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Absolute geometry

Absolute geometry is a branch of plane geometry that derives its theorems solely from the first four postulates of Euclid's Elements, excluding the parallel postulate, thereby forming a neutral framework valid in both and geometries. This system, also known as neutral geometry, encompasses Euclid's propositions up to Book I, Proposition 28, where the parallel postulate is first invoked in Proposition 29. The axiomatic foundation of absolute geometry, as formalized by in 1899, divides into five groups: incidence, order (betweenness), , parallels (omitted in the absolute case), and continuity. Incidence axioms establish that any two distinct points determine a unique line and that any three non-collinear points determine a unique plane. Order axioms define betweenness relations, ensuring properties like the Pasch axiom for line intersections with . axioms include the side-angle-side () criterion for and the ability to construct congruent segments and . Notable theorems in absolute geometry include the (Proposition 5), which states that the base angles of an are equal, and the exterior angle inequality (Proposition 16), asserting that an exterior angle of a exceeds each of the non-adjacent interior angles. Additionally, the sum of the interior angles of a is at most 180 degrees, as proven by Legendre's theorem, with equality holding only in the case. Continuity axioms, such as Archimedes', Cantor's nested interval principle, and Dedekind's cut axiom, ensure the geometry is complete and Dedekind-complete, supporting the real number line for measurements. Absolute geometry serves as the common core for non-elliptic geometries, excluding where no parallels exist, and highlights the independence of the parallel postulate from the other axioms. It has applications in understanding the foundations of geometry and in contexts where varies.

Foundations

Definition and Historical Context

Absolute geometry, also known as neutral geometry, is the system of geometry derived from Euclid's postulates and common notions, excluding the parallel postulate. This framework allows for the development of theorems that hold true in both and geometries without relying on assumptions about . Statements proven within absolute geometry are independent of the parallel postulate, meaning they apply universally to plane geometries where the postulate is either affirmed or negated. The historical roots of absolute geometry trace back to Euclid's Elements around 300 BCE, where the first four postulates—concerning the construction of lines, circles, and right angles—were used implicitly to derive many propositions without invoking the fifth postulate on parallels. Efforts to rigorously examine the parallel postulate began in the 18th and 19th centuries, but absolute geometry emerged explicitly during the development of non-Euclidean geometries. formulated it in 1832 as the common foundation underlying both Euclidean and his newly discovered , building on ideas from his father Wolfgang Bolyai and independently from Nikolai Lobachevsky's parallel work in the 1820s. A systematic axiomatization of absolute geometry appeared in David Hilbert's Grundlagen der Geometrie in 1899, where he refined Euclid's original axioms into five groups: incidence, order, congruence, parallelism (excluding the parallel postulate), and continuity, providing a logically complete and independent basis for neutral geometry.

Axiomatic Basis

Absolute geometry is formalized through an that captures the common foundations of and geometries, excluding any postulate governing parallel lines. This framework draws primarily from David Hilbert's rigorous axiomatization in his , where the axioms are organized into groups, omitting the single axiom of parallelism (Group III). The remaining groups—incidence, order (betweenness), congruence (Group IV), and continuity—provide the basis for absolute geometry, enabling the development of theorems independent of the parallel postulate. The axioms of incidence establish the fundamental relationships among points, lines, and planes. For instance, any two distinct points determine a unique line (I, 2), and there exist at least three points not lying on the same line (I, 3), ensuring a non-degenerate plane structure. These axioms, seven in the system presented, underpin the connectivity of geometric elements without presupposing metric properties. The order or betweenness axioms introduce a linear arrangement on lines, defining when a point lies between two others. A key example is the axiom stating that for any three distinct collinear points A, B, and C, exactly one lies between the other two (II, 4), which formalizes the betweenness relation and prevents circular orders. This group, comprising five axioms, ensures consistent sequencing and separation in the geometry. The axioms address the preservation of lengths and under rigid motions, forming the basis for measurement and similarity. They include six statements, such as the side--side () : if two segments and the included of one are congruent to those of another, the triangles are congruent (IV, 6). is defined via , allowing to be carried along lines without change (IV, 4). These axioms enable constructions like equilateral triangles on given segments. Continuity axioms, often including the , guarantee the density and completeness of the geometric . The (V, 1) states that for any segments AB and CD, a finite number of copies of CD can exceed AB in length, ruling out elements. Basic versions of absolute geometry may omit fuller assumptions like Dedekind's (V, 2) to focus on first-order properties. Together with the other groups, these form a of 19 in Hilbert's formulation. An equivalent, though less rigorous, axiomatic basis appears in Euclid's Elements, where the first four postulates suffice for absolute geometry. These include: drawing a line between any two points (Postulate 1, incidence); extending a indefinitely (Postulate 2, order and continuity); constructing a with given center and radius (Postulate 3, congruence via circles); and the equality of all right angles (Postulate 4, angle congruence by transport). Euclid employed these for the initial propositions before invoking the parallel postulate. In Hilbert's system, the primitives—points, lines, planes, and the relations of incidence ("lies on"), betweenness, and (for segments and )—remain undefined, allowing in various models. This setup constitutes a theory, expressible in predicate logic with quantifiers over these primitives, facilitating proofs of consistency relative to arithmetic.

