1. Introduction
Just as the existence of unknown elementary particles is predicted in the world of elementary particles, there may also be unknown numbers in mathematics. The goal of this paper is to introduce and discuss unknown numbers. In this paper, this unknown number is called the dark numbers. Unknown numbers can be likened to dark matter in physics. The set of dark numbers and ordinary numbers is called the Mother numbers. The biggest feature is that a differential concept exists in the world of Mother numbers. That is, a Mother number can be differentiated by a dark number. Note that since ordinary numbers are included in the Mother number, a Mother number can not be differentiated by an ordinary number. Therefore, this differentiation is called a partial differentiation.
We will explain the reason for introducing the concept of Mother numbers. Kurokawa is studying absolute mathematics in order to challenge the Riemann hypothesis [1]. In particular, Kurokawa has studied the concept of absolute differentiation, which is differentiation by a prime element on a monoid [1]-[3]. Kurokawa’s absolute differentiation satisfies the Leibniz rule but does not satisfy linearity. We would like to make Kurokawa’s absolute differentiation also satisfy linearity. By extending the concept of number to Mother numbers, we can make it satisfy linearity. This also extends the Kurokawa’s category of monoid to the category of commutative ring.
The Mother number considered in this paper is a countable set, and therefore it is a discrete concept. Because of these properties, we want to develop continuous mathematics in discrete mathematics. This corresponds to turning classical physics into quantum physics. Let us explain the Mother number below.
Gotyou has described the concept of elementary Mother space [4]. Gotyou has explained that there are the following types of elementary Mother space:
In this paper, we will limit our discussion to the elementary Mother space of type
.
Let us explain about elementary Mother space of type
.
The generating function of the sequence
is
We substitute a set
for variable
. We also replace sum
with direct sum
of sets,
with direct product of sets
, divide it in
with the action of permutation group
in direct product of set
. Hence we have
In this paper, this
is called elementary Mother space.
We introduce the set
different from the usual set of natural numbers
. However, 1 is a common, ordinary 1. We will call
the set of dark natural numbers.
is the monoid. Note that
and
are monoid isomorphisms.
The elementary Mother space of
is the following.
For any unordered pair
, we define the element of
as follows.
By defining the commutative product
and the commutative sum
of the set
, it becomes a commutative semiring
(cf. Section 3).
We introduce the set
different from the usual set of rational integers without zero
. We will call
the set of dark rational integers. However, ±1 is a common, ordinary ±1.
is the monoid. Note that
and
are monoid isomorphisms.
The elementary Mother space of
is the following.
For any unordered pair
, we define the element of
as follows.
By defining the commutative product
, sum
and difference
of the set
, it becomes a commutative ring
(cf. Section 3).
Each piece
and
of
and
is producing a new number
.
Each piece of
and
is only a set with new elements
, but the set
of the entire union of each piece is commutative semiring and the set
is commutative ring.
Furthermore,
contains a natural total ordering structure
. We write
, which is a totally order semiring. And
contains a natural total ordering structure
. We write
, which is a totally order ring (cf. Section 4 and 5). These are the new totally order semiring and totally order ring corresponding
and
.
The reason for considering
is as follows. The coefficient
that appears
in the expansion of
corresponds to the fact that the permutation group
is invariant with respect to
. This means that the resulting ring is commutative. In this paper, we will only discuss commutative rings. Furthermore, although the mother number can be defined without using the notation of
, using the notation of
allows us to express various examples in a unified manner (cf. section 3).
Using
as an example, we will explain what kind of number Mother number is,
According to this decomposition,
is
Ordinary numbers in the set
are grouped as follows.
Dark numbers in the set
are grouped as follows.
Both dark prime and dark prime element are numbers that can not be factored into prime factors.
For example, it is
,
,
,
.
Primes in set
of Mother numbers are grouped as follows.
For example, it is
One of the advantages of introducing
and
is that they have the following properties.
There are monoid isomorphisms
,
. Kurokawa’s absolute differential exists for these four monoids. Absolute differentiation satisfies the Leibniz rule but does not satisfy the linearity. It is a nonlinear differential (cf. [1]-[3]).
We want to linearly extend the nonlinear absolute differential on
. For this purpose, linear differentiation can be defined by extending the concept of number to
. The same goes for
(cf. Section 7).
We put
and
. Furthermore, the quotient field of the commutative ring
is written as
.
In this paper, we will consider the following expansion of numbers.
We examine various arithmetic, algebraic and geometric properties of
,
and
. We also discuss the algebraic extension of
and the algebraically closed field
.
Each section of this paper is organized as follows.
