Publications

2019

• The potential of electric and plasma propulsion for medium and long- term planetary exploration : research at LPP and in the Poseidon industrial chair
  
  • Bourdon Anne
  , 2019.
• Interactions of ozone and acetic acid with natural Gobi dust
  
  • Wang Xianjie
  , 2019. This PhD thesis investigates the interactions of ozone and acetic acid with a natural mineral dust from Gobi Desert in China, under room temperature, atmospheric pressure, dry and wet conditions, using post-situ and in-situ characterization techniques to address gas phase and adsorbed phase species. First, ozone uptake at the surface of Gobi dust is investigated over a large ozone concentration range (20 ppb – 10 ppm) to provide new insights on the heterogeneous processes of ozone with potential interest for both atmospheric chemistry and industrial frameworks. Gobi dust exhibits catalytic properties regarding ozone decomposition with a steady-state uptake coefficient ranging from 2.6  10-9 to 6.2  10-8 depending on ozone concentration. Water molecules compete with ozone for the same surface sites while thermal treatment at 150˚C can significantly regenerate the surface sites after surface exposure to ozone. Second, the physisorptive and chemisorptive interaction modes of acetic acid on Gobi dust have been studied evidencing the formation of molecularly adsorbed acetic acid in monomer and dimer forms as well as bidentate chelating acetate. The amount and the partition of reversibly and irreversibly adsorbed fractions of acetic acid taken up on Gobi dust exhibit contrasted behaviors under dry and 20% RH conditions. Finally, the oxidation of adsorbed acetic acid by ozone at the surface of Gobi dust is investigated to typify the ability of that geo-material to act as a catalyst of interest.
• IONOSPHERIC TOTAL ELECTRON CONTENT AT LOW LATITUDE
  
  • Hammou Ali O.
  • Zaourar Naima
  • Fleury Rolland
  • Amory-Mazaudier Christine
  , 2019.
• GNSS and Ionospheric studies
  
  • Amory-Mazaudier Christine
  , 2019.
• Nanosecond surface dielectric barrier discharge at high pressure: application for plasma-assisted combustion
  
  • Starikovskaia Svetlana
  , 2019.
• 63rd Course of the International School of Quantum Electronics
  
  • Guaitella Olivier
  • Morillo-Candas Ana-Sofia
  • Drag Cyril
  • Booth Jean-Paul
  • Klarenaar Bart
  • Engeln Richard
  • Dias Tiago
  • Ogloblina P.
  • Grofulovic Marija
  • Silva Tiago
  • Guerra V.
  , 2019.
• Reconnection and turbulence: what would bring multiscale aspects ?
  
  • Retino A.
  , 2019.
• PROSPERO and constellation missions
  
  • Retino A.
  , 2019.
• B2 thickness parameter response to Equinoctial geomagnetic storms
  
  • Migoya-Orué Yenca
  • Alazo-Cuartas K.
  • Radicella S.
  • Nava B.
  • Kashcheyev A.
  • Amory-Mazaudier Christine
  • Ezquer R.G.
  , 2019.
• Direct measurement of the two components of the spin-orbit-torque (SOT) in NiFe/Pt bilayers by an AMR-based Wheatstone bridge (Conference Presentation)
  
  • Jaffrès Henri
  • Mansour Malik
  • Jouy Augustin
  • Vissière David
  • Collin Sophie
  • George Jean-Marie
  , 2019, pp.23. (10.1117/12.2530802)
  DOI : 10.1117/12.2530802
• On Exact Laws in Incompressible Hall Magnetohydrodynamic Turbulence
  
  • Ferrand R.
  • Galtier Sebastien
  • Sahraoui F.
  • Meyrand R.
  • Andrés N.
  • Banerjee S.
  The Astrophysical Journal, American Astronomical Society, 2019, 881 (1), pp.50. (10.3847/1538-4357/ab2be9)
  DOI : 10.3847/1538-4357/ab2be9
• Cold atmospheric plasma modulates endothelial nitric oxide synthase signalling and enhances burn wound neovascularisation
  
