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												  Projective Geometry: a Short IntroductionProjective Geometry: A Short Introduction Lecture Notes Edmond Boyer Master MOSIG Introduction to Projective Geometry Contents 1 Introduction 2 1.1 Objective . .2 1.2 Historical Background . .3 1.3 Bibliography . .4 2 Projective Spaces 5 2.1 Definitions . .5 2.2 Properties . .8 2.3 The hyperplane at infinity . 12 3 The projective line 13 3.1 Introduction . 13 3.2 Projective transformation of P1 ................... 14 3.3 The cross-ratio . 14 4 The projective plane 17 4.1 Points and lines . 17 4.2 Line at infinity . 18 4.3 Homographies . 19 4.4 Conics . 20 4.5 Affine transformations . 22 4.6 Euclidean transformations . 22 4.7 Particular transformations . 24 4.8 Transformation hierarchy . 25 Grenoble Universities 1 Master MOSIG Introduction to Projective Geometry Chapter 1 Introduction 1.1 Objective The objective of this course is to give basic notions and intuitions on projective geometry. The interest of projective geometry arises in several visual comput- ing domains, in particular computer vision modelling and computer graphics. It provides a mathematical formalism to describe the geometry of cameras and the associated transformations, hence enabling the design of computational ap- proaches that manipulates 2D projections of 3D objects. In that respect, a fundamental aspect is the fact that objects at infinity can be represented and manipulated with projective geometry and this in contrast to the Euclidean geometry. This allows perspective deformations to be represented as projective transformations. Figure 1.1: Example of perspective deformation or 2D projective transforma- tion. Another argument is that Euclidean geometry is sometimes difficult to use in algorithms, with particular cases arising from non-generic situations (e.g.
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												![Arxiv:1910.10745V1 [Cond-Mat.Str-El] 23 Oct 2019 2.2 Symmetry-Protected Time Crystals](https://docslib.b-cdn.net/cover/4942/arxiv-1910-10745v1-cond-mat-str-el-23-oct-2019-2-2-symmetry-protected-time-crystals-304942.webp)  Arxiv:1910.10745V1 [Cond-Mat.Str-El] 23 Oct 2019 2.2 Symmetry-Protected Time CrystalsA Brief History of Time Crystals Vedika Khemania,b,∗, Roderich Moessnerc, S. L. Sondhid aDepartment of Physics, Harvard University, Cambridge, Massachusetts 02138, USA bDepartment of Physics, Stanford University, Stanford, California 94305, USA cMax-Planck-Institut f¨urPhysik komplexer Systeme, 01187 Dresden, Germany dDepartment of Physics, Princeton University, Princeton, New Jersey 08544, USA Abstract The idea of breaking time-translation symmetry has fascinated humanity at least since ancient proposals of the per- petuum mobile. Unlike the breaking of other symmetries, such as spatial translation in a crystal or spin rotation in a magnet, time translation symmetry breaking (TTSB) has been tantalisingly elusive. We review this history up to recent developments which have shown that discrete TTSB does takes place in periodically driven (Floquet) systems in the presence of many-body localization (MBL). Such Floquet time-crystals represent a new paradigm in quantum statistical mechanics — that of an intrinsically out-of-equilibrium many-body phase of matter with no equilibrium counterpart. We include a compendium of the necessary background on the statistical mechanics of phase structure in many- body systems, before specializing to a detailed discussion of the nature, and diagnostics, of TTSB. In particular, we provide precise definitions that formalize the notion of a time-crystal as a stable, macroscopic, conservative clock — explaining both the need for a many-body system in the infinite volume limit, and for a lack of net energy absorption or dissipation. Our discussion emphasizes that TTSB in a time-crystal is accompanied by the breaking of a spatial symmetry — so that time-crystals exhibit a novel form of spatiotemporal order.