Section 2 briefly reviews monoids and absolute algebras. Section 3 defines commutative semiring
and commutative ring
. And we will introduce various examples of elementary Mother spaces and elementary Mother number spaces. In Sections 4 and 5, we rewrite
and
as isomorphic objects to improve the clarity of the discussion. We also define a total order structure into them. Section 6 describes the fundamental theorem of number theory and the division theorem in
. In Section 7, we define the differential concept on
,
and the Mother Pythagoras filed
. There are two important concepts of differentiation. One is point differentiation and the other is functional differentiation. Sections 8, 9 and 10 are the applications in this paper. In Section 8, we define partially differentiable Riemann manifolds with metric topology on
. In Section 9 and 10, we construct the ABC type conjectures about
,
and the Mother algebraic extensions of
denoted by
. We also introduce the Diophantine type equations related to the concept of this paper.
2. Monoids and Absolute Algebras
We explain the monoids and the absolute algebras by Kurokawa (cf. [1]-[3] [5]).
Let
and
be the set of all natural numbers and rational integers, respectively.
Definition 2.1. A monoid
will be a semigroup with identity element
. An absolute algebra
will be a monoid with zero element
,
Example 2.1.
is the monoid. The corresponding absolute algebra is
.
Example 2.2.
is the monoid. The corresponding absolute algebra is
.
Example 2.3.
is the monoid. The corresponding absolute algebra is
.
Example 2.4.
is the monoid. The corresponding absolute algebra is
.
In general,
is considered (cf. [1]).
Example 2.5.
is the monoid and
is the absolute algebra.
Kurokawa has defined the following interesting monoid.
Example 2.6. The
are ordinary primes. Then we define
If
then
. Hence
becomes the monoid.
Example 2.7. The
are ordinary primes. Then we define
If
then
. Hence
becomes the absolute algebra.
Then the following important monoid isomorphic expression holds.
3. Mother Number Ring
and Mother Number
Semiring
Let
be a vector space over a field
. Let
be a symmetric tensor algebra.
, defined below, is similar to
. The difference is that
can be a general set. Also, products and sums are different. The product of
is a tensor product, and the sum is a direct sum.
Elementary Mother space is defined as follows [4].
where
is the permutation group and we can set
and
.
For example,
means for
, it is as follows.
.
The following example is from Nakajima [6].
Definition 3.1. We define the set
as the set of dark natural numbers and also define the set
as the set of dark rational integers.
±1 are common to ordinary natural numbers and rational integers.
For the product
of elements of
,
is the monoid.
For the product
of elements of
,
is the monoid.
Below, we define two examples of the most basic elementary Mother number space in this paper.
The elementary Mother number space of
is defined as follows.
For any unordered pair
, we define the element of
as follows.
By defining the product and sum of the set
as follows, it becomes a commutative semiring
.
for any
,
.
The identity element for the product
is
.
The identity element for sum
is
.
The elementary Mother number space of
is defined as follows.
For any unordered pair
, we define the element of
as follows.
By defining the product, sum and difference of the set
as follows, it becomes a commutative ring
.
for any
,
.
The identity element for the product
is
.
The identity element for sum
is
.
The inverse of
with respect to the sum
is
.
Each piece
and
of
and
is only a set with a new number
, but the set
of the entire union of each piece is a commutative semiring, and the set
is a commutative ring. We also define as follows.
and
This generally turns out to be
Proposition 3.1.
is a subsemiring and
is a subring.
Proof. Let us consider that
is a subset of
. If it can be shown that it is a subset, it is trivial that it is subsemiring. For any
, the special element
can be calculated and
, and
is in
. Therefore,
is a subset of
. The same applies to
.
Below, we will discuss various examples of elementary Mother spaces other than those mentioned above.
For the monoid
, it can be expressed as follows.
This is written as
.
For the monoid
, it can be expressed as follows.
This is written as
.
As we will see in section 5,
and
are subrings of
.
The following eight examples are obtained by taking the mother number
of a known monoid
for a known commutative ring or commutative semiring.
For the monoid
, it can be expressed as follows.
The following semiring isomorphism holds
For the monoid
, it can be expressed as follows.
The following ring isomrphism holds
For the monoid
, it can be expressed as follows.
The following ring isomorphism holds
For the monoid
, it can be expressed as follows.
The following ring isomorphism holds
Examples of the
and
show that
and
are hidden in the underground structure of
and
. This is an example of the importance of Kurokawa’s philosophy of absolute mathematics (cf. [1]).
For the monoid
, it can be expressed as follows.
The following ring isomorphism holds
For the monoid
, it can be expressed as follows.
The following semiring isomorphism holds
Let us introduce yet another example.
A polynomial ring with one variable or infinite variables can also be constructed as an elementary Mother space as shown below.
For the monoid
of indefinite element
, it can be expressed as follows.