  • Duchesne Constance
  • Banzet Sébastien
  • Lataillade Jean‐jacques
  • Rousseau Antoine
  • Frescaline Nadira
  Journal of Pathology, Wiley, 2019, 249 (3), pp.368-380. Abstract Treatment with cold atmospheric plasma (CAP) has been reported to promote wound healing in animals. However, how this process is mediated remains unclear. In this study we examined the mechanisms which underlie the improved wound healing effects of CAP and the roles of associated reactive oxygen and nitrogen species (RONS), which are generated by plasma. By using in vitro models which mimicked various steps of angiogenesis, we demonstrated that CAP triggered the production of nitric oxide (NO), and enhanced cell migration and the assembly of endothelial cells into vessel‐like structures. These are both hallmarks of the proliferative phase of wound healing. Using a mouse model of a third‐degree burn wound, we went on to show that CAP treatment was associated with enhanced angiogenesis, characterised by accelerated in vivo wound healing and increased cellular proliferation. Here, CAP significantly increased the in vivo production of endothelial NO synthase (eNOS), an enzyme that catalyses NO synthesis in endothelial cells, and significantly increased the expression of pro‐angiogenic PDGFRβ and CD31 markers in mouse wounds. Mechanistically, we showed that CAP induced eNOS phosphorylation and activation, thereby increasing the levels of endogenous NO in endothelial cells. Increased NO generation facilitated by CAP further stimulated important pro‐angiogenic VEGFA/VEGFR2 signalling in vitro . This proof‐of‐concept study may guide future efforts aimed at addressing the use of physical plasma and its therapeutic applications in a variety of pathological scenarios. © 2019 Pathological Society of Great Britain and Ireland. Published by John Wiley & Sons, Ltd. (10.1002/path.5323)
  DOI : 10.1002/path.5323
• Oxygen atom kinetics in CO₂ plasmas ignited in a DC glow discharge
  
  • S Morillo-Candas A.
  • Drag Cyril
  • Booth Jean-Paul
  • C Dias T.
  • Guerra V.
  • Guaitella Olivier
  Plasma Sources Science and Technology, IOP Publishing, 2019, 28 (7), pp.075010. Oxygen atom densities were measured in situ in a CO2 glow discharge, at pressures between 0.2 and 5 Torr (26.7?666.6 Pa). Two measurement techniques were compared, namely optical emission actinometry (using Ar as the actinometer) and high-resolution two-photon absorption laser induced fluorescence normalised to Xe, and were found to give consistent results. The variation of the atomic oxygen density with gas pressure shows two different regimes with a transition around 1 Torr. Measurements of the O atom loss frequency under plasma exposure showed that this behaviour is caused by a change in the O atom loss mechanisms, which are dominated by surface processes in our experimental conditions. The corresponding recombination probabilities on Pyrex ? O are found to vary with the gas temperature near the wall for a constant surface temperature, similarly to what has recently been obtained in pure O2. However, the measured values are more than two times lower than ? O obtained in a O2 plasma in similar conditions. The O atom densities are also compared to the dissociation fraction of CO2 determined by infra-red absorption. The obtained CO and O densities show different behaviour as a function of the energy input. The simultaneous measurement of gas temperature, electric field, O, CO and CO2 densities and O atoms loss frequency in the same conditions provides an ideal set of constraints for validating CO2 plasma kinetic models. (10.1088/1361-6595/ab2b84)
  DOI : 10.1088/1361-6595/ab2b84
• Overview of physics studies on ASDEX Upgrade
  
