Philippe JEAN-PIERRE

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• Type de publi. : Communication dans un congrès
• Date de publi. : 22/10/2025
• Auteurs : Bruno da Silva HenriquesBenjamin AllaertNicolas Sutton-CharaniPierre SlangenJean-Philippe Vandeborre
• Organismes : Centre for Digital Systems Ecole nationale supérieure Mines-Télécom Lille Douai Centre for Digital Systems Ecole nationale supérieure Mines-Télécom Lille Douai IMT - MINES ALES EuroMov - Digital Health in Motion Centre for Digital Systems Ecole nationale supérieure Mines-Télécom Lille Douai

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Résumé : Accurate egocentric body-pose estimation is essential for delivering immersive experiences in Virtual, Augmented, and Mixed Reality (VR/AR/MR) applications. A major challenge in this setting arises from the limited field of view provided by head-mounted cameras, which often leads to self-occlusion and poor visibility of certain body joints—particularly in the lower body. Current state-of-the-art methods typically perform pose estimation frame-by-frame in a view-aligned manner. While this is computationally efficient and performs well for visible joints, it struggles to estimate occluded joints due to the lack of contextual information. In this work, we explore the role of temporal information in improving joint estimation. We propose a lightweight model that refines pose predictions by leveraging a large temporal window. Our results show that incorporating such module improves the accuracy of joint estimation without incurring a large computation overhead.

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Fichiers liés : CBMICameraReady.pdf