The following ring isomorphism holds
For the monoid
with infinite number of indefinite elements
, the following ring isomorphism holds.
Furthermore, the elementary Mother spaces of groups
,
and
with respect to the product are respectively
,
and
which are fields.
As we can see from these examples, it can be seen that the monoid before taking the elementary Mother space representation is an extremely basic object. By taking the elementary Mother space representation of the monoid, natural sums and differences can be added. In order to obtain a new number concept, we introduced new monoids
and
.
Let us introduce another interesting example of elementary Mother space.
For monoid
,
is a monoid ideal if
,
then
.
Monoid ideal
is a monoid prime ideal if
then
.
Kurokawa thought of the following [5].
is a set of monoid prime ideals of monoid
. Then the monoid prime ideals of
are
and we know that
.
Lemma 3.1. For the set
of ordinary primes, elementary Mother space is
Then we have
Proof. We identify the following.
,
, in particular
,
, in particular
and
. The same applies below.
We define the sum
as follows.
The identity element for the sum is
. Therefore, we have
. This is a Zariski topological monoid for the sum.
On the other hand,
is only a Zariski topological space and does not contain a monoid structure for the sum.
4. Rewriting Equivalent to Mother Number Semiring
and Total Order Structure
In this section we will give an expression equivalent to
. It turns out that
is a polynomial semiring. However, it can be seen that total order structure is different.
Definition 4.1
where
except for a finite number is zero.
From now on,
will be abbreviated as
.
For the set
, the product
and the sum
are defined as follows.
Hence
becomes the commutative semiring.
Note that
can be calculated and
, and
is an ordinary number. On the other hand, for example,
is a single number and can not be calculated any further.
Lemma 4.1. The following semiring isomorphism holds.
Proof.
where,
are dark primes and
,
,
,
.
is finite.
We write this as
.
Integer partitions of
is as follows.
is the set in which all integer partitions of
are treated as different elements. Then, as shown above, it becomes commutative semiring due to the inclusion of natural products and sums.
If we rewrite this using our symbols, then it becomes the following.
The equivalence of (1), (2), (3) in the following Lemma 4.2 is a well-known fact (cf. [7]).
Lemma 4.2. The following four are equivalent as a set.
(1) The partitions of positive integer
.
(2) Yang diagrams of
.
(3) Type of conjugate class of symmetry group
.
(4) The piece
of
.
From Lemma 4.2, we can see that
is the set of all
in (1), (2) or (3).
The set
has the following total order structure.
It can be seen that
is in the total order semiring. We write this as
.
5. Rewriting Equivalent to Mother Number Ring
and Total Order Structure
In this section we will give an expression equivalent to
. It turns out that
is a polynomial ring. However, it can be seen that total order structure is different.
From now on,
will be abbreviated as
.
Definition 7.1. For the set
we extend
to
. Therefore, it is defined as
For the set
, the product
, the sum
and the difference
are defined as follows.
Hence,
becomes the commutative ring.
Note that
can be calculated and
, and
is an ordinary number. On the other hand, for example,
is a single number and can not be calculated any further, just like
.
Lemma 5.1. The following ring isomorphism holds.
Proof. The proof is similar to Lemma 4.1.
We write this as
.
We define the map
For example,
,
,
,
.
The map
is called the cardinal evaluation map.
The set
has the following total order structure.
Definition 5.2. The total order structure of
is defined as follows.
Assuming that
,
and
are satisfied, the total order relation of
is defined by the following procedure.
(1)
(left side) <
(right side).
(2) If it satisfies
(left side) =
(right side)
(I), then
(3) If it satisfies (I) and
(II), then
(4) If it satisfies (I), (II) and
(III), then
Hereafter repeat in the same way.
The total order structure of
mentioned earlier is included in Definition 5.2.
The quotient feild
of
is also a totally ordered set, same as
is a totally ordered set.
Example 5.1.
Lemma 5.2. The ordinal number of
is
, and the ordinal number of
is
.
Proof. The sequence of numbers in
is as follows.
Hence, the ordinal number of
is
. It is trival that the ordinal number of
is
.
We write this as
.
Proposition 5.1. For
, the following isomorphism as a commutative ring holds.
Here, the element of
is a polynomial with respect to a finite number of variables among
, but we can consider polynomials with as many variables as we like.
Proof.
is subring. The element of
are commutative with all elements of
.
When we write
,
is called an element of
obtained by substituting
for
.
The substitution map
is a surjective ring homomorphism, that is
is the smallest subring of
that includes the elements of
and
, and it can be written as follows.