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												  The Fractal Dimension of Product SetsTHE FRACTAL DIMENSION OF PRODUCT SETS A PREPRINT Clayton Moore Williams Brigham Young University [email protected] Machiel van Frankenhuijsen Utah Valley University [email protected] February 26, 2021 ABSTRACT Using methods from nonstandard analysis, we define a nonstandard Minkowski dimension which exists for all bounded sets and which has the property that dim(A × B) = dim(A) + dim(B). That is, our new dimension is “product-summable”. To illustrate our theorem we generalize an example of Falconer’s1 to show that the standard upper Minkowski dimension, as well as the Hausdorff di- mension, are not product-summable. We also include a method for creating sets of arbitrary rational dimension. Introduction There are several notions of dimension used in fractal geometry, which coincide for many sets but have important, distinct properties. Indeed, determining the most proper notion of dimension has been a major problem in geometric measure theory from its inception, and debate over what it means for a set to be fractal has often reduced to debate over the propernotion of dimension. A classical example is the “Devil’s Staircase” set, which is intuitively fractal but which has integer Hausdorff dimension2. As Falconer notes in The Geometry of Fractal Sets3, the Hausdorff dimension is “undoubtedly, the most widely investigated and most widely used” notion of dimension. It can, however, be difficult to compute or even bound (from below) for many sets. For this reason one might want to work with the Minkowski dimension, for which one can often obtain explicit formulas. Moreover, the Minkowski dimension is computed using finite covers and hence has a series of useful identities which can be used in analysis.
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												  The Projective Geometry of the Spacetime Yielded by Relativistic Positioning Systems and Relativistic Location Systems Jacques RubinThe projective geometry of the spacetime yielded by relativistic positioning systems and relativistic location systems Jacques Rubin To cite this version: Jacques Rubin. The projective geometry of the spacetime yielded by relativistic positioning systems and relativistic location systems. 2014. hal-00945515 HAL Id: hal-00945515 https://hal.inria.fr/hal-00945515 Submitted on 12 Feb 2014 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. The projective geometry of the spacetime yielded by relativistic positioning systems and relativistic location systems Jacques L. Rubin (email: [email protected]) Université de Nice–Sophia Antipolis, UFR Sciences Institut du Non-Linéaire de Nice, UMR7335 1361 route des Lucioles, F-06560 Valbonne, France (Dated: February 12, 2014) As well accepted now, current positioning systems such as GPS, Galileo, Beidou, etc. are not primary, relativistic systems. Nevertheless, genuine, relativistic and primary positioning systems have been proposed recently by Bahder, Coll et al. and Rovelli to remedy such prior defects. These new designs all have in common an equivariant conformal geometry featuring, as the most basic ingredient, the spacetime geometry. In a first step, we show how this conformal aspect can be the four-dimensional projective part of a larger five-dimensional geometry.
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												  Convex Sets in Projective Space Compositio Mathematica, Tome 13 (1956-1958), PCOMPOSITIO MATHEMATICA J. DE GROOT H. DE VRIES Convex sets in projective space Compositio Mathematica, tome 13 (1956-1958), p. 113-118 <http://www.numdam.org/item?id=CM_1956-1958__13__113_0> © Foundation Compositio Mathematica, 1956-1958, tous droits réser- vés. L’accès aux archives de la revue « Compositio Mathematica » (http: //http://www.compositio.nl/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utili- sation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Convex sets in projective space by J. de Groot and H. de Vries INTRODUCTION. We consider the following properties of sets in n-dimensional real projective space Pn(n > 1 ): a set is semiconvex, if any two points of the set can be joined by a (line)segment which is contained in the set; a set is convex (STEINITZ [1]), if it is semiconvex and does not meet a certain P n-l. The main object of this note is to characterize the convexity of a set by the following interior and simple property: a set is convex if and only if it is semiconvex and does not contain a whole (projective) line; in other words: a subset of Pn is convex if and only if any two points of the set can be joined uniquely by a segment contained in the set. In many cases we can prove more; see e.g.
