1 CURVATURE CHANGES in BIOLOGICAL DYNAMICS Arturo Tozzi
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On the Geometry of Space
On the geometry of Space Frederik Vantomme∗ Madrid, Spain 23rd of April 2015 Abstract In this paper, we explore the possibility that black holes and Space could be the geometrically Compactified Transverse Slices ("CTS"s) of their higher (+1) dimen- sional space. Our hypothesis is that we might live somewhere in between partially 1 compressed regions of space, namely 4dL+R hyperspace compactified to its 3d transverse slice, and fully compressed dark regions, i.e. black holes, still containing all Ld432-1-234dR dimensional fields. This places the DGP, ADD, Kaluza-Klein, Randall-Sundrum, Holographic and Vanishing Dimensions theories in a different perspective. We first postulate that a black hole could be the result of the compactification (fibration) of a 3d burned up S2 star to its 2d transverse slice; the 2d dimensional discus itself further spiralling down into a bundle of one-dimensional fibres. Similarly, Space could be the compactified transverse slice (fibration) of its higher 3 4dL+R S hyper-sphere to its 3d transverse slice, the latter adopting the topology of a closed and flat left+right handed trefoil knot. By further extending these two ideas, we might consider that the Universe in its initial state was a "Matroska" 4dL+R hyperspace compactified, in cascading order, to a bundle of one-dimensional fibres. The Big Bang could be an explosion from within that broke the cascadingly compressed Universe open. ∗[email protected] 1As we shall only consider spatial dimensions and leave the time dimension out, ordinary 3d+1t spacetime will be reduced to '3d' space; 4d+1t spacetime will be denoted '4d' space, etc. -
Arxiv:1204.4952V2 [Math.HO] 17 May 2012
Sculptures in S3 Saul Schleimer Henry Segerman∗ Mathematics Institute Department of Mathematics and Statistics University of Warwick University of Melbourne Coventry CV4 7AL Parkville VIC 3010 United Kingdom Australia [email protected] [email protected] Abstract We construct a number of sculptures, each based on a geometric design native to the three-dimensional sphere. Using stereographic projection we transfer the design from the three-sphere to ordinary Euclidean space. All of the sculptures are then fabricated by the 3D printing service Shapeways. 1 Introduction The three-sphere, denoted S3, is a three-dimensional analog of the ordinary two-dimensional sphere, S2. In n+ general, the n–dimensional sphere is a subset of Euclidean space, R 1, as follows: n n+1 2 2 2 S = f(x0;x1;:::;xn) 2 R j x0 + x1 + ··· + xn = 1g: Thus S2 can be seen as the usual unit sphere in R3. Visualising objects in dimensions higher than three is non-trivial. However for S3 we can use stereographic projection to reduce the dimension from four to three. n n n Let N = (0;:::;0;1) be the north pole of S . We define stereographic projection r : S − fNg ! R by x0 x1 xn−1 r(x0;x1;:::;xn) = ; ;:::; : 1 − xn 1 − xn 1 − xn See [1, page 27]. Figure 1a displays stereographic projection in dimension one. For any point (x;y) 2 S1 − fNg draw the straight line L through N and (x;y). Then L meets R1 at a single point; this is r(x;y). Notice that the figure is also a two-dimensional cross-section of stereographic projection in any dimension. -
Sculptures in S3
Bridges 2012: Mathematics, Music, Art, Architecture, Culture Sculptures in S3 Saul Schleimer Henry Segerman∗ Mathematics Institute Department of Mathematics and Statistics University of Warwick University of Melbourne Coventry CV4 7AL Parkville VIC 3010 United Kingdom Australia [email protected] [email protected] Abstract We construct a number of sculptures, each based on a geometric design native to the three-dimensional sphere. Using stereographic projection we transfer the design from the three-sphere to ordinary Euclidean space. All of the sculptures are then fabricated by the 3D printing service Shapeways. 1 Introduction The three-sphere, denoted S3, is a three-dimensional analog of the ordinary two-dimensional sphere, S2. In n+ general, the n–dimensional sphere is a subset of Euclidean space, R 1, as follows: n n+1 2 2 2 S = f(x0;x1;:::;xn) 2 R j x0 + x1 + ··· + xn = 1g: Thus S2 can be seen as the usual unit sphere in R3. Visualising objects in dimensions higher than three is non-trivial. However for S3 we can use stereographic projection to reduce the dimension from four to three. n n n Let N = (0;:::;0;1) be the north pole of S . We define stereographic projection r : S − fNg ! R by x0 x1 xn−1 r(x0;x1;:::;xn) = ; ;:::; : 1 − xn 1 − xn 1 − xn See [1, page 27]. Figure 1a displays stereographic projection in dimension one. For any point (x;y) 2 S1 − fNg draw the straight line L through N and (x;y). Then L meets R1 at a single point; this is r(x;y). -
