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String Theory and M-Theory

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360 <strong>String</strong> geometry<br />

Noncompact examples<br />

A simple noncompact example of an orbifold results from considering the<br />

complex plane £ , described by a local coordinate z in the usual way, <strong>and</strong><br />

the isometry given by the transformation<br />

z → −z. (9.1)<br />

This operation squares to one, <strong>and</strong> therefore it generates the two-element<br />

group 2. The orbifold £ / 2 is defined by identifying points that are in the<br />

same orbit of the group action, that is, by identifying z <strong>and</strong> −z. Roughly<br />

speaking, this operation divides the complex plane into two half-planes.<br />

More precisely, the orbifold corresponds to taking the upper half-plane <strong>and</strong><br />

identifying the left <strong>and</strong> right halves of the boundary (the real axis) according<br />

to the group action. As depicted in Fig. 9.3, the resulting space is a cone.<br />

Fig. 9.3. To construct the orbifold ¦ /¥ 2 the complex plane is divided into two<br />

parts <strong>and</strong> identified along the real axis (z ∼ −z). The resulting orbifold is a cone.<br />

This orbifold is smooth except for a conical singularity at the point (0, 0),<br />

because this is the fixed point of the group action. One consequence of<br />

the conical singularity is that the circumference of a circle of radius R,<br />

centered at the origin, is πR <strong>and</strong> the conical deficit angle is π. An obvious<br />

generalization is the orbifold £ / N, where the group is generated by a<br />

rotation by 2π/N. In this case there is again a singularity at the origin<br />

<strong>and</strong> the conical deficit angle is 2π(N − 1)/N. This type of singularity is<br />

an AN singularity. It is included in the more general ADE classification of<br />

singularities, which is discussed in Sections 9.11 <strong>and</strong> 9.12.<br />

The example £ / 2 illustrates the following general statement: points<br />

that are invariant (or fixed) under some nontrivial group element map to<br />

singular points of the quotient space. Because of the singularities, these<br />

quotient spaces are not manifolds (which, by definition, are smooth), <strong>and</strong>

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