multilevel domain decomposition at extreme scales
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Multilevel domain decomposition at extreme scales S. Badia, A. Martin, J. Principe Universitat Politcnica de Catalunya & CIMNE Jeju, July 7th, 2015 0 / 24 Outline 1 Motivation 2 Multilevel framework 3 Multilevel linear solvers 4


  1. Multilevel domain decomposition at extreme scales S. Badia, A. Martin, J. Principe Universitat Politècnica de Catalunya & CIMNE Jeju, July 7th, 2015 0 / 24

  2. Outline 1 Motivation 2 Multilevel framework 3 Multilevel linear solvers 4 Conclusions 0 / 24

  3. Outline 1 Motivation 2 Multilevel framework 3 Multilevel linear solvers 4 Conclusions 0 / 24

  4. Current trends of supercomputing • Transition from today’s 10 Petaflop/s supercomputers (SCs) • ... to exascale systems w/ 1 Exaflop/s expected in 2020 • × 100 performance based on concurrency (not higher freq) • Future: Multi-Million- core (in broad sense) SCs 1 / 24

  5. Current trends of supercomputing • Transition from today’s 10 Petaflop/s supercomputers (SCs) • ... to exascale systems w/ 1 Exaflop/s expected in 2020 • × 100 performance based on concurrency (not higher freq) • Future: Multi-Million- core (in broad sense) SCs 1 / 24

  6. Weakly scalable solvers • This talk: One challenge, weakly scalable algorithms Weak scalability If we increase X times the number of Source: Dey et al, 2010 processors, we can solve an X times larger problem • Key property to face more complex problems / increase accuracy Source: parFE project 2 / 24

  7. Scalable linear solvers (AMG) • Most scalable solvers for CSE are parallel AMG (Trilinos [Lin, Shadid, Tuminaro, ...], Hypre [Falgout, Yang,...],...) • Hard to scale up to largest SCs today (one million cores, < 10 PFs) • Problems: large communication/computation ratios at coarser levels, densification coarser problems,... 3 / 24

  8. Multilevel framework • Propose a highly scalable implementation of Multilevel DD methods (MLBDDC [Mandel et al’08]) • MLDD based on a hierarchy of meshes/functional spaces • It involves local subdomain problems at all levels (L1, L2, ...) FE mesh Subdomains (L1) Subdomains (L2) 4 / 24

  9. Outline 1 Motivation I: Develop a multilevel framework suitable for extremely scalable implementations 2 Motivation II: Apply the multilevel framework for scalable linear algebra (MLBDDC) 5 / 24

  10. Outline 1 Motivation I: Develop a multilevel framework suitable for extremely scalable implementations 2 Motivation II: Apply the multilevel framework for scalable linear algebra (MLBDDC) 5 / 24

  11. Outline 1 Motivation I: Develop a multilevel framework suitable for extremely scalable implementations 2 Motivation II: Apply the multilevel framework for scalable linear algebra (MLBDDC) All implementations in FEMPAR (in-house code) to be dis- tributed as open-source SW soon * * Funded by Proof of Concept Grant 640957 - FEXFEM: On a free open source extreme scale finite element software 5 / 24

  12. Outline 1 Motivation 2 Multilevel framework 3 Multilevel linear solvers 4 Conclusions 5 / 24

  13. Premilinaries • Element-based (non-overlapping DD) distribution (+ limited ghost info) ˜ T 1 h , T 2 h , T 3 T 1 T h h h • Gluing info based on objects • Object: Maximum set of interface nodes that belong to the same set of subdomains 6 / 24

  14. Premilinaries • Element-based (non-overlapping DD) distribution (+ limited ghost info) ˜ T 1 h , T 2 h , T 3 T 1 T h h h • Gluing info based on objects • Object: Maximum set of interface nodes that belong to the same set of subdomains 6 / 24

  15. Automatic hierarchical mesh generator Classification of objects (vef’s at the next level) in 3D • Faces: Objects that belong to 2 subdomains • Edges: Objects that belong to more than 2 subdomains • Corners: Edges and faces with cardinality 1 7 / 24

