- Page 1 and 2: Lecture Notes in Computational Scie
- Page 3 and 4: Editors Karl Heinz Hoffmann Institu
- Page 5 and 6: Preface High performance computing
- Page 7 and 8: Contents Part I Implementions Paral
- Page 9 and 10: Parallel Programming Models for Irr
- Page 11 and 12: Parallel Programming Models for Irr
- Page 13 and 14: surface element j Parallel Programm
- Page 15 and 16: quadtree of polygon A Parallel Prog
- Page 17: Parallel Programming Models for Irr
- Page 21 and 22: Parallel Programming Models for Irr
- Page 23 and 24: Parallel Programming Models for Irr
- Page 25 and 26: Parallel Programming Models for Irr
- Page 27 and 28: References Parallel Programming Mod
- Page 29: Parallel Programming Models for Irr
- Page 32 and 33: 26 Arnd Meyer 2 Finite element comp
- Page 34 and 35: 28 Arnd Meyer and (7). Here we watc
- Page 36 and 37: 30 Arnd Meyer (1) v s := Ksq s (2)
- Page 38 and 39: 32 Arnd Meyer w = Q˜y This is agai
- Page 40 and 41: 34 Arnd Meyer and constant number o
- Page 43 and 44: A Performance Analysis of ABINIT on
- Page 45 and 46: A Performance Analysis of ABINIT on
- Page 47 and 48: A Performance Analysis of ABINIT on
- Page 49 and 50: Call graph A Performance Analysis o
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- Page 57: A Performance Analysis of ABINIT on
- Page 60 and 61: 54 Matthias Pester and obvious fiel
- Page 62 and 63: 56 Matthias Pester • The program
- Page 64 and 65: 58 Matthias Pester SFB 393 - TU Che
- Page 66 and 67: 60 Matthias Pester SFB 393 - TU Che
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62 Matthias Pester or time-dependen
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64 Matthias Pester 5. G. Haase, T.
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68 Arnd Meyer TL = {T ⊂ Ω},T ar
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70 Arnd Meyer 3 Basic facts on hier
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72 Arnd Meyer Φl = ΦLQl ∀l =0,.
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74 Arnd Meyer Example 5: VL = V (3,
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76 Arnd Meyer (c) piecewise quadrat
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78 Arnd Meyer 6 Crack growth Table
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80 Arnd Meyer can access from its e
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82 Arnd Meyer where and This leads
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84 Arnd Meyer 10 A numerical exampl
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Nitsche Finite Element Method for E
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Nitsche Finite Element Method for E
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Nitsche Finite Element Method for E
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Nitsche Finite Element Method for E
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Nitsche Finite Element Method for E
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Nitsche Finite Element Method for E
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Nitsche Finite Element Method for E
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approximate solution u h pointwise
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Nitsche Finite Element Method for E
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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Hierarchical Adaptive FEM at Finite
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130 Helmut Harbrecht et al. scheme,
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132 Helmut Harbrecht et al. We emph
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134 Helmut Harbrecht et al. piecewi
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136 Helmut Harbrecht et al. Herein,
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138 Helmut Harbrecht et al. Fig. 3.
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140 Helmut Harbrecht et al. Γi,j,k
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142 Helmut Harbrecht et al. This pr
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144 Helmut Harbrecht et al. unknown
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146 Helmut Harbrecht et al. 200 400
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148 Helmut Harbrecht et al. 20. W.
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Numerical Solution of Optimal Contr
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Numerical Solution of Optimal Contr
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Numerical Solution of Optimal Contr
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Numerical Solution of Optimal Contr
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Numerical Solution of Optimal Contr
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Numerical Solution of Optimal Contr
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max. deviation of temperature in [
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Numerical Solution of Optimal Contr
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Numerical Solution of Optimal Contr
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Numerical Solution of Optimal Contr
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174 Thomas Vojta disorder. Examples
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176 Thomas Vojta thermal ones. Exam
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178 Thomas Vojta 3 Classical Ising
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180 Thomas Vojta Fig. 1. Average ma
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182 Thomas Vojta Fig. 3. Local magn
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184 Thomas Vojta J ⊥ / J || 2.5 2
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186 Thomas Vojta Fig. 5. Upperpanel
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188 Thomas Vojta criterion. These r
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190 Thomas Vojta ways to actually i
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192 Thomas Vojta ρ 10 0 10 -2 10 -
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194 Thomas Vojta ln(ρ st ) -4 -6 -
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196 Thomas Vojta Fortunately, this
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198 Thomas Vojta Acknowledgements T
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200 Thomas Vojta 39. Motrunich, O.,
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Localization of Electronic States i
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Localization of Electronic States i
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Localization of Electronic States i
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Localization of Electronic States i
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Localization of Electronic States i
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〈ln g 4 〉 0 -0.5 -1 -1.5 -2 -2.
