Evaluating the previous relationship for v = I h , i , we obtain
( T ρ h I h , i ) ( y ) = h 1 Δ h , i ρ ( y , x ) I h , i ( x ) d x I h , i ( y ) . Then,
T ρ h I h . i , I h , j = 0 for i j and the matrix representation of the finite rank operator P h r ( T ρ ) : = T ρ h ,
is:
M h r ( T ρ ) = h 1 diag d k k h k = 1 , n , a sparse diagonal because d i j h = 0 for i j and with the diagonal entries given by:
d k k h = Δ h , k Δ h , k I h , k ( y ) ρ ( y , x ) I h , k ( x ) d x d y : = Δ h , k Δ h , k ρ ( y , x ) d x d y , k = 1 , n
Follows: M h r ( T ρ ) = h 1 M h ( T ρ ) , i.e. both matrices are or are not simultaneous positive. □
Pointing out:
T ρ h v h , v h = h 1 T ρ v h , v h = h 1 k = 1 , n c k c k ¯ d k k h , for any v h = k = 1 , n c k I h , k S h , v h 0 .
Remark 3. 
If d k k h > 0 , k = 1 , n , n h = 1 , because v h 2 = h k = 1 , n c k c k ¯ we obtain:
T ρ h v h , v h α h ( T ρ h ) v h 2 where
α h ( T ρ h ) = h 2 m i n ( k = 1 , n ) d k k h
is the positivity parameter of the finite rank operator approximation T ρ h .
From T ρ v h , v h = k = 1 , n c k c k ¯ d k k h   = h T ρ h v h , v h results that T ρ is positive on S h if and only if T ρ h is positive on S h . Then, if on every subspace S h F , d k k h > 0 k = 1 , n , n h = 1 , the following relationship holds
α h ( T ρ ) = h 1 m i n ( k = 1 , n ) ( d k k h ) : = h α h ( T ρ h ) , n h = 1
Remark 4. 
Thus, the positivity of the linear bounded integral operator T ρ on the dense set S is determined by the diagonal entries in its matrix representations.