  • Meyer H.
  • Angioni C.
  • Albert C.G.
  • Arden N.
  • Arredondo Parra R.
  • Asunta O.
  • de Baar M.
  • Balden M.
  • Bandaru V.
  • Behler K.
  • Bergmann A.
  • Bernardo J.
  • Bernert M.
  • Biancalani A.
  • Bilato R.
  • Birkenmeier G.
  • Blanken T.C.
  • Bobkov V.
  • Bock A.
  • Bolzonella T.
  • Bortolon A.
  • Böswirth B.
  • Bottereau C.
  • Bottino A.
  • van den Brand H.
  • Brezinsek S.
  • Brida D.
  • Brochard F.
  • Bruhn C.
  • Buchanan J.
  • Buhler A.
  • Burckhart A.
  • Camenen Y.
  • Carlton D.
  • Carr M.
  • Carralero D.
  • Castaldo C.
  • Cavedon M.
  • Cazzaniga C.
  • Ceccuzzi S.
  • Challis C.
  • Chankin A.
  • Chapman S.
  • Cianfarani C.
  • Clairet F.
  • Coda S.
  • Coelho R.
  • Coenen J.W.
  • Colas L.
  • Conway G.D.
  • Costea S.
  • Coster D.P.
  • Cote T.B.
  • Creely A.
  • Croci G.
  • Cseh G.
  • Czarnecka A.
  • Cziegler I.
  • D’arcangelo O.
  • David P.
  • Day C.
  • Delogu R.
  • de Marné P.
  • Denk S.S.
  • Denner P.
  • Dibon M.
  • Di Siena A.
  • Douai D.
  • Drenik A.
  • Drube R.
  • Dunne M.
  • Duval B.P.
  • Dux R.
  • Eich T.
  • Elgeti S.
  • Engelhardt K.
  • Erdös B.
  • Erofeev I.
  • Esposito B.
  • Fable E.
  • Faitsch M.
  • Fantz U.
  • Faugel H.
  • Faust I.
  • Felici F.
  • Ferreira J.
  • Fietz S.
  • Figuereido A.
  • Fischer R.
  • Ford O.
  • Frassinetti L.
  • Freethy S.
  • Fröschle M.
  • Fuchert G.
  • Fuchs J.C.
  • Fünfgelder H.
  • Galazka K.
  • Galdon-Quiroga J.
  • Gallo A.
  • Gao Y.
  • Garavaglia S.
  • Garcia-Carrasco A.
  • Garcia-Muñoz M.
  • Geiger B.
  • Giannone L.
  • Gil L.
  • Giovannozzi E.
  • Gleason-González C.
  • Glöggler S.
  • Gobbin M.
  • Görler T.
  • Gomez Ortiz I.
  • Gonzalez Martin J.
  • Goodman T.
  • Gorini G.
  • Gradic D.
  • Gräter A.
  • Granucci G.
  • Greuner H.
  • Griener M.
  • Groth M.
  • Gude A.
  • Günter S.
  • Guimarais L.
  • Haas G.
  • Hakola A.H.
  • Ham C.
  • Happel T.
  • den Harder N.
  • Harrer G.F.
  • Harrison J.
  • Hauer V.
  • Hayward-Schneider T.
  • Hegna C.C.
  • Heinemann B.
  • Heinzel S.
  • Hellsten T.
  • Henderson S.
  • Hennequin P.
  • Herrmann A.
  • Heyn M.F.
  • Heyn E.
  • Hitzler F.
  • Hobirk J.
  • Höfler K.
  • Hölzl M.
  • Höschen T.
  • Holm J.H.
  • Hopf C.
  • Hornsby W.A.
  • Horvath L.
  • Houben A.
  • Huber A.
  • Igochine V.
  • Ilkei T.
  • Ivanova-Stanik I.
  • Jacob W.
  • Jacobsen A.S.
  • Janky F.
  • Jansen van Vuuren A.
  • Jardin A.
  • Jaulmes F.
  • Jenko F.
  • Jensen T.
  • Joffrin E.
  • Käsemann C.-P.
  • Kallenbach A.
  • Kálvin S.
  • Kantor M.
  • Kappatou A.
  • Kardaun O.
  • Karhunen J.
  • Kasilov S.
  • Kazakov Y.
  • Kernbichler W.
  • Kirk A.
  • Kjer Hansen S.
  • Klevarova V.
  • Kocsis G.
  • Leuthold N.
  • Köhn A.
  • Koubiti M.
  • Krieger K.
  • Krivska A.
  • Krämer-Flecken A.
  • Kudlacek O.
  • Kurki-Suonio T.
  • Kurzan B.
  • Labit B.
  • Lackner K.
  • Laggner F.
  • Lang P.T.
  • Lauber P.
  • Lebschy A.
  • Madsen J.
  • Li M.
  • Linder O.
  • Lipschultz B.
  • Liu F.
  • Liu Y.
  • Lohs A.
  • Lu Z.
  • Luda Di Cortemiglia T.
  • Luhmann N.C.
  • Lunsford R.
  • Lunt T.
  • Lyssoivan A.
  • Maceina T.
  • Maggiora R.
  • Maier H.
  • Maj O.
  • Mailloux J.
  • Maingi R.
  • Maljaars E.
  • Manas P.
  • Mancini A.
  • Manhard A.
  • Manso M.-E.
  • Mantica P.
  • Mantsinen M.
  • Manz P.
  • Maraschek M.
  • Martens C.
  • Martin P.
  • Marrelli L.
  • Martitsch A.
  • Mayer M.
  • Mazon D.
  • Mccarthy P.J.
  • McDermott R.
  • Meister H.
  • Medvedeva A.
  • Merkel R.
  • Merle A.
  • Mertens V.
  • Meshcheriakov D.
  • Meyer O.
  • Miettunen J.
  • Milanesio D.
  • Mink F.
  • Mlynek A.
  • Monaco F.
  • Moon C.
  • Nabais F.
  • Nemes-Czopf A.
  • Neu G.
  • Neu R.
  • Nielsen A.H.
  • Nielsen S.K.
  • Nikolaeva V.
  • Nocente M.
  • Noterdaeme J.-M.
  • Novikau I.
  • Nowak S.
  • Oberkofler M.
  • Oberparleiter M.
  • Ochoukov R.
  • Odstrcil T.
  • Olsen J.
  • Orain F.
  • Palermo F.
  • Pan O.
  • Papp G.
  • Paradela Perez I.
  • Pau A.
  • Pautasso G.
  • Prisiazhniuk D.
  • Penzel F.
  • Petersson P.
  • Pinzón Acosta J.
  • Piovesan P.
  • Piron C.
  • Pitts R.
  • Plank U.
  • Plaum B.
  • Ploeckl B.
  • Plyusnin V.
  • Pokol G.
  • Poli E.
  • Porte L.
  • Potzel S.
  • Pütterich T.
  • Ramisch M.
  • Rasmussen J.
  • Rattá G.A.
  • Ratynskaia S.
  • Raupp G.
  • Ravera G.L.
  • Réfy D.
  • Reich M.
  • Reimold F.
  • Reiser D.
  • Ribeiro T.
  • Riesch J.
  • Riedl R.
  • Rittich D.
  • Rivero-Rodriguez J.F.
  • Rocchi G.
  • Rodriguez-Ramos M.
  • Rohde V.
  • Ross A.
  • Rott M.
  • Rubel M.
  • Ryan D.
  • Ryter F.
  • Saarelma S.
  • Salewski M.
  • Salmi A.
  • Sanchis-Sanchez L.
  • Santos J.
  • Sauter O.