From the ring homomorphism theorem, we have
When
, it becomes
. It is clear that
that satisfy
do not exist. Hence, we have
and
For example, the following can be considered
,
and
etc.. This is collectively written as
. Increasing the dark prime variable,
,
,
,
,
etc. are also possible. These are all subrings of
.
Proposition 5.2. The commutative ring
and polynomial rings of infinite variables are not totally order isomorphic.
Proof.
is usually considered in lexicographical order. On the other hand,
enters the total order structure according to Definition 5.2. Therefore, the two are different. Let us give you a counterexample. We consider the following mapping.
Although it is
, it becomes
. Therefore,
is not totally order isomorphic.
6. Fundamental Theorem of Number Theory and Division Theorem
From now on, we will often write symbols that equate
with
and
with
.
For example, we write
as
and
as
.
Lemma 6.1.
and
has an infinite number of dark prime elements.
Proof. The proof is trivial.
The following analogy to the fundamental theorem of number theory holds.
Theorem 6.1.
,
can be factorized into prime factors, which are unique.
Proof.
,
. If
is an irreducible element, leave it as is. If
is not irreducible,
. If we repeat the above,
.
Let
. Since
, then
. Since
is also a prime element,
divides either
. Even if
divides
, generality is not lost. Since the prime element is an irreducible element,
and
are irreducible elements, so
. Therefore, dividing
by
,
. If we repeat this
,
,
,
. In other words, uniqueness is established. Therefore
is a unique factorization domain.
is also a unique factorization domain.
Definition 6.1. An integral domain
is called a Euclidean domain if it satisfies the following conditions. There exists a mapping
, for any
,
. Then there exists
that satisfies the following.
(6.1)
Examples:
When
, if
, then
is a Euclidean domain.
When
with field
, if
, then
is a Euclidean domain.
is not a principal ideal domain, so it is not a Euclidean domain.
and
are also not Euclidean domains.
Lemma 6.2.
is not a Euclidean domain.
Proof. There is an example in which mapping
does not satisfy
for
,
. The counterexample is if
,
then it can divide
, but
,
. Hence
.
Example 6.1. The following example can be considered for
,
or
.
(1)
,
.
,
.
(2)
,
.
,
.
(3)
,
.
,
.
(4)
,
.
,
.
(5)
,
.
,
.
(6)
,
.
,
.
Although
is not a Euclidean domain, the following division theorem holds.
Theorem 6.2. For any
,
, there exist
that satisfy
(6.2)
The uniqueness does not hold. The division theorem does not hold for
.
Proof.
: We will show by induction on
. If
, we set
.
When
, regarding
less than
, we assume that
exists that satisfies
(6.3)
If
, then
. If
, then
. Therefore, by assumption (6.3), there exists
such that
,
. If we rewrite this, then
. Hence, if we set
,
, (6.2) holds.
:
since
, as shown above, there exist
,
such that
At this time, if
, then
and
,
. If
, then
Therefore, it should be
,
.
We give a counterexample in which uniqueness does not hold.
As we can see from this counterexample, the division theorem does not hold for
. To satisfy this theorem, we must use the difference
. But there is no difference
in
.
Lemma 6.3.
is not Euclidean algorithm.
Proof. The definition of the Euclidean algorithm is that
holds for
,
. When this is repeated, the remainder at the end becomes zero. However, this
does not become
at the end.
For example, we consider the case when
and
.
,
.
,
.
,
.
It stops here. If we calculate further than it becomes
.
Remark 6.1. (1) For any
, if
is monic, then it satisfy
For any
, even if
is monic, then it does not satisfy
For example, the first equation of Example 6.1
is a counterexample for
.
(2) The essential difference between
and
is that they are not totally order isomorphic according to Proposition 5.2. The ordered structure of
and
is lexicographical order
, and
and
have an ordered structure such as
. In other words, the structure of division is different. Also, for
, the sum
, the difference
, the product
and the quotients
and
can all be computed no further. On the other hand, for
, the sum
, the difference
, the product
and the quotient
,
can all be calculated.
While
and
are formal indeterminate elements without individuality,
and
are dark primes with individuality. Therefore, these two essentially different.
(3) For
,
,
,
are principal ideals.
,
,
are prime ideals that are not principal ideals.
is a maximal ideal. Therefore,
is not a principal ideal domain. This gives another proof of Lemma 6.2.
Problem.
Determine the structure of affine scheme
.
7. Derivation of Points and Derivation of Functions
The following definition of a Pythagoras field is well known.
Definition 7.1. Let
be a field. For any
, the extension field
is called Pythagoras extension of
. When all Pythagoras extensions of
coincide with
,
is called a Pythagoras field.
is a Pythagoras field if the Pythagoras theorem always holds for any element in
.
