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您的检索式：作者名="Matthieu Pedros"
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| 1 | Micro and nano cellular amorphouspolymers(PMMA,PS)in supercritical CO2assisted bynanostructured C02-philic block copolymers-one stepfoaming process显示文摘 | Jose Antonio Reglero Ruiz Matthieu Pedros Jean-Marc Tallon | 2011 | J of Supercritical Fluids2011，，58： | 1 |
| 2 | Polyamines: molecules with regulatory functions in plant abiotic stress tolerance显示文摘 | Rubén Alcázar Teresa Altabella Francisco Marco Cristina Bortolotti Matthieu Reymond Csaba Koncz Pedro Carrasco Antonio F. Tiburcio | 2010 | Planta2010，，6： | 1 |
| 3 | Review of the Occurrence of Anti-infectives in Contaminated Wastewaters and Natural and Drinking Waters显示文摘 | Segura Pedro A Fran?ois Matthieu Gagnon Christian Sauvé Sébastien | 2009 | Environmental Health Perspectives2009，，5： | 1 |
| 4 | High-throughput analysis of Fröhlich-type polaron models显示文摘The electron–phonon interaction is central to condensed matter,e.g.through electrical resistance,superconductivity or the formation of polarons,and has a strong impact on observables such as band gaps or optical spectra.The most common framework for band energy corrections is the Fröhlich model,which often agrees qualitatively with experiments in polar materials,but has limits for complex cases.A generalized version includes anisotropic and degenerate electron bands,and multiple phonons.In this work,we identify trends and outliers for the Fröhlich models on 1260 materials.We test the limits of the Fröhlich models and their perturbative treatment,in particular the large polaron hypothesis.Among our extended dataset most materials host perturbative large polarons,but there are many instances that are non-perturbative and/or localize on distances of a few bond lengths.We find a variety of behaviors,and analyze extreme cases with huge zero-point renormalization using the first-principles Allen-Heine-Cardona approach. | Pedro Miguel M.C.de Melo Joao C.de Abreu Bogdan Guster Matteo Giantomassi Zeila Zanolli Xavier Gonze Matthieu J.Verstraete | 2023 | npj Computational Materials2023，，1： | 0 |
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