59 research outputs found
Study of phagocytic function with a quantitative nitroblue-tetrazolium (NBT) reduction test in diabetes mellitus
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Radial variation of heat transport in L-mode JET discharges
- Author
- Abduallev S
- Abhangi M
- Abreu P
- Afzal M
- Aggarwal KM
- Agostini FD
- Ahlgren T
- Ahn JH
- Aho-Mantila L
- Aiba N
- Airila M
- Albanese R
- Aldred V
- Alegre D
- Alessi E
- Aleynikov P
- Alfier A
- Alkseev A
- Allinson M
- Alper B
- Alves E
- Ambrosino G
- Ambrosino R
- Amicucci L
- Amosov V
- Angelone M
- Anghel M
- Angioni C
- Appel L
- Appelbee C
- Arena P
- Ariola M
- Arnichand H
- Arshad S
- Asakura NN
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- Auriemma F
- Austin Y
- Avotina L
- Axton MD
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- Baciero A
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- Zhang W
- Zhou Y
- Zilli E
- Zoita V
- Zoletnik S
- Zychor I
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
In this paper, we analyze heat transport in the JET tokamak using data from its high resolution ECE diagnostic and analyses based on the transfer entropy (TE). The analysis reveals that heat transport is not smooth and continuous, but is characterized by 'trapping regions' separated by `minor transport barriers'. Meat may 'jump over' these barriers and when the heating power is raised, this 'jumping' behavior becomes more prominent. To check that our results are relevant for global heat transport, we deduced an effective diffusion coefficient from the TE results. Both its value and overall radial variation are consistent with heat diffusivities reported in literature. The detailed radial structure of the effective diffusion coefficient was shown to be linked to the mentioned minor transport barriers
Long-lived coupled peeling ballooning modes preceding ELMs on JET
- Author
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- Zhang W
- Zhou Y
- Zilli E
- Zoita V
- Zoletnik S
- Zychor I
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
In some JET discharges, type-I edge localised modes (ELMs) are preceded by a class of low-frequency oscillations (Perez et al 2004 Nucl. Fusion 44 609). While in many cases the ELM is triggered during the growth phase of this oscillation, it is also observed that this type of oscillation can saturate and last for several tens of ms until an ELM occurs. In order to identify the nature of these modes, a wide pre-ELM oscillation database, including detailed pedestal profile information, has been assembled and analysed in terms of MHD stability parameters. The existence domain of these pre-ELM oscillations and the statistical distribution of toroidal mode numbers (n) up to n = 16 have been mapped in ballooning alpha (alpha(ball)) and either edge current density (J(edge)) or pedestal collisionality (nu(ee,ped)*) coordinates and compared to linear MHD stability predictions. The pre-ELM oscillations are reliably observed when the J/alpha ratio is high enough for the pedestal to access the coupled peeling-ballooning (PB) domain (aka stability nose). Conversely, when the pedestal is found to be in or near the high-n ballooning domain (which is at low J/alpha ratio), ELMs are usually triggered promptly, i.e. with no detectable pre-ELM oscillations, or with pre-ELM oscillations only observable on ECE whose n appears to be too high to be resolved by the magnetics. Individual discharges can sometimes exhibit a fairly wide range of pre-ELM mode numbers, but for a wider database, the statistical n-number domains are found to be well ordered along the J - alpha stability boundary and behave as expected from PB theory: the higher the J/alpha ratio, the lower the mode's measured n tends to be. Within the measurement uncertainties, the measured n is usually found to be compatible with the most unstable n predicted by the linear stability code MISHKA1. These results confirm the earlier hypothesis that these modes are coupled peeling-ballooning modes, and extend and generalise to higher-mode numbers the work by Huysmans et al (1998 Nucl. Fusion 38 179), who identified the lowest n modes as pure external kink modes. Since the destabilisation of PB modes is widely accepted to give rise to ELMs, the mode saturation and delayed ELM triggering that is sometimes observed is rather unexpected. Possibilities to reconcile the extended lifetime of these modes with current ELM models are briefly discussed, but will require further investigation