We define the quotient field (localization) of
as
. In general, a completeness uniquely exists in the metric space
.
is defined by the Archimedean metric
. Let
be a completion of
with respect to
.
is the set of Mother real number.
corresponds to
This algebraic number and Mother algebraic number do not include
. We put
is an example of a Mother Pythagoras field. From now on, we will focus on this
.
The following Definition 7.2 is well known. We will omit the details (cf. [8]-[11]).
Definition 7.2. Let
be a commutative ring.
is
-algebra and
is
-module. Then the
-derivation
is a map
and this derivation satisfies the following three conditions:
(1)
,
: Leibniz rule.
(2)
,
: Linearity.
(3)
,
.
We denote the set of
-derivation as
. When
, we write
.
The following is a well-known typical example.
Example 7.1.
,
.
The property corresponding to (3) is
In general, it is important that
is unrelated to the elements of
.
First, we consider the case when
,
.
Definition 7.3. Let
be a dark prime in
.
(I) We can define the set of derivation as
Note that since
except for a finite number of
for each
.
is a finite sum.
is the finite direct sum.
(II) Furthermore, the dual space of
is defined as follows:
and
Combining Definition 7.2 and Definition 7.3, we can see the following.
Differential with a dark prime
on
is defined as follows.
For any
, we have
These are indicating that the Leibniz rule is satisfied and that the operation is linear. This is the derivation of the elementary Mother number ring
.
Remark 7.1. We will answer the question of whether
are sufficient without introducing dark numbers such as
. For example, let
, which is
, be an ordinary number. Using linearity, the left side becomes
On the other hand, the right side becomes
So this is a contradiction.
The differential that satisfies only the Leibniz rule and does not require linearity is called Kurokawa’s absolute differential [1]-[3]. It is known that with absolute differentiation, the elements of
can be differentiated by ordinary primes.
The following definition is the most general differentiation of points.
Definition 7.4. Differentiation of points: Let
be a general point in
.
In particular, we add the following to the definition:
For
, we define
for all
.
It satisfies Definition 7.2 (1) and (2), but it satisfies Definition 7.2 (3) for
,
.
Example 7.2. For an element
, we calculate as follows.
,
,
,
,
,
,
,
.
Let us explain the differentiation of composite points.
Definition 7.5. A composite of
,
is
. Then we have
Example 7.3. Two-variable composition of two variables:
For an element
in
, we calculate as follows.
,
,
,
,
We can define the differential formula for the quotient element for
,
.
Definition 7.6. Differentiation of polynomial functions:
Let
be a polynomial ring with coefficients in the Mother Pythagoras field
.
The elements
are related to the elements of
, that is
. Then we define that
if
, then
is not well-defined and if
, then
is well-defined, that is
if
is well-defined then
is well-defined.
Although it does not satisfy Definition 7.2 (3), but it does satisfy Definition 7.2 (1) and (2).
Example 7.4. When
, for
,
, we calculate as follows.
For
, then
and
for
and
, then
.
For
, then
.
For
, then
.
We derive the differentiation of function on
from Definition 7.6 and its derivatives and differential coefficients.
Let
be the Mother Pythagoras field and
be a coordinate function. We denote all functions
as
.
Definition 7.7. Differentiation of functions:
For any
, we define that
if
, then
is not well-defined and if
, then
is well-defined. We also define that
(1) When
is not equal to the coefficient
of
, we define
is derivative.
(2) When
is not equal to the coefficient
of
, we define
is differential coefficient, where
.
In particular, when the function is continuous at
, we define the following independently of point differentiation:
(3) When
is equal to the coefficient
of
, we define
is differential coefficient.
The differentiation can not be well-defined at
. Therefore, we denote partially differentiable functional ring as
(cf. Definition 8.2).
Very important:
Although we have defined two differentiations which are point differentiation (Definition 7.4) and function differentiation (Definition 7.7), the point differentiation takes precedence. In other words, function differentiation can be considered only after the point differentiation has been defined.
For example, when
, let
. The differential coefficient at
appears in two forms:
and
.
By prioritizing the latter, we achieve internal consistency in the differential calculation. Furthermore, when dealing with discrete objects, point differentiation should be prioritized. See also Appendix B.
Let us look at the following example.
Example 7.5. For a function
, its derivative and differential coefficient are as follows.
(1) When
,
is derivative.
(2) When
,
is differential coefficient.
In this case, we define that the following also holds:
(3) When
,
is differential coefficient.
is not considered. Differentiation at
uses point differentiation, that is,
is adopted.
Point differentiations take precedence over functional differentiations, so the following must be satisfied.
not well-defined,
.