  16. Coarser triangulation • Similar to FE triangulation object but wo/ reference element • Instead, aggregation info object level 1 = aggregation (vef’s level 0) 8 / 24

  17. Coarser FE space • On top of coarser triangulation, we create a FE-like functional space • DOFs on geometrical objects at the coarser level (as in FEs) • Aggregation info for DOFs ( u α 1 = F α ( u 1 )) 9 / 24

  18. Coarser FE space • On top of coarser triangulation, we create a FE-like functional space • DOFs on geometrical objects at the coarser level (as in FEs) • Aggregation info for DOFs ( u α 1 = F α ( u 1 )) 9 / 24

  19. Coarser FE space • On top of coarser triangulation, we create a FE-like functional space • DOFs on geometrical objects at the coarser level (as in FEs) • Aggregation info for DOFs ( u α 1 = F α ( u 1 )) 1 X u α 1 = u 1 ( p ) #( p ) p ∈E α 9 / 24

  20. Hierarchical FE spaces • The under-assembled space ¯ V 0 = { v ∈ ˜ V 0 | continuous F 1 ( v ) } • ¯ V 0 is a multiscale space ˜ ¯ V 0 V 0 V 0 • Compute sol’on in V 0 using ¯ V 0 correction as preconditioner (multilevel precond) • BDDC DD preconditioner is a particular realization of ¯ V 0 (corners/edges/faces) 10 / 24

  21. Hierarchical FE spaces • The under-assembled space ¯ V 0 = { v ∈ ˜ V 0 | continuous F 1 ( v ) } • ¯ V 0 is a multiscale space ˜ ¯ V 0 V 0 V 0 • Compute sol’on in V 0 using ¯ V 0 correction as preconditioner (multilevel precond) • BDDC DD preconditioner is a particular realization of ¯ V 0 (corners/edges/faces) 10 / 24

  22. Hierarchical FE spaces • The under-assembled space ¯ V 0 = { v ∈ ˜ V 0 | continuous F 1 ( v ) } • ¯ V 0 is a multiscale space ˜ ¯ V 0 V 0 V 0 • Compute sol’on in V 0 using ¯ V 0 correction as preconditioner (multilevel precond) • BDDC DD preconditioner is a particular realization of ¯ V 0 (corners/edges/faces) 10 / 24

  23. Hierarchical FE spaces The under-assembled space ¯ V 0 can be decomposed as [Dohrmann’03]: • Its bubble space ¯ 0 = { v ∈ ¯ V b V 0 |F ( v ) = 0 } • The coarser FE space V 1 = { v ∈ ¯ A ¯ V b V 0 | v ⊥ ˜ 0 } F ( u 0 ) = 0 ¯ ¯ V b = ⊕ V 0 V 1 0 11 / 24

  24. Hierarchical FE spaces The under-assembled space ¯ V 0 can be decomposed as [Dohrmann’03]: • Its bubble space ¯ 0 = { v ∈ ¯ V b V 0 |F ( v ) = 0 } • The coarser FE space V 1 = { v ∈ ¯ A ¯ V b V 0 | v ⊥ ˜ 0 } F ( u 0 ) = 0 ¯ ¯ V b = ⊕ V 0 V 1 0 11 / 24

  25. Coarse corner function • Compute via local problems a basis for V 1 = { Φ 1 , . . . , Φ n c } • Every Φ is a coarse shape function related to a coarse DoF Circle domain partitioned into 9 V 1 corner basis function subdomains 12 / 24

  26. Coarse edge function • Compute via local problems a basis for V 1 = { Φ 1 , . . . , Φ n c } • Every Φ is a coarse shape function related to a coarse DoF Circle domain partitioned into 9 V 1 edge basis function subdomains 13 / 24

  27. Multilevel/scale concurrency The problem in ¯ V 0 = V 1 ⊕ V b 0 : u 0 ∈ ¯ v 0 ∈ ¯ ¯ V 0 : a (¯ u 0 , ¯ v 0 ) = ( f , ¯ v 0 ) ∀ ¯ V 0 A ¯ u b V b can be decomposed as ¯ u 0 = ¯ 0 + u 1 (orthogonality V 1 ⊥ ˜ 0 ) 0 ∈ ¯ 0 ) ∀ v 0 ∈ ¯ u b V b : a ( u b 0 , v b 0 ) = ( f 0 , v b V b 0 0 u 1 ∈ V 1 : a ( u 1 , v 1 ) = ( f 1 , v 1 ) ∀ v 1 ∈ V 1 • Bubble component is local to every subdomain (parallel) • Coarse global problem 14 / 24

