| Year | Rank | Type | Title / Venue / Authors |
|---|---|---|---|
| 2026 | J | jnl |
CoRR
|
| 2026 | J | jnl |
J. Comput. Phys.
|
| 2026 | J | jnl |
CoRR
|
| 2025 | J | jnl |
CoRR
|
| 2025 | J | jnl |
J. Comput. Phys.
|
| 2025 | J | jnl |
CoRR
|
| 2025 | J | jnl |
J. Comput. Phys.
|
| 2025 | J | jnl |
CoRR
|
| 2025 | J | jnl |
CoRR
|
| 2025 | J | jnl |
CoRR
|
| 2025 | J | jnl |
CoRR
|
| 2025 | J | jnl |
CoRR
|
| 2024 | J | jnl |
CoRR
|
| 2024 | J | jnl |
CoRR
|
| 2024 | J | jnl |
J. Comput. Phys.
|
| 2024 | J | jnl |
J. Comput. Phys.
|
| 2024 | J | jnl |
CoRR
|
| 2024 | J | jnl |
CoRR
|
| 2024 | J | jnl |
CoRR
|
| 2023 | J | jnl |
A pressure-free long-time stable reduced-order model for two-dimensional Rayleigh-Bénard convection.
CoRR
|
| 2023 | J | jnl |
Comput. Math. Appl.
|
| 2023 | J | jnl |
CoRR
|
| 2023 | J | jnl |
Energy-consistent discretization of viscous dissipation with application to natural convection flow.
CoRR
|
| 2023 | J | jnl |
CoRR
|
| 2023 | J | jnl |
Comput. Math. Appl.
|
| 2023 | J | jnl |
J. Comput. Phys.
|
| 2022 | J | jnl |
CoRR
|
| 2022 | J | jnl |
CoRR
|
| 2022 | J | jnl |
CoRR
|
| 2022 | J | jnl |
CoRR
|
| 2022 | J | jnl |
CoRR
|
| 2022 | J | jnl |
CoRR
|
| 2021 | J | jnl |
J. Comput. Appl. Math.
|
| 2021 | J | jnl |
J. Comput. Phys.
|
| 2021 | J | jnl |
CoRR
|
| 2021 | J | jnl |
CoRR
|
| 2021 | J | jnl |
PLoS Comput. Biol.
|
| 2020 | J | jnl |
CoRR
|
| 2020 | J | jnl |
J. Comput. Phys.
|
| 2020 | J | jnl |
ERCIM News
|
| 2020 | J | jnl |
SIAM/ASA J. Uncertain. Quantification
|
| 2020 | J | jnl |
CoRR
|
| 2020 | J | jnl |
J. Comput. Phys.
|
| 2019 | J | jnl |
CoRR
|
| 2019 | J | jnl |
SIAM J. Sci. Comput.
|
| 2019 | J | jnl |
J. Comput. Phys.
|
| 2019 | J | jnl |
CoRR
|
| 2019 | J | jnl |
CoRR
|
| 2019 | J | jnl |
CoRR
|
| 2018 | J | jnl |
ERCIM News
|
| 2014 | J | jnl |
J. Comput. Phys.
|
| 2013 | J | jnl |
J. Comput. Phys.
|
| 2012 | J | jnl |
J. Comput. Phys.
|