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												  Positive Geometries and Canonical FormsPrepared for submission to JHEP Positive Geometries and Canonical Forms Nima Arkani-Hamed,a Yuntao Bai,b Thomas Lamc aSchool of Natural Sciences, Institute for Advanced Study, Princeton, NJ 08540, USA bDepartment of Physics, Princeton University, Princeton, NJ 08544, USA cDepartment of Mathematics, University of Michigan, 530 Church St, Ann Arbor, MI 48109, USA Abstract: Recent years have seen a surprising connection between the physics of scat- tering amplitudes and a class of mathematical objects{the positive Grassmannian, positive loop Grassmannians, tree and loop Amplituhedra{which have been loosely referred to as \positive geometries". The connection between the geometry and physics is provided by a unique differential form canonically determined by the property of having logarithmic sin- gularities (only) on all the boundaries of the space, with residues on each boundary given by the canonical form on that boundary. The structures seen in the physical setting of the Amplituhedron are both rigid and rich enough to motivate an investigation of the notions of \positive geometries" and their associated \canonical forms" as objects of study in their own right, in a more general mathematical setting. In this paper we take the first steps in this direction. We begin by giving a precise definition of positive geometries and canonical forms, and introduce two general methods for finding forms for more complicated positive geometries from simpler ones{via \triangulation" on the one hand, and \push-forward" maps between geometries on the other. We present numerous examples of positive geome- tries in projective spaces, Grassmannians, and toric, cluster and flag varieties, both for the simplest \simplex-like" geometries and the richer \polytope-like" ones.
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												  Fractal-Based Methods As a Technique for Estimating the Intrinsic Dimensionality of High-Dimensional Data: a SurveyINFORMATICA, 2016, Vol. 27, No. 2, 257–281 257 2016 Vilnius University DOI: http://dx.doi.org/10.15388/Informatica.2016.84 Fractal-Based Methods as a Technique for Estimating the Intrinsic Dimensionality of High-Dimensional Data: A Survey Rasa KARBAUSKAITE˙ ∗, Gintautas DZEMYDA Institute of Mathematics and Informatics, Vilnius University Akademijos 4, LT-08663, Vilnius, Lithuania e-mail: [email protected], [email protected] Received: December 2015; accepted: April 2016 Abstract. The estimation of intrinsic dimensionality of high-dimensional data still remains a chal- lenging issue. Various approaches to interpret and estimate the intrinsic dimensionality are deve- loped. Referring to the following two classifications of estimators of the intrinsic dimensionality – local/global estimators and projection techniques/geometric approaches – we focus on the fractal- based methods that are assigned to the global estimators and geometric approaches. The compu- tational aspects of estimating the intrinsic dimensionality of high-dimensional data are the core issue in this paper. The advantages and disadvantages of the fractal-based methods are disclosed and applications of these methods are presented briefly. Key words: high-dimensional data, intrinsic dimensionality, topological dimension, fractal dimension, fractal-based methods, box-counting dimension, information dimension, correlation dimension, packing dimension. 1. Introduction In real applications, we confront with data that are of a very high dimensionality. For ex- ample, in image analysis, each image is described by a large number of pixels of different colour. The analysis of DNA microarray data (Kriukien˙e et al., 2013) deals with a high dimensionality, too. The analysis of high-dimensional data is usually challenging.
