Homeomorphisms of the Sierpinski Carpet
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Review On: Fractal Antenna Design Geometries and Its Applications
www.ijecs.in International Journal Of Engineering And Computer Science ISSN:2319-7242 Volume - 3 Issue -9 September, 2014 Page No. 8270-8275 Review On: Fractal Antenna Design Geometries and Its Applications Ankita Tiwari1, Dr. Munish Rattan2, Isha Gupta3 1GNDEC University, Department of Electronics and Communication Engineering, Gill Road, Ludhiana 141001, India [email protected] 2GNDEC University, Department of Electronics and Communication Engineering, Gill Road, Ludhiana 141001, India [email protected] 3GNDEC University, Department of Electronics and Communication Engineering, Gill Road, Ludhiana 141001, India [email protected] Abstract: In this review paper, we provide a comprehensive review of developments in the field of fractal antenna engineering. First we give brief introduction about fractal antennas and then proceed with its design geometries along with its applications in different fields. It will be shown how to quantify the space filling abilities of fractal geometries, and how this correlates with miniaturization of fractal antennas. Keywords – Fractals, self -similar, space filling, multiband 1. Introduction Modern telecommunication systems require antennas with irrespective of various extremely irregular curves or shapes wider bandwidths and smaller dimensions as compared to the that repeat themselves at any scale on which they are conventional antennas. This was beginning of antenna research examined. in various directions; use of fractal shaped antenna elements was one of them. Some of these geometries have been The term “Fractal” means linguistically “broken” or particularly useful in reducing the size of the antenna, while “fractured” from the Latin “fractus.” The term was coined by others exhibit multi-band characteristics. Several antenna Benoit Mandelbrot, a French mathematician about 20 years configurations based on fractal geometries have been reported ago in his book “The fractal geometry of Nature” [5]. -
Spatial Accessibility to Amenities in Fractal and Non Fractal Urban Patterns Cécile Tannier, Gilles Vuidel, Hélène Houot, Pierre Frankhauser
Spatial accessibility to amenities in fractal and non fractal urban patterns Cécile Tannier, Gilles Vuidel, Hélène Houot, Pierre Frankhauser To cite this version: Cécile Tannier, Gilles Vuidel, Hélène Houot, Pierre Frankhauser. Spatial accessibility to amenities in fractal and non fractal urban patterns. Environment and Planning B: Planning and Design, SAGE Publications, 2012, 39 (5), pp.801-819. 10.1068/b37132. hal-00804263 HAL Id: hal-00804263 https://hal.archives-ouvertes.fr/hal-00804263 Submitted on 14 Jun 2021 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. TANNIER C., VUIDEL G., HOUOT H., FRANKHAUSER P. (2012), Spatial accessibility to amenities in fractal and non fractal urban patterns, Environment and Planning B: Planning and Design, vol. 39, n°5, pp. 801-819. EPB 137-132: Spatial accessibility to amenities in fractal and non fractal urban patterns Cécile TANNIER* ([email protected]) - corresponding author Gilles VUIDEL* ([email protected]) Hélène HOUOT* ([email protected]) Pierre FRANKHAUSER* ([email protected]) * ThéMA, CNRS - University of Franche-Comté 32 rue Mégevand F-25 030 Besançon Cedex, France Tel: +33 381 66 54 81 Fax: +33 381 66 53 55 1 Spatial accessibility to amenities in fractal and non fractal urban patterns Abstract One of the challenges of urban planning and design is to come up with an optimal urban form that meets all of the environmental, social and economic expectations of sustainable urban development. -
Homology of Hom Complexes