4. Proof of the Alcantara-Bode equivalent of RH.

We are now in position to prove RH showing that the integral operator
( T ρ u ) ( y ) = 0 1 ρ ( y , x ) u ( x ) d x , u L 2 ( 0 , 1 ) , where ρ ( y , x ) = { y / x } is the fractional function of the ratio y / x , has its null space N T ρ = { 0 } .
Alcantara-Bode ([2], pg. 151) in his theorem of the equivalent formulation of RH obtained from Beurling equivalent formulation ([4]), states:
The Riemann Hypothesis holds if and only if N T ρ = { 0 } .
Its kernel function ρ L 2 ( 0 , 1 ) 2 defined by the fractional part of the ratio ( y / x ) is continue almost everywhere, the discontinuities in ( 0 , 1 ) 2 consisting in a set of numerable one dimensional lines of the form y = k x , k N , being of Lebesgue measure zero. The integral operator is Hilbert-Schmidt ([2]) and so compact, allowing us to consider its approximations on finite dimension subspaces ([3]).
The entries in the diagonal matrix representation M h ( T ρ h ) of the finite rank integral operator T ρ h are given by:
d k k h = Δ h , k Δ h , k ρ ( y , x ) d x d y , and valued (see also [1]) as follows:
d 11 h = h 2 ( 3 2 γ ) / 4 ; d k k h = h 2 2 ( 1 + 2 k 1 k 1 l n ( k k 1 ) k 1 )
for k 2 , where γ is the Euler-Mascheroni constant (≃ 0.5772156...). The formula (9) has been computed using for the fractional part the suggestion found in [4]: for 0 < a < b < 2 a , { b / a } = ( b / a ) 1 . Then,
Δ h , k Δ h , k ρ ( y , x ) d x d y = Δ h , k Δ h , k ( y / x ) d x ( k 1 ) h y d x d y .
The sequence from (9)
f ( k ) : = h 2 d k k h = ( 1 + 2 k 1 k 1 l n ( k k 1 ) k 1 ) / 2 is monotone decreasing for k 2 and converges to 0.5 for k . For k 2 , we have: d k k h > 0.5 h 2 > d 11 h . Then:
α h ( T ρ h ) = h 2 d 11 h = ( 3 2 γ ) / 4 > 0 , n 2 , n h = 1 .
showing that the finite rank approximations of the integral operator have the sequence of the positivity parameters inferior bounded.
Theorem 3. 
(Finite Rank Approximations): The Alcantara-Bode equivalent of RH holds.
Proof. 
From (10) results that the sequence of the positivity parameters of the finite rank operator approximations T ρ h on the dense family F is inferior bounded, α h ( T ρ h ) being a constant mesh independent. Then, N T ρ = { 0 } is obtained from Lemma 1 (or Theorem 2). □
We use now the method covered by Lemma 2 (see also [1], Injectivity Criteria). The integral operator T ρ is (strict) positive on S h F , n 2 , n h = 1 with the parameter valued from (8) and (10),
α h ( T ρ ) = h α h ( T ρ h ) = h ( 3 2 γ ) / 4 0 with n .
In order to apply Lemma 2, we should invoke the adjoint operator of T ρ whose kernel function is ρ * ( y , x ) = ρ ( x , y ) ¯ = ρ ( x , y ) . For v h = k = 1 , n c k I h k S h
T ρ * v h = k = 1 , n c k Δ h , k ρ ( x , y ) I h k ( y ) d y = k = 1 , n c k Δ h , k ρ h , k ( x , y ) d y ,
where ρ h , k = I h , k ( x ) ρ ( x , y ) I h , k ( y ) . Follows:
T ρ * v h 2 = k = 1 , n c k Δ h , k ρ h , k ( x , y ) d y , j = 1 , n c j Δ h , j ρ h , j ( x , y ) d y
= k = 1 , n c k c k ¯ Δ h , k Δ h , k ρ ( x , y ) I h , k ( y ) d y 2 I h , k ( x ) d x .
Because ρ ( x , y ) is valued in [0,1), ρ ( y , x ) < 1 for every x , y ( 0 , 1 ) , we obtaining:
T ρ * v h 2 k = 1 , n c k c k ¯ h 3 = h 2 v h 2 and, T ρ * v h h v h .
Taking ω h ( T ρ * ) = h , the injectivity parameter of T on S h is given by:
μ h = ( 3 2 γ ) / 4 , a mesh independent constant n , n h = 1
Theorem 4. 
(Injectivity Criteria): The Alcantara-Bode equivalent of RH holds.
Proof. 
Because μ h is a constant (see (11)) for any h , n h = 1 , applying Lemma 2 we obtain N T ρ = { 0 } . □
Proposition. 
From Theorem 3 or Theorem 4 we have N T ρ = { 0 } , meaning that half from Alcantara-Bode equivalent of RH holds. Then, the other half should hold, i.e.: the Riemann Hypothesis is true.
Observations.
We considered the subspaces S h spanned by indicator of semi-open intervals functions of a partition of the domain and so, the subspaces are including ( S h S h / 2 ) providing the monotony of the positivity parameters. If we take instead the indicator open-intervals functions for generating the subspace S h o as well of the indicator closed-intervals functions generating the subspace S h c , n h = 1 , n 1 then both sets S o and S c are dense like S, easy to show ([11]). Moreover, because on any level of discretisation the support of the corresponding indicator intervals from S h , S h o , S h c differ only by the sets of the subintervals end points, a finite number and so of measure Lebesgue zero, all the estimations and results obtained for the dense set S are valid for the dense sets S o and S c . See [11] for more details.
The dense sets S and S c have been used in [5] and respectively [6] for obtaining optimal evaluations of the decay rate of convergence to zero of the eigenvalues of Hermitian integral operators having the kernel like Mercer kernels ([9]).

Acknowledgments

With this version of the preprint, we ended our investigations on the injectivity of the linear bounded operators on separable Hilbert spaces, focusing on proving the Alcantara-Bode equivalent formulation of RH. The observations below copied ’as is’ were obtained running AI Adobe Acrobat Assistant against plagiarism and key methods used.

Conflicts of Interest

No Competing Interests.
The references [13-16] are related to other RH equivalents, [8] to exotic integrals and [12] to multi-level discretizations on separable Hilbert spaces.

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