Musical Actions of Dihedral Groups
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Chapter 1 Geometric Generalizations of the Tonnetz and Their Relation To
November 22, 2017 12:45 ws-rv9x6 Book Title yustTonnetzSub page 1 Chapter 1 Geometric Generalizations of the Tonnetz and their Relation to Fourier Phases Spaces Jason Yust Boston University School of Music, 855 Comm. Ave., Boston, MA, 02215 [email protected] Some recent work on generalized Tonnetze has examined the topologies resulting from Richard Cohn's common-tone based formulation, while Tymoczko has reformulated the Tonnetz as a network of voice-leading re- lationships and investigated the resulting geometries. This paper adopts the original common-tone based formulation and takes a geometrical ap- proach, showing that Tonnetze can always be realized in toroidal spaces, and that the resulting spaces always correspond to one of the possible Fourier phase spaces. We can therefore use the DFT to optimize the given Tonnetz to the space (or vice-versa). I interpret two-dimensional Tonnetze as triangulations of the 2-torus into regions associated with the representatives of a single trichord type. The natural generalization to three dimensions is therefore a triangulation of the 3-torus. This means that a three-dimensional Tonnetze is, in the general case, a network of three tetrachord-types related by shared trichordal subsets. Other Ton- netze that have been proposed with bounded or otherwise non-toroidal topologies, including Tymoczko's voice-leading Tonnetze, can be under- stood as the embedding of the toroidal Tonnetze in other spaces, or as foldings of toroidal Tonnetze with duplicated interval types. 1. Formulations of the Tonnetz The Tonnetz originated in nineteenth-century German harmonic theory as a network of pitch classes connected by consonant intervals. -
Arxiv:Hep-Th/0510191V1 22 Oct 2005
Maximal Subgroups of the Coxeter Group W (H4) and Quaternions Mehmet Koca,∗ Muataz Al-Barwani,† and Shadia Al-Farsi‡ Department of Physics, College of Science, Sultan Qaboos University, PO Box 36, Al-Khod 123, Muscat, Sultanate of Oman Ramazan Ko¸c§ Department of Physics, Faculty of Engineering University of Gaziantep, 27310 Gaziantep, Turkey (Dated: September 8, 2018) The largest finite subgroup of O(4) is the noncrystallographic Coxeter group W (H4) of order 14400. Its derived subgroup is the largest finite subgroup W (H4)/Z2 of SO(4) of order 7200. Moreover, up to conjugacy, it has five non-normal maximal subgroups of orders 144, two 240, 400 and 576. Two groups [W (H2) × W (H2)]×Z4 and W (H3)×Z2 possess noncrystallographic structures with orders 400 and 240 respectively. The groups of orders 144, 240 and 576 are the extensions of the Weyl groups of the root systems of SU(3)×SU(3), SU(5) and SO(8) respectively. We represent the maximal subgroups of W (H4) with sets of quaternion pairs acting on the quaternionic root systems. PACS numbers: 02.20.Bb INTRODUCTION The noncrystallographic Coxeter group W (H4) of order 14400 generates some interests [1] for its relevance to the quasicrystallographic structures in condensed matter physics [2, 3] as well as its unique relation with the E8 gauge symmetry associated with the heterotic superstring theory [4]. The Coxeter group W (H4) [5] is the maximal finite subgroup of O(4), the finite subgroups of which have been classified by du Val [6] and by Conway and Smith [7]. -
324 COHOMOLOGY of DIHEDRAL GROUPS of ORDER 2P Let D Be A
