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On a solution of the U(N) ⊃ O(N) state labelling problem, for two-rowed representation

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ON A SOL TION OF T U

f,o

STATE LAB L I ROBLEM

FOR TI'IO-ROÌíED REPRESENTATIONS

by

P.D. Jarvís, B.Se. (Ilons.)

A thesis

submitted for the degree of Master of Science

Departmeot of Mathemat,ical Physics, Unívers ity of Adel aide.

March, L974

I

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TABLE OF CONTENTS

ABSTRACT

PREFACE S

Ch. 1 INTRODUCTION

1.1 Irreducible Representations and Abstract ' Bases

L,2 Physical Applications

ch. 2 TtlE U(N)r O(N) REDUCTTON VrA TENSoR REPRE- SENTAT I ONS

Page No.

13

L7

18 21

1

2

2.I

2.2 2.3

2.4 2.5

25 35 39

Irreducíb1e Tensor Representations Symmetríes of Irreducíb1e Tensors

U(N) > Q(N) Branching Theorem for Two-Rowed

Representations

U(N). O(N) Reduction by Character Analysis Conparison for the Case U(4) [gr¿J

2.6 Explicít Tensor Reduction for Some Specíal

Cases

ch. 3 u(N) AND 0(N) TNVARTANTS

3.1 General Properties Independent Invariants

Invariants for Two-Rowed Representations 3,2

3.3

40

42 43 46 50

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Ch. 4 EVALUATION OF INVARIANTS

4.2

Pre 1 iminar ie s

U(N) Invariants and Cubic Polynônial Identity

o(N) rnvarianÈ <t¿>

=

<â2)

-

å<.,t).

o(N) Invariant å(a¡a + ãaã).

Operational Def inition of /I 4.3

4 5

APPENDI CE S

REFERENCES 4-.4

Pace No.

52 53

56

6L 65 67

70

87

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ABSTRACT

Considerations of the number of 1abe11ing oPeTators in a general state 1abel1ing problem inply that for two- rowed irreducible representations of U(N), 1abe1led

[n,e,o,..ro], jusE one additional commuting labelling

operaÈor, Â , í" required for the soluÈion of the U(N) = 0(N) state labe1ling problem. A detailed investigation of the U(N)) O(N) reduction via tensor rePresentaEion, f."a, to a proposal of an integral label x , irplying a non-orthogonal l_abelling s cheme. A simp 1e u (N) ) O (N) branching theorem for two-rohled representations is formulated in teïms of 1 .

The additional labe11ing operator A , with eigen- value tr, ís to be defined inplícitly by an equation of

ttre form f(A,iÞ,"') - o, where f i" a polynomial inA;

Ëhe additional O (N) invariants (D in the represenËatí on subduced by U(N) [pr9ro,..,o] , and other known labels and

invariants. The o(N) invariants, which are cubic and quartic in the generators of U(N) ' are discussed. Tech- níques developed by Green and nt""k"rr(1) for the U(3) ) SO (3) problem are used Èo evaluate the single independent cubic

ínvariant, and it is shown how this is used in obtaining the desired inplícit operational definition of A

A cubic characteristic polynomial identity, satisfied by the generaÈors of U (N) in two-rowed rePresentatíons, is also found using these teehniques.

Some possible physical applications of the U(N)> 0(N)

state labelling problem are briefly discussed.

t

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This thesis conÈains no material which has been áccepted for the award of any other degree or diplorna in any university. To the best of the auEhorls knowledge and belief, the thesis contains no material prevíous1y published or \dritten by another Persoûr except when due reference ís made in the text.

London

ApríL 197 4

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The author gratefully acknowledges the assistance of Professor H. S. Green, DeparÈment of MaÈhematical Physics, University of Adelaider urder whose guidance the work here presented was carried out.

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