Julien Guénolé

Dr. Julien Guénolé

CNRS, Université de Lorraine, Arts et Métiers ParisTech, LEM3, Metz, France
orcid

Research Focus & Metrics

Academic Career Length

17Years (2010-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 April 2020 in Computational Materials Science
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Journal Article
Open access
Julien GuénoléJulien Guénolé
Julien Guénolé
WNWolfram G. Nöhring
Wolfram G. Nöhring
AVAviral Vaid
Aviral Vaid
FHFrédéric Houllé
Frédéric Houllé
ZXZhuocheng Xie
Zhuocheng Xie
EBErik Bitzek
Erik Bitzek

26 February 2019 in Nature Communications
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YCYanhong Chang
Yanhong Chang
WLWenjun Lu
Wenjun Lu
Julien GuénoléJulien Guénolé
Julien Guénolé
LSLeigh T. Stephenson
Leigh T. Stephenson
ASAgnieszka Szczpaniak
Agnieszka Szczpaniak
BGBaptiste Gault
Baptiste Gault
Hydrogen pick-up leading to hydride formation is often observed in commercially pure Ti (CP-Ti) and Ti-based alloys prepared for microscopic observation by conventional methods, such as electro-polishing and room temperature focused ion beam (FIB) milling. Here, we demonstrate that cryogenic FIB milling can effectively prevent undesired hydrogen pick-up. Specimens of CP-Ti and a Ti dual-phase alloy (Ti-6Al-2Sn-4Zr-6Mo, Ti6246, in wt.%) were prepared using a xenon-plasma FIB microscope equipped with a cryogenic stage reaching −135 °C. Transmission electron microscopy (TEM), selected area electron diffraction, and scanning TEM indicated no hydride formation in cryo-milled CP-Ti lamellae. Atom probe tomography further demonstrated that cryo-FIB significantly reduces hydrogen levels within the Ti6246 matrix compared with conventional methods. Supported by molecular dynamics simulations, we show that significantly lowering the thermal activation for H diffusion inhibits undesired environmental hydrogen pick-up during preparation and prevents pre-charged hydrogen from diffusing out of the sample, allowing for hydrogen embrittlement mechanisms of Ti-based alloys to be investigated at the nanoscale.

1 June 2015 in Acta Materialia
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Journal Article
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Aruna PrakashAruna Prakash
Aruna Prakash
Julien GuénoléJulien Guénolé
Julien Guénolé
JWJ. Wang
J. Wang
JMJ. Müller
J. Müller
ESE. Spiecker
E. Spiecker
EBErik Bitzek
Erik Bitzek

1 June 2019 in Scripta Materialia
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Journal Article
Closed access
Julien GuénoléJulien Guénolé
Julien Guénolé
FMFatim-Zahra Mouhib
Fatim-Zahra Mouhib
LHLiam Huber
Liam Huber
BGBlazej Grabowski
Blazej Grabowski
SKSandra Korte-Kerzel
Sandra Korte-Kerzel

12 May 2020 in Nature Communications
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SLSubin Lee
Subin Lee
AVAviral Vaid
Aviral Vaid
JIJiseong Im
Jiseong Im
BKBongsoo Kim
Bongsoo Kim
Aruna PrakashAruna Prakash
Aruna Prakash
SOSang Ho Oh
Sang Ho Oh
The elastic-to-plastic transition during the deformation of a dislocation-free nanoscale volume is accompanied by displacement bursts associated with dislocation nucleation. The dislocations that nucleate during the so-called “pop-in” burst take the form of prismatic dislocation loops (PDLs) and exhibit characteristic burst-like emission and plastic recovery. Here, we report the in-situ transmission electron microscopy (TEM) observation of the initial plasticity ensued by burst-like emission of PDLs on nanoindentation of dislocation-free Au nanowires. The in-situ TEM nanoindentation showed that the nucleation and subsequent cross slip of shear loop(s) are the rate-limiting steps. As the indentation size increases, the cross slip of shear loop becomes favored, resulting in a transition from PDLs to open half-loops to helical dislocations. In the present case of nanoindentation of dislocation-free volumes, the PDLs glide out of the indentation stress field while spreading the plastic zone, as opposed to the underlying assumption of the Nix-Gao model.

8 January 2013 in Journal of Physics: Condensed Matter
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LPL Pizzagalli
L Pizzagalli
JGJ Godet
J Godet
Julien GuénoléJulien Guénolé
Julien Guénolé
SBS Brochard
S Brochard
EHE Holmstrom
E Holmstrom
TAT Albaret
T Albaret
A new parametrization of the widely used Stillinger-Weber potential is proposed for silicon, allowing for an improved modelling of defects and plasticity-related properties. The performance of the new potential is compared to the original version, as well as to another parametrization (Vink et al 2001 J. Non-Cryst. Solids, 282 248), in the case of several situations: point defects and dislocation core stability, threshold displacement energies, bulk shear, generalized stacking fault energy surfaces, fracture, melting temperature, amorphous structure, and crystalline phase stability. A significant improvement is obtained in the case of dislocation cores, bulk behaviour under high shear stress, the amorphous structure, and computation of threshold displacement energies, while most of the features of the original version (elastic constants, point defects) are retained. However, despite a slight improvement, a complex process like fracture remains difficult to model.