324 PHYLLIS GRAHAM [March 2. P. M. Cohn, Unique factorization in noncommutative power series rings, Proc. Cambridge Philos. Soc 58 (1962), 452-464. 3. Y. Kawada, Cohomology of group extensions, J. Fac. Sci. Univ. Tokyo Sect. I 9 (1963), 417-431. 4. J.-P. Serre, Cohomologie Galoisienne, Lecture Notes in Mathematics No. 5, Springer, Berlin, 1964, 5. , Corps locaux et isogênies, Séminaire Bourbaki, 1958/1959, Exposé 185 6. , Corps locaux, Hermann, Paris, 1962. UNIVERSITY OF MICHIGAN COHOMOLOGY OF DIHEDRAL GROUPS OF ORDER 2p BY PHYLLIS GRAHAM Communicated by G. Whaples, November 29, 1965 Let D be a dihedral group of order 2p, where p is an odd prime. D is generated by the elements a and ]3 with the relations ap~fi2 = 1 and (ial3 = or1. Let A be the subgroup of D generated by a, and let p-1 Aoy Ai, • • • , Ap-\ be the subgroups generated by j8, aft, • * • , a /3, respectively. Let M be any D-module. Then the cohomology groups n n H (A0, M) and H (Aif M), i=l, 2, • • • , p — 1 are isomorphic for 1 l every integer n, so the eight groups H~ (Df Af), H°(D, M), H (D, jfef), 2 1 Q # (A Af), ff" ^. M), H (A, M), H-Wo, M), and H»(A0, M) deter mine all cohomology groups of M with respect to D and to all of its subgroups. We have found what values this array takes on as M runs through all finitely generated -D-modules. All possibilities for the first four members of this array are deter mined as a special case of the results of Yang [4]. -
Dihedral Groups Ii
DIHEDRAL GROUPS II KEITH CONRAD We will characterize dihedral groups in terms of generators and relations, and describe the subgroups of Dn, including the normal subgroups. We will also introduce an infinite group that resembles the dihedral groups and has all of them as quotient groups. 1. Abstract characterization of Dn −1 −1 The group Dn has two generators r and s with orders n and 2 such that srs = r . We will show every group with a pair of generators having properties similar to r and s admits a homomorphism onto it from Dn, and is isomorphic to Dn if it has the same size as Dn. Theorem 1.1. Let G be generated by elements x and y where xn = 1 for some n ≥ 3, 2 −1 −1 y = 1, and yxy = x . There is a surjective homomorphism Dn ! G, and if G has order 2n then this homomorphism is an isomorphism. The hypotheses xn = 1 and y2 = 1 do not mean x has order n and y has order 2, but only that their orders divide n and divide 2. For instance, the trivial group has the form hx; yi where xn = 1, y2 = 1, and yxy−1 = x−1 (take x and y to be the identity). Proof. The equation yxy−1 = x−1 implies yxjy−1 = x−j for all j 2 Z (raise both sides to the jth power). Since y2 = 1, we have for all k 2 Z k ykxjy−k = x(−1) j by considering even and odd k separately. Thus k (1.1) ykxj = x(−1) jyk: This shows each product of x's and y's can have all the x's brought to the left and all the y's brought to the right. -
Fourier Phase and Pitch-Class Sum
Fourier Phase and Pitch-Class Sum Dmitri Tymoczko1 and Jason Yust2(B) Author Proof 1 Princeton University, Princeton, NJ 08544, USA [email protected] 2 Boston University, Boston, MA 02215, USA [email protected] AQ1 Abstract. Music theorists have proposed two very different geometric models of musical objects, one based on voice leading and the other based on the Fourier transform. On the surface these models are completely different, but they converge in special cases, including many geometries that are of particular analytical interest. Keywords: Voice leading Fourier transform Tonal harmony Musical scales Chord geometry· · · · 1Introduction Early twenty-first century music theory explored a two-pronged generalization of traditional set theory. One prong situated sets and set-classes in continuous, non-Euclidean spaces whose paths represented voice leadings, or ways of mov- ing notes from one chord to another [4,13,16]. This endowed set theory with a contrapuntal aspect it had previously lacked, embedding its discrete entities in arobustlygeometricalcontext.AnotherpronginvolvedtheFouriertransform as applied to pitch-class distributions: this provided alternative coordinates for describing chords and set classes, coordinates that made manifest their harmonic content [1,3,8,10,19–21]. Harmonies could now be described in terms of their resemblance to various equal divisions of the octave, paradigmatic objects such as the augmented triad or diminished seventh chord. These coordinates also had a geometrical aspect, similar to yet distinct from voice-leading geometry. In this paper, we describe a new convergence between these two approaches. Specifically, we show that there exists a class of simple circular voice-leading spaces corresponding, in the case of n-note nearly even chords, to the nth Fourier “phase spaces.” An isomorphism of points exists for all chords regardless of struc- ture; when chords divide the octave evenly, we can extend the isomorphism to paths, which can then be interpreted as voice leadings. -