Core Properties

Basic Constructions and Incidence

In absolute geometry, the incidence axioms form the foundational structure for point-line interactions, independent of the parallel postulate. These axioms ensure a consistent framework for defining lines and their relations to points. Specifically, any two distinct points determine a unique line, and every line contains at least two distinct points. Additionally, there exist at least three points that are not collinear, guaranteeing a non-degenerate . Basic constructions in absolute geometry rely on Euclid's first three postulates, which allow for the creation of lines, extensions, and without invoking parallelism. The first postulate permits drawing a straight line between any two points, while the second allows continuous extension of a finite straight line. The third postulate enables the description of a with any and distance as . These postulates support a range of elementary constructions, such as erecting a from a point on a line (Euclid's I.11) or from a point not on the line ( I.12), and bisecting a given ( I.9). The first 28 propositions of Euclid's Elements (Book I) are provable within absolute geometry, establishing key constructions like forming an on a given base (Proposition I.1) by intersecting two circles centered at the endpoints with the base as radius. These propositions build incrementally: for instance, Proposition I.10 bisects a straight using the bisector constructed via circles, and Proposition I.22 constructs a from three given line segments provided their lengths satisfy the . Such constructions emphasize the ability to manipulate segments and angles through intersection and superposition, laying the groundwork for more complex figures without assuming parallel behavior. To ensure orderly plane configurations, absolute geometry incorporates Pasch's , which addresses betweenness and separation in the . This states that if a line intersects one side of a but passes through none of its vertices, it must intersect exactly one of the other two sides. Formally, in the context of a \triangle ABC and a line l entering the interior via side BC, l cannot exit without crossing either AB or AC, preventing pathological "jumps" across the . This , implicit in Euclid's work but explicitly formalized later, supports the of line segments and the convexity of triangular regions in absolute geometry.

Congruence and Betweenness

In absolute geometry, the axioms of betweenness establish the linear order of points on a line and the separation properties in the , providing the foundation for notions of and without assuming a . The betweenness relation is defined such that for points A, B, C on a line, B is between A and C if it lies on the segment AC. The trichotomy axiom states that for any three distinct collinear points A, B, C, exactly one of the following holds: B is between A and C, A is between B and C, or C is between A and B. of betweenness ensures that if B is between A and C, and C is between B and D, then B is between A and D, allowing the extension of order relations along lines. Pasch's separation further specifies that if a line intersects one side of a but misses the other two vertices, it must intersect exactly one of the remaining sides, preventing pathological configurations and ensuring planar separation. The axioms define equality of lengths and , enabling measurement and comparison independent of embedding in or spaces. Reflexivity holds as every is congruent to itself, and every is congruent to itself. and follow from the axioms: if AB is congruent to A'B', then A'B' is congruent to AB, and if AB ≅ A'B' and A'B' ≅ A''B'', then AB ≅ A''B''; the same applies to . For triangles, the side--side () axiom asserts that if two sides and the included of one triangle are congruent to two sides and the included of another, then the triangles are congruent. A key result from Hilbert's axioms is that all right are congruent to one another, establishing their uniformity across the plane. Segment addition is captured by the axiom that if points B and B' lie between A and C, and A'B' ≅ AB, B'C ≅ BC, then AC ≅ A'C', allowing the composition of lengths along a line. Similarly, angle addition enables the decomposition of an angle into adjacent sub-angles whose congruences sum to the whole, provided they share a common . These addition properties underpin key results, such as the proof that in an , the base are equal (corresponding to Euclid's I.5), achieved by constructing congruent triangles via and applying angle addition to show symmetry in the vertex .