  • Scarabosio A.
  • Schall G.
  • Schmid K.
  • Schmitz O.
  • Schneider P.A.
  • Schrittwieser R.
  • Schubert M.
  • Schwarz-Selinger T.
  • Schweinzer J.
  • Scott B.
  • Sehmer T.
  • Seliunin E.
  • Sertoli M.
  • Shabbir A.
  • Shalpegin A.
  • Shao L.
  • Sharapov S.
  • Sias G.
  • Siccinio M.
  • Sieglin B.
  • Sigalov A.
  • Silva A.
  • Silva C.
  • Silvagni D.
  • Simon P.
  • Simpson J.
  • Smigelskis E.
  • Snicker A.
  • Sommariva C.
  • Sozzi C.
  • Spolaore M.
  • Stegmeir A.
  • Stejner M.
  • Stober J.
  • Stroth U.
  • Strumberger E.
  • Suarez G.
  • Sun H.-J.
  • Tudisco O.
  • Suttrop W.
  • Sytova E.
  • Szepesi T.
  • Tál B.
  • Tala T.
  • Tardini G.
  • Tardocchi M.
  • Teschke M.
  • Terranova D.
  • Tierens W.
  • Thorén E.
  • Told D.
  • Tolias P.
  • Treutterer W.
  • Trier E.
  • Tripský M.
  • Valisa M.
  • Valovic M.
  • Vanovac B.
  • van Vugt D.
  • Varoutis S.
  • Verdoolaege G.
  • Vianello N.
  • Vicente J.
  • Vierle T.
  • Viezzer E.
  • von Toussaint U.
  • Wagner D.
  • Wang N.
  • Wang X.
  • Weiland M.
  • White A.E.
  • Wiesen S.
  • Willensdorfer M.
  • Wiringer B.
  • Wischmeier M.
  • Wolf R.
  • Wolfrum E.
  • Xiang L.
  • Yang Q.
  • Yang Z.
  • Yu Q.
  • Zagórski R.
  • Zammuto I.
  • Zhang W.
  • van Zeeland M.
  • Zehetbauer T.
  • Zilker M.
  • Zoletnik S.
  • Zohm H.
  Nuclear Fusion, IOP Publishing, 2019, 59 (11), pp.112014. Abstract The ASDEX Upgrade (AUG) programme, jointly run with the EUROfusion MST1 task force, continues to significantly enhance the physics base of ITER and DEMO. Here, the full tungsten wall is a key asset for extrapolating to future devices. The high overall heating power, flexible heating mix and comprehensive diagnostic set allows studies ranging from mimicking the scrape-off-layer and divertor conditions of ITER and DEMO at high density to fully non-inductive operation ( q 95 = 5.5, ) at low density. Higher installed electron cyclotron resonance heating power 6 MW, new diagnostics and improved analysis techniques have further enhanced the capabilities of AUG. Stable high-density H-modes with MW m −1 with fully detached strike-points have been demonstrated. The ballooning instability close to the separatrix has been identified as a potential cause leading to the H-mode density limit and is also found to play an important role for the access to small edge-localized modes (ELMs). Density limit disruptions have been successfully avoided using a path-oriented approach to disruption handling and progress has been made in understanding the dissipation and avoidance of runaway electron beams. ELM suppression with resonant magnetic perturbations is now routinely achieved reaching transiently . This gives new insight into the field penetration physics, in particular with respect to plasma flows. Modelling agrees well with plasma response measurements and a helically localised ballooning structure observed prior to the ELM is evidence for the changed edge stability due to the magnetic perturbations. The impact of 3D perturbations on heat load patterns and fast-ion losses have been further elaborated. Progress has also been made in understanding the ELM cycle itself. Here, new fast measurements of and E r allow for inter ELM transport analysis confirming that E r is dominated by the diamagnetic term even for fast timescales. New analysis techniques allow detailed comparison of the ELM crash and are in good agreement with nonlinear MHD modelling. The observation of accelerated ions during the ELM crash can be seen as evidence for the reconnection during the ELM. As type-I ELMs (even mitigated) are likely not a viable operational regime in DEMO studies of ‘natural’ no ELM regimes have been extended. Stable I-modes up to have been characterised using -feedback. Core physics has been advanced by more detailed characterisation of the turbulence with new measurements such as the eddy tilt angle—measured for the first time—or the cross-phase angle of and fluctuations. These new data put strong constraints on gyro-kinetic turbulence modelling. In addition, carefully executed studies in different main species (H, D and He) and with different heating mixes highlight the importance of the collisional energy exchange for interpreting energy confinement. A new regime with a hollow profile now gives access to regimes mimicking aspects of burning plasma conditions and lead to nonlinear interactions of energetic particle modes despite the sub-Alfvénic beam energy. This will help to validate the fast-ion codes for predicting ITER and DEMO. (10.1088/1741-4326/ab18b8)
  DOI : 10.1088/1741-4326/ab18b8
• ${k}_{\perp }^{-8/3}$ Spectrum in Kinetic Alfvén Wave Turbulence: Implications for the Solar Wind
  