  28. Multilevel/scale concurrency The problem in ¯ V 0 = V 1 ⊕ V b 0 : u 0 ∈ ¯ v 0 ∈ ¯ ¯ V 0 : a (¯ u 0 , ¯ v 0 ) = ( f , ¯ v 0 ) ∀ ¯ V 0 A ¯ u b V b can be decomposed as ¯ u 0 = ¯ 0 + u 1 (orthogonality V 1 ⊥ ˜ 0 ) 0 ∈ ¯ 0 ) ∀ v 0 ∈ ¯ u b V b : a ( u b 0 , v b 0 ) = ( f 0 , v b V b 0 0 u 1 ∈ V 1 : a ( u 1 , v 1 ) = ( f 1 , v 1 ) ∀ v 1 ∈ V 1 • Bubble component is local to every subdomain (parallel) • Coarse global problem 14 / 24

  29. Multilevel/scale concurrency The problem in ¯ V 0 = V 1 ⊕ V b 0 : u 0 ∈ ¯ v 0 ∈ ¯ ¯ V 0 : a (¯ u 0 , ¯ v 0 ) = ( f , ¯ v 0 ) ∀ ¯ V 0 A ¯ u b V b can be decomposed as ¯ u 0 = ¯ 0 + u 1 (orthogonality V 1 ⊥ ˜ 0 ) 0 ∈ ¯ 0 ) ∀ v 0 ∈ ¯ u b V b : a ( u b 0 , v b 0 ) = ( f 0 , v b V b 0 0 u 1 ∈ V 1 : a ( u 1 , v 1 ) = ( f 1 , v 1 ) ∀ v 1 ∈ V 1 • Bubble component is local to every subdomain (parallel) • Coarse global problem 14 / 24

  30. Multilevel/scale concurrency The problem in ¯ V 0 = V 1 ⊕ V b 0 : u 0 ∈ ¯ v 0 ∈ ¯ ¯ V 0 : a (¯ u 0 , ¯ v 0 ) = ( f , ¯ v 0 ) ∀ ¯ V 0 A ¯ u b V b can be decomposed as ¯ u 0 = ¯ 0 + u 1 (orthogonality V 1 ⊥ ˜ 0 ) 0 ∈ ¯ 0 ) ∀ v 0 ∈ ¯ u b V b : a ( u b 0 , v b 0 ) = ( f 0 , v b V b 0 0 u 1 ∈ V 1 : a ( u 1 , v 1 ) = ( f 1 , v 1 ) ∀ v 1 ∈ V 1 • Bubble component is local to every subdomain (parallel) • Coarse global problem Multilevel concurrency is BASIC for extreme scalability implementations 14 / 24

  31. Multilevel concurrency P 0 P 1 P 2 t = • L1 duties are fully parallel • L2 duties destroy scalability because • # L1 proc’s ∼ × 1000 # L2 proc’s • L2 problem size increases w/ number of proc’s 15 / 24

  32. Multilevel concurrency P 0 P 1 P 2 P 3 t = • Every processor has one level/scale duties • Idling dramatically reduced (energy-aware solvers) • Overlapped communications / computations among levels 15 / 24

  33. Multilevel concurrency P 0 P 1 P 2 P 3 t = Inter-level overlapped bulk asynchronous (MPMD) im- plementation in FEMPAR 15 / 24

  34. FEMPAR implementation Multilevel extension straightforward (starting the alg’thm with V 1 and level-1 mesh) 3rd level 1st level MPI comm 2nd level MPI comm MPI comm 1 2 1 2 3 4 P 1 2 P 1 ..... ..... e e e e e e e e e r r r r r r r r o o o o o o o o r o c c c c c c c c c parallel (distributed) global communication ..... global communication ..... time ..... 16 / 24

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