8. Partially Differentiable Riemann Manifold
Let
and
be the Pythagoras field and the Mother Pythagoras field. Let
be the Cartesian product of
elements of
, and
be the Cartesian product of
elements of
.
and
are n-dimensional with respect to the Zariski topology. However, in this paper, we consider the metric topology. We define the metric as follows:
is a metric topological space. Continuous mappings and homeomorphisms for
can be defined in the same way as in the classical case. Topology of
can be understood as Hausdorff but non-connected. As a topological space,
has dimension zero. However, as a vector space, it has dimension
. Focusing on this, when defining the following manifold, we consider that the dimension of the tangent vector space = the number of linearly independent tangent vectors.
The philosophy is to understand the manifold by understanding the tangent space.
The important conclusion of this paper is that, as we will see in Definition 8.1 below, if the point differentiation of Definition 7.4 can be defined, then dimension arises even in non-connected topological spaces.
Definition 8.1. A metric topological space
is called
-dimensional partially differentiable manifold as
model (
) if it satisfies the following three conditions.
(1)
is the family of open subset on
.
(2) For any
,
is the open set of
and
is homeomorphic, where,
is the induced topology of the metric topology
, and
has the inverse image topology
.
(3) For any
,
, the coordinate transformation
is homeomorphic.
Moreover, when the number of definable linearly independent derivatives of
is
,
is called partially diffeomorphic.
From now on, we will also write
.
Example 8.1. The sphere on
is 0 or 1 or 2-dimensional partially differentiable manifold.
Proof.
produces the decomposition
Suppose that
,
,
.
This
and
are open sets. If
, then we have
and
,
,
,
,
,
.
is the partially diffeomorphic for any
. The same applies to
.
When
,
,
can be defined, but
cannot. Therefore, the manifold is
.
When
, both
and
cannot be defined,
is not partially
diffeomorphic. The manifold is
. Note that while
is a two-point set but
is an infinite set of
points.
Definition 8.2. A function
on the
-dimensional partially differentiable manifold
as
model is partially differentiable function as follows.
For any coordinate neighborhood
,
is a partially differentiable function on
, where
is the inverse mapping of
.
We write all of partially differentiable functions on
as
.
is called the partially differentiable functional ring on
.
Let
be the
-dimensional partial differential manifold of the
model.
We define
-dimensional tangent space
,
as follows:
When
,
, if we put
, then we have
is the Jacobi matrix.
Let
be the positive inner product of
,
;
Performing calculations exactly as in classical theory, we obtain
is a Riemann metric on a partially differentiable manifold
,
are called partially Riemannian manifolds.
Example 8.2. From Example 8.1, let
and
. Then, let us set the following:
When
,
, i.e., when
, we have
The left-hand side represents the Riemannian metric on
induced by
, and the right-hand side represents the Riemannian metric on
obtained by projecting
onto
by stereographic projection.
is Riemann metric on
. When
,
,
,
, we can see that
is a Riemannian metric over
.
In the classical circle
,
is a Riemannian metric. When
,
, i.e., on
, there is no Riemannian metric.
We next define the affine algebraic variety (cf. [9] [10]). For the following definition of affine algebraic variety, we use Definition 7.6 to define the derivation.
Definition 8.3. The algebraic set is defined by
The coordinate ring is defined by
where
Then the affine algebraic variety is defined by
Definition 8.4. For a subset
of
,
is open set
is algebraic set,
that is, ideal
exists and satisfies the following
. This is the Zariski topology of
.
Example 8.3. (1)
This is the 0 or 1-dimensional sphere
(
).
(2)
Assume that
is cubic or higher and does not have multiple solutions. They are the Mother elliptic curves and Mother hyperelliptic curves. It is an interesting problem to investigate these in detail.
Example 8.4. The differentiation follows Definition 7.6. If
is well-defined, then
is computable. For example, for
, the derivative of
is
.
The differential coefficient at
is
.
The differential coefficient at
is
.
9. ABC Type Conjectures and Diophantine Type Equations
Let
,
or
be a prime element. Then we define
The following results use references [12]-[15]. First, we will describe the polynomial version of the ABC theorem by Stothers and Mason [16] [17].
Theorem 9.1 (Stother-$Mason). Let
be a field. For any functions
,
,
.
. Then
implies
The proof uses the differentiation of
and
with respect to
.
Theorem 9.2 (Mochizuki, ABC Theorem on
). Suppose that
.
. Then
implies for any
,
exist such that
This is the famous ABC conjecture of
. Below, we will write the ABC conjectures for
and
.
From now on, we write
.
Conjecture 1 (ABC type Conjecture on
). Suppose that
and not
and
.
. Then
implies
Conjecture 2 (ABC type Conjecture on
). Suppose that
and not
and
.
