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HOMAR Associate Team

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October 18, 2017, at 07:46 AM by 138.96.200.15 -
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October 18, 2017, at 07:46 AM by 138.96.200.15 -
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October 17, 2017, at 04:23 PM by 138.96.200.15 -
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October 17, 2017, at 04:14 PM by 138.96.200.15 -
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October 17, 2017, at 04:14 PM by 138.96.200.15 -
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October 17, 2017, at 04:14 PM by 138.96.200.15 -
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October 17, 2017, at 04:12 PM by 138.96.200.15 -
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>><<
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>><<

>>frame bgcolor='white'<<
%center% %width=260px% http://www-sop.inria.fr/nachos/pics/homar/mhm_4_16_16_mesh.png

>><<
October 17, 2017, at 03:06 PM by 138.96.200.15 -
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[[HOMAR/Meetings    | Meetings]]
October 13, 2015, at 01:48 PM by 138.96.201.175 -
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# To implement the proposed MHM-DGTD solution strategy on modern parallel computing architectures combining coarse grain (MIMD - Multiple Instruction Multiple Data) and fine grian (SIMD - Single Instruction Multiple Data) processing units;
to:
# To implement the proposed MHM-DGTD solution strategy on modern parallel computing architectures combining coarse grain (MIMD - Multiple Instruction Multiple Data) and fine grain (SIMD - Single Instruction Multiple Data) processing units;
October 13, 2015, at 01:48 PM by 138.96.201.175 -
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# To design and analyse new MHM methods for the system of time-domain elastodynamic equations for modeling elastic wave propagation in anisotropic media;
to:
# To design and analyze new MHM methods for the system of time-domain elastodynamic equations for modeling elastic wave propagation in anisotropic media;
October 08, 2015, at 06:20 PM by 138.96.201.175 -
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Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]-[Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptivity); (v) Locally conservative.
to:
Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevertheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]-[Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptivity); (v) Locally conservative.
August 03, 2015, at 07:59 AM by 138.96.201.175 -
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HOMAR is funded by Inria's Direction of the European and International Partnerships Department and by FAPERJ (Fundação de Amparo à Pesquisa do Estado do Rio de Janeiro)
to:
HOMAR is funded by Inria's Direction of the European and International Partnerships Department and by FAPERJ (Fundação de Amparo à Pesquisa do Estado do Rio de Janeiro).
August 03, 2015, at 07:59 AM by 138.96.201.175 -
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(:linebreaks:)

August 03, 2015, at 07:58 AM by 138.96.201.175 -
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>><<

>>frame<<
!! Sponsors
HOMAR is funded by Inria's Direction of the European and International Partnerships Department and by FAPERJ (Fundação de Amparo à Pesquisa do Estado do Rio de Janeiro)
August 03, 2015, at 07:53 AM by 138.96.201.175 -
July 16, 2015, at 09:08 AM by 82.228.254.112 -
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[[Partnership  | Partners and participants]]
[[Meetings    | Meetings]]
[[Publications | Publications]]
[[HOMAR/Results | Results]]
to:
[[HOMAR/Partnership  | Partners and participants]]
[[HOMAR/Meetings    | Meetings]]
[[HOMAR/Publications | Publications]]
[[HOMAR/Results     | Results]]
July 16, 2015, at 09:07 AM by 82.228.254.112 -
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[[Results     | Results]]
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[[HOMAR/Results | Results]]
July 16, 2015, at 09:04 AM by 82.228.254.112 -
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[[Partnership | Partners and participants]]
to:
[[Partnership  | Partners and participants]]
[[Meetings    | Meetings]]
[[Publications | Publications]]
[[Results      | Results
]]
July 16, 2015, at 08:57 AM by 82.228.254.112 -
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* [[Partnership | Partners and participants]]
>>

>>frame<<
!! Partners and participants

(:linebreaks:)

!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/S-Lanteri | Stéphane Lanteri]]
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/M-Lallemand | Marie Hélène Lallemand]]
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/R-Leger | Raphaël Léger]]
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/C-Scheid | Claire Scheid]]

