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Symmetries and Group Theory in Particle Physics: An Introduction to ...

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1.2 Lie groups <strong>and</strong> Lie algebras 9<br />

We are now <strong>in</strong> the position of giv<strong>in</strong>g a more precise def<strong>in</strong>ition of a Lie<br />

group.<br />

Lie group - A Lie group G of dimension n is a set of elements which satisfy<br />

the follow<strong>in</strong>g conditions:<br />

1. they form a group;<br />

2. they form an analytic manifold of dimension n;<br />

3. for any two elements a <strong>and</strong> b of G, the mapp<strong>in</strong>g φ(a, b) = a ◦ b of the<br />

Cartesian product G × G on<strong>to</strong> G is analytic;<br />

4. for any element a of G, the mapp<strong>in</strong>g φ(a) = a −1 of G on<strong>to</strong> G is analytic.<br />

1.2.1 L<strong>in</strong>ear Lie groups<br />

The Lie groups that are important for physical applications are of the type<br />

known as l<strong>in</strong>ear Lie groups, for which a simpler def<strong>in</strong>ition can be given.<br />

Let us consider a n-dimensional vec<strong>to</strong>r space V over the field F (such<br />

as the field R of real numbers <strong>and</strong> the field C of complex numbers) <strong>and</strong> the<br />

general l<strong>in</strong>ear group GL(N, F) of N × N matrices. A Lie group G is said <strong>to</strong><br />

be a l<strong>in</strong>ear Lie group if it is isomorphic <strong>to</strong> a subgroup G ′ of GL(N, F). In<br />

particular, a real l<strong>in</strong>ear Lie group is isomorphic <strong>to</strong> a subgroup of the l<strong>in</strong>ear<br />

group GL(N, R) of N × N real matrices.<br />

A l<strong>in</strong>ear Lie group G of dimension n satisfies the follow<strong>in</strong>g conditions:<br />

1. G possesses a faithful f<strong>in</strong>ite-dimensional representation D. Suppose that<br />

this representation has dimension m; then the distance between two elements<br />

g <strong>and</strong> g ′ of G is given, accord<strong>in</strong>g <strong>to</strong> Eq. (1.16), by<br />

{ ∑<br />

m<br />

d(g, g ′ ) = | D(g) ij − D(g ′ ) ij | 2} 1/2<br />

, (1.17)<br />

i,j=1<br />

<strong>and</strong> the set of matrices D(g) satisfies the requirement of a metric space.<br />

2. There exists a real number δ > 0 such that every element g of G ly<strong>in</strong>g <strong>in</strong><br />

the open set V δ , centered on the identity e <strong>and</strong> def<strong>in</strong>ed by d(g, e) < δ, can<br />

be parametrized by n <strong>in</strong>dependent real parameters (x 1 , x 2 , ..., x n ), with<br />

e correspond<strong>in</strong>g <strong>to</strong> x 1 = x 2 = ... = x n = 0. Then every element of V δ<br />

corresponds <strong>to</strong> one <strong>and</strong> only one po<strong>in</strong>t <strong>in</strong> a n-dimensional real Euclidean<br />

space R n . The number n is the dimension of the l<strong>in</strong>ear Lie group.<br />

3. There exists a real number ǫ > 0 such that every po<strong>in</strong>t <strong>in</strong> R n for which<br />

n∑<br />

x 2 i < ǫ 2 (1.18)<br />

i=1<br />

corresponds <strong>to</strong> some element g <strong>in</strong> the open set V δ def<strong>in</strong>ed above <strong>and</strong> the<br />

correspondence is one-<strong>to</strong>-one.

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