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Source

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 22/10/2025
• Auteurs : Aram HayrapetyanVladimir MakarenkoArmen TumasyanWolfgang AdamLisa BenatoThomas BergauerMarko DragicevicCristina GiordanoPriya Sajid HussainManfred JeitlerNatascha KrammerAng LiDietrich LikoMark MatthewmanJochen SchieckRobert SchöfbeckMaryam ShooshtariMangesh SonawaneWolfgang WaltenbergerClaudia-Elisabeth WulzTahys JanssenHyejin KwonDaniel Ocampo HenaoThomas van LaerPierre van MechelenJas BierkensNordin BreugelmansJorgen d'HondtSoumya DansanaAlexandre de MoorMartin DelcourtFelix HeyenYanwen HongPavlo KashkoSteven LowetteInna MakarenkoDenise MüllerJuhee SongStefaan TavernierMichael TytgatGerrit Patrick van OnsemSenne van PutteDavid VanneromBugra BilinBarbara ClerbauxAloke Kumar DasIsabelle de BruynGilles de LentdeckerHugues EvardLaurent FavartParaskevas GianneiosAli KhalilzadehFakhri Alam KhanAndrea MalaraMuhammad Aamir ShahzadArchana SharmaLaurent ThomasMax Vanden BemdenCatherine Vander VeldePascal VanlaerFengwangdong ZhangMaarten de CoenDidar DoburGul GokbulutDavid MarckxKirill SkovpenAdina Maria TomaruNiels van den BosscheJan van der LindenJules VandenbroeckLiam WezenbeekHenriette Aarup PetersenSamuel BeinAnna BeneckeAgni BethaniGiacomo BrunoAlessandra CappatiJerome de Favereau de JeneretChristophe DelaereFrancisco Gameiro CasalinhoAndrea GiammancoAhmet Oguz GuzelVincent LemaitreJindrich LidrychPaul MalekPaola MastrapasquaSemra TurkcaparGilvan AlvesMapse Barroso Ferreira FilhoEduardo CoelhoCarsten HenselDiego Matos FigueiredoThales Menezes de OliveiraClemencia Mora HerreraPatricia Rebello TelesMariana SoeiroEdmilson José Tonelli ManganoteAntonio Vilela PereiraWalter Luiz Aldá JúniorHelena Brandao MalbouissonWagner CarvalhoJose ChinellatoMatheus Costa ReisEliza Melo da CostaGustavo Gil da SilveiraDilson de Jesus DamiaoSandro Fonseca de SouzaRaphael Gomes de SouzaSilas JesusTulio Laux KuhnMatheus MacedoKevin Mota AmariloLuiz MundimHelio NogimaJoao Pedro PinheiroAlberto SantoroAndre SznajderMauricio ThielFelipe Torres da Silva de AraujoCesar 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LaiDavid LangeAndrew LoeligerDaniel MarlowIsabel OjalvoJames OlsenFarrah SimpsonDavid SticklandChristopher TullySudhir MalikRicha SharmaSoumik ChandraAn GuLaszlo GutayMarc HuwilerMatthew JonesAndreas Werner JungDmitry KondratyevJingyan LiMiaoyuan LiuGiulia NegroNorbert NeumeisterGaryfallia PaspalakiStefan PiperovNihar Ranjan SahaJan-Frederik SchulteFuqiang WangAndrew WildridgeWei XieYao YaoYibo ZhongNeeti ParasharAtanu PathakElton ShumkaDarin AcostaAman AgrawalCollin ArbourTaylor CarnahanPallabi DasKarl Matthew EcklundFrank J.M GeurtsTao HuangIason KrommydasNicole LewisWei LiJiazhao LinOsvaldo Miguel ColinBrian Paul PadleyRadia RedjimiJohn RotterCarlos Vico VillalbaMeutia WulansatitiEfe YigitbasiYousen ZhangOlga Bessidskaia BylundArie BodekPawel de BarbaroRegina DeminaAran Garcia-BellidoHonor Suzanne HareOtto HindrichsNukulsinh ParmarPavel ParyginHyonsan SeoRhys TausBrandon ChiaritoJohn Paul ChouSteven Vincent ClarkSean DonnellyDivya GadkariYuri GershteinEva HalkiadakisConnor HoughtonDavid JaroslawskiAdam KobertIan LaflotteAmitabh LathJordan MartinsMaximilian Perez PradaBenjamin RandJoseph ReichertPrafulla SahaSevil SalurSteve SchnetzerSunil SomalwarRobert StoneSteffie Ann ThayilScott ThomasJay VoraDaniel AllyAndrés G DelannoySara FiorendiJesse HarrisTova HolmesAnkush Reddy KanugantiNimmitha KarunarathnaJohn LawlessLawrence LeeEmery NibigiraBrandi SkipworthStefan SpanierDevin AebiMuhammad AhmadTowsifa AkhterKonstantin AndrosovAashwin BasnetArtem BolshovOthmane BouhaliAntimo CagnottaValeria d'AmanteRicardo EusebiPatrick FlanaganJason GilmoreYumeng GuoTeruki KamonSifu LuoRyan MuellerAlexei SafonovNural AkchurinJordan DamgovYongbin FengNiramay GogateWeijie JinYelbir KazhykarimKamal LamichhaneSung Won LeeChristopher MadridAaron MankelTimo PeltolaIgor VolobouevEric AppeltYi ChenSenta GreeneAlfredo GurrolaWillard JohnsRaghav Kunnawalkam ElayavalliAndrew MeloDenis RathjensFrancesco RomeoPaul SheldonShengquan TuoJulia VelkovskaJussi ViinikainenJingyu ZhangBryan CardwellHeewon ChungBradley CoxJohn HakalaGabriela Hamilton Ilha MachadoRobert HiroskyMaria JoseAlexander LedovskoyCristina MantillaChristopher NeuClara Ramón ÁlvarezZhenyu WuSaptaparna BhattacharyaPaul Edmund KarchinAnagha AravindSunanda BanerjeeKevin BlackTulika BoseElise ChavezSridhara DasuPieter EveraertsCamilla GalloniHe HeMatthew HerndonAlain HerveCharis Kleio KorakaShivani LomteRichard LovelessAbhishikth MallampalliAbdollah MohammadiSusmita MondalTrevor NelsonGanesh ParidaLaurent PétréDeborah PinnaAlexander SavinVictor ShangVarun SharmaWesley H SmithDylan TeagueHo Fung TsoiWren VetensAbigail WardenSerguei AfanasievVadim AlexakhinYuri AndreevTagir AushevDzmitry BudkouskiRuslan ChistovMikhail DanilovTatyana DimovaAlexander ErshovSergei GninenkoIlya GorbunovAndrey GribushinAlexey KamenevVladimir KarjavineMikhail KirsanovVyacheslav KlyukhinOlga KodolovaVladimir KorenkovIurii KorsakovAleksei KozyrevNikolai KrasnikovAlexander LanevAlexander MalakhovViktor MatveevAlexander NikitenkoVladimir PalichikVictor PerelyginSergey PetrushankoOlesia RadchenkoMaria SavinaVladislav ShalaevSergey ShmatovSiarhei ShulhaYuri SkovpenKirill SlizhevskiyVitaly SmirnovOleg TeryaevIrina TlisovaAlexander ToropinNikolay VoytishinAnatoli ZarubinIlia ZhizhinLev DudkoVictor KimVictor MurzinVadim OreshkinDmitry SosnovEdouard BoosViacheslav BunichevMikhail DubininViktor SavrinAlexander Snigirev
• Organismes : Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Institut Pluridisciplinaire Hubert Curien Université de Haute-Alsace (UHA) Mulhouse - Colmar Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Centre de Calcul de l'IN2P3 Centre de Calcul de l'IN2P3 Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon

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Résumé : A hot and dense state of nuclear matter, known as the quark-gluon plasma, is created in collisions of ultrarelativistic heavy nuclei. Highly energetic quarks and gluons, collectively referred to as partons, lose energy as they travel through this matter, leading to suppressed production of particles with large transverse momenta ($p_\mathrm{T}$). Conversely, high-$p_\mathrm{T}$ particle suppression has not been seen in proton-lead collisions, raising questions regarding the minimum system size required to observe parton energy loss. Oxygen-oxygen (OO) collisions examine a region of effective system size that lies between these two extreme cases. The CMS detector at the CERN LHC has been used to quantify charged-particle production in inclusive OO collisions for the first time via measurements of the nuclear modification factor ($R_\mathrm{AA}$). The $R_\mathrm{AA}$ is derived by comparing particle production to expectations based on proton-proton (pp) data and has a value of unity in the absence of nuclear effects. The data for OO and pp collisions at a nucleon-nucleon center-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.36 TeV correspond to integrated luminosities of 6.1 nb$^{-1}$ and 1.02 pb$^{-1}$, respectively. The $R_\mathrm{AA}$ is below unity with a minimum of 0.69 $\pm$ 0.04 around $p_\mathrm{T}$ = 6 GeV. The data exhibit better agreement with theoretical models incorporating parton energy loss as compared to baseline models without energy loss.

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Source

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• Type de publi. : Communication dans un congrès
• Date de publi. : 22/10/2025
• Auteurs : Nicolas MartinPhilippe MulhemJean-Pierre Chevallet
• Organismes : Modélisation et Recherche d’Information Multimédia [Grenoble] PEEKTORIA Modélisation et Recherche d’Information Multimédia [Grenoble] Laboratoire d'Informatique de Grenoble Centre National de la Recherche Scientifique Modélisation et Recherche d’Information Multimédia [Grenoble]