Theorems and Results

Angle and Parallel Theorems

In absolute geometry, the exterior angle theorem states that the measure of an of a is greater than the measure of either of its remote interior . This result follows from the axioms of and betweenness, utilizing to establish through . The theorem holds without invoking the parallel postulate and underscores the strict convexity of triangles in this geometric framework. A fundamental result concerning transversals is the alternate interior angles theorem, which asserts that if a transversal intersects two lines and forms congruent alternate interior angles, then the two lines are parallel. The proof relies on the side-angle-side () congruence criterion and leads to a contradiction if the lines were assumed to intersect, as it would violate the exterior angle inequality. This theorem provides a for parallelism based solely on angular measures, independent of the parallel postulate. An important in absolute geometry is that two lines each to a third line are to each other. This follows directly from the alternate interior angles theorem, as the right angles formed by the are congruent, ensuring the lines do not intersect. The result aligns with Euclid's I.31 but is provable within the absolute framework without additional assumptions. The crossbar theorem plays a crucial role in establishing the formation of angles and their relation to parallelism. It states that a ray emanating from the vertex of a non-degenerate angle will intersect the interior of the opposite side if and only if the ray's endpoint lies within the angle's interior. This theorem, grounded in Pasch's axiom and the properties of half-planes, ensures consistent angle division and supports definitions of parallels through equal alternate interior angles. By guaranteeing such intersections, it facilitates proofs of non-intersection for parallel lines in absolute geometry.

Triangle and Area Theorems

In absolute geometry, the Saccheri–Legendre theorem establishes a fundamental bound on the angular measure of triangles. This theorem states that the sum of the interior angles of any triangle is at most 180 degrees (or \leq \pi radians). The result was first demonstrated by Giovanni Girolamo Saccheri in his 1733 work Euclides ab omni naevo vindicatus, where he explored hypotheses on the acute angle of a , and independently by in the late through proofs involving triangle constructions. The proof of the Saccheri–Legendre theorem proceeds by contradiction in neutral geometry. Assume the angle sum of a triangle \triangle ABC exceeds 180 degrees, say by \epsilon > 0. Drop a perpendicular from vertex A to side BC at point D, dividing \triangle ABC into two right triangles \triangle ABD and \triangle ACD. The angle sum of each right triangle is then greater than 90 degrees. By constructing a midpoint on the hypotenuse of one right triangle and forming a new isosceles right triangle, the process halves the excess angle iteratively, yielding a sequence of triangles with progressively smaller angles but the same excess \epsilon. This leads to a triangle where two interior angles sum to more than 180 degrees, contradicting the exterior angle theorem, which implies that the sum of any two interior angles is less than 180 degrees. Thus, the angle sum cannot exceed 180 degrees. Absolute geometry also yields theorems relating sides and angles in triangles, independent of the parallel postulate. Euclid's Proposition I.18 asserts that in any triangle, the larger angle is opposite the longer side. For instance, if side BC > AB in \triangle ABC, then \angle BAC > \angle ACB. The proof relies on the congruence and the : assuming the contrary leads to an where equal sides would imply equal angles, yielding a via the exterior angle exceeding an interior one. The converse, Proposition I.19, states that the longer side is opposite the larger angle; if \angle ABC > \angle ACB, then side AC > AB. This is established by , constructing an on the longer side and using to show the assumed inequality violates angle-side relations. These propositions hold in absolute geometry as they depend only on incidence, betweenness, and axioms. Regarding areas, absolute geometry implies that every non-degenerate has positive area, derived from the of triangles preserving s. The area axioms include: (1) congruent triangles have equal areas, (2) areas are additive over disjoint polygonal regions, and (3) a has area 1, ensuring non-zero measure for figures with positive extent. Thus, three non-collinear points determine a triangular with positive area, as to a standard triangle with known positive measure follows from or other criteria. However, without the parallel postulate, no universal formula relates area directly to angle defect; areas are bounded but not precisely quantified in terms of angular excess.

