Introduction to the AdS/CFT correspondence

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13/22 A confining potential Let us assume that the AdS warp factor 1 z 2 is cut-off at some finite value z 0 of the coordinate z
14/22 A confining potential. 2. The solution of the equation f 11 1 ¡ d z f 1 ¡ pk 2 pmRq 2 q f 0 z 2 may be written as f pk, zq e i k¤x z d{2 K ν p|k| zq, ν ∆ ¡ ∆ ¡ 2 The boundary condition f pk, z 0 q 0 leads to the quantization of k 2 n λ n — the spectrum of masses of the mesons
Page 1 and 2: 1/22 Introduction to the AdS/CFT co
Page 3 and 4: 2/22 The main concept Quantum fi
Page 5 and 6: 2/22 The main concept Quantum fi
Page 7 and 8: 3/22 The AdS space A non-compac
Page 9 and 10: 3/22 The AdS space A non-compac
Page 11 and 12: 4/22 The AdS space. 2. The global
Page 13 and 14: 4/22 The AdS space. 2. The global
Page 15 and 16: 5/22 The AdS space. 3. Hence we ar
Page 17 and 18: 6/22 The AdS space. 4. AdS has a
Page 19 and 20: 7/22 Partition functions The corr
Page 25 and 26: Partition functions. 2. Imagine a
Page 27 and 28: Partition functions. 2. Imagine a
Page 29 and 30: 9/22 Partition functions. 3. Use
Page 31 and 32: 10/22 Partition functions. 4. In
Page 33 and 34: 10/22 Partition functions. 4. In
Page 35 and 36: Partition functions. 5. Therefor
Page 37 and 38: Partition functions. 5. Therefor
Page 39 and 40: 12/22 Partition functions. 6. To
Page 41: 13/22 A confining potential Let us
Page 45 and 46: 14/22 A confining potential. 2. T
Page 47 and 48: 15/22 The Wilson loop µ An impo
Page 49 and 50: 15/22 The Wilson loop µ An impo
Page 51 and 52: The quark-antiquark potential Let
Page 53 and 54: The quark-antiquark potential Let
Page 55 and 56: 17/22 The quark-antiquark potential
Page 61 and 62: 18/22 The advent of mesons What wi
Page 63 and 64: 18/22 The advent of mesons What wi
Page 65 and 66: 19/22 AdS 5 ¢ S 5 vs. N 4 SYM N
Page 71 and 72: 20/22 AdS 5 ¢ S 5 vs. N 4 SYM
Page 77 and 78: 21/22 Questions / Answers We have d
Page 79 and 80: 21/22 Questions / Answers We have d

Introduction to the AdS/CFT correspondence

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