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Résumé : While the Segment Anything Model (SAM) has demonstrated remarkable capabilities in general image segmentation, its direct application to medical images faces significant challenges, leading to domain-specific adaptations like MedSAM. In current medical literature, SAM-like models are often evaluated using "simulated" bounding box prompts derived from ground truth annotations, potentially overestimating their real world performance. This paper addresses this underexplored problem by systematically evaluating the influence of bounding box quality on melanoma segmentation performance using the ISIC 2018 dataset (RGB skin image corpus). Experiments were conducted on both the foundational SAM and MedSAM, utilizing a structured protocol that includes ideal bounding boxes, baseline heuristic prompts (full image, most probable location, centered point for SAM), and controlled perturbations. These perturbations comprise five levels of expanding, shrinking, and shifting the ideal bounding box (random disturbance between 5% and 25%). Our results demonstrate a significant dependence of segmentation performance on bounding box quality for both models. Depending on the type of bounding box perturbation, the Dice score decreases from 84% under ideal conditions to 37% with inaccurate bounding boxes, corresponding to a reduction of more than 50%. Notably, shrinking the bounding box has a more detrimental effect than expanding it, with accuracy dropping substantially (e.g., MedSAM's Dice score decreases from 91.5 to 60.9 under a 25% shrinkage). Moreover, medical pre-training significantly improves robustness, as MedSAM outperforms SAM by approximately 7 Dice points under ideal conditions. These findings highlight that although SAM-like models offer promising capabilities, their reliance on high-quality bounding box prompts currently limits their applicability for fully unsupervised segmentation in medical image processing pipelines. This underscores the need for either human intervention or more advanced automated prompting strategies in clinical applications.

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Fichiers liés : CBMI_2025___Bounding_box_SAM.pdf

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Source

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 21/10/2025
• Auteurs : Philippe LamyYannick BoursierJean LoiratAndrei Zhukov
• Organismes : Laboratoire Atmosphères, Milieux, Observations Spatiales Centre de Physique des Particules de Marseille Laboratoire d'Astrophysique de Marseille

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Résumé : We report on the characterization of a coronal mass ejection (CME) observed on 22 October 2003 by the LASCO-C2 and C3 coronagraphs over a time interval of 6 hours. This CME clearly appears as an asymmetric flux-rope in self-similar expansion and in spite of having a single vantage point, this relatively simple morphology and the geometry of the observations allow us to reconstruct its shape and its trajectory. The images are first processed in order to remove most of the background or foreground coronal structures (essentially streamers) which are superimposed on the CME. The analysis is based on forward modeling of an asymmetric structure where the plasma is homogeneously distributed in a thin shell and synthetic images are calculated from Thomson scattering by the electrons. They are best fitted to the images to determine the exact shape of the flux rope, and to track its evolution characterized by a radial propagation in self-similar expansion. The analysis supports the forward propagation (over the backward one) characterized by constant accelerations of 76 and 46 m/sec^2 for the front and rear parts of the CME, respectively. The respective velocities at 20 Rsun reach 2000 and 1100 km/s, and its mass unbiased by projection effects is estimated at 1.7x10^16 g. Altogether, these are quite exceptionally large values among CMEs and imply a very energetic event. No erupting event could be identified at or near the calculated initial location of the CME. It lies 25° west of the active region NOAA 10484, the site of contemporary, violent, and recurrent solar eruptions (the ``Halloween event'') and a putative connection would require a strong deflection over a very short path. Therefore, the origin of this CME remains unclear.

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• Type de publi. : Communication dans un congrès
• Date de publi. : 20/10/2025
• Auteurs : Mary de FeudisKin On HoLaura HenryVanna PuglieseBoris YavkinMarie-Pierre AdamNicolas GuignotJean-Sébastien LauretFabien J BénédicJocelyn AchardPhilippe GoldnerSerge DesgreniersJean-François Roch
• Organismes : Institut de Recherche de Chimie Paris CY Cergy Paris Université Laboratoire Lumière, Matière et Interfaces Synchrotron SOLEIL Università degli studi di Torino = University of Turin Laboratoire Lumière, Matière et Interfaces Laboratoire Lumière, Matière et Interfaces Synchrotron SOLEIL Laboratoire Lumière, Matière et Interfaces Laboratoire des Sciences des Procédés et des Matériaux Laboratoire des Sciences des Procédés et des Matériaux Institut de Recherche de Chimie Paris Laboratoire de physique des solides denses, Department of Physics, University of Ottawa Laboratoire Lumière, Matière et Interfaces