Relations to Other Geometries

Similarities with and Geometries

Absolute geometry encompasses the body of theorems that are valid in both and geometries, forming a shared axiomatic foundation independent of the parallel postulate. Specifically, the first 28 propositions of Euclid's Elements, Book I, along with I.31—which establishes the existence of a line through a given point to a given line—are provable within absolute geometry and thus hold true in both and settings. These propositions cover fundamental results on , inequalities, and basic constructions, such as the (I.1) and side-angle-side (I.4), demonstrating the overlap in core structural properties. A key shared property is the behavior of angles in triangles, where the Saccheri–Legendre theorem proves that the sum of the interior angles is at most 180°, with equality holding in and a positive defect (less than 180°) in . This upper bound on the angle sum underscores a commonality in triangular configurations across both geometries, without specifying the exact value until the parallel postulate is invoked. Absolute geometry can thus be viewed as the logical intersection of and geometries: the emerges by adding the axiom of unique parallels through a point, while the plane allows for multiple parallels. Basic geometric constructions, such as drawing a with a given and or erecting a from a point to a line, proceed identically in both and hyperbolic geometries under the axioms of absolute geometry, relying solely on incidence and without parallel assumptions. These constructions highlight the practical similarities, as the tools of and yield the same outcomes for such operations in both contexts.

Contrasts with Elliptic and Spherical Geometries

Absolute geometry, based on excluding the parallel postulate, assumes an ordered structure with unbounded lines and proper betweenness relations that do not hold in or spherical geometries. In , lines are closed curves analogous to great circles on a , lacking the infinite extent required for the betweenness axioms, which define points lying strictly between two others on an unbounded line. This failure arises because elliptic spaces are compact and closed, preventing the linear ordering presupposed in absolute geometry's incidence and order axioms. In closed elliptic spaces, standard plane separation by a line into two distinct half-planes does not align with the , as lines bound finite regions and reconnect, differing from the open half-planes assumed in absolute geometry. , as a model for , exacerbates this by treating great circles as lines, where betweenness cannot be consistently defined along closed paths that loop indefinitely. Furthermore, absolute geometry permits the existence of through a point not on a given line, a derivable from its axioms, but in elliptic and spherical geometries, all lines intersect. On a , any two great circles intersect at two antipodal points, directly contradicting the possibility of non-intersecting lines assumed in absolute geometry. This universal intersection eliminates the concept of parallels entirely, rendering absolute geometry's framework inapplicable. As a concrete example, constructing an in is possible using arcs, but extending its sides infinitely as rays—as required in absolute geometry for theorems on and incidence—fails because the sides back and meet, forming a closed figure without unbounded extension. This closure inherent to elliptic spaces prevents the open-ended constructions central to absolute geometry's betweenness and incidence properties.

Models and Interpretations

Hilbert Planes

A Hilbert plane is defined as a model of plane geometry consisting of points and lines that satisfies in the first three groups: incidence (I 1–I 8), order (II 1–II 4, governing betweenness), and congruence (III 1–III 8), while excluding the parallel postulate and continuity axioms. These axioms establish the basic structure of points on lines, the ordering of points along lines, and the preservation of distances and angles under congruence, providing a foundation for absolute geometry without committing to the behavior of parallels. Prominent examples of Hilbert planes include the , where exactly one parallel line passes through a point not on a given line, and the hyperbolic plane, such as the , where multiple parallels exist. Both models embed absolute geometry fully, meaning all theorems derivable from the incidence, order, and axioms hold within them, demonstrating how Hilbert planes capture the shared properties of these geometries prior to introducing parallelism. Hilbert planes are inherently , as they neither affirm nor deny the parallel postulate, allowing for consistent extensions by adding either the Euclidean parallel (yielding ) or the hyperbolic parallel (yielding ). This neutrality underscores their role as abstract frameworks for absolute geometry, independent of specific metric assumptions beyond . All Hilbert planes share the same theory with respect to the axioms of absolute geometry, implying that any statement provable from these axioms is true in every such model, ensuring uniformity in their logical structure. This property, rooted in the axiomatic foundation, is explored in classifications like that of K. A. Pejas, who classified all Hilbert planes up to into types such as (satisfying the parallel postulate), (with multiple parallels), and semi-versions like semi- or semi-elliptic without full .