Frustrated Self-Assembly of Non-Euclidean Crystals of Nanoparticles ✉ Francesco Serafin1, Jun Lu2, Nicholas Kotov 2, Kai Sun 1 & Xiaoming Mao 1
ARTICLE https://doi.org/10.1038/s41467-021-25139-9 OPEN Frustrated self-assembly of non-Euclidean crystals of nanoparticles ✉ Francesco Serafin1, Jun Lu2, Nicholas Kotov 2, Kai Sun 1 & Xiaoming Mao 1 Self-organized complex structures in nature, e.g., viral capsids, hierarchical biopolymers, and bacterial flagella, offer efficiency, adaptability, robustness, and multi-functionality. Can we program the self-assembly of three-dimensional (3D) complex structures using simple 1234567890():,; building blocks, and reach similar or higher level of sophistication in engineered materials? Here we present an analytic theory for the self-assembly of polyhedral nanoparticles (NPs) based on their crystal structures in non-Euclidean space. We show that the unavoidable geometrical frustration of these particle shapes, combined with competing attractive and repulsive interparticle interactions, lead to controllable self-assembly of structures of com- plex order. Applying this theory to tetrahedral NPs, we find high-yield and enantiopure self- assembly of helicoidal ribbons, exhibiting qualitative agreement with experimental observa- tions. We expect that this theory will offer a general framework for the self-assembly of simple polyhedral building blocks into rich complex morphologies with new material cap- abilities such as tunable optical activity, essential for multiple emerging technologies. 1 Department of Physics, University of Michigan, Ann Arbor, MI, USA. 2 Department of Chemical Engineering, University of Michigan, Ann Arbor, MI, USA. ✉ email: [email protected] NATURE COMMUNICATIONS | (2021) 12:4925 | https://doi.org/10.1038/s41467-021-25139-9 | www.nature.com/naturecommunications 1 ARTICLE NATURE COMMUNICATIONS | https://doi.org/10.1038/s41467-021-25139-9 hemically synthesized nanoparticles (NPs) display a great Euclidean 3D space, they can form non-Euclidean crystals in diversity of polyhedral shapes1. -
Interactive 4-D Visualization of Stereographic Images from the Double Orthogonal Projection
Interactive 4-D Visualization of Stereographic Images From the Double Orthogonal Projection. Michal Zamboj Charles University, Faculty of Education M. D. Rettigov´e4, 116 39 Prague 1. Abstract The double orthogonal projection of the 4-space onto two mutually perpendicular 3-spaces is a method of visualization of four-dimensional objects in a three-dimensional space. We present an interactive animation of the stereographic projection of a hyperspherical hexahedron on a 3-sphere embedded in the 4-space. Described are synthetic constructions of stereographic images of a point, hyperspherical tetrahedron, and 2-sphere on a 3-sphere from their double orthogonal projections. Consequently, the double-orthogonal projection of a freehand curve on a 3-sphere is created inversely from its stereographic image. Furthermore, we show an application to a synthetic construction of a spherical inversion and visualizations of double orthogonal projections and stereographic images of Hopf tori on a 3-sphere generated from Clelia curves on a 2-sphere. Keywords: Four-dimensional visualization, orthogonal projection, stereographic projection, Hopf fibration, Clelia curve, spherical inversion, descriptive geometry. 1 Introduction The double orthogonal projection is a four-dimensional generalization of Monge's projection. In Monge's projection, an object in the 3-space is orthogonally projected into two mutually perpen- dicular planes (horizontal and vertical, i.e. top and front view). One of these planes is chosen to be the drawing (or picture) plane and the second is rotated about their intersecting line to the drawing plane. Therefore, each point in the 3-space has two conjugated images in the drawing plane. In the double orthogonal projection, an object is in the 4-space, and we project it orthogonally into two mutually perpendicular 3-spaces.