Rose-Hulman Undergraduate Mathematics Journal Volume 13 Issue 1 Article 10 Homology of Hom Complexes Mychael Sanchez New Mexico State University, [email protected] Follow this and additional works at: https://scholar.rose-hulman.edu/rhumj Recommended Citation Sanchez, Mychael (2012) "Homology of Hom Complexes," Rose-Hulman Undergraduate Mathematics Journal: Vol. 13 : Iss. 1 , Article 10. Available at: https://scholar.rose-hulman.edu/rhumj/vol13/iss1/10 Rose- Hulman Undergraduate Mathematics Journal Homology of Hom Complexes Mychael Sancheza Volume 13, No. 1, Spring 2012 Sponsored by Rose-Hulman Institute of Technology Department of Mathematics Terre Haute, IN 47803 Email: [email protected] a http://www.rose-hulman.edu/mathjournal New Mexico State University Rose-Hulman Undergraduate Mathematics Journal Volume 13, No. 1, Spring 2012 Homology of Hom Complexes Mychael Sanchez Abstract. The hom complex Hom (G; K) is the order complex of the poset com- posed of the graph multihomomorphisms from G to K. We use homology to provide conditions under which the hom complex is not contractible and derive a lower bound on the rank of its homology groups. Acknowledgements: I acknowledge my advisor, Dr. Dan Ramras and the National Science Foundation for funding this research through Dr. Ramras' grants, DMS-1057557 and DMS-0968766. Page 212 RHIT Undergrad. Math. J., Vol. 13, No. 1 1 Introduction In 1978, László Lovász proved the Kneser Conjecture [8]. His proof involves associating to a graph G its neighborhood complex N (G) and using its topological properties to locate obstructions to graph colorings. This proof illustrates the fruitful interaction between graph theory, combinatorics and topology. -
Constructing Covers of the Rose
Constructing Covers of the rose. Robert Kropholler April 25, 2017 This was discussed in class but does not appear in any of the lecture notes. I will outline the constructions and proof here. Definition 0.1. Let F (X) be the free group on the set X. Assume jXj = n. Let H be any subgroup of F (X), we define the Schrier graph G(H) as follows: • The vertices of G(H) are the left cosets of H in G. • Two cosets gH; g0H are joined by an edge if there exists an x 2 X such that xgH = g0H. It should be noted that the Schrier graph of a normal subgroup N is the Cayley graph of G=N with respect to the generating set X. Let Rn be a cell complex with 1 vertex and n edges. We identify the fundamental group of Rn with F (X). Pick a bijection between the edges of X and give each edge an orientation. Proposition 0.2. The graph G(H) is a cover of Rn. Proof. We can label each edge with an element of X and give it an orientation so that the edge (gH; xgH) points towards xgH. We can then define a map p : G(H) ! Rn. This sends each vertex of G(H) to the unique vertex of Rn and each edge to the edge with same label by an orientation preserving homeomorphism. This defines a covering map. We must check that every point has a neighbourhood such that p is a homeomorphism on this neighbourhood. -
Moduli Spaces of Colored Graphs
MODULI SPACES OF COLORED GRAPHS MARKO BERGHOFF AND MAX MUHLBAUER¨ Abstract. We introduce moduli spaces of colored graphs, defined as spaces of non-degenerate metrics on certain families of edge-colored graphs. Apart from fixing the rank and number of legs these families are determined by var- ious conditions on the coloring of their graphs. The motivation for this is to study Feynman integrals in quantum field theory using the combinatorial structure of these moduli spaces. Here a family of graphs is specified by the allowed Feynman diagrams in a particular quantum field theory such as (mas- sive) scalar fields or quantum electrodynamics. The resulting spaces are cell complexes with a rich and interesting combinatorial structure. We treat some examples in detail and discuss their topological properties, connectivity and homology groups. 1. Introduction The purpose of this article is to define and study moduli spaces of colored graphs in the spirit of [HV98] and [CHKV16] where such spaces for uncolored graphs were used to study the homology of automorphism groups of free groups. Our motivation stems from the connection between these constructions in geometric group theory and the study of Feynman integrals as pointed out in [BK15]. Let us begin with a brief sketch of these two fields and what is known so far about their relation. 