MAT313 Fall 2017 Practice Midterm II the Actual Midterm Will Consist of 5-6 Problems
MAT313 Fall 2017 Practice Midterm II The actual midterm will consist of 5-6 problems. It will be based on subsections 127-234 from sections 6-11. This is a preliminary version. I might add few more problems to make sure that all important concepts and methods are covered. Problem 1. 2 Let P be a set of lines through 0 in R . The group SL(2; R) acts on X by linear transfor- mations. Let H be the stabilizer of a line defined by the equation y = 0. (1) Describe the set of matrices H. (2) Describe the orbits of H in X. How many orbits are there? (3) Identify X with the set of cosets of SL(2; R). Solution. (1) Denote the set of lines by P = fLm;ng, where Lm;n is equal to f(x; y)jmx+ny = 0g. a b Note that Lkm;kn = Lm;n if k 6= 0. Let g = c d , ad − bc = 1 be an element of SL(2; R). Then gLm;n = f(x; y)jm(ax + by) + n(cx + dy) = 0g = Lma+nc;mb+nd. a b By definition the line f(x; y)jy = 0g is equal to L0;1. Then c d L0;1 = Lc;d. The line Lc;d coincides with L0;1 if c = 0. Then the stabilizer Stab(L0;1) coincides with a b H = f 0 d g ⊂ SL(2; R). (2) We already know one trivial H-orbit O = fL0;1g. The complement PnfL0;1g is equal to fLm:njm 6= 0g = fL1:n=mjm 6= 0g = fL1:tg. -
Notes on Geometry of Surfaces
Notes on Geometry of Surfaces Contents Chapter 1. Fundamental groups of Graphs 5 1. Review of group theory 5 2. Free groups and Ping-Pong Lemma 8 3. Subgroups of free groups 15 4. Fundamental groups of graphs 18 5. J. Stalling's Folding and separability of subgroups 21 6. More about covering spaces of graphs 23 Bibliography 25 3 CHAPTER 1 Fundamental groups of Graphs 1. Review of group theory 1.1. Group and generating set. Definition 1.1. A group (G; ·) is a set G endowed with an operation · : G × G ! G; (a; b) ! a · b such that the following holds. (1) 8a; b; c 2 G; a · (b · c) = (a · b) · c; (2) 91 2 G: 8a 2 G, a · 1 = 1 · a. (3) 8a 2 G, 9a−1 2 G: a · a−1 = a−1 · a = 1. In the sequel, we usually omit · in a · b if the operation is clear or understood. By the associative law, it makes no ambiguity to write abc instead of a · (b · c) or (a · b) · c. Examples 1.2. (1)( Zn; +) for any integer n ≥ 1 (2) General Linear groups with matrix multiplication: GL(n; R). (3) Given a (possibly infinite) set X, the permutation group Sym(X) is the set of all bijections on X, endowed with mapping composition. 2 2n −1 −1 (4) Dihedral group D2n = hr; sjs = r = 1; srs = r i. This group can be visualized as the symmetry group of a regular (2n)-polygon: s is the reflection about the axe connecting middle points of the two opposite sides, and r is the rotation about the center of the 2n-polygon with an angle π=2n. -
Generalized Tonnetze and Zeitnetz, and the Topology of Music Concepts
June 25, 2019 Journal of Mathematics and Music tonnetzTopologyRev Submitted exclusively to the Journal of Mathematics and Music Last compiled on June 25, 2019 Generalized Tonnetze and Zeitnetz, and the Topology of Music Concepts Jason Yust∗ School of Music, Boston University () The music-theoretic idea of a Tonnetz can be generalized at different levels: as a network of chords relating by maximal intersection, a simplicial complex in which vertices represent notes and simplices represent chords, and as a triangulation of a manifold or other geomet- rical space. The geometrical construct is of particular interest, in that allows