. Furthermore, suppose that
. Then
implies
Remark 9.1. As mentioned in Section 6, there are elements
or
. Suppose that
. When
,
,
for
,
is maximum at
. Because
,
, we see that
Therefore,
satisfies
. Since
is arbitrary, there are an infinite number of
. Hence, in this case, the ABC type conjecture has no meaning. On the other hand, there is no problem when
. The usual ABC Theorem of
and
are essentially equivalent but ABC type conjecture of
and
are essentially different for the reasons explained above.
These conjectures may be possible to use differentiation, as in Theorem 9.1. Therefore, they are expected to be easier to prove than the usual ABC Theorem 9.2. Theorem 9.2 on
does not have the concept of differentiation. This is one of the reasons why it is considered difficult. However, Conjecture 1 and Conjecture 2 on
and
have the concept of differentiation. In the case of original ABC theorem 9.2, it means that multiplication and addition are intertwined, but in Conjecture 1 and Conjecture 2, it is predicted that multiplication and addition are not very intertwined.
The following also holds for Pythagorean triplets:
Lemma 9.1. Suppose that
and
.
For
, there are an infinite number of Pythagorean numbers and it can be written as
Proof. The proof is exactly the same as the classical
case.
Furthermore, we would like to introduce Conjectures 3 to 7 below. Conjectures 3 to 7 are proved using Conjecture 1 and Conjecture 2, so this may not be meaningful, but what we want to say here is that they are much easier to prove than the classical case, which is proven using the original ABC theorem 9.2. Also, solving Conjecture 1 and Conjecture 2 will solve many problems for us, so we believe there is value in solving Conjecture 1 and Conjecture 2.
Conjecture 3 (Fermat-Catalan type Conjecture). Suppose that
,
, and not
and
.
. If
then there are no pairs
that satisfy
Contrary to this result, classical theory suggests that a finite number of them exist.
Proof. When
, it is Fermat type conjecture. Using ABC type conjecture 1, we prove Fermat-Catalan type conjecture. We have
From ABC conjecture 1, we see that
Hence, we have
Therefore, this is a contradiction. Hence,
does not exist.
Conjecture 4 (Darmon-Granville type Conjecture). Suppose that
,
,
and not
and
.
. Furthermore, suppose that
and
Then there are a finite number of pairs
that satisfy
Classical theory also suggests that a finite number of them exist.
Proof. It can be assumed that
. Using ABC type conjecture 2, we see that
From
, so
is bounded. Hence,
are a finite number.
Conjecture 5 (Tijdeman-Zagier type Conjecture). Suppose that
,
, and not
and
.
. Then there is no set
that satisfies
Classical theory also suggests that they do not exist.
Proof. When
, it is Fermat type conjecture. Since it is
the condition of Fermat-Catalan type conjecture 3 is satisfied. Therefore, form Fermat-Catalan type conjecture 3,
does not exist.
Conjecture 6 (Peyre type Conjecture). Suppose that
,
and not
and
. Assume that
,
,
. Then there are a finite number of pairs
that satisfy
Classical theory also suggests that a finite number of them exist.
Proof. Suppose that
,
,
. Then we have
From ABC type conjecture 1, we have
and
Hence, we have
By taking the product of these, we see that
From
the maximum value of
is
, so we have
Hence, we have
so
Therefore, we see that
is finite.
Conjecture 7 (strong Hall type Conjecture). Suppose that
,
,
,
and not
and
. Then the following inequality is satisfied
In classical theory,
,
is constant, is satisfied.
Proof. Hall-Lang-Waldschmidt-Szpiro conjecture is that
if
then
and
.
We will first show this using the ABC type conjecture 1. Then we have
and
Using
we have
When
, we have
Hence, we have
Corollary 9.1. There is no solution
to Thue equation
, Pell equation
and Catalan equation
.
Proof. The left side of this three equations is a dark composite number and the right side is 1. It is clear that calculating the left side does not result in 1.
10. ABC Type Conjecture for Mother Algebraic Number Fields
A finite extension field of
is called a Mother algebraic number field and is denoted by
. Next, we will formulate the ABC type conjecture for Mother algebraic number fields
. At that time, new integral domains and fields will naturally appear, as described below.
is a well-known fact. In our case, such a relationship does not hold.
is not a finite field, but an infinite set and an integral domain.
and
are local rings, and the only maximal ideals are
and
, respectively. Then the following holds.
The quotient field of
is defined by
Then it can be seen that
The new rings and fields appear as shown above.
Definition 10.1. (cf. [8]) Let
be a Mother algebraic number field and
be a prime element.
(1)
(2)
This
is called additive valuation. Sometimes it is written as
.
Definition 10.2. (cf. [8]) Let
be a Mother algebraic number field.