1.1. Background. The analysis of Feynman integrals as complex functions of their external parameters (e.g. momenta and masses) is a special instance of a very gen- eral problem, understanding the analytic structure of functions defined by integrals. That is, given complex manifolds X; T and a function f : T ! C defined by Z f(t) = !t; Γ what can be deduced about f from studying the integration contour Γ ⊂ X and the integrand !t 2 Ω(X)? There is a mathematical treatment for a class of well-behaved cases [Pha11], arXiv:1809.09954v3 [math.AT] 2 Jul 2019 but unfortunately Feynman integrals are generally too complicated to answer this question thoroughly. -
Knot Theory and the Alexander Polynomial
Knot Theory and the Alexander Polynomial Reagin Taylor McNeill Submitted to the Department of Mathematics of Smith College in partial fulfillment of the requirements for the degree of Bachelor of Arts with Honors Elizabeth Denne, Faculty Advisor April 15, 2008 i Acknowledgments First and foremost I would like to thank Elizabeth Denne for her guidance through this project. Her endless help and high expectations brought this project to where it stands. I would Like to thank David Cohen for his support thoughout this project and through- out my mathematical career. His humor, skepticism and advice is surely worth the $.25 fee. I would also like to thank my professors, peers, housemates, and friends, particularly Kelsey Hattam and Katy Gerecht, for supporting me throughout the year, and especially for tolerating my temporary insanity during the final weeks of writing. Contents 1 Introduction 1 2 Defining Knots and Links 3 2.1 KnotDiagramsandKnotEquivalence . ... 3 2.2 Links, Orientation, and Connected Sum . ..... 8 3 Seifert Surfaces and Knot Genus 12 3.1 SeifertSurfaces ................................. 12 3.2 Surgery ...................................... 14 3.3 Knot Genus and Factorization . 16 3.4 Linkingnumber.................................. 17 3.5 Homology ..................................... 19 3.6 TheSeifertMatrix ................................ 21 3.7 TheAlexanderPolynomial. 27 4 Resolving Trees 31 4.1 Resolving Trees and the Conway Polynomial . ..... 31 4.2 TheAlexanderPolynomial. 34 5 Algebraic and Topological Tools 36 5.1 FreeGroupsandQuotients . 36 5.2 TheFundamentalGroup. .. .. .. .. .. .. .. .. 40 ii iii 6 Knot Groups 49 6.1 TwoPresentations ................................ 49 6.2 The Fundamental Group of the Knot Complement . 54 7 The Fox Calculus and Alexander Ideals 59 7.1 TheFreeCalculus ............................... -
NON-POSITIVELY CURVED CUBE COMPLEXES Henry Wilton Last Updated: June 29, 2012
Cube complexes Winter 2011 NON-POSITIVELY CURVED CUBE COMPLEXES Henry Wilton Last updated: June 29, 2012 1 Some basics of topological and geometric group theory 1.1 Presentations and complexes Let Γ be a discrete group, defined by a presentation P = hai j rji, say, or as the fundamental group of a connected CW-complex X. 0 1 Remark 1.1. Let XP be the CW-complex with a single 0-cell E , one 1-cell Ei 2 for each ai (oriented accordingly), and one 2-cell Ej for each rj, with attaching 2 (1) map @Ej ! XP that reads off the word rj in the generators faig. Then, by the Seifert{van Kampen Theorem, the fundamental group of XP is the group presented by P. Conversely, restricting attention to X(2) and contracting a maximal tree in (1) X , we obtain XP for some presentation P of Γ. So we see that these two situations are equivalent. We will call XP a pre- sentation complex for Γ. Here are two typical questions that we might want to be able to answer about Γ. ∗ Question 1.2. Can we compute the homology H∗(Γ) or cohomology H (Γ)? Question 1.3. Can we solve the word problem in Γ? That is, is there an algorithm to determine whether a word in the generators represents the trivial element in Γ? 1.2 Non-positively curved manifolds In general, the answer to both of these questions is `no'. Novikov (1955) and Boone (1959) constructed a finitely presentable group with an unsolvable word problem, and Cameron Gordon proved that the rank of H2(Γ) is not computable. -
