Sebastijan Brezinsek

Prof. Dr. Sebastijan Brezinsek

orcid

Research Focus & Metrics

Academic Career Length

26Years (2001-Present)

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

Representative Publications

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1 June 2009 in Journal of Nuclear Materials
Verified
Journal Article
Closed access
JRJoachim Roth
Joachim Roth
ETE. Tsitrone
E. Tsitrone
ALA. Loarte
A. Loarte
TLTh. Loarer
Th. Loarer
GCG. Counsell
G. Counsell
AKA. Kukushkin
A. Kukushkin

21 August 2008 in Plasma Physics and Controlled Fusion
Verified
Journal Article
Closed access
JRJoachim Roth
Joachim Roth
ETEmmanuelle Tsitrone
Emmanuelle Tsitrone
TLThierry Loarer
Thierry Loarer
VPVolker Philipps
Volker Philipps
SBSebastijan Brezinsek
Sebastijan Brezinsek
RCRion A Causey
Rion A Causey

1 December 2011 in Physica Scripta
Verified
Journal Article
Closed access
GMG F Matthews
G F Matthews
MBM Beurskens
M Beurskens
SBSebastijan Brezinsek
Sebastijan Brezinsek
MGM Groth
M Groth
EJE Joffrin
E Joffrin
ECEfda-Jet Contributors
Efda-Jet Contributors

22 July 2013 in Nuclear Fusion
Verified
Journal Article
Closed access
PDF file
SBSebastijan Brezinsek
Sebastijan Brezinsek
TLT. Loarer
T. Loarer
VPV. Philipps
V. Philipps
HEH.G. Esser
H.G. Esser
SGS. Grünhagen
S. Grünhagen
JCJet Efda Contributors
Jet Efda Contributors
JET underwent a transformation from a full carbon-dominated tokamak to a fully metallic device with beryllium in the main chamber and a tungsten divertor. This material combination is foreseen for the activated phase of ITER. The ITER-Like Wall (ILW) experiment at JET shall demonstrate the plasma compatibility with metallic walls and the reduction in fuel retention. We report on a set of experiments (Ip = 2.0 MA, Bt = 2.0–2.4 T, δ = 0.2–0.4) in different confinement and plasma conditions with global gas balance analysis demonstrating a strong reduction in the long-term retention rate by more than a factor of 10 with respect to carbon-wall reference discharges. All experiments are executed in a series of identical plasma discharges in order to achieve maximum plasma duration until the analysis limit of the active gas handling system is reached. The composition analysis shows high purity of the recovered gas, typically 99% D. For typical L-mode discharges (Paux = 0.5 MW), type III (Paux = 5.0 MW) and type-I ELMy H-mode plasmas (Paux = 12.0 MW) a drop of the deuterium retention rate normalized to the operational time in divertor configuration is measured from 1.27 × 1021, 1.37 × 1021 and 1.97 × 1021 D s−1 down to 4.8 × 1019, 7.2 × 1019 and 16 × 1019 D s−1, respectively. The dynamic retention increases in the limiter phase in comparison with carbon-fibre composite, but also the outgassing after the discharge has risen in the same manner and overcompensates this transient retention. Overall an upper limit of the long-term retention rate of 1.5 × 1020 D s−1 is obtained with the ILW. The observed reduction by one order of magnitude confirms the expected predictions concerning the plasma-facing material change in ITER and is in line with identification of fuel co-deposition with Be as the main mechanism for the residual long-term retention. The reduction widens the operational space without active cleaning in the DT phase in comparison with a full carbon device.

1 August 2015 in Journal of Nuclear Materials
Verified
Journal Article
Open access
SBSebastijan Brezinsek
Sebastijan Brezinsek
The JET ITER-Like Wall experiment (JET-ILW) provides an ideal test bed to investigate plasma-surface interaction (PSI) and plasma operation with the ITER plasma-facing material selection employing beryllium in the main chamber and tungsten in the divertor. The main PSI processes: material erosion and migration, (b) fuel recycling and retention, (c) impurity concentration and radiation have be1en studied and compared between JET-C and JET-ILW. The current physics understanding of these key processes in the JET-ILW revealed that both interpretation of previously obtained carbon results (JET-C) and predictions to ITER need to be revisited. The impact of the first-wall material on the plasma was underestimated.Main observations are: (a) low primary erosion source in H-mode plasmas and reduction of the material migration from the main chamber to the divertor (factor7) as well as within the divertor from plasma-facing to remote areas (factor30-50). The energetic threshold for beryllium sputtering minimises the primary erosion source and inhibits multi-step re-erosion in the divertor. The physical sputtering yield of tungsten is low as 10-5 and determined by beryllium ions. (b) Reduction of the long-term fuel retention (factor10-20) in JET-ILW with respect to JET-C. The remaining retention is caused by implantation and co-deposition with beryllium and residual impurities. Outgassing has gained importance and impacts on the recycling properties of beryllium and tungsten. (c) The low effective plasma charge (Zeff=1.2) and low radiation capability of beryllium reveal the bare deuterium plasma physics. Moderate nitrogen seeding, reaching Zeff=1.6, restores in particular the confinement and the L-H threshold behaviour. ITER-compatible divertor conditions with stable semi-detachment were obtained owing to a higher density limit with ILW. Overall JET demonstrated successful plasma operation in the Be/W material combination and confirms its advantageous PSI behaviour and gives strong support to the ITER material selection

18 November 2011 in Nuclear Fusion
Verified
Journal Article
Closed access
MLM. Lehnen
M. Lehnen
AAA. Alonso
A. Alonso
GAG. Arnoux
G. Arnoux
NBN. Baumgarten
N. Baumgarten
SBS.A. Bozhenkov
S.A. Bozhenkov
MSM.F. Stamp
M.F. Stamp
Disruption mitigation is mandatory for ITER in order to reduce forces, to mitigate heat loads during the thermal quench and to avoid runaway electrons (REs). A fast disruption mitigation valve has been installed at JET to study mitigation by massive gas injection. Different gas species and amounts have been investigated with respect to timescales and mitigation efficiency. We discuss the mitigation of halo currents as well as sideways forces during vertical displacement events, the mitigation of heat loads by increased energy dissipation through radiation, the heat loads which could arise by asymmetric radiation and the suppression of REs.