- Page 4 and 5: Quantum Field Theory and Gravity Co
- Page 6 and 7: Contents Preface ..................
- Page 8 and 9: Preface The present volume arose fr
- Page 10 and 11: Preface ix 6. (How) can we test qua
- Page 12 and 13: Preface xi Felix Finster, Andreas G
- Page 14 and 15: Preface xiii it is related to other
- Page 18 and 19: Quantum Gravity: Whence, Whither? 3
- Page 20 and 21: Quantum Gravity: Whence, Whither? 5
- Page 22 and 23: Quantum Gravity: Whence, Whither? 7
- Page 24 and 25: Quantum Gravity: Whence, Whither? 9
- Page 26 and 27: Quantum Gravity: Whence, Whither? 1
- Page 28: Quantum Gravity: Whence, Whither? 1
- Page 31 and 32: 16 K. Fredenhagen and K. Rejzner fi
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- Page 35 and 36: 20 K. Fredenhagen and K. Rejzner 4.
- Page 37 and 38: 22 K. Fredenhagen and K. Rejzner 5.
- Page 40 and 41: The “Big Wave” Theory for Dark
- Page 42 and 43: The “Big Wave” Theory for Dark
- Page 44 and 45: The “Big Wave” Theory for Dark
- Page 46 and 47: The “Big Wave” Theory for Dark
- Page 48 and 49: The “Big Wave” Theory for Dark
- Page 50 and 51: The “Big Wave” Theory for Dark
- Page 52 and 53: The “Big Wave” Theory for Dark
- Page 54 and 55: The “Big Wave” Theory for Dark
- Page 56 and 57: Discrete and Continuum Third Quanti
- Page 58 and 59: Discrete and Continuum Third Quanti
- Page 60 and 61: Discrete and Continuum Third Quanti
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Discrete and Continuum Third Quanti
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Discrete and Continuum Third Quanti
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Discrete and Continuum Third Quanti
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Discrete and Continuum Third Quanti
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Discrete and Continuum Third Quanti
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Discrete and Continuum Third Quanti
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Discrete and Continuum Third Quanti
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Unsharp Values, Domains and Topoi A
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Unsharp Values, Domains and Topoi 6
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Unsharp Values, Domains and Topoi 6
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Unsharp Values, Domains and Topoi 7
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Unsharp Values, Domains and Topoi 7
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Unsharp Values, Domains and Topoi 7
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Unsharp Values, Domains and Topoi 7
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Unsharp Values, Domains and Topoi 7
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Unsharp Values, Domains and Topoi 8
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Unsharp Values, Domains and Topoi 8
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Unsharp Values, Domains and Topoi 8
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Unsharp Values, Domains and Topoi 8
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Unsharp Values, Domains and Topoi 8
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Unsharp Values, Domains and Topoi 9
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Unsharp Values, Domains and Topoi 9
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Unsharp Values, Domains and Topoi 9
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Causal Boundary of Spacetimes: Revi
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Causal Boundaries 99 to the Gromov
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Causal Boundaries 101 I + (ρ) ρ P
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Causal Boundaries 103 Figure 2. The
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Causal Boundaries 105 more pairings
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Causal Boundaries 107 point of the
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Causal Boundaries 109 (0, 1) x n x
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Causal Boundaries 111 to Busemann f
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Causal Boundaries 113 respectively.
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Causal Boundaries 115 6.3. Structur
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Causal Boundaries 117 Qualitative F
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Causal Boundaries 119 [26] E. Mingu
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122 D. Häfner Let us give an idea
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124 D. Häfner Figure 1. The collap
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126 D. Häfner Figure 2. The manifo
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128 D. Häfner and the angular mome
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130 D. Häfner Lemma 3.5. There exi
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132 D. Häfner Proposition 4.4. The
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134 D. Häfner 6. Strategy of the p
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136 D. Häfner [3] B. Carter, Black
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138 R. Oeckl it is less compelling
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140 R. Oeckl Depending on the theor
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142 R. Oeckl 2.3. Recovery of stand
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144 R. Oeckl where the condition A
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146 R. Oeckl Before we proceed to i
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148 R. Oeckl the complex classical
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150 R. Oeckl The corresponding anni
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152 R. Oeckl Proposition 4.1 (Coher
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154 R. Oeckl much larger than the s
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156 R. Oeckl Setting F equal to F
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158 F. Finster, A. Grotz and D. Sch
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160 F. Finster, A. Grotz and D. Sch
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162 F. Finster, A. Grotz and D. Sch
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164 F. Finster, A. Grotz and D. Sch
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166 F. Finster, A. Grotz and D. Sch
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168 F. Finster, A. Grotz and D. Sch
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170 F. Finster, A. Grotz and D. Sch
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172 F. Finster, A. Grotz and D. Sch
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174 F. Finster, A. Grotz and D. Sch
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176 F. Finster, A. Grotz and D. Sch
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178 F. Finster, A. Grotz and D. Sch
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180 F. Finster, A. Grotz and D. Sch
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182 F. Finster, A. Grotz and D. Sch
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184 C. Bär and N. Ginoux treat the
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186 C. Bär and N. Ginoux the categ
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188 C. Bär and N. Ginoux Example 2
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190 C. Bär and N. Ginoux 3.2. Diff
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192 C. Bär and N. Ginoux In other
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194 C. Bär and N. Ginoux Here (e j
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196 C. Bär and N. Ginoux Remark 3.