(1)
(2)
(3)
This
is called non-Archimedean normal valuation.
is a distance.
is a valuation ring.
is a maximal ideal of
.
is a local domain and principal ideal domain with
as the maximal ideal.
is residue field.
is a quotient field of
and
is an integral domain, so
is a field, which is a quotient field of
.
is a discrete valuation ring. Maximal ideal
is a principal ideal
. A fractional ideal of
is
,
. In particular, any nonzero element
of the field
is written as
where,
is a unit of
and
. The way
is taken is not unique. However,
is unique regardless of how
is taken.
Example 10.1. When
,
is a prime element of
.
If
,
,
, then we have
.
In this case, it becomes as follows.
,
,
,
, A residue field
. The quotient field of
is
.
We summarize as follows.
We extend the above example to the finite extension field
.
is a Mother algebraic number field.
is the integer ring of
.
is a prime ideal of
.
is integral domain.
is a quotient field of
.
is a prime ideal of
.
Example 10.2. When
, we have the following.
Let us consider the case where
is a finite place, which is equivalence class of non-archimedean valuation. In this case, the place
of
is as follows.
We define
as ramification index and
as residue degree. We also define the norm as
.
From
and
, normal valuation
is
Example 10.3. When
and
, we will consider when
.
Then residue degree
is
is not like
, so
.
Since the maximal ideal
of the local ring
is a principal ideal, we write
.
In particular, for the field
and for any
,
is
is a unit of
,
. This
depends on the valuation
, so it is written as
. This
is called a local parameter.
For
, we make it correspond as follows.
Then
is called the heights on
. And we write
, where, the elements of
is called a place, the elements of
is called a non Archimedean place, the elements of
is called an Archimedean place. Note that
is
.
Based on what has been said above, we can predict that the following conjecture holds (cf. [13] [18]).
Conjecture 8. Let
be a finite extension and
be a fixed Mother algebraic field. The following inequality always hold for
and
.
where
In particular, when
, we may replace
with
.
Example 10.4.
and
.
We consider when
is
. When
,
does not exist. When
,
is
. When
,
is
.
Regarding
of
,
.
Regarding
of
,
.
On the other hand, the following holds for
.
Hence, we have
Note that when
in the case of ordinary numbers is
,
In this case, the inequality sign is reversed.
Example 10.5.
,
.
If we consider when
is
, then we have the following from the same calculation as the previous example
Note that when
in the case of ordinary numbers is
,
In this case, the inequality sign is not reversed.
Acknowledgements
I would like to thank Professor Oliver Lorscheid for his suggestions on this study. I would especially like to thank Shinichi Kakuta for his advice and encouragement during the course of this study.
Appendix
Appendix A. Blueprint and Monoid
-Module
Below, we can see that the semiring
and the ring
are examples of blueprints by Lorscheid [19].
Definition A.1 [19]
A blueprint
is a monoid
with zero together with a preaddition
, i.e.
is an equivalence relation on the semiring
of finite formal sums of elements of
that satisfies the following axioms, where we write
whenever
:
(i) The relation
is additive and multiplicative, i.e. if
and
, then
(ii) The absorbing element 0 of
is in relation with the zero of
, i.e.
(empty sum).
(iii) If
, then
as elements in
.
and
are monoids. We put
and
.
Equivalence relations are
,
whenever
and
,
whenever
, respectively.
Then
and
are the blueprints, respectively.
Given a blueprint
, we can construct the ring
, where is the ideal. Then
. Hence,
. Therefore,
is the commutative ring. Hence, we know that
.
Next, we define a monoid module.
Using
,
and
, we consider new sets
and
By defining the sum, product and difference of the set
(
) as follows, it becomes a commutative ring (semiring)
(
).
for any
(
).
For any
(
), the scalar multiple is defined by
Hence
is the monoid
-module (
is the monoid
-module).
Lemma A.1. For
and
, the following ring isomorphism holds
and the following semiring isomorphism holds
Appendix B. Further Considerations on Differentiation
We will consider the differentiation of the following three cases.
(I) Case with continuous but sharp points.
(II) Case with discontinuous points.
(III) Case with continuous points.
Definition B.1 The derivative at
is defined as follows:
In the cases (I) and (II),
, for any
.
In the case (III),
The same applies to multivariate functions
.
Example B.1. (I) Case with continuous but sharp differential:
When this
, the differential at
is
, and the equation of the tangent is
.
When this
, the derivative at
is
, and the equation of the tangent is
.
When this
, the differential at
is
, and the equation of the tangent is
.
(II) Case with discontinuous points:
When this
, the derivative at
is
. The equation of the tangent is
.
When this
, the derivative at
is
. The equation of the tangent is
.
(III) Differential at the continuous point
:
When this
, the differential at
is
. The equation of the tangent is
.