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Contributions à l'Etude du Vertex Topologique en Théorie ... - Toubkal

Contributions à l'Etude du Vertex Topologique en Théorie ... - Toubkal

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338 L.B. Drissi et al. / Nuclear Physics B 804 [PM] (2008) 307–341Complex curves in P 2Complex curves (real Riemann surfaces) in P 2 are complex codim<strong>en</strong>sion one submanifoldsobtained by imposing one more complex constraint relation f(z i ) = 0 on the projective complexvariables z 1 ,z 2 and z 3 . The most common curves in P 2 are obviously the projective lines P 1 ,conics and elliptic curves.G<strong>en</strong>erally speaking, the constraint equation f(z i ) = 0 can be stated as follows,f(λz 1 ,λz 2 ,λz 3 ) = λ n f(z 1 ,z 2 ,z 3 ) = 0,(A.11)where n stands for the degree of homog<strong>en</strong>eity of the curve. The case n = 3 is giv<strong>en</strong> by thefollowing typical cubicz 3 1 + z3 2 + z3 3 + μz 1z 2 z 3 = 0.(A.12)This relation describes an elliptic curve E of degree 3 with a complex structure μ. This curve Ehas be<strong>en</strong> ext<strong>en</strong>sively used in physical literature; in particular in the geometric <strong>en</strong>gineering of4D superconformal field theories embedded in 10D type IIB superstring on elliptically fiberedCalabi–Yau threefolds [44–46] and [51,52].Before proceeding further, it is interesting to notice that the elliptic curve E is a g<strong>en</strong>us oneRiemann surface having a real 3d mo<strong>du</strong>li space; parameterized by(μ 1 ,μ 2 ; r)(A.13)with μ = μ 1 + iμ 2 is the complex structure and r is its Kähler mo<strong>du</strong>lus. So, elliptic curves maybe g<strong>en</strong>erally d<strong>en</strong>oted as followsE (r,μ) .(A.14)Regarding the complex parameter μ of the elliptic curve E (r,μ) , it is explicitly exhibited in typeIIB geometry set up as shown on Eq. (A.12).However, it is interesting to notice that the Kähler parameter r cannot be exhibited explicitlysince E (r,μ) has no standard type IIA geometry realization 8 of the type giv<strong>en</strong> by Eq. (A.5).The construction developed in this paper gives a way to circumv<strong>en</strong>t this difficulty by usingthe deg<strong>en</strong>erate repres<strong>en</strong>tation (A.3).With the above features in mind, we turn now to the derivation of Eq. (A.1).∂(P 2 ) as the deg<strong>en</strong>erate elliptic curve E (r,∞)Here we would like to show that ∂(P 2 ) is E (r,μ) but with a large complex structure μ; that is|μ|→∞.To get the key point behind the id<strong>en</strong>tity (A.1) as well as the deg<strong>en</strong>eracy of the elliptic curveE (r,μ) , we give the two following properties:(a) the projective plane P 2 has three particular intersecting divisors D i . These are associatedwith the hyperlinesz i = 0in P 2 which, up on using Eq. (A.5), lead to the following relations(A.15)8 In toric geometry the real base of the fibration B n × T n of complex n-dim<strong>en</strong>sional toric manifolds involves projectivelines. Torii appear rather in the fiber.

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