!! %newwin% [[http://www.lncc.br | LNCC]], Petrópolis, Brazil
* %newwin% [[http://www.lncc.br/~atagomes | Antônio Tadeu Azevedo Gomes]]
* %newwin% [[http://www.lncc.br/~alm | Alexandre Madureira]]
* %newwin% [[http://www.lncc.br/~valentin | Frédéric Valentin]]

!! Universidad Católica de Valparaiso, Chile
* %newwin% [[http://dparedesfem.wix.com/home | Diego Paredes
]]
to:
[[Partnership | Partners and participants]]
July 16, 2015, at 08:56 AM by 82.228.254.112 -
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>>frame<<
* [[Partnership | Partners and participants]]
>>
July 16, 2015, at 08:55 AM by 82.228.254.112 -
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The main scientific goals of this collaboration iare:
to:
The main scientific goals of this collaboration are:
July 16, 2015, at 08:30 AM by 82.228.254.112 -
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The main scientific goals of HOMAR  are:
to:
The main scientific goals of this collaboration iare:
July 16, 2015, at 08:27 AM by 82.228.254.112 -
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!! [+High performance Multiscale Algorithms for wave pRopagation problems+]
to:
!! High performance Multiscale Algorithms for wave pRopagation problems
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>><<

>>frame<<
!! Objectives

(:linebreaks:)

The main scientific goals of HOMAR  are:
# To design and analyze new MHM methods for the system of time-domain Maxwell equations coupled to models of physical dispersion, in view of their application to light interaction with nanometer scale structures;
# To design and analyse new MHM methods for the system of time-domain elastodynamic equations for modeling elastic wave propagation in anisotropic media;
# To devise appropriate discrete versions of the proposed MHM methods using DG (Discontinuous Galerkin) formulations for the discretization of the local solvers, and to study the mathematical properties (stability, convergence) of the combined MHM-DGTD strategies;
# To implement the proposed MHM-DGTD solution strategy on modern parallel computing architectures combining coarse grain (MIMD - Multiple Instruction Multiple Data) and fine grian (SIMD - Single Instruction Multiple Data) processing units;
# To demonstrate the capabilities of the developed MHM-DGTD parallel solution strategies for the simulation of selected problems in the fields of nanophotonics and elastodynamics.
July 16, 2015, at 08:18 AM by 82.228.254.112 -
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!! High performance Multiscale Algorithms for wave pRopagation problems
to:
!! [+High performance Multiscale Algorithms for wave pRopagation problems+]
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! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
to:
!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
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! %newwin% [[http://www.lncc.br | LNCC]], Petrópolis, Brazil
to:
!! %newwin% [[http://www.lncc.br | LNCC]], Petrópolis, Brazil
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! Universidad Católica de Valparaiso, Chile
to:
!! Universidad Católica de Valparaiso, Chile
July 16, 2015, at 08:17 AM by 82.228.254.112 -
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!!! Scientific context
to:
!! Scientific context
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!!! Partners and participants
to:
!! Partners and participants
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!!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
to:
! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
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!!! %newwin% [[http://www.lncc.br | LNCC]], Petrópolis, Brazil
to:
! %newwin% [[http://www.lncc.br | LNCC]], Petrópolis, Brazil
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!!! Universidad Católica de Valparaiso, Chile
to:
! Universidad Católica de Valparaiso, Chile
July 16, 2015, at 07:59 AM by 82.228.254.112 -
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!!! LNCC, Petrópolis, Brazil
*
[[http://www.lncc.br/~atagomes | Antônio Tadeu Azevedo Gomes]]
* [[http://www.lncc.br/~alm | Alexandre Madureira]]
* [[http://www.lncc.br/~valentin | Frédéric Valentin]]
to:
!!! %newwin% [[http://www.lncc.br | LNCC]], Petrópolis, Brazil
* %newwin%
[[http://www.lncc.br/~atagomes | Antônio Tadeu Azevedo Gomes]]
* %newwin% [[http://www.lncc.br/~alm | Alexandre Madureira]]
* %newwin%
[[http://www.lncc.br/~valentin | Frédéric Valentin]]
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* [[http://dparedesfem.wix.com/home | Diego Paredes]]
to:
* %newwin% [[http://dparedesfem.wix.com/home | Diego Paredes]]
July 16, 2015, at 07:56 AM by 82.228.254.112 -
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!!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]\\\
to:
!!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
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!!! LNCC, Petrópolis, Brazil\\\
to:
!!! LNCC, Petrópolis, Brazil
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!!! Universidad Católica de Valparaiso, Chile\\\
to:
!!! Universidad Católica de Valparaiso, Chile
July 16, 2015, at 07:55 AM by 82.228.254.112 -
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!!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
to:
!!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]\\\
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!!! LNCC, Petrópolis, Brazil
* [[http://www.lncc.br/~atagomes | Antônio Tadeu Azevedo Gomes]],
to:
!!! LNCC, Petrópolis, Brazil\\\
* [[http://www.lncc.br/~atagomes | Antônio Tadeu Azevedo Gomes]]
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to:
!!! Universidad Católica de Valparaiso, Chile\\\
* [[http://dparedesfem.wix.com/home | Diego Paredes]]
July 16, 2015, at 07:51 AM by 82.228.254.112 -
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Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]- [Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptivity); (v) Locally conservative.
to:
Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]-[Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptivity); (v) Locally conservative.
Changed line 26 from:
@@ %black% Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]@@
to:
!!! Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]
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!!! LNCC, Petrópolis, Brazil
* [[http://www.lncc.br/~atagomes | Antônio Tadeu Azevedo Gomes]],
* [[http://www.lncc.br/~alm | Alexandre Madureira]]
* [[http://www.lncc.br/~valentin | Frédéric Valentin]]

