Introduction to the AdS/CFT correspondence
Introduction to the AdS/CFT correspondence
Introduction to the AdS/CFT correspondence
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14/22<br />
A confining potential. 2.<br />
<br />
<br />
The solution of <strong>the</strong> equation<br />
f 11 1 ¡ d<br />
z f 1 ¡ pk 2 pmRq 2<br />
q f 0<br />
z 2<br />
may be written as<br />
f pk, zq e i k¤x z d{2 K ν p|k| zq, ν ∆ ¡ ∆ ¡<br />
2<br />
The boundary condition f pk, z 0 q 0 leads<br />
<strong>to</strong> <strong>the</strong> quantization of k 2 n λ n — <strong>the</strong><br />
spectrum of masses of <strong>the</strong> mesons