Bachelorarbeit Im Studiengang Audiovisuelle Medien Die
Bachelorarbeit im Studiengang Audiovisuelle Medien Die Nutzbarkeit von Fraktalen in VFX Produktionen vorgelegt von Denise Hauck an der Hochschule der Medien Stuttgart am 29.03.2019 zur Erlangung des akademischen Grades eines Bachelor of Engineering Erst-Prüferin: Prof. Katja Schmid Zweit-Prüfer: Prof. Jan Adamczyk Eidesstattliche Erklärung Name: Vorname: Hauck Denise Matrikel-Nr.: 30394 Studiengang: Audiovisuelle Medien Hiermit versichere ich, Denise Hauck, ehrenwörtlich, dass ich die vorliegende Bachelorarbeit mit dem Titel: „Die Nutzbarkeit von Fraktalen in VFX Produktionen“ selbstständig und ohne fremde Hilfe verfasst und keine anderen als die angegebenen Hilfsmittel benutzt habe. Die Stellen der Arbeit, die dem Wortlaut oder dem Sinn nach anderen Werken entnommen wurden, sind in jedem Fall unter Angabe der Quelle kenntlich gemacht. Die Arbeit ist noch nicht veröffentlicht oder in anderer Form als Prüfungsleistung vorgelegt worden. Ich habe die Bedeutung der ehrenwörtlichen Versicherung und die prüfungsrechtlichen Folgen (§26 Abs. 2 Bachelor-SPO (6 Semester), § 24 Abs. 2 Bachelor-SPO (7 Semester), § 23 Abs. 2 Master-SPO (3 Semester) bzw. § 19 Abs. 2 Master-SPO (4 Semester und berufsbegleitend) der HdM) einer unrichtigen oder unvollständigen ehrenwörtlichen Versicherung zur Kenntnis genommen. Stuttgart, den 29.03.2019 2 Kurzfassung Das Ziel dieser Bachelorarbeit ist es, ein Verständnis für die Generierung und Verwendung von Fraktalen in VFX Produktionen, zu vermitteln. Dabei bildet der Einblick in die Arten und Entstehung der Fraktale -
1 SL2(R) Problems 1 2 1
1 SL2(R) problems 1 2 1. Show that SL2(R) is homeomorphic to S R . 2 × Hint 1: SL2(R) acts on R 0 transitively with stabilizer of (1, 0) equal − to the set of upper triangular matrices with 1’s on the diagonal, which is homeomorphic to R. This gives a “principal bundle”, i.e. a map 2 SL2(R) R 0 whose point inverses are lines. Construct a section 2 → − R 0 SL2(R) and then a homeomorphism to the product. − → Hint 2: Same thing, but for the action of SL2(R) on the upper half plane, with point inverses circles. Better yet (but uses more sophisticated math): PSL2(R)= SL2(R)/ I can be identified with the unit tangent bundle 2 ± 2 T1H of the hyperbolic plane H , which in turn can be identified with 2 1 H S∞, product with the circle at infinity. This shows that PSL2(R) × 1 2 is homeomorphic to S R , but SL2(R) is a double cover of PSL2(R). × 2. We have seen that trace Tr(A) determines the conjugacy class of A ∈ SL2(R) provided Tr(A) > 2. Show that this conjugacy class, as a subset | | 1 of SL2(R), is a closed subset homeomorphic to S R. × 3. The set of parabolics is not closed and consists of four conjugacy classes (two with trace 2 and two with trace 2), each homeomorphic to S1 R. − × 4. There are two conjugacy classes of elements of SL2(R) whose trace is a given number in ( 2, 2), each closed and homeomorphic to R2. -
Fractals a Fractal Is a Shape That Seem to Have the Same Structure No Matter How Far You Zoom In, Like the figure Below
Fractals A fractal is a shape that seem to have the same structure no matter how far you zoom in, like the figure below. Sometimes it's only part of the shape that repeats. In the figure below, called an Apollonian Gasket, no part looks like the whole shape, but the parts near the edges still repeat when you zoom in. Today you'll learn how to construct a few fractals: • The Snowflake • The Sierpinski Carpet • The Sierpinski Triangle • The Pythagoras Tree • The Dragon Curve After you make a few of those, try constructing some fractals of your own design! There's more on the back. ! Challenge Problems In order to solve some of the more difficult problems today, you'll need to know about the geometric series. In a geometric series, we add up a sequence of terms, 1 each of which is a fixed multiple