July 16, 2015, at 07:39 AM by 82.228.254.112 -
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@@Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]@@
to:
@@ %black% Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]@@
July 16, 2015, at 07:38 AM by 82.228.254.112 -
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'''Inria Sophia Antipolis - Méditerranée, Nachos project-team'''
to:
@@Inria Sophia Antipolis - Méditerranée, %newwin% [[http://www-sop.inria.fr/nachos | Nachos project-team]]@@
July 16, 2015, at 07:37 AM by 82.228.254.112 -
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!!! Partner and participants
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!!! Partners and participants
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Inria Sophia Antipolis - Méditerranée, Nachos project-team
to:
'''Inria Sophia Antipolis - Méditerranée, Nachos project-team'''
July 16, 2015, at 07:35 AM by 82.228.254.112 -
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* %newwin% [[http://www-sop.inria.fr/nachos/index.php/Main/StephaneLanteri | Stéphane Lanteri]]
* Marie Hélène Lallemand
* Raphaël Léger
* %newwin%
[[http://math.unice.fr/~cscheid | Claire Scheid]]
to:
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/S-Lanteri | Stéphane Lanteri]]
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/M-Lallemand | Marie Hélène Lallemand]]
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/R-Leger | Raphaël Léger]]
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/People/C-Scheid
| Claire Scheid]]
July 16, 2015, at 07:25 AM by 82.228.254.112 -
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* %newwin% [[http://www-sop.inria.fr/nachos/index.php/Main/St%E9phaneLanteri | Stéphane Lanteri]]
to:
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/Main/StephaneLanteri | Stéphane Lanteri]]
July 16, 2015, at 07:24 AM by 82.228.254.112 -
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!!! Partnership
to:
!!! Partner and participants
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Inria Sophia Antipolis - Méditerranée, Nachos project-team
* %newwin% [[http://www-sop.inria.fr/nachos/index.php/Main/St%E9phaneLanteri | Stéphane Lanteri]]
* Marie Hélène Lallemand
* Raphaël Léger
* %newwin% [[http://math.unice.fr/~cscheid | Claire Scheid]]
July 15, 2015, at 12:21 PM by 82.228.254.112 -
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! High performance Multiscale Algorithms for wave pRopagation problems
to:
!! High performance Multiscale Algorithms for wave pRopagation problems
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>><<

>>frame<<
!!! Partnership

(:linebreaks:)

July 15, 2015, at 12:20 PM by 82.228.254.112 -
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!! High performance Multiscale Algorithms for wave pRopagation problems
to:
! High performance Multiscale Algorithms for wave pRopagation problems
July 15, 2015, at 12:20 PM by 82.228.254.112 -
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>>
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>><<
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(:linebreaks:)
July 15, 2015, at 12:19 PM by 82.228.254.112 -
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>>
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!!! Scientific context
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Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]- [Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptivity); (v) Locally conservative.
to:
Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]- [Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptivity); (v) Locally conservative.
>><<
July 13, 2015, at 12:50 PM by 82.228.254.112 -
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Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]- [Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptativity); (v) Locally conservative.
to:
Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]- [Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptivity); (v) Locally conservative.
July 13, 2015, at 12:49 PM by 82.228.254.112 -
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The general scientific context of this collaboration is the study of time dependent wave propagation problems with strong multiscale features (in space and time). The general goal is the design, analysis and implementation of a family of innovative high performance numerical methods particularly well suited to the simulation of multiscale wave propagation problems. Mathematical models based on partial differential equations (PDE) embedding multiscale features occur in a wide range of scientific and technological applications involving wave propagation in heterogeneous media.
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The general scientific context of this collaboration is the study of time dependent wave propagation problems with strong multiscale features (in space and time). The general goal is the design, analysis and implementation of a family of innovative high performance numerical methods particularly well suited to the simulation of multiscale wave propagation problems. Mathematical models based on partial differential equations (PDE) embedding multiscale features occur in a wide range of scientific and technological applications involving wave propagation in heterogeneous media.

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Finite element methods are frequently adopted to approximate the solution of such PDE  models. Nevetheless, it is well-known that the accuracy of numerical solutions may seriously deteriorate on coarse meshes when they show multiscale or high-contrast features. Such an issue has led to the concept of multiscale basis functions in the seminal work [Babuska and Osborn, 1983] (further extended to the two-dimensional case in [Hou and Wu, 1997]) and allowed numerical methods to be precise on coarse meshes. Such physically rooted basis functions are the counterpart of polynomial basis functions generally adopted in classical finite element schemes, which are defined on a purely algebraic setting. Recently, researchers at LNCC introduced a family of finite element methods particularly adapted to be used in high-contrast or heterogeneous coefficients problems, [Araya et al., 2013]- [Harder et al., 2013], named Multiscale Hybrid-Mixed (MHM) methods. These novel finite element methods share the following properties: (i) Stable and high-order convergent; (ii) Accurate on coarse meshes; (iii) Naturally adapted to high-performance parallel computing; (iv) Induce a face-based a posteriori error estimator (to drive mesh adaptativity); (v) Locally conservative
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July 13, 2015, at 12:34 PM by 82.228.254.112 -
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The general scientific context of this collaboration is the study of time dependent wave propagation problems with strong multiscale features (in space and time). The general goal is the design, analysis and implementation of a family of innovative high performance numerical meth- ods particularly well suited to the simulation of multiscale wave propagation problems. Math- ematical models based on partial differential equations (PDE) embedding multiscale features occur in a wide range of scientific and technological applications involving wave propagation in heterogenous media.
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The general scientific context of this collaboration is the study of time dependent wave propagation problems with strong multiscale features (in space and time). The general goal is the design, analysis and implementation of a family of innovative high performance numerical methods particularly well suited to the simulation of multiscale wave propagation problems. Mathematical models based on partial differential equations (PDE) embedding multiscale features occur in a wide range of scientific and technological applications involving wave propagation in heterogeneous media.
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High performance Multiscale Algorithms for wave pRopagation problems
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!! High performance Multiscale Algorithms for wave pRopagation problems

The general scientific context of this collaboration is the study of time dependent wave propagation problems with strong multiscale features (in space and time). The general goal is the design, analysis and implementation of a family of innovative high performance numerical meth- ods particularly well suited to the simulation of multiscale wave propagation problems. Math- ematical models based on partial differential equations (PDE) embedding multiscale features occur in a wide range of scientific and technological applications involving wave propagation in heterogenous media.
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(:title HOMAR Associate Team:)
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(:title HOMAR Associate Team:)

High performance Multiscale Algorithms for wave pRopagation problems
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(:title HOMAR Associate Team:)