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ρ(E) 0.062 0.06 0.058 0.056 0.054
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ρ(E) 0.14 0.12 0.1 0.08 0.06 0.04
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ρ(E) 0.06 0.05 0.04 0.03 0.02 0.01
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| ξ | 100 10 1 Localization of Ele
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Localization of Electronic States i
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Localization of Electronic States i
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Optimizing Simulated Annealing Sche
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Optimizing Simulated Annealing Sche
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Optimizing Simulated Annealing Sche
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Optimizing Simulated Annealing Sche
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Amorphisation at Heterophase Interf
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Amorphisation at Heterophase Interf
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Amorphisation at Heterophase Interf
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[010] Amorphisation at Heterophase
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Amorphisation at Heterophase Interf
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4.2 Stability at low temperature Am
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RDF 28 26 24 22 20 18 16 14 12 10 8
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Amorphisation at Heterophase Interf
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Amorphisation at Heterophase Interf
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Amorphisation at Heterophase Interf
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Energy-Level and Wave-Function Stat
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Energy-Level and Wave-Function Stat
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3 Summary of theoretical expectatio
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Energy-Level and Wave-Function Stat
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˙ ¸ 2 |ψ(r)| V t 10 1 10 1 Energ
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Energy-Level and Wave-Function Stat
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Fine Structure of the Integrated De
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Fine Structure of the Integrated DO
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Fine Structure of the Integrated DO
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Fine Structure of the Integrated DO
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DOS Fine Structure of the Integrate
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ρ min , ρ max Fine Structure of t
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Fine Structure of the Integrated DO
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Modelling Aging Experiments in Spin
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2.1 ZFC-experiments Modelling Aging
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Modelling Aging Experiments in Spin
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Modelling Aging Experiments in Spin
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Modelling Aging Experiments in Spin
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Modelling Aging Experiments in Spin
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density 10 3 10 2 10 1 10 0 -2 -1 0
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Magnetization M(t) Modelling Aging
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Modelling Aging Experiments in Spin
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TRM (a.u.) Modelling Aging Experime
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Modelling Aging Experiments in Spin
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Random Walks on Fractals Astrid Fra
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Random Walks on Fractals 305 The di
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log��r 18 2�� 16 14 12 10 8
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(a) 10 3 10 1 10 2 〈r 2 〉 10 0
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Random Walks on Fractals 311 Fig. 7
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Random Walks on Fractals 313 11. A.
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316 Hong-liu Yang and Günter Radon
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318 Hong-liu Yang and Günter Radon
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320 Hong-liu Yang and Günter Radon
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322 Hong-liu Yang and Günter Radon
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324 Hong-liu Yang and Günter Radon
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326 Hong-liu Yang and Günter Radon
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328 Hong-liu Yang and Günter Radon
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330 Hong-liu Yang and Günter Radon
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332 Hong-liu Yang and Günter Radon
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The Cumulant Method for Gas Dynamic
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The Cumulant Method for Gas Dynamic
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The Cumulant Method for Gas Dynamic
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0.2 0.1 0.0 0.2 0.1 0.0 0 -5 The Cu
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The Cumulant Method for Gas Dynamic
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The Cumulant Method for Gas Dynamic
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The Cumulant Method for Gas Dynamic
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n = eC0 � x C v = Cy � σ = 1 2
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The Cumulant Method for Gas Dynamic
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The Cumulant Method for Gas Dynamic
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(a) gas wall wall The Cumulant Meth
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The Cumulant Method for Gas Dynamic
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The Cumulant Method for Gas Dynamic
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Index ab-initio calculation 37 abin
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Editorial Policy 1. Volumes in the
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Lecture Notes in Computational Scie
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Vol. 39 S. Attinger, P. Koumoutsako