of the previous one. For example, if the ratio is 2 , then a geometric series looks like 1 1 1 1 1 1 1 + + · + · · + ::: 2 2 2 2 2 2 1 12 13 = 1 + + + + ::: 2 2 2 The geometric series has the incredibly useful property that we have a good way of 1 figuring out what the sum equals. Let's let r equal the common ratio (like 2 above) and n be the number of terms we're adding up. Our series looks like 1 + r + r2 + ::: + rn−2 + rn−1 If we multiply this by 1 − r we get something rather simple. (1 − r)(1 + r + r2 + ::: + rn−2 + rn−1) = 1 + r + r2 + ::: + rn−2 + rn−1 − ( r + r2 + ::: + rn−2 + rn−1 + rn ) = 1 − rn Thus 1 − rn 1 + r + r2 + ::: + rn−2 + rn−1 = : 1 − r If we're clever, we can use this formula to compute the areas and perimeters of some of the shapes we create. -
Design and Development of Sierpinski Carpet Microstrip Fractal Antenna for Multiband Applications
ISSN (Online) 2278-1021 ISSN (Print) 2319-5940 IJARCCE International Journal of Advanced Research in Computer and Communication Engineering NCRICT-2017 Ahalia School of Engineering and Technology Vol. 6, Special Issue 4, March 2017 Design and Development of Sierpinski Carpet Microstrip Fractal Antenna for Multiband Applications Suvarna Sivadas1, Saneesh V S2 PG Scholar, Department of ECE, Jawaharlal College of Engineering & Technology, Palakkad, India1 Assistant Professor, Department of ECE, Jawaharlal College of Engineering & Technology, Palakkad, India2 Abstract: The rapid growth of wireless technologies has drawn new demands for integrated components including antennas. Antenna miniaturization is necessary for achieving optimal design of modern handheld wireless communication devices. Numerous techniques have been proposed for the miniaturization of microstrip fractal antennas having multiband characteristics. A sierpinski carpet microstrip fractal antennas is designed in a centre frequency of 2.4 GHz which is been simulated. This is to understand the concept of antenna. Perform numerical solutions using HFSS software and to study the antenna properties by comparison of measurements and simulation results. Keywords: fractal; sierpinski carpet; multiband. I. INTRODUCTION In modern wireless communication systems wider Multiband frequency response that derives from bandwidth, multiband and low profile antennas are in great the inherent properties of the fractal geometry of the demand for various communication applications. This has antenna. -
Covering Spaces and the Fundamental Group
FUNDAMENTAL GROUPS AND COVERING SPACES NICK SALTER, SUBHADIP CHOWDHURY 1. Preamble The following exercises are intended to introduce you to some of the basic ideas in algebraic topology, namely the fundamental group and covering spaces. Exercises marked with a (B) are basic and fundamental. If you are new to the subject, your time will probably be best spent digesting the (B) exercises. If you have some familiarity with the material, you are under no obligation to attempt the (B) exercises, but you should at least convince yourself that you know how to do them. If you are looking to focus on specific ideas and techniques, I've made some attempt to label exercises with the sorts of ideas involved. 2. Two extremely important theorems If you get nothing else out of your quarter of algebraic topology, you should know and understand the following two theorems. The exercises on this sheet (mostly) exclusively rely on them, along with the ability to reason spatially and geometrically. Theorem 2.1 (Seifert-van Kampen). Let X be a topological space and assume that X = U[V with U; V ⊂ X open such that U \ V is path connected and let x0 2 U \ V . We consider the commutative diagram π1(U; x0) i1∗ j1∗ π1(U \ V; x0) π1(X; x0) i2∗ j2∗ π1(V; x0) where all maps are induced by the inclusions. Then for any group H and any group homomor- phisms φ1 : π1(U; x0) ! H and φ2 : π1(V; x0) ! H such that φ1i1∗ = φ2i2∗; Date: September 20, 2015. 1 2 NICK SALTER, SUBHADIP CHOWDHURY there exists a unique group homomorphism φ : π1(X; x0) ! H such that φ1 = φj1∗, φ2 = φj2∗.