Introduction to Matrix Models and Non-Critical String Theory Akikazu ...

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74CFT <strong>and</strong> <strong>Matrix</strong> Model agree e.g. annulus∫Z = dτZ ghost Z Lioville Z matterZ Liouville (τ) = 〈l 1 |e −τ(L 0+¯L 0 ) |l 2 〉Z(l 1 , l 2 ) ∼ ∑ k=1k sin(πk/q)Kkq(l 1 )Ikq(l 2 )Small l 2 limit: loops = ∑ BRST cohomology
75FZZT expectation value probe target space (as functionof µ B )xφ=−(1/b)log(µ B )....
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1Introduction to Matrix Modelsand N
Page 3 and 4:
3The subject is reviewed extensivel
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5Non-critical string theoryBosonic
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7S L =∫dξ 2√ g( 12 gab ∂ a
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9T (z)T (w) ∼ 1 c+ ..., c = 1 + 3
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11These can be coupled to d free bo
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13Other interesting example: (p, q)
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15Gravitational dressing[e αϕ O]
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17Under this transformation∫Qd 2
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19Physical observables are correlat
Page 21 and 22:
21ParametrizingM = U † ΛU,dM = d
Page 23 and 24: 23Simplest Matrix Model: Gaussian e
Page 25 and 26: 25Solution:ρ(m) = 1 π√2N − m2
Page 27 and 28: 27Such generalization is interestin
Page 29 and 30: 29So we arrive at an identity( ) 1
Page 31 and 32: 31• Constant c fixed by requireme
Page 33 and 34: 33With this ansatz, one hasR(z) =
Page 35 and 36: 35Now, series∑kΓ−3( gg c) 2k=
Page 37 and 38: 37All this was for pure 2D gravity
Page 39 and 40: 39Double Scaling LimitIf one also c
Page 41 and 42: 41Now, define a set of polynomialsP
Page 43 and 44: 43Need f n for large n.This can be
Page 45 and 46: 45Similarly,∫=∫e −V (P ′ n(
Page 47 and 48: 47P n+1soλ : P n (λ) ↗ ↘r n P
Page 49 and 50: 49For generic W (r),gξ = W (r) = g
Page 51 and 52: 51Now, if one is interested in high
Page 53 and 54: 53Summary of Orthogonal Polynomials
Page 55 and 56: 55Along similar lines, define∂∂
Page 57 and 58: 57(2,3) model:1 = [P, Q] =( 34 u2 +
Page 59 and 60: 59Key identity: Itzykson-Zuber inte
Page 61 and 62: 61P = (Q p/q ) + , [P, Q] = 1define
Page 63 and 64: 63∂∂t nQ = [(Q n/q ) + , Q]α n
Page 65 and 66: 65So we haveDouble Scaled Matrix Mo
Page 67 and 68: 67In double scaling limit1M ΦM = 1
Page 69 and 70: 69What does the resolvent measure?1
Page 71 and 72: 71In this limit, one obtainsT 2 (y)
Page 73: 73CFT side: one has the Liouville B
Page 77 and 78: 77Non-perturbativelyW (x) = log(Φ
Page 79 and 80: 79〈e W (x) 〉 ==∫∫= 12πg= 1
Page 81 and 82: 81Recursion relationλP n (λ) =
Page 83 and 84: 83Multi-FZZT amplitude generalizes
Page 85 and 86: 85• Airy function: Non-perturbati
Page 87 and 88: 87Airy integral has three saddle po
Page 89 and 90: 89• Perturbatively, many possible
Page 91 and 92: 91Open SFTS =∫Ψ ∗ QΨ + Ψ ∗
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Introduction to Matrix Models and Non-Critical String Theory Akikazu ...

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