SOME HOMOTOPY GROUPS OF STIEFEL MANIFOLDS 1

Similar documents
MULTIPLICATIVE FIBRE MAPS

i;\-'i frz q > R>? >tr E*+ [S I z> N g> F 'x sa :r> >,9 T F >= = = I Y E H H>tr iir- g-i I * s I!,i --' - = a trx - H tnz rqx o >.F g< s Ire tr () -s

The Fundamental Basis Theorem of Geometry from an algebraic point of view

ON THE GROUP &[X] OF HOMOTOPY EQUIVALENCE MAPS BY WEISHU SHIH 1. Communicated by Deane Montgomery, November 13, 1963

'NOTAS"CRITICAS PARA UNA TEDRIA DE M BUROCRACIA ESTATAL * Oscar Oszlak

NORMAL VECTOR FIELDS ON MANIFOLDS1 W. S. MASSEY

NON-COMMUTATIVE GRÖBNER BASES FOR COMMUTATIVE ALGEBRAS

Algebraic Montgomery-Yang problem: the log del Pezzo surface case

Mathematische Zeitschrift

A L A BA M A L A W R E V IE W

APPH 4200 Physics of Fluids

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9

A note on the multiplication of sparse matrices

Math 262A Lecture Notes - Nechiporuk s Theorem

LATTICE POINT SOLUTION OF THE GENERALIZED PROBLEM OF TERQUEi. AND AN EXTENSION OF FIBONACCI NUMBERS.

necessita d'interrogare il cielo

ON THE DENSITY OF SOME SEQUENCES OF INTEGERS P. ERDOS

2 Q 10. Likewise, in case of multiple particles, the corresponding density in 2 must be averaged over all

THE HOMOTOPY TYPES OF SU(5)-GAUGE GROUPS. Osaka Journal of Mathematics. 52(1) P.15-P.29

Chapter II TRIANGULAR NUMBERS

THE AVERAGE NORM OF POLYNOMIALS OF FIXED HEIGHT

Homotopy Analysis Method for Nonlinear Jaulent-Miodek Equation

A note on Samelson products in the exceptional Lie groups

APPH 4200 Physics of Fluids

ON THE SLOPE OF THE SCHUR FUNCTOR OF A VECTOR BUNDLE

#A52 INTEGERS 10 (2010), COMBINATORIAL INTERPRETATIONS OF BINOMIAL COEFFICIENT ANALOGUES RELATED TO LUCAS SEQUENCES

PROPER HOLOMORPHIC MAPPINGS THAT MUST BE RATIONAL

#A62 INTEGERS 16 (2016) REPRESENTATION OF INTEGERS BY TERNARY QUADRATIC FORMS: A GEOMETRIC APPROACH

4 = (0.02) 3 13, = 0.25 because = 25. Simi-

176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s

A geometric solution of the Kervaire Invariant One problem

Explicit solution of the polynomial least-squares approximation problem on Chebyshev extrema nodes

Metric Entropy of Convex Hulls

ON RANDERS CHANGE OF GENERALIZED mth ROOT METRIC

Element Cube Project (x2)

KONINKL. NEDERL. AKADEMIE VAN WETENSCHAPPEN AMSTERDAM Reprinted from Proceedings, Series A, 61, No. 1 and Indag. Math., 20, No.

The Hilbert Schmidt version of the commutator theorem for zero trace matrices

nx ~p Us x Uns2"'-1,» i

A Bernstein-Markov Theorem for Normed Spaces

ON THE TWO-LEVEL PRECONDITIONING IN LEAST SQUARES METHOD

Some remarks on the root invariant

The Distribution of the Covariance Matrix for a Subset of Elliptical Distributions with Extension to Two Kurtosis Parameters

THE S 1 -EQUIVARIANT COHOMOLOGY RINGS OF (n k, k) SPRINGER VARIETIES

}, (n 0) be a finite irreducible, discrete time MC. Let S = {1, 2,, m} be its state space. Let P = [p ij. ] be the transition matrix of the MC.

lecture 37: Linear Multistep Methods: Absolute Stability, Part I lecture 38: Linear Multistep Methods: Absolute Stability, Part II

The Periodic Table of Elements

P a g e 5 1 of R e p o r t P B 4 / 0 9

Feature Extraction Techniques

arxiv: v1 [math.pr] 17 May 2009

Infinitely Many Trees Have Non-Sperner Subtree Poset

MODULAR HYPERBOLAS AND THE CONGRUENCE ax 1 x 2 x k + bx k+1 x k+2 x 2k c (mod m)