us to represent inherently topological aspects to important musical concepts. Two kinds of music-theoretical geometry have been proposed that can house Tonnetze: geometrical duals of voice-leading spaces, and Fourier phase spaces. Fourier phase spaces are particularly appropriate for Ton- netze in that their objects are pitch-class distributions (real-valued weightings of the twelve pitch classes) and proximity in these space relates to shared pitch-class content. They admit of a particularly general method of constructing a geometrical Tonnetz that allows for interval and chord duplications in a toroidal geometry. The present article examines how these du- plications can relate to important musical concepts such as key or pitch-height, and details a method of removing such redundancies and the resulting changes to the homology the space. The method also transfers to the rhythmic domain, defining Zeitnetze for cyclic rhythms. A number of possible Tonnetze are illustrated: on triads, seventh chords, ninth-chords, scalar tetrachords, scales, etc., as well as Zeitnetze on a common types of cyclic rhythms or time- lines. -
Dihedral Group of Order 8 (The Number of Elements in the Group) Or the Group of Symmetries of a Square
CHAPTER 1 Introduction to Groups Symmetries of a Square A plane symmetry of a square (or any plane figure F ) is a function from the square to itself that preserves distances, i.e., the distance between the images of points P and Q equals the distance between P and Q. The eight symmetries of a square: 22 1. INTRODUCTION TO GROUPS 23 These are all the symmetries of a square. Think of a square cut from a piece of glass with dots of di↵erent colors painted on top in the four corners. Then a symmetry takes a corner to one of four corners with dot up or down — 8 possibilities. A succession of symmetries is a symmetry: Since this is a composition of functions, we write HR90 = D, allowing us to view composition of functions as a type of multiplication. Since composition of functions is associative, we have an operation that is both closed and associative. R0 is the identity: for any symmetry S, R0S = SR0 = S. Each of our 1 1 1 symmetries S has an inverse S− such that SS− = S− S = R0, our identity. R0R0 = R0, R90R270 = R0, R180R180 = R0, R270R90 = R0 HH = R0, V V = R0, DD = R0, D0D0 = R0 We have a group. This group is denoted D4, and is called the dihedral group of order 8 (the number of elements in the group) or the group of symmetries of a square. 24 1. INTRODUCTION TO GROUPS We view the Cayley table or operation table for D4: For HR90 = D (circled), we find H along the left and R90 on top. -
MTO 25.1 Examples: Willis, Comprehensibility and Ben Johnston’S String Quartet No
MTO 25.1 Examples: Willis, Comprehensibility and Ben Johnston’s String Quartet No. 9 (Note: audio, video, and other interactive examples are only available online) http://mtosmt.org/issues/mto.19.25.1/mto.19.25.1.willis.html Example 1. Partch’s 5-limit tonality diamond, after Partch (1974, 110) also given with pitch names and cent deviations from twelve-tone equal temperament Example 2. Partch’s 11-limit tonality diamond, after Partch (1974, 159) Example 3. The just-intoned diatonic shown in ratios, cents, and on a Tonnetz Example 4. Johnston’s accidentals, the 5-limit ration they inflect, the target ratio they bring about, their ratio and cent value. As an example of how this table works, take row 11. If we multiply 4:3 by 33:32 it sums to 11:8. This is equivalent to raising a perfect fourth by Johnston’s 11 chroma. Example 5. The overtone and undertone series of C notated using Johnston’s method Example 6. A Tonnetz with the syntonic diatonic highlighted in grey. The solid lines connect the two 5-limit pitches that may be inflected to produce a tonal or tonal seventh against the C. This makes clear why the tonal seventh of C is notated as lowered by a syntonic comma in addition to an inverse 7 sign. It is because the pitch is tuned relative to the D- (10:9), which is a syntonic comma lower than the D that appears in the diatonic gamut. Example 7. Johnston, String Quartet No. 9/I, m. 109. A comma pump progression shown with Roman Numerals and a Tonnetz. -