Radial variation of heat transport in L-mode JET discharges
- Author
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- Abhangi M
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- Aggarwal KM
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- Wang E
- Wang N
- Warder S
- Warren RJ
- Waterhouse J
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- Weckmann A
- Weiland J
- Weisen H
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- Wellstood C
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- Whitehead BD
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- Wiechec AB
- Wiesen S
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- Wischmeier M
- Withenshaw G
- Withycombe A
- Witts DM
- Wood D
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- Wray S
- Wright J
- Wright JC
- Wu J
- Wukitch S
- Wynn A
- Xu T
- Yadikin D
- Yanling W
- Yao L
- Yavorskij V
- Yoo MG
- Young C
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- Young ID
- Young R
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- Zagorski R
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- Zanino R
- Zarins A
- Zastrow KD
- Zerbini M
- Zhang W
- Zhou Y
- Zilli E
- Zoita V
- Zoletnik S
- Zychor I
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
In this paper, we analyze heat transport in the JET tokamak using data from its high resolution ECE diagnostic and analyses based on the transfer entropy (TE). The analysis reveals that heat transport is not smooth and continuous, but is characterized by 'trapping regions' separated by `minor transport barriers'. Meat may 'jump over' these barriers and when the heating power is raised, this 'jumping' behavior becomes more prominent. To check that our results are relevant for global heat transport, we deduced an effective diffusion coefficient from the TE results. Both its value and overall radial variation are consistent with heat diffusivities reported in literature. The detailed radial structure of the effective diffusion coefficient was shown to be linked to the mentioned minor transport barriers
Long-lived coupled peeling ballooning modes preceding ELMs on JET
- Author
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- von Thun CP
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- Vondracek P
- Vora N
- Vu T
- Wakeling B
- Waldon CWF
- Walkden N
- Walker M
- Walker R
- Walsh M
- Wang E
- Wang N
- Warder S
- Warren RJ
- Waterhouse J
- Watkins NW
- Watts C
- Wauters T
- Weckmann A
- Weiland J
- Weisen H
- Weiszflog M
- Wellstood C
- West AT
- Wheatley MR
- Whetham S
- Whitehead AM
- Whitehead BD
- Widdowson AM
- Wiechec AB
- Wiesen S
- Wilkinson J
- Williams J
- Williams M
- Wilson AR
- Wilson DJ
- Wilson HR
- Wilson J
- Wischmeier M
- Withenshaw G
- Withycombe A
- Witts DM
- Wood D
- Wood R
- Woodley C
- Wray S
- Wright J
- Wright JC
- Wu J
- Wukitch S
- Wynn A
- Xu T
- Yadikin D
- Yanling W
- Yao L
- Yavorskij V
- Yoo MG
- Young C
- Young D
- Young ID
- Young R
- Zacks J
- Zagorski R
- Zaitsev FS
- Zanino R
- Zarins A
- Zastrow KD
- Zerbini M
- Zhang W
- Zhou Y
- Zilli E
- Zoita V
- Zoletnik S
- Zychor I
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
In some JET discharges, type-I edge localised modes (ELMs) are preceded by a class of low-frequency oscillations (Perez et al 2004 Nucl. Fusion 44 609). While in many cases the ELM is triggered during the growth phase of this oscillation, it is also observed that this type of oscillation can saturate and last for several tens of ms until an ELM occurs. In order to identify the nature of these modes, a wide pre-ELM oscillation database, including detailed pedestal profile information, has been assembled and analysed in terms of MHD stability parameters. The existence domain of these pre-ELM oscillations and the statistical distribution of toroidal mode numbers (n) up to n = 16 have been mapped in ballooning alpha (alpha(ball)) and either edge current density (J(edge)) or pedestal collisionality (nu(ee,ped)*) coordinates and compared to linear MHD stability predictions. The pre-ELM oscillations are reliably observed when the J/alpha ratio