  • David Vincent
  • Galtier Sebastien
  The Astrophysical Journal Letters, Bristol : IOP Publishing, 2019, 880 (1), pp.L10. The nature of solar wind turbulence at large scale is rather well understood in the theoretical framework of magnetohydrodynamics. The situation is quite different at subproton scales where the magnetic energy spectrum measured by different spacecraft does not fit with the classical turbulence predictions: a power-law index close to −8/3 is generally reported, which is far from the predictions of strong and wave turbulence, −7/3 and −5/2, respectively. This discrepancy is considered as a major problem for solar wind turbulence. Here, we show with a nonlinear diffusion model of weak kinetic Alfvén wave turbulence where the cascade is driven by local triadic interactions that a magnetic spectrum with a power-law index of −8/3 can emerge. This scaling corresponds to a self-similar solution of the second kind with a front propagation following the law kf ∼ (t * −t) −3/4 , with t < t *. This solution appears when we relax the implicit assumption of stationarity generally made in turbulence. The agreement between the theory and observations can be interpreted as an evidence of the nonstationarity of solar wind turbulence at subproton scales. (10.3847/2041-8213/ab2fe6)
  DOI : 10.3847/2041-8213/ab2fe6
• Instability-enhanced transport in low temperature magnetized plasma
  
  • Lucken Romain
  • Bourdon A.
  • Lieberman M. A.
  • Chabert Pascal
  Physics of Plasmas, American Institute of Physics, 2019, 26, pp.070702. It is shown that the transport in low temperature, collisional, bound plasma is enhanced by instabilities at a high magnetic field. While the magnetic field confines the electrons in a stable plasma, the instability completely destroys the confinement such that the transport becomes independent of the magnetic field in the highly magnetized limit. An analytical expression of the instability-enhanced collision frequency is proposed, based on a magnetic field independent edge-to-center density ratio. (10.1063/1.5094422)
  DOI : 10.1063/1.5094422
• Pulsed nanosecond discharges and their applications
  