From Schritte and Wechsel to Coxeter Groups 3
From Schritte and Wechsel to Coxeter Groups Markus Schmidmeier1 Abstract: The PLR-moves of neo-Riemannian theory, when considered as re- flections on the edges of an equilateral triangle, define the Coxeter group S3. The elements are in a natural one-to-one correspondence with the trianglese in the infinite Tonnetz. The left action of S3 on the Tonnetz gives rise to interest- ing chord sequences. We compare the systeme of transformations in S3 with the system of Schritte and Wechsel introduced by Hugo Riemann in 1880e . Finally, we consider the point reflection group as it captures well the transition from Riemann’s infinite Tonnetz to the finite Tonnetz of neo-Riemannian theory. Keywords: Tonnetz, neo-Riemannian theory, Coxeter groups. 1. PLR-moves revisited In neo-Riemannian theory, chord progressions are analyzed in terms of elementary moves in the Tonnetz. For example, the process of going from tonic to dominant (which differs from the tonic chord in two notes) is decomposed as a product of two elementary moves of which each changes only one note. The three elementary moves considered are the PLR-transformations; they map a major or minor triad to the minor or major triad adjacent to one of the edges of the triangle representing the chord in the Tonnetz. See [4] and [5]. C♯ G♯ .. .. .. .. ... ... ... ... ... PR ... ... PL ... A ................E ................ B′ .. .. R.. .. L .. .. ... ... ... ... ... ... ... LR ... ... ∗ ... ... RL ... ( ) ′ F′ ................C ................ G ................ D .. .. P .. .. ... ... ... ... ... LP ... ... RP ... A♭ ................E♭ ................ B♭′ arXiv:1901.05106v3 [math.CO] 4 Apr 2019 Figure 1. Triads in the vicinity of the C-E-G-chord Our paper is motivated by the observation that PLR-moves, while they provide a tool to measure distance between triads, are not continuous as operations on the Tonnetz: Let s be a sequence of PLR-moves. -
A Tonnetz Model for Pentachords
A Tonnetz model for pentachords Luis A. Piovan KEYWORDS. neo-Riemann network, pentachord, contextual group, Tessellation, Poincaré disk, David Lewin, Charles Koechlin, Igor Stravinsky. ABSTRACT. This article deals with the construction of surfaces that are suitable for repre- senting pentachords or 5-pitch segments that are in the same T {I class. It is a generalization of the well known Öttingen-Riemann torus for triads of neo-Riemannian theories. Two pen- tachords are near if they differ by a particular set of contextual inversions and the whole contextual group of inversions produces a Tiling (Tessellation) by pentagons on the surfaces. A description of the surfaces as coverings of a particular Tiling is given in the twelve-tone enharmonic scale case. 1. Introduction The interest in generalizing the Öttingen-Riemann Tonnetz was felt after the careful analysis David Lewin made of Stockhausen’s Klavierstück III [25, Ch. 2], where he basically shows that the whole work is constructed with transformations upon the single pentachord xC,C#, D, D#, F #y. A tiled torus with equal tiles like the usual Tonnetz of Major and Minor triads is not possible by using pentagons (you cannot tile a torus or plane by regular convex pentagons). Therefore one is forced to look at other surfaces and fortunately there is an infinite set of closed surfaces where one can gather regular pentagonal Tilings. These surfaces (called hyperbolic) are distinguished by a single topological invariant: the genus or arXiv:1301.4255v1 [math.HO] 17 Jan 2013 number of holes the surface has (see Figure 8)1. The analysis2 of Schoenberg’s, Opus 23, Number 3, made clear the type of transfor- mations3 to be used.