“…[15,16] Here we briefly summarize some fundamental properties of hyperbolic numbers. This number system has been introduced by S. Lie [11] as a two dimensional example of the more general class of the commutative hypercomplex numbers systems [13]. Now let us introduce a hyperbolic plane on the analogy of the Gauss-Argand plane of the complex variable.…”
Section: Basic Definitionsmentioning
confidence: 99%
“…Even if Minkowski gave a geometrical interpretation of the special relativity space-time shortly after (1907-1908) Einstein's fundamental paper, a mathematical tool exploitable in the context of the Minkowski space-time has begun to be carried out only few decades ago ( [5]- [10]). This mathematical tool is based on the use of hyperbolic numbers, introduced by S. Lie in the late XIX century [11]. In analogy with the procedures applied in the case of complex numbers, it is possible to formalize, also for the hyperbolic numbers, a space-time geometry and a trigonometry following the same Euclidean axiomatic-deductive method [10,12].…”
-The formal structure of the early Einstein's Special Relativity follows the axiomatic deductive method of Euclidean geometry. In this paper we show the deep-rooted relation between Euclidean and space-time geometries that are both linked to a two-dimensional number system: the complex and hyperbolic numbers, respectively. By studying the properties of these numbers together, pseudo-Euclidean trigonometry has been formalized with an axiomatic deductive method and this allows us to give a complete quantitative formalization of the twin paradox in a familiar "Euclidean" way for uniform motions as well as for accelerated ones.
“…[15,16] Here we briefly summarize some fundamental properties of hyperbolic numbers. This number system has been introduced by S. Lie [11] as a two dimensional example of the more general class of the commutative hypercomplex numbers systems [13]. Now let us introduce a hyperbolic plane on the analogy of the Gauss-Argand plane of the complex variable.…”
Section: Basic Definitionsmentioning
confidence: 99%
“…Even if Minkowski gave a geometrical interpretation of the special relativity space-time shortly after (1907-1908) Einstein's fundamental paper, a mathematical tool exploitable in the context of the Minkowski space-time has begun to be carried out only few decades ago ( [5]- [10]). This mathematical tool is based on the use of hyperbolic numbers, introduced by S. Lie in the late XIX century [11]. In analogy with the procedures applied in the case of complex numbers, it is possible to formalize, also for the hyperbolic numbers, a space-time geometry and a trigonometry following the same Euclidean axiomatic-deductive method [10,12].…”
-The formal structure of the early Einstein's Special Relativity follows the axiomatic deductive method of Euclidean geometry. In this paper we show the deep-rooted relation between Euclidean and space-time geometries that are both linked to a two-dimensional number system: the complex and hyperbolic numbers, respectively. By studying the properties of these numbers together, pseudo-Euclidean trigonometry has been formalized with an axiomatic deductive method and this allows us to give a complete quantitative formalization of the twin paradox in a familiar "Euclidean" way for uniform motions as well as for accelerated ones.
“…1, requires L p (h) to be in the ideal generated by h. This condition is also only sufficient and was mentioned as early as 1878 [7]. The Lie proof rule gives Lie's criterion [15,21,25] for invariance of h = 0 and characterizes smooth invariant manifolds. The rule DW is called differential weakening [24] and covers the trivial case when the evolution constraint implies the invariant candidate; in contrast to all other rules in the table, DW can work with arbitrary invariant assertions.…”
Section: Sufficient Conditions For Invariance Of Equationsmentioning
confidence: 99%
“…Furthermore, differential cuts [23] are shown to fundamentally improve the deductive power of Lie's criterion [15].…”
Section: Introductionmentioning
confidence: 99%
“…• It explores an approach combining deductively less powerful rules [15,27,17,25] using differential cuts [23] to exploit the structure of the system to yield efficient proofs even for non-polynomial systems. Furthermore, differential cuts [23] are shown to fundamentally improve the deductive power of Lie's criterion [15].…”
In this paper we seek to provide greater automation for formal deductive verification tools working with continuous and hybrid dynamical systems. We present an efficient procedure to check invariance of conjunctions of polynomial equalities under the flow of polynomial ordinary differential equations. The procedure is based on a necessary and sufficient condition that characterizes invariant conjunctions of polynomial equalities. We contrast this approach to an alternative one which combines fast and sufficient (but not necessary) conditions using differential cuts for soundly restricting the system evolution domain.
We obtain a complete classification of scalar
th‐order ordinary differential equations for all subalgebras of vector fields in the real plane. While softwares like Maple can compute invariants of a given order, our results are for a general
. The
cases are well‐known in the literature. Further, it is known that there are three types of
th‐order equations depending upon the point symmetry algebra they possess, namely, first‐order equations which admit an infinite dimensional Lie algebra of point symmetries, second‐order equations possessing the maximum 8‐point symmetries, and higher‐order,
, admitting the maximum
dimensional point symmetry algebra. We show that scalar
th‐order equations for
do not admit maximally an
dimensional real Lie algebra of point symmetries. Moreover, we prove that for
, equations can admit two types of
dimensional real Lie algebra of point symmetries: one type resulting in nonlinear equations which are not linearizable via a point transformation and the second type yielding linearizable (via point transformation) equations. Furthermore, we present the types of maximal real
dimensional and higher than
‐dimensional point symmetry algebras admissible for equations of order
and their canonical forms. The types of lower‐dimensional point symmetry algebras which can be admitted are shown, and the equations are constructible as well. We state the relevant results in tabular form and in theorems.
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