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Résumé : Diamonds and nanodiamonds (NDs) containing quantum color centers, such as nitrogen-vacancy (NV) centers, have been widely studied in recent years for their promising applications across various fields, including cryptography and telecommunications, medical sciences, and sensing. In the context of sensing, recent studies on color centers such as silicon-vacancy (SiV) and germanium-vacancy (GeV) centers have shown great potential for measuring physical quantities like magnetic fields, temperature, and strain. This is due to their intense zero-phonon line (ZPL) optical signal, which accounts for about 80% of their total luminescence and is characteristic of group-IV color centers (G4V) [1]. In our recent papers, we demonstrated that as-grown CVD NDs containing SiV and GeV centers, featuring luminescent ZPLs and excellent photostability at room temperature, can function effectively as nanosensors under high stress and pressure conditions (up to 180 GPa) [2, 3]. To advance our research, in this work we investigate the optical properties of SiV centers in as-grown NDs at cryogenic temperatures. For SiV centers, which have spin 1/2, the fine structure should become accessible through the Jahn-Teller effect, which lifts the degeneracy at cryogenic temperatures (< 20 K). However, experiments on our as-grown NDs reveal significant spectral broadening even at around 9 K, caused by lattice strain, which prevents access to the optically addressable electronic spin states of the SiV center. To overcome this limitation, we propose an original post-treatment involving high-pressure and high-temperature (HPHT) annealing using the Paris–Edinburgh press. This approach allows the gradual increase of temperature and pressure allows for control over the undesired diamond-to-graphite phase transition. HPHT annealing experiments were conducted at the PSICHE beamline of Synchrotron SOLEIL [4], where X-ray diffraction and tomography analyses enabled precise monitoring of P-T parameters and made it possible for the first time to access single fine-structure transitions of SiV centers in such NDs. References [1] C. Bradac, et al., Nat. Commun. 10, 1 (2019). [2] B. Vindolet, et al., Phys. Rev. B 106, 214109 (2022). [3] M. De Feudis, et al., Adv. Mater. Interfaces 7, 1901408 (2019). [4] L. Henry et al., J. Synchrotron Rad. 29 (2022).

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• Type de publi. : Article dans une revue
• Date de publi. : 20/10/2025
• Auteurs : Solène RenaudineauFrédéric FrappartMarc PeaucelleValentine SollierWigneron J.-P.Philippe CiaisBertrand Ygorra
• Organismes : Interactions Sol Plante Atmosphère Interactions Sol Plante Atmosphère Interactions Sol Plante Atmosphère Interactions Sol Plante Atmosphère Interactions Sol Plante Atmosphère Laboratoire des Sciences du Climat et de l'Environnement [Gif-sur-Yvette] Interactions Sol Plante Atmosphère
• Publié dans Forests le 21/10/2020

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Résumé :

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Fichiers liés : forests-16-01609-v2.pdf

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• Type de publi. : Article dans une revue
• Date de publi. : 17/10/2025
• Auteurs : Philippe BoyerJean-Pierre Butault
• Organismes : Académie d'Agriculture de France Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement
• Publié dans Economie et Statistique / Economics and Statistics le 28/10/2020

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Résumé : L'article propose une comparaison européenne de la répartition de la dépense de consommation de produits agroalimentaires en valeurs ajoutées induites dans les différentes branches, taxes et importations. Il étudie plus particulièrement le niveau de la part de l'agriculture dans cette consommation ainsi que ses déterminants. L'étude, fondée sur les calculs initiés par W. Leontief, adaptés aux données disponibles (tableaux entrées-sorties d'Eurostat), enrichit les deux approches nationales de même nature existantes : l'« euro alimentaire » en France et le « food dollar » aux États-Unis. Les résultats montrent que les pays plus importateurs et à fortes taxes se distinguent de ceux où le partage de la dépense de consommation est plus favorable aux valeurs ajoutées. Les pays se distinguent également selon la répartition de ces valeurs ajoutées entre commerce et services d'une part, agriculture et industrie agroalimentaire d'autre part. En France, relativement à d'autres pays européens, le partage de la dépense est plutôt favorable aux valeurs ajoutées, avec une part de l'agriculture proche de la moyenne.