Executive Committee and Officers ( )

arxiv: v1 [math.co] 22 Oct 2018

Chapter 8 Deflection. Structural Mechanics 2 Dept of Architecture

REMARK ON LOOP SPACES

Page 1 Lab 1 Elementary Matrix and Linear Algebra Spring 2011

Linear Algebra. Solving Linear Systems. Copyright 2005, W.R. Winfrey

arxiv:math/ v1 [math.nt] 15 Jul 2003

Sub: Submission of the copy of Investor presentation under regulation 30 of SEBI (Listing Obligations & Disclosure Reguirements) Regulations

RIEMANN-ROCH FOR PUNCTURED CURVES VIA ANALYTIC PERTURBATION THEORY [SKETCH]

LOCALLY ^-CLOSED SPACES AND RIM /»-CLOSED SPACES

Curious Bounds for Floor Function Sums

Exponential sums and the distribution of inversive congruential pseudorandom numbers with prime-power modulus

RIGIDITY OF QUASI-EINSTEIN METRICS

( G 2,2 i 4; Z 2. n+k

The Periodic Table. Periodic Properties. Can you explain this graph? Valence Electrons. Valence Electrons. Paramagnetism

ma x = -bv x + F rod.

Low complexity bit parallel multiplier for GF(2 m ) generated by equally-spaced trinomials

Sequence Analysis, WS 14/15, D. Huson & R. Neher (this part by D. Huson) February 5,

CLOSED (J-I)-CONNECTED (2J+1)-MANIFOLDS, s = 3, 7.

Nilpotency of Atomic Steenrod Squares

NAME: 3rd (final) EXAM

ON THE OSCILLATION OF DIFFERENTIAL EQUATIONS WITH PERIODIC COEFFICIENTS

Chapter 6 1-D Continuous Groups

o C *$ go ! b», S AT? g (i * ^ fc fa fa U - S 8 += C fl o.2h 2 fl 'fl O ' 0> fl l-h cvo *, &! 5 a o3 a; O g 02 QJ 01 fls g! r«'-fl O fl s- ccco

Geometric dimension of stable vector bundles over spheres

Atomic Positive Linear Maps in Matrix Algebras

Cohomology operations and the Steenrod algebra

Last 4 Digits of USC ID:

ON THE CONSTRUCTION OF DUALLY FLAT FINSLER METRICS

THE EILENBERG-MOORE SPECTRAL SEQUENCE AND THE MOD 2 COHOMOLOGY OF

Importance of Sources using the Repeated Fusion Method and the Proportional Conflict Redistribution Rules #5 and #6

ON JONES'S KAHN-PRIDDY THEOREM. Haynes Miller~ Massachusetts Institute of Technology Cambridge, MA 02139/USA

Algorithms for Bernoulli and Related Polynomials

Tausend Und Eine Nacht

F l a s h-b a s e d S S D s i n E n t e r p r i s e F l a s h-b a s e d S S D s ( S o-s ltiad t e D r i v e s ) a r e b e c o m i n g a n a t t r a c

Lean Walsh Transform

Speed of light c = m/s. x n e a x d x = 1. 2 n+1 a n π a. He Li Ne Na Ar K Ni 58.

(for. We say, if, is surjective, that E has sufficiently many sections. In this case we have an exact sequence as U-modules:

Block designs and statistics

Bonding/Lewis Dots Lecture Page 1 of 12 Date. Bonding. What is Coulomb's Law? Energy Profile: Covalent Bonds. Electronegativity and Linus Pauling

Smith theory. Andrew Putman. Abstract

Solutions and Ions. Pure Substances

Solutions of Discretized Affine Toda Field Equations for A (1)

Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia

Anton Bourdine. 1. Introduction. and approximate propagation constants by following simple ratio (Equation (32.22) in [1]):

MANIFOLDS WITH FUNDAMENTAL GROUP A GENERALIZED FREE PRODUCT. I

G G G G G. Spec k G. G Spec k G G. G G m G. G Spec k. Spec k

Radiometric Dating (tap anywhere)

Linear estimation in models based on a graph

Transcription:

SME HMTPY GRUPS F STIEFEL MAIFLDS 1 BY C. S. H AD M. E. MAHWALD Counicated by W. S. Massey, February 1, 1965 Paechter [7] ade soe putations of Tk p (Vk,) where Vk, is the Stiefel anifold of fraes in k space. In this note we give a table (Table 1) extending his results in the case where is large. Since Vk, >Vki,i >S k is a fibering it is clear that Tk p (Vk,) depends only on k and p for p^ra. This is called the stable range and we feel that these stable groups are the ost iportant ones. n the other hand for sall values of ra, one of us [] has ade extensive putations and the results are available. Jaes' periodicity [5, Theore 3.1] is reflected in the table but the basic periodicity of period is also present. In [l] it is proved that if n > 1, then TT ; (5(W)) = TT/S) 7r J i(fn,n) for j<n 1. Hence it is easy to deduce the first fourteen nonstable groups of S(n) fro this table. Tables of hootopy groups are uch ore useful if generators are given. Instead of generators we settle for giving the order of the iage of i*: 7rjb p(5*) *Trkp(Vk, ) (Table ). ne can nstruct the generators fro this inforation and this ap has iportant nnections with Whitehead products []. The groups have been puted by using odified Postnikov towers [6]. An outline of the putation for one case, 6 od 3, is given. The case k = 6 od 3. This procedure is essentially the sae as the Adas spectral sequence ethod. Let = 3»6 and we suppose ra is large. Consider the fibering F3n«,7-*Fn,i-^F n,-6. We are only interested in groups in the hootopy stable range so that we can nstruct a new fibering ~ Vzn,-& ""* Vzn6,1 ~~* Vzn,l' We will build the odified Postnikov tower to this fibering. By [3] the hoology of T^n.i is given by ^'(P^n.i; Z ) =, < i < 3fl - 1. = Z, 3n - 1 ^ i ^ 3» - 1. Let hi generate H i (Vzn,i) Z ) when it is nonzero. Then Sq*hi 1 This research was supported by a grant fro the U. S. Ary Research ffice (Durha). 661

66 C. S. H AD M. E. MAHWALD [July I J ) J ( I J ^ J S S t-» rh Î r 1 J v T J I ^ r-1 t^ J I W r-h c* J Csl <* ^Tf î 'M v c* < f I * rh "* C* I e* I l 'W I <* C^ J cst cî T vo r-1 J l I! J tb J I I i 't J t i-h "e* I J <"<* 5(3) Z I "fcl S i t I *î vo l rh ^ I i «I J I I T I I I I < J fr I < I I ( J' I M < W < J ) "k v i» in i-h J ( I iu J. <M ^ C* I irt ^< J 9 vj I 1 "*

1965] SME HMTPY GRUPS F STIEFEL MAIFLDS 663 J J J I I «" l J oo J l J -* vo «a ss a ^c W < "" *->» ^ '-*» ^f S 3. r- 5» r-l l l vo vo -* vo vo I ^jp; ta "fe S V eo \o H r J l "feo "to " "^ " T J l J a s s ^ cf ci ci et «-» «a» l r-l t-i I ^ ] J J ^ * 'S? *""* ^" ^ ^-f ^C 'ir' H I-H *-» V w *_* r-l r-h r-l t/3 1-1 f J *< l J -, _. s s s s I J I I * Ç \ 3 rh «K S d H -«* r-l J J I I I I s I s a S Ci Ct o rh * r-h in i-h I I et. I «I I ««J» 1/5 «-H i-* I w w r-«"f* r-* l r-h J l ^ J vo l l CS I I I I S c- ^ oc So <*

66 C. S. H AD M. E. MAHWALD [July TABLE rder of i(fc et$ n )->7iï( V*n,n)) Top row is the nae of the ste»() i V 17 V p* a V 17* 77 77P rpa M i7ju r oo 1 oo 3 115(1) oo 5 53(6) 6 oo (3) 7 15 = (J)A» y. Hence the hoology of the base space is given by hnn = 5c7* 1 A n-i. We let /W-i = A. 1st level. ver the Steenrod algebra the basis for ker p* is given by {Sq 7 h, Sq s h, Sq l *h}. f these three only the first two can be spherical in the sense of [6]. Indeed using ii Vk, *BS(k) each class in Trj(Vk,) represents a fe-plane bundle over S' which bees trivial when sued with a trivial -plane bundle. It is also easy to see that the bundle is a fraed tangent bundle of S' if and only if the hoology ap is nontrivial. Since the 153«sphere has only an eight field, Sq l *h is not spherical. It is useful to kill it anyway but one has to be careful and identify the eleent at a later stage which is produced because of this. nd level. Consider the following fibering Kx(Z, 3n 5) K (Z, 3n 6) K(Z, 3n 1) with ^-invariants Sq 7 h, Sq*h and Sq h. i q ~* E 1 Vzn t l