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												  Characterization of Quantum Entanglement Via a Hypercube of Segre EmbeddingsCharacterization of quantum entanglement via a hypercube of Segre embeddings Joana Cirici∗ Departament de Matemàtiques i Informàtica Universitat de Barcelona Gran Via 585, 08007 Barcelona Jordi Salvadó† and Josep Taron‡ Departament de Fisíca Quàntica i Astrofísica and Institut de Ciències del Cosmos Universitat de Barcelona Martí i Franquès 1, 08028 Barcelona A particularly simple description of separability of quantum states arises naturally in the setting of complex algebraic geometry, via the Segre embedding. This is a map describing how to take products of projective Hilbert spaces. In this paper, we show that for pure states of n particles, the corresponding Segre embedding may be described by means of a directed hypercube of dimension (n − 1), where all edges are bipartite-type Segre maps. Moreover, we describe the image of the original Segre map via the intersections of images of the (n − 1) edges whose target is the last vertex of the hypercube. This purely algebraic result is then transferred to physics. For each of the last edges of the Segre hypercube, we introduce an observable which measures geometric separability and is related to the trace of the squared reduced density matrix. As a consequence, the hypercube approach gives a novel viewpoint on measuring entanglement, naturally relating bipartitions with q-partitions for any q ≥ 1. We test our observables against well-known states, showing that these provide well-behaved and fine measures of entanglement. arXiv:2008.09583v1 [quant-ph] 21 Aug 2020 ∗ [email protected] † [email protected] ‡ [email protected] 2 I. INTRODUCTION Quantum entanglement is at the heart of quantum physics, with crucial roles in quantum information theory, superdense coding and quantum teleportation among others.
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												  PROJECTIVE GEOMETRY Contents 1. Basic Definitions 1 2. Axioms OfPROJECTIVE GEOMETRY KRISTIN DEAN Abstract. This paper investigates the nature of finite geometries. It will focus on the finite geometries known as projective planes and conclude with the example of the Fano plane. Contents 1. Basic Definitions 1 2. Axioms of Projective Geometry 2 3. Linear Algebra with Geometries 3 4. Quotient Geometries 4 5. Finite Projective Spaces 5 6. The Fano Plane 7 References 8 1. Basic Definitions First, we must begin with a few basic definitions relating to geometries. A geometry can be thought of as a set of objects and a relation on those elements. Definition 1.1. A geometry is denoted G = (Ω,I), where Ω is a set and I a relation which is both symmetric and reflexive. The relation on a geometry is called an incidence relation. For example, consider the tradional Euclidean geometry. In this geometry, the objects of the set Ω are points and lines. A point is incident to a line if it lies on that line, and two lines are incident if they have all points in common - only when they are the same line. There is often this same natural division of the elements of Ω into different kinds such as the points and lines. Definition 1.2. Suppose G = (Ω,I) is a geometry. Then a flag of G is a set of elements of Ω which are mutually incident. If there is no element outside of the flag, F, which can be added and also be a flag, then F is called maximal. Definition 1.3. A geometry G = (Ω,I) has rank r if it can be partitioned into sets Ω1,..., Ωr such that every maximal flag contains exactly one element of each set.
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												![Arxiv:1810.02861V1 [Math.AG] 5 Oct 2018 CP Oyoileuto N Ae Xeddt Ufcsadhge Dim Using Higher Besides and Equations](https://docslib.b-cdn.net/cover/1655/arxiv-1810-02861v1-math-ag-5-oct-2018-cp-oyoileuto-n-ae-xeddt-ufcsadhge-dim-using-higher-besides-and-equations-1381655.webp)  Arxiv:1810.02861V1 [Math.AG] 5 Oct 2018 CP Oyoileuto N Ae Xeddt Ufcsadhge Dim Using Higher Besides and EquationsOctober 9, 2018 ALGEBRAIC HYPERSURFACES JANOS´ KOLLAR´ Abstract. We give an introduction to the study of algebraic hypersurfaces, focusing on the problem of when two hypersurfaces are isomorphic or close to being isomorphic. Working with hypersurfaces and emphasizing examples makes it possible to discuss these questions without any previous knowledge of algebraic geometry. At the end we formulate the main recent results and state the most important open questions. Contents 1. Stereographic projection 2 2. Projective hypersurfaces 4 3. Rational and birational maps 5 4. The main questions 8 5. Rationality of cubic hypersurfaces 10 6. Isomorphism of hypersurfaces 12 7. Non-rationalityoflargedegreehypersurfaces 14 8. Non-rationalityoflowdegreehypersurfaces 17 9. Rigidity of low degree hypersurfaces 18 10. Connections with the classification of varieties 18 11. Openproblemsabouthypersurfaces 19 References 21 Algebraic geometry started as the study of plane curves C R2 defined by a polynomial equation and later extended to surfaces and higher⊂ dimensional sets defined by systems of polynomial equations. Besides using Rn, it is frequently more advantageous to work with Cn or with the corresponding projective spaces RPn and n arXiv:1810.02861v1 [math.AG] 5 Oct 2018 CP . Later it was realized that the theory also works if we replace R or C by other fields, for example the field of rational numbers Q or even finite fields Fq. When we try to emphasize that the choice of the field is pretty arbitrary, we use An to denote affine n-space and Pn to denote projective n-space. Conceptually the simplest algebraic sets are hypersurfaces; these are defined by 1 equation.