Other Models and Examples

, also known as the Manhattan plane, serves as a semi-absolute model by retaining the incidence and betweenness structures of the while altering the metric to the L1 norm, defined as the in coordinates. This modification preserves the axioms of incidence—where two distinct points determine a unique line—and betweenness, allowing collinear points to be ordered along lines in a manner consistent with absolute geometry. However, it deviates from full axioms, particularly failing the side-angle-side () criterion, as triangles with congruent sides and included angle may not be congruent under the taxicab distance. Finite incidence geometries provide approximations of the incidence properties in absolute geometry, where points and lines form finite structures satisfying Hilbert's incidence axioms without requiring infinite extent. These models demonstrate that arbitrary finite cardinalities are possible for the number of points, lines, and planes while adhering to set membership for incidence relations. Unlike the continuous Hilbert planes, which embed absolute geometry in a complete , finite incidence geometries highlight discrete analogs useful for combinatorial studies, though they lack the full betweenness and required for complete absolute models. Coordinate models of absolute geometry can be constructed over ordered fields, providing a systematic way to interpret the axioms through algebraic structures. In such models, lines are coordinatized by bijections to the field elements, with betweenness defined via the field's , ensuring compatibility with incidence and Pasch's . For instance, the real numbers yield the standard model, but other ordered fields allow adaptable interpretations that satisfy the and axioms of absolute geometry without committing to the parallel postulate. This approach, rooted in Birkhoff's axiomatization, underscores the flexibility of absolute geometry across different ordered structures.

Extensions and Applications

Incompleteness and Axiomatic Extensions

Absolute geometry, also known as neutral geometry, constitutes an incomplete because the parallel postulate is independent of its other axioms, rendering it undecidable within the framework. This independence means that the axioms neither prove nor disprove the existence or uniqueness of through a point not on a given line, allowing for consistent models where the postulate holds and others where it fails. for ensures that any consistent extension of absolute geometry, such as by adding the parallel postulate or its negation, admits models, implying that infinite models of absolute geometry can differ fundamentally in their parallel behavior, leading to distinct geometries. To resolve this incompleteness, the or equivalent axioms are added to the system. Incorporating Euclid's —or Hilbert's equivalent formulation, which states that through any point not on a given line, exactly one line can be drawn—yields , where the sum of angles in a triangle equals 180 degrees. Conversely, adopting a , which asserts that through such a point, at least two non-intersecting lines (parallels) exist, produces , characterized by triangle angle sums strictly less than 180 degrees. The independence of the parallel postulate is demonstrated through explicit models that satisfy all axioms of absolute geometry but violate the Euclidean version. For instance, hyperbolic models such as the Beltrami-Klein model (where points lie inside a disk and lines are chords) and the (where lines are circular arcs orthogonal to the boundary) uphold incidence, , , and axioms while allowing multiple parallels, resulting in angle defect in triangles as per the Saccheri–Legendre theorem, which establishes that the angle sum is at most 180 degrees in absolute geometry. Hilbert's complete for extends absolute geometry by incorporating the parallelism axiom alongside the groups for incidence, (betweenness), , and , thereby resolving the undecidability and enabling the derivation of all classical theorems. This extension ensures the system's consistency relative to and distinguishes it from non-Euclidean alternatives.

Applications in Physics and Beyond

Absolute geometry finds significant application in physics, particularly within the framework of , where it provides a foundation for describing without presupposing the nature of parallelism or . In their seminal 1912 work, Edwin B. Wilson and developed the geometry of using nine axioms and eleven propositions derived from absolute geometry to construct invariant spacetime diagrams. This approach ensures geometric consistency across inertial frames by relying solely on neutral properties shared by and geometries. A key advantage of this formulation is that absolute geometry underpins the Lorentz transformations in flat Minkowski spacetime, circumventing the inconsistencies inherent in elliptic geometry, where the angle sum of a triangle exceeds 180 degrees, contradicting the absolute geometry theorem that the sum is at most 180 degrees. In elliptic models, the absence of parallel lines and finite spatial extent would conflict with the infinite, flat structure required for special relativistic invariance, whereas absolute geometry's neutrality allows seamless integration with the pseudo-Riemannian metric of spacetime.

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