I96j] SME HMTPY GRUPS F STIEFEL MAIFLDS 665 * «o ) J 5 * ^ eo^ ff 1 i i S tiikov tower 1 ified Post A od jr f c? 1 of y cr. CJ. ' < er. Cl * ir a» 59- ' T er ' 5 r esr <*, " 1 QQ. Cl eo P- 1/5 1r 1 CJ tf \ -1 S 1 "Sr CJ^ eo * «y Cl cî * i-t *3r cr M eo* ^cr CI Ir j. cô* «g* x 5 1r cî 1 "cr x* eo^ l cr Ê CJ <* eo "è èfs f f 1 cç iô A cfi <ô 1-» t. > x-r* Ir «r «S 1 «S * <3^ rs " -l i "L "* î^ x x 3 t» ^5cr x * o * t^

666 C. S. H AD M. E. MAHWALD [July PRPSITI. A class vgh 3 \E 1 1Z ) suchthatvç iq*andj^6n 3 satisfies: i*v?-i &&% where ai is the fundaental class of Ki and /3* is an eleent of the Steenrod algebra such that pisqtfasqtfizsq 1 *, as an eleent in the Steenrod algebra, has only classes of length or ore in its Cartan basis representation. Using this representation of H*(E ) it is now just a lengthy but straight forward putation to verify that the classes in Table 3, lun do for a basis over the Steenrod algebra for H J '(E l ) if 3w7^j = 3tt1. 3rd level. Consider the fibering with ^-invariants given by Table 3. We use & to represent also the fundaental class of Ki. The value of w,- can be inferred fro the table. Consider the diagra i * à* H*(E ) -> H*(TKi(Z,»<)) -* H*(E\ wki) \ î^ T H*(E l ) -? H*(Kx K K z ) PRPSITI. A classv(elh 3 '(E ), 7 j 3n 1, by a su ]C?-i a A satisfying: (1)*>= J^i-idiPiand () I(*ÎT&)=. is defined uniquely This is a special case of 3.3. of [6]. Using this proposition the hoology of E? in the interesting range can be puted. Another lengthy putation shows that lun 3 of Table 3 is a basis over the Steenrod algebra for Hi(E ), 7 ël/ 3n = 1. th and higher levels. The putations are ade as in the third level, using 3.3. of [6]. othing unusual happens. The class rresponding to 76SB is the extraneous class produced by killing Sq l %. This follows fro Toda []. It is ausing to note that the forula of Adas [o] Sqi* = J^aij tz <l>u with efficients, for exaple, 3,3,3 = Sq 1 and #1,3,3 = Sq 7 Sq*Sq Sq l, essentially given by ye.

1965] SME HMTPY GRUPS F STIEFEL MAIFLDS 667 BIBLIGRAPHY. J. F. Adas, n the non-existence of eleents of Hopf invariant one, Ann. of Math. () 7 (196), -1. 1. M. G. Barratt and M. E. Mahowald, The etastable hootopy of (n), Bull. Aer. Math. Soc. 7 (196), 75-76.., The etastable hootopy of S n (to appear). 3. A. Borel, La hoologie od de certains espaces hoogènes, Coent. Math. Helv. 7 (1953), 5-197.. C. S. Hoo, Hootopy groups of Stiefel anifolds, Ph.D. Thesis, Syracuse University, Syracuse,. Y., 196 (ieographed notes, orthwestern University). 5. I. M. Jaes, Cross-sections of Stiefel anifolds, Proc. London Math. Soc. (195), 536-57. 6. M. E. Mahowald, bstruction theory in orientablefiberbundles, Trans. Aer. Math. Soc. 11 (196), 315-39. 7. G. F. Paechter, The group 7r r (F, ). I, Quart. J. Math. xford Ser. 7 (1956), 9-6.. H. Toda, Vectorfieldson spheres, Bull. Aer. Math. Soc. 67 (1961), -1. UIVERSITY F ILLIIS AD RTHWESTER UIVERSITY