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June 14, 2016, at 02:16 PM by 138.96.200.15 -
Changed line 27 from:

(:cellnr align='center':) More details?

to:

(:cellnr align='center':) More details

June 14, 2016, at 02:14 PM by 138.96.200.15 -
Changed line 27 from:

(:cellnr align='center':) More details

to:

(:cellnr align='center':) More details?

June 14, 2016, at 02:14 PM by 138.96.200.15 -
Changed line 27 from:

(:cellnr align='center':) More details?

to:

(:cellnr align='center':) More details

December 16, 2015, at 03:59 PM by 138.96.200.15 -
Changed line 67 from:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/p_loc/bowtie3.png

to:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/p_loc/bowtie3.png

December 16, 2015, at 03:58 PM by 138.96.200.15 -
Changed line 67 from:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/p_loc/bowtie3.png

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(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/p_loc/bowtie3.png

Changed line 73 from:

(:cell align='center':)

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(:cell align='center':) More details

December 16, 2015, at 03:57 PM by 138.96.200.15 -
December 16, 2015, at 03:57 PM by 138.96.200.15 -
Changed line 67 from:

(:cell align='center':)

to:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/p_loc/bowtie3.png

Changed lines 69-71 from:

(:cell align='center':)

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(:cell align='center':) Simulation of near-field plasmonic interactions (:cellnr align='center':) (:cell align='center':) with a local approximation order DGTD method

July 22, 2015, at 01:19 PM by 193.51.208.251 -
Changed lines 72-73 from:
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(:tableend:)

(:table border='0' align='center':)

July 22, 2015, at 01:18 PM by 193.51.208.251 -
Added line 72:
July 22, 2015, at 01:17 PM by 193.51.208.251 -
Deleted lines 68-69:

(:cell align='center':) (:cellnr align='center':)

July 22, 2015, at 01:16 PM by 193.51.208.251 -
Changed line 66 from:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/eels/eels_visu_t1.png %width=170px% http://www-sop.inria.fr/nachos/pics/results/eels/

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/eels/eels_visu_t3.png

July 22, 2015, at 01:16 PM by 193.51.208.251 -
Added lines 64-73:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/eels/eels_visu_t1.png %width=170px% http://www-sop.inria.fr/nachos/pics/results/eels/ (:cell align='center':) (:cellnr align='center':) Electron energy loss spectroscopy (:cell align='center':) (:cellnr align='center':) (:cell align='center':) (:cellnr align='center':) More details (:cell align='center':)

July 22, 2015, at 01:13 PM by 193.51.208.251 -
April 30, 2015, at 07:45 PM by 88.128.80.245 -
Changed line 31 from:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/imex/surfint=40616.png

to:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/imex/surfint=40616.png

April 30, 2015, at 07:44 PM by 88.128.80.245 -
Changed line 31 from:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/imex/surfint=40616.png

to:

(:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/imex/surfint=40616.png

April 30, 2015, at 07:42 PM by 88.128.80.245 -
Changed lines 10-22 from:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_hyb_mesh.jpg %width=120px% http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_X_g1_L.png (:cellnr align='center':)High-order DGTD method on (:cell align='center':)Hybrid cubic/tetrahedral DGTD method (:cellnr align='center':)curvilinear tetrahedral meshes (:cell align='center':)with application to nanophotonics (:cellnr align='center':)with application to plasmonics (:cell align='center':) (:cellnr align='center':)More details (:cell align='center':)More details

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_hyb_mesh.jpg %width=120px% http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_X_g1_L.png (:cellnr align='center':) High-order DGTD method on (:cell align='center':) Hybrid cubic/tetrahedral DGTD method (:cellnr align='center':) curvilinear tetrahedral meshes (:cell align='center':) with application to nanophotonics (:cellnr align='center':) with application to plasmonics (:cell align='center':) (:cellnr align='center':) More details (:cell align='center':) More details

Added lines 22-39:

(:cell align='center':) (:cellnr align='center':) DGTD method for a non-local Drude model (:cell align='center':) (:cellnr align='center':) with application to plasmonics (:cell align='center':) (:cellnr align='center':) More details? (:cell align='center':)