is high enough for the pedestal to access the coupled peeling-ballooning (PB) domain (aka stability nose). Conversely, when the pedestal is found to be in or near the high-n ballooning domain (which is at low J/alpha ratio), ELMs are usually triggered promptly, i.e. with no detectable pre-ELM oscillations, or with pre-ELM oscillations only observable on ECE whose n appears to be too high to be resolved by the magnetics. Individual discharges can sometimes exhibit a fairly wide range of pre-ELM mode numbers, but for a wider database, the statistical n-number domains are found to be well ordered along the J - alpha stability boundary and behave as expected from PB theory: the higher the J/alpha ratio, the lower the mode's measured n tends to be. Within the measurement uncertainties, the measured n is usually found to be compatible with the most unstable n predicted by the linear stability code MISHKA1. These results confirm the earlier hypothesis that these modes are coupled peeling-ballooning modes, and extend and generalise to higher-mode numbers the work by Huysmans et al (1998 Nucl. Fusion 38 179), who identified the lowest n modes as pure external kink modes. Since the destabilisation of PB modes is widely accepted to give rise to ELMs, the mode saturation and delayed ELM triggering that is sometimes observed is rather unexpected. Possibilities to reconcile the extended lifetime of these modes with current ELM models are briefly discussed, but will require further investigation
Overview of JET results
- Author
- Abel I
- Afanesyev V
- Agarici G
- Aggarwal KM
- Airila M
- Akers R
- Alarcon T
- Albanese R
- Alexeev A
- Alfier A
- Allan P
- Almaviva S
- Alonso A
- Alonso M
- Alper B
- Altmann H
- Alves D
- Ambrosino G
- Amosov V
- Anda G
- Andersson F
- Andersson-Sunden E
- Andreev V
- Andrew Y
- Angelone M
- Anghel A
- Anghel M
- Angioni C
- Apruzzese G
- Arcis N
- Arena P
- Argouarch A
- Ariola M
- Armitano A
- Armstrong R
- Arnoux G
- Arshad S
- Artaserse G
- Artaud JF
- Ash A
- Asp E
- Asunta O
- Atanasiu CV
- Atkins G
- Axton MD
- Ayres C
- Baciero A
- Bailescu V
- Baiocchi B
- Baker RA
- Balboa I
- Balorin C
- Balshaw N
- Banks JW
- Baranov YF
- Barbier D
- Barlow IL
- Barnard MA
- Barnsley R
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- Barrera L
- Baruzzo M
- Basiuk V
- Bateman G
- Batiston P
- Baumgarten N
- Baylor L
- Bazylev B
- Beaumont PS
- Beausang K
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- Beldishevski M
- Bell AC
- Belli F
- Bellinger M
- Bellizio T
- Belo PSA
- Belonohy E
- Bennett PE
- Benterman NA
- Berger-By G
- Bergsaker H
- Berk H
- Bernardo J
- Bertrand B
- Beurskens MNA
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- Bienkowska B
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- Bizarro J
- Blackman TR
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- Blum J
- Bobkov V
- Boboc A
- Boilson D
- Bolshakova I
- Bolzonella T
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- Boyer HJ
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- Bradshaw JMA
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- Vlad M
- Voitsekhovitch I
- Vrancken M
- Vulliez K
- Waldon CWF
- Walker M
- Walsh MJ
- Waterhouse J
- Watkins ML
- Watson MJ
- Wauters T
- Way MW
- Webb CR
- Weiland J
- Weisen H
- Weiszflog M
- Wenninger R
- West AT
- Weulersse JM
- Weyssow B
- Wheatley MR
- Whiteford AD
- Whitehead AM
- Whitehurst AG
- Widdowson AM
- Wieggers RC
- Wiegmann C
- Wiesen S
- Wilson A
- Wilson D
- Wilson DJ
- Wilson HR
- Wischmeier M
- Witts DM
- Wolf RC
- Wolowski J
- Woscov P
- Wright GM
- Wright J
- Xu GS
- Yavorskij V
- Yerashok V
- Yorkshades J
- Young C
- Young D
- Young ID
- Yuhong X
- Zabeo L
- Zabolotsky A
- Zaccarian L
- Zagorski R
- Zaitsev FS
- Zajac S
- Zakharov L
- Zanino R
- Zaroschi V
- Zastrow KD
- Zatz I
- Zefran B
- Zeidner W
- Zerbini M
- Zhang T
- Zhu Y
- Zilli E
- Zimmermann O
- Zoita V
- Zoletnik S
- Zwingman W
- Publication venue
- IOP PUBLISHING LTD
- Publication date
- 01/01/2011
- Field of study
Investigation of deuterium trapping and release in the JET divertor during the third ILW campaign using TDS
- Author
- Abduallev S
- Abhangi M
- Abreu P
- Afzal M
- Aggarwal KM
- Agostini FD
- Ahlgren T
- Ahn JH
- Aho-Mantila L
- Aiba N
- Airila M
- Albanese R
- Aldred V
- Alegre D