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198 C. Bär and N. Ginoux Proof. Th
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200 C. Bär and N. Ginoux To prove
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202 C. Bär and N. Ginoux We refer
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204 C. Bär and N. Ginoux where Glo
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206 C. Bär and N. Ginoux [24] R. M
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208 C. J. Fewster well-described by
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210 C. J. Fewster and J + M (p) ∩
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212 C. J. Fewster commute. As funct
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214 C. J. Fewster ι + ι − M +
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216 C. J. Fewster ϕ(ψ) M M ϕ(M)(
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218 C. J. Fewster theory. The resul
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220 C. J. Fewster Following [7], a
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222 C. J. Fewster Sketch of proof.
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224 C. J. Fewster The relative Cauc
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226 C. J. Fewster [2] Bär, C., Gin
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Local Covariance, Renormalization A
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Local Thermal Equilibrium and Cosmo
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Shape Dynamics. An Introduction Jul
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Shape Dynamics. An Introduction 259
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Shape Dynamics. An Introduction 261
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Shape Dynamics. An Introduction 263
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Shape Dynamics. An Introduction 265
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Shape Dynamics. An Introduction 267
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where dx bm a Shape Dynamics. An In
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Shape Dynamics. An Introduction 271
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Shape Dynamics. An Introduction 273
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Shape Dynamics. An Introduction 275
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Shape Dynamics. An Introduction 277
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Shape Dynamics. An Introduction 279
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Shape Dynamics. An Introduction 281
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Shape Dynamics. An Introduction 283
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Shape Dynamics. An Introduction 285
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Shape Dynamics. An Introduction 287
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Shape Dynamics. An Introduction 289
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Shape Dynamics. An Introduction 291
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Shape Dynamics. An Introduction 293
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Shape Dynamics. An Introduction 295
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Shape Dynamics. An Introduction 297
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300 M. Kiessling In the following,
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302 M. Kiessling where “δ( · )
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304 M. Kiessling the point charge,
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306 M. Kiessling (2.17) and (2.18)
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308 M. Kiessling Maxwell’s “law
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310 M. Kiessling argued that E f (
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312 M. Kiessling the Maxwell-Born-I
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314 M. Kiessling removal. For insta
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316 M. Kiessling ∂ 4πc that for
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318 M. Kiessling d dt Dirac, on the
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320 M. Kiessling The Lorenz-Lorentz
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322 M. Kiessling ( 1 c Lorentz and
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324 M. Kiessling potential fields
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326 M. Kiessling as I have done her
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328 M. Kiessling just the Hamilton-
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330 M. Kiessling 7. Closing remarks
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332 M. Kiessling [Bor1937] Born, M.
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334 M. Kiessling [Lié1898] Liénar
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How Unique Are Higher-dimensional B
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How Unique Are Higher-dimensional B
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How Unique Are Higher-dimensional B
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How Unique Are Higher-dimensional B
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Equivalence Principle, Quantum Mech
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Atom Interferometry 347 The second
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Atom Interferometry 349 α CR , aim
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Atom Interferometry 351 of this mas
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Atom Interferometry 353 height B A
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Atom Interferometry 355 iff ψ = (
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Atom Interferometry 357 have be rea
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Atom Interferometry 359 where F (t
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Atom Interferometry 361 5.2. Interf
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Atom Interferometry 363 Evaluating
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Atom Interferometry 365 where the l
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Atom Interferometry 367 Then they s
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Atom Interferometry 369 [8] T.M. Fo
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Index n-point function, 51, 146, 23
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Index 373 conformal field theory, 1
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Index 375 gravitational redshift, 2
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Index 377 operator product, 138 par
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Index 379 standard model of particl