Foreword |
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xi | |
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Preface |
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xv | |
Introduction |
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1 | (2) |
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1.1 Configuration space and the basic field |
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3 | (2) |
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1.2 The space of fields F |
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5 | (4) |
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1.3 Derivatives and support of functionals, local fields |
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9 | (7) |
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16 | (2) |
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18 | (3) |
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21 | (4) |
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1.7 Perturbative expansion of retarded fields |
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25 | (2) |
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1.8 The Poisson algebra of the free theory |
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27 | (4) |
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1.9 An explicit formula for the classical retarded product |
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31 | (7) |
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1.10 Basic properties of the retarded product |
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38 | (8) |
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2 Deformation Quantization of the Free Theory |
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2.1 Star products of fields |
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46 | (3) |
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2.2 Solutions for the two-point function Hm |
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49 | (4) |
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2.3 Equivalence of the several star products |
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53 | (4) |
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2.4 Existence and properties of the star product |
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57 | (3) |
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60 | (3) |
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2.6 Connection to the algebra of Wick polynomials |
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63 | (9) |
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3 Perturbative Quantum Field Theory |
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3.1 Axioms for the retarded product |
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72 | (35) |
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73 | (6) |
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79 | (1) |
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3.1.3 Discussion of the GLZ relation |
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80 | (3) |
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3.1.4 Further axioms: Renormalization conditions |
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83 | (8) |
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3.1.5 The scaling and mass expansion |
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91 | (12) |
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3.1.6 The classical limit |
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103 | (1) |
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104 | (3) |
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3.2 Construction of the retarded product |
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107 | (52) |
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3.2.1 Inductive step, off the thin diagonal Δn |
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107 | (7) |
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3.2.2 The extension to the thin diagonal Δn |
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114 | (15) |
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3.2.3 Maintaining scaling and mass expansion in the extension |
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129 | (1) |
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3.2.4 Completing the inductive step |
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130 | (6) |
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3.2.5 Scaling degree axiom versus Sm-expansion axiom |
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136 | (3) |
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3.2.6 The general solution of the axioms |
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139 | (6) |
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3.2.7 Maintaining symmetries in the extension of distributions |
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145 | (7) |
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3.2.8 Explicit computation of an interacting field -- renormalization of two-point functions using the Kallen--Lehmann representation |
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152 | (7) |
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3.3 The time-ordered product |
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159 | (21) |
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3.3.1 Heuristic explanation of the physical relevance of the time-ordered product |
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159 | (2) |
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3.3.2 Axioms for the time-ordered product and its inductive construction |
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161 | (10) |
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3.3.3 Connection between the T- and the R-product |
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171 | (9) |
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3.4 The time-ordered (or retarded) product for on-shell fields |
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180 | (13) |
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3.4.1 Definition of the on-shell T-product |
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180 | (5) |
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3.4.2 Properties of the on-shell T-product |
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185 | (8) |
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3.5 Techniques to renormalize in practice |
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193 | (26) |
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3.5.1 Differential renormalization |
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193 | (9) |
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3.5.2 Analytic regularization |
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202 | (17) |
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3.6 The Stuckelberg--Petermann renormalization group |
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219 | (23) |
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3.6.1 Definition of the Stuckelberg--Petermann RG |
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220 | (5) |
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3.6.2 The Main Theorem of perturbative renormalization |
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225 | (9) |
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3.6.3 The Gell-Mann--Low cocycle |
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234 | (8) |
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3.7 The algebraic adiabatic limit |
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242 | (6) |
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3.8 The renormalization group in the algebraic adiabatic limit |
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248 | (23) |
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3.8.1 Renormalization of the interaction |
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248 | (7) |
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3.8.2 Wave function, mass and coupling constant renormalization |
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255 | (10) |
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3.8.3 Field renormalization |
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265 | (6) |
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3.9 A version of Wilson's renormalization group and of the flow equation |
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271 | (29) |
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3.9.1 Outline of the procedure |
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271 | (3) |
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3.9.2 The regularized S-matrix |
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274 | (12) |
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3.9.3 Effective potential and flow equation |
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286 | (6) |
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3.9.4 A version of Wilson's renormalization "group" |
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292 | (1) |
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3.9.5 Comparison with the functional integral approach |
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293 | (7) |
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4 Symmetries -- the Master Ward Identity |
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4.1 Derivation of the Master Ward Identity in classical field theory |
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300 | (1) |
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4.2 The Master Ward Identity as a universal renormalization condition |
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301 | (13) |
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4.2.1 Formulation of the MWI |
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301 | (1) |
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4.2.2 Verification that the MWI is a renormalization condition |
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302 | (2) |
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4.2.3 A few applications of the MWI |
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304 | (10) |
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4.3 Anomalous Master Ward Identity (Quantum Action Principle) |
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314 | (9) |
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4.4 Reduction of the MWI to the "quantum part" |
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323 | (13) |
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323 | (10) |
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4.4.2 The Master Ward Identity in terms of proper vertices |
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333 | (3) |
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4.5 Removing violations of the Master Ward Identity |
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336 | (14) |
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4.5.1 Proceeding analogously to algebraic renormalization |
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336 | (9) |
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4.5.2 Proof of the relevant MWI for the scalar O(N)-model |
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345 | (5) |
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5 Quantum Electrodynamics |
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5.1 Deformation quantization for fermionic and gauge fields |
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350 | (53) |
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350 | (23) |
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5.1.2 Faddeev--Popov ghosts: A pair of anticommuting scalar fields |
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373 | (2) |
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375 | (3) |
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5.1.4 Definition of the retarded and time-ordered product in QED |
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378 | (4) |
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5.1.5 Charge conjugation invariance |
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382 | (4) |
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386 | (10) |
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5.1.7 Reducing the computation of R- and T-products to scalar field renormalization |
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396 | (7) |
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5.2 The relevant Master Ward Identity for Quantum Electrodynamics |
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403 | (13) |
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5.2.1 Formulation of the QED Master Ward Identity |
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403 | (4) |
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5.2.2 Proof of the QED-MWI |
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407 | (6) |
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5.2.3 Conservation of the interacting current and the corresponding charge |
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413 | (3) |
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5.3 The local algebras of interacting fields |
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416 | (3) |
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5.4 Connection of observable algebras and field algebras |
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419 | (17) |
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5.4.1 Local construction of observables in gauge theories |
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419 | (5) |
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5.4.2 Construction of physical states on the algebra of observables |
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424 | (3) |
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5.4.3 Stability under deformations |
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427 | (9) |
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5.5 Verification of the assumptions for QED |
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436 | (24) |
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436 | (14) |
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5.5.2 The interacting theory: The interacting Kugo--Ojima charge |
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450 | (10) |
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5.6 Reasons in favour of a LOCAL construction |
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460 | (3) |
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A.1 Some notations and a few mathematical preliminaries |
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463 | (6) |
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A.2 Propagators: Conventions and properties |
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469 | (4) |
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A.3 A short introduction to wave front sets |
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473 | (5) |
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A.4 Perturbative QFT based on quantization with a Hadamard function |
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478 | (6) |
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484 | (11) |
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A.6 Weak adiabatic limit: Wightman- and Green functions |
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495 | (10) |
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A.7 Remarks about the connection to traditional approaches |
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505 | (8) |
Glossary of Abbreviations and Symbols |
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513 | (6) |
Bibliography |
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519 | (12) |
Index |
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531 | |