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												  Euclidean Versus Projective GeometryProjective Geometry Projective Geometry Euclidean versus Projective Geometry n Euclidean geometry describes shapes “as they are” – Properties of objects that are unchanged by rigid motions » Lengths » Angles » Parallelism n Projective geometry describes objects “as they appear” – Lengths, angles, parallelism become “distorted” when we look at objects – Mathematical model for how images of the 3D world are formed. Projective Geometry Overview n Tools of algebraic geometry n Informal description of projective geometry in a plane n Descriptions of lines and points n Points at infinity and line at infinity n Projective transformations, projectivity matrix n Example of application n Special projectivities: affine transforms, similarities, Euclidean transforms n Cross-ratio invariance for points, lines, planes Projective Geometry Tools of Algebraic Geometry 1 n Plane passing through origin and perpendicular to vector n = (a,b,c) is locus of points x = ( x 1 , x 2 , x 3 ) such that n · x = 0 => a x1 + b x2 + c x3 = 0 n Plane through origin is completely defined by (a,b,c) x3 x = (x1, x2 , x3 ) x2 O x1 n = (a,b,c) Projective Geometry Tools of Algebraic Geometry 2 n A vector parallel to intersection of 2 planes ( a , b , c ) and (a',b',c') is obtained by cross-product (a'',b'',c'') = (a,b,c)´(a',b',c') (a'',b'',c'') O (a,b,c) (a',b',c') Projective Geometry Tools of Algebraic Geometry 3 n Plane passing through two points x and x’ is defined by (a,b,c) = x´ x' x = (x1, x2 , x3 ) x'= (x1 ', x2 ', x3 ') O (a,b,c) Projective Geometry Projective Geometry
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												  Eduard Čech, 1893–1960Czechoslovak Mathematical Journal Bohuslav Balcar; Václav Koutník; Petr Simon Eduard Čech, 1893–1960 Czechoslovak Mathematical Journal, Vol. 43 (1993), No. 3, 567–575 Persistent URL: http://dml.cz/dmlcz/128420 Terms of use: © Institute of Mathematics AS CR, 1993 Institute of Mathematics of the Czech Academy of Sciences provides access to digitized documents strictly for personal use. Each copy of any part of this document must contain these Terms of use. This document has been digitized, optimized for electronic delivery and stamped with digital signature within the project DML-CZ: The Czech Digital Mathematics Library http://dml.cz Czechoslovak Matheшatical Joumal, 43 (118) 1993, Praha NEWS AND NOTICES EDUARD CECH, 1893-1960 BOHUSLAV BALCAR, VÁCLAV KOUTNÍK, PETR SIMON, Praha This year we observe the 100th anniversary of the birthday of Eduard Cech, one of the leading world specialists in topology and differential geometry. To these fields he contributed works of fundamental importance. He was born on June 29, 1893 in Stracov in northeastern Bohemia. During his high school studies in Hradec Kralove he became interested in mathematics and in 1912 he entered the Philosophical Faculty of Charles University in Prague. At that time there were very few opportunities for mathematicians other than to become a high school teacher. For a position of a high school teacher two fields of study were required. Since Cech was not much interested in physics, the standard second subject, he chose descriptive geometry. During his studies at the university he spent a lot of time in the library of the Union of Czech Mathematicians and Physicists and read many mathematical books of his own choice.