  • Chng Tat Loon
  • Orel Inna
  • Ding Ch
  • Shcherbanev S.A.
  • Popov N A
  • Starikovskaia Svetlana M
  , 2019. Review of nanosecond discharges in the pressure range 10 mbar-15 bar will be presented. The discharges will be classified by specific delivered energy, increasing from 0.001 eV per molecule in the moderate pressure fast ionization waves (FIWs) to 5-7 eV per molecule in high pressure filamentary nanosecond surface dielectric barrier discharges (nSDBD). Peculiarities of experimental study and peculiarities of kinetics will be underlined for each case. Potential applications of nanosecond discharges will be discussed.
• Experimental Demonstration of Multifrequency Matching for Tailored Voltage Waveform Plasma Excitation
  
  • Dine Sebastien
  • Booth Jean-Paul
  • Johnson E.V.
  • Wang Junkang
  , 2019.
• XXXIV ICPIG & ICRP-10
  
  • Guaitella Olivier
  • Morillo-Candas Ana-Sofia
  • Dias Tiago
  • Baratte Edmond
  • Ogloblina P.
  • Silva Tiago
  • Booth Jean-Paul
  • Klarenaar Bart
  • Engeln Richard
  • Guerra V.
  , 2019.
• Changing the chemical kinetic mechanism of ignition under the influence of SDBD in a rapid compression machine
  
  • Filimonova E.
  • Dobrovolskaya A.
  • Starikovskaia Svetlana
  • Bocharov A.
  • Bityurin V.
  , 2019.
• Continuous GPS network and some study results on time variation of the Equatorial Ionization Anomaly in the Southeast Asia
  
  • Le Huy Minh
  • Amory-Mazaudier Christine
  • Fleury Rolland
  • Nguyen Chien Thang
  • Le Truong Thanh
  • Nguyen Thanh Dung
  , 2019.
• Ramping up RF power and increasing pulse length in the full tungsten environment of WEST
  
  • Bourdelle C.
  • Bucalossi J.
  • Fedorczak N.
  • Loarer T.
  • Moreau E.
  • Tsitrone J.-F
  • Artaud V
  • Brezinsek S.
  • Bufferand H.
  • Colas L.
  • Corre Y.
  • Courtois X.
  • Delpech L.
  • Desgranges C.
  • Devynck P.
  • Dittmar T
  • Drenik A
  • Douai D
  • Dumont R.
  • Durodié F
  • Ekedahl A.
  • Garcia J.
  • Gaspar J
  • Gil C.
  • Goniche M.
  • Gunn J.
  • Helou W
  • Hillairet J.
  • Hennequin P
  • Klepper C C
  • Lerche E
  • Maget P.
  • Marandet Y
  • Mazon D.
  • Meyer O
  • Lombard G.
  • Manas P.
  • Mollard P.
  • Morales J.
  • Nardon E.
  • Nouailletas R.
  • Peret M
  • Peysson Y.
  • Reux C.
  • Saint-Laurent F.
  • Schwob J.-L
  • Tamain P.
  • Urbanczyk G.
  • Vartanian S
  • Vermare L
  • Vézinet D
  • Yang X
  , 2019.
• Observations on edge GAM-turbulence interactions in ASDEX Upgrade
  
  • Conway G.C
  • Palermo F.
  • Novikau I.
  • Manz P.
  • Simon P.
  • Hennequin Pascale
  • Asdex Upgrade Team The
  , 2019 (P2.1091).
• Inner versus outer ExB shear layer: an attempt to radially localize the L-H transition
  
  • Cavedon M.
  • Dux R.
  • Happel T.
  • Hennequin Pascale
  • Plank U.
  • Pütterich T.
  • Ryter F.
  • Stroth U.
  • Viezzer E.
  • Wolfrum E.
  • Asdex Upgrade Team The
  , 2019 (P5.1069).
• Turbulence driven widening of the near-SOL power width for H-mode operation in ASDEX Upgrade
  
  • Eich T.
  • Goldston R.J.
  • Manz P.
  • Hennequin Pascale
  • David P.
  • Faitsch M.
  • Kurzan B.
  • Sieglin B.
  • Wolfrum E.
  • Asdex Upgrade Team The
  • Eurofusion Mst1 Team The
  , 2019 (04.106).