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/imex/surfint=40616.png (:cellnr align='center':) Hybridized DGFD methods (:cell align='center':) Locally implicit DGTD methods (:cellnr align='center':) for electromagnetics (:cell align='center':) for electromagnetics (:cellnr align='center':) More details (:cell align='center':) More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png

Changed line 41 from:

(:cellnr align='center':)DGTD method for a non-local Drude model

to:

(:cellnr align='center':)Hybrid MIMD/SIMD high order DGTD solver

Changed line 43 from:

(:cellnr align='center':)with application to plasmonics

to:

(:cellnr align='center':)More details

Deleted lines 44-65:

(:cellnr align='center':)More details? (:cell align='center':)

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='center':) (:cellnr align='center':)Hybridized DGFD methods (:cell align='center':)Locally implicit DGTD methods (:cellnr align='center':)for electromagnetics (:cell align='center':)for electromagnetics (:cellnr align='center':)More details (:cell align='center':)More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png (:cell align='center':) (:cellnr align='center':)Hybrid MIMD/SIMD high order DGTD solver (:cell align='center':) (:cellnr align='center':)More details (:cell align='center':)

Changed lines 58-69 from:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png (:cellnr align='center':)Light scattering by optical nanoantennas (:cell align='center':)Light absorption by MIM structures (:cellnr align='center':)More details (:cell align='center':)More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg %width=170px% http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg (:cell align='center':)

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png (:cellnr align='center':) Light scattering by optical nanoantennas (:cell align='center':) Light absorption by MIM structures (:cellnr align='center':) More details (:cell align='center':) More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg %width=170px% http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg (:cell align='center':)

Changed line 68 from:

(:cell align='center':)

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(:cell align='center':)

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(:cell align='center':)

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(:cell align='center':)

Changed line 72 from:

(:cell align='center':)

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(:cell align='center':)

April 30, 2015, at 06:11 PM by 212.194.65.231 -
April 30, 2015, at 06:11 PM by 212.194.65.231 -
Changed lines 52-53 from:
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Changed lines 82-83 from:
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(:tableend:)

April 30, 2015, at 06:10 PM by 212.194.65.231 -
Deleted lines 51-54:

======= (:tableend:) >>>>>>>

April 30, 2015, at 06:09 PM by 212.194.65.231 -
Deleted line 19:

<<<<<<<

April 30, 2015, at 06:09 PM by 212.194.65.231 -
Changed lines 20-42 from:

(:tableend:)

(:linebreaks:) (:linebreaks:)

Applications related results

(:linebreaks:) (:linebreaks:)

(:table border='0' align='center':) (:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png (:cellnr align='center':)Light scattering by optical nanoantennas (:cell align='center':)Light absorption by MIM structures (:cellnr align='center':)More details (:cell align='center':)More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg %width=170px% http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg

to:

<<<<<<<

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_nonloc_drude/2DiscClExZ.png

Changed lines 26-27 from:

(:cellnr align='center':) Realistic numerical modeling of microwave interaction

to:

(:cellnr align='center':)DGTD method for a non-local Drude model

Changed line 28 from:

(:cellnr align='center':) with biological tissues

to:

(:cellnr align='center':)with application to plasmonics

Changed line 30 from:

(:cellnr align='center':) More details

to:

(:cellnr align='center':)More details?

Changed lines 32-86 from:
to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='center':) (:cellnr align='center':)Hybridized DGFD methods (:cell align='center':)Locally implicit DGTD methods (:cellnr align='center':)for electromagnetics (:cell align='center':)for electromagnetics (:cellnr align='center':)More details (:cell align='center':)More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png (:cell align='center':) (:cellnr align='center':)Hybrid MIMD/SIMD high order DGTD solver (:cell align='center':) (:cellnr align='center':)More details (:cell align='center':) (:tableend:) ======= (:tableend:) >>>>>>>

(:linebreaks:) (:linebreaks:)

Applications related results

(:linebreaks:) (:linebreaks:)

(:table border='0' align='center':) (:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png (:cellnr align='center':)Light scattering by optical nanoantennas (:cell align='center':)Light absorption by MIM structures (:cellnr align='center':)More details (:cell align='center':)More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg %width=170px% http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg (:cell align='center':)

(:cellnr align='center':) Realistic numerical modeling of microwave interaction (:cell align='center':) (:cellnr align='center':) with biological tissues (:cell align='center':) (:cellnr align='center':) More details (:cell align='center':)

Deleted lines 19-51:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_nonloc_drude/2DiscClExZ.png (:cell align='center':) (:cellnr align='center':)DGTD method for a non-local Drude (:cell align='center':) (:cellnr align='center':)model with application to plasmonics (:cell align='center':) (:cellnr align='center':)More details? (:cell align='center':)

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='center':) (:cellnr align='center':)Hybridized DGFD methods (:cell align='center':)Locally implicit DGTD methods (:cellnr align='center':)for electromagnetics (:cell align='center':)for electromagnetics (:cellnr align='center':)More details (:cell align='center':)More details

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png (:cell align='center':) (:cellnr align='center':)Hybrid MIMD/SIMD high order (:cell align='center':) (:cellnr align='center':)DGTD solver (:cell align='center':) (:cellnr align='center':)More details (:cell align='center':)

April 30, 2015, at 06:08 PM by jviquera - Alignement des cases
Changed lines 10-11 from:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg (:cell align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_hyb_mesh.jpg %width=120px% http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_X_g1_L.png

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_hyb_mesh.jpg %width=120px% http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_X_g1_L.png

Changed lines 20-25 from:

(:tableend:)

(:table border='0' align='center':) (:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_nonloc_drude/2DiscClExZ.png (:cell align='center' width='10%':) (:cellnr align='center':)DGTD method for a non-local Drude model

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/nano_nonloc_drude/2DiscClExZ.png

Changed line 25 from:

(:cellnr align='center':)with application to plasmonics

to:

(:cellnr align='center':)DGTD method for a non-local Drude

Added lines 27-28:

(:cellnr align='center':)model with application to plasmonics (:cell align='center':)

Changed lines 31-35 from:

(:tableend:)

(:table border='0' align='center':) (:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='center' width='10%':)

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='center':)

Changed lines 42-47 from:

(:tableend:)

(:table border='0' align='center':) (:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png (:cell align='center' width='10%':) (:cellnr align='center':)Hybrid MIMD/SIMD high order DGTD solver

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png

Changed line 47 from:

(:cellnr align='center':)More details

to:

(:cellnr align='center':)Hybrid MIMD/SIMD high order

Added lines 49-52:

(:cellnr align='center':)DGTD solver (:cell align='center':) (:cellnr align='center':)More details (:cell align='center':)

Changed lines 66-67 from:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png

Changed lines 72-86 from:

(:tableend:)

(:linebreaks:) (:linebreaks:)

(:table border='0' align='center':) (:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg
http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg (:cell align='left' width='10%':) (:tableend:) Realistic numerical modeling of microwave interaction
with biological tissues More details

to:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg %width=170px% http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg (:cell align='center':)

(:cellnr align='center':) Realistic numerical modeling of microwave interaction (:cell align='center':) (:cellnr align='center':) with biological tissues (:cell align='center':) (:cellnr align='center':) More details (:cell align='center':)

April 30, 2015, at 05:34 PM by 212.194.65.231 -
April 30, 2015, at 05:34 PM by 212.194.65.231 -
Changed lines 76-77 from:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg (:cell align='left':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg

to:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg
http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg (:cell align='left' width='10%':)

April 30, 2015, at 05:33 PM by 212.194.65.231 -
April 30, 2015, at 05:33 PM by 212.194.65.231 -
Changed line 77 from:

(:cell align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg

to:

(:cell align='left':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg

April 30, 2015, at 05:33 PM by 212.194.65.231 -
Changed lines 76-77 from:

(:cellnr align='center':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg (:cell align='center':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg

to:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/tet+tel-1.jpg (:cell align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/new_headexp/E_peau-1.jpg

April 30, 2015, at 05:33 PM by 212.194.65.231 -
Changed lines 64-69 from:

(:cellnr align='left':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='left':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png (:cellnr align='left':) Light scattering by optical nanoantennas (:cell align='left':) Light absorption by MIM structures (:cellnr align='left':) More details (:cell align='left':) More details

to:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/UoB/antenna_array-mesh.jpg (:cell align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/mim_structure/Hx_view4.png (:cellnr align='center':)Light scattering by optical nanoantennas (:cell align='center':)Light absorption by MIM structures (:cellnr align='center':)More details (:cell align='center':)More details

April 30, 2015, at 05:32 PM by 212.194.65.231 -
Changed lines 10-19 from:

(:cellnr align='left' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg (:cell align='left' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_hyb_mesh.jpg %width=120px% http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_X_g1_L.png (:cellnr align='left':)High-order DGTD method on (:cell align='left':)Hybrid cubic/tetrahedral DGTD method (:cellnr align='left':)curvilinear tetrahedral meshes (:cell align='left':)with application to nanophotonics (:cellnr align='left':)with application to plasmonics (:cell align='left':) (:cellnr align='left':)More details (:cell align='left':)More details

to:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg (:cell align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_hyb_mesh.jpg %width=120px% http://www-sop.inria.fr/nachos/pics/results/nano_L-guide/Lguide_X_g1_L.png (:cellnr align='center':)High-order DGTD method on (:cell align='center':)Hybrid cubic/tetrahedral DGTD method (:cellnr align='center':)curvilinear tetrahedral meshes (:cell align='center':)with application to nanophotonics (:cellnr align='center':)with application to plasmonics (:cell align='center':) (:cellnr align='center':)More details (:cell align='center':)More details

April 30, 2015, at 05:32 PM by 212.194.65.231 -
Changed lines 23-30 from:

(:cellnr align='left' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_nonloc_drude/2DiscClExZ.png (:cell align='left' width='10%':) (:cellnr align='left':)DGTD method for a non-local Drude model (:cell align='left':) (:cellnr align='left':)with application to plasmonics (:cell align='left':) (:cellnr align='left':)More details? (:cell align='left':)

to:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/nano_nonloc_drude/2DiscClExZ.png (:cell align='center' width='10%':) (:cellnr align='center':)DGTD method for a non-local Drude model (:cell align='center':) (:cellnr align='center':)with application to plasmonics (:cell align='center':) (:cellnr align='center':)More details? (:cell align='center':)

April 30, 2015, at 05:32 PM by 212.194.65.231 -
Changed lines 34-41 from:

(:cellnr align='left' width='10%':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='left' width='10%':) (:cellnr align='left':)Hybridized DGFD methods (:cell align='left':)Locally implicit DGTD methods (:cellnr align='left':)for electromagnetics (:cell align='left':)for electromagnetics (:cellnr align='left':)More details (:cell align='left':)More details

to:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/hdg/hdg_cyl_pec.png (:cell align='center' width='10%':) (:cellnr align='center':)Hybridized DGFD methods (:cell align='center':)Locally implicit DGTD methods (:cellnr align='center':)for electromagnetics (:cell align='center':)for electromagnetics (:cellnr align='center':)More details (:cell align='center':)More details

April 30, 2015, at 05:32 PM by 212.194.65.231 -
Changed lines 45-50 from:

(:cellnr align='left':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png (:cell align='left':) (:cellnr align='left':) Hybrid MIMD/SIMD high order DGTD solver (:cell align='left':) (:cellnr align='left':) More details (:cell align='left':)

to:

(:cellnr align='center' width='10%':) http://www-sop.inria.fr/nachos/pics/results/hpc/Yguide-2.png (:cell align='center' width='10%':) (:cellnr align='center':)Hybrid MIMD/SIMD high order DGTD solver (:cell align='center':) (:cellnr align='center':)More details (:cell align='center':)

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April 17, 2015, at 05:02 PM by 138.96.201.175 -
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Numerical modeling of optical nanoantennas
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with biological tissues using a DGDT method

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with biological tissues

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http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg High-order DGTD method
on curvilinear tetrahedral meshes
with application to plasmonics
More details

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with application to light propagation in
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with application to nanophotonics \\

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with biological tissues using a DGDT method More details

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curvilinear structures in a high-order DGTD method
with application to plasmonics
DGTD_curvi

http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg Hybrid cubic/tetrahedral DGTD method with application to light propagation in a L-shaped waveguide composed of nanospheres

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with application to plasmonics

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with application to light propagation
in a L-shaped waveguide composed of nanospheres More details

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Classical finite element methods rely on tessellations composed of straight-edged elements mapped linearly from a reference element, on domains which physical boundaries and interfaces are indifferently straight or curved. This approximation represents serious hindrance for high-order methods, since they limit the precision of the spatial discretization to second order. Thus, exploiting an enhanced representation of the physical geometry of a considered problem is in agreement with the natural procedure of high-order methods, such as the discontinuous Galerkin method. In the latter framework, we propose and validate an implementation of a high-order mapping for tetrahedra, and then focus on specific nanophotonics setups to assess the gains of the method in terms of memory and performances.

http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg Tetrahedral mesh for plasmonic resonance of a gold nanosphere. The scatterer (in red) is enclosed by the total field (TF) region (in blue), delimited by the TF/SF interface on which the incident field is imposed. Then we find the scattered field (SF) region (in purple), surrounded by UPMLs (in gray).

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Classical finite element methods rely on tessellations composed of straight-edged elements mapped linearly from a reference element, on domains which physical boundaries and interfaces are indifferently straight or curved. This approximation represents serious hindrance for high-order methods, since they limit the precision of the spatial discretization to second order. Thus, exploiting an enhanced representation of the physical geometry of a considered problem is in agreement with the natural procedure of high-order methods, such as the discontinuous Galerkin method. In the latter framework, we propose and validate an implementation of a high-order mapping for tetrahedra, and then focus on specific nanophotonics setups to assess the gains of the method in terms of memory and performances.

http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg Tetrahedral mesh for plasmonic resonance of a gold nanosphere. The scatterer (in red) is enclosed by the total field (TF) region (in blue), delimited by the TF/SF interface on which the incident field is imposed. Then we find the scattered field (SF) region (in purple), surrounded by UPMLs (in gray).

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Classical finite element methods rely on tessellations composed of straight-edged elements mapped linearly from a reference element, on domains which physical boundaries and interfaces are indifferently straight or curved. This approximation represents serious hindrance for high-order methods, since they limit the precision of the spatial discretization to second order. Thus, exploiting an enhanced representation of the physical geometry of a considered problem is in agreement with the natural procedure of high-order methods, such as the discontinuous Galerkin method. In the latter framework, we propose and validate an implementation of a high-order mapping for tetrahedra, and then focus on specific nanophotonics setups to assess the gains of the method in terms of memory and performances.

http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg Tetrahedral mesh for plasmonic resonance of a gold nanosphere. The scatterer (in red) is enclosed by the total field (TF) region (in blue), delimited by the TF/SF interface on which the incident field is imposed. Then we find the scattered field (SF) region (in purple), surrounded by UPMLs (in gray).

to:

.

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Classical finite element methods rely on tessellations composed of straight-edged elements mapped linearly from a reference element, on domains which physical boundaries and interfaces are indifferently straight or curved. This approximation represents serious hindrance for high-order methods, since they limit the precision of the spatial discretization to second order. Thus, exploiting an enhanced representation of the physical geometry of a considered problem is in agreement with the natural procedure of high-order methods, such as the discontinuous Galerkin method. In the latter framework, we propose and validate an implementation of a high-order mapping for tetrahedra, and then focus on specific nanophotonics setups to assess the gains of the method in terms of memory and performances.

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http://www-sop.inria.fr/nachos/pics/results/nano_sphere/nano_sphere-mesh.jpg Tetrahedral mesh for plasmonic resonance of a gold nanosphere. The scatterer (in red) is enclosed by the total field (TF) region (in blue), delimited by the TF/SF interface on which the incident field is imposed. Then we find the scattered field (SF) region (in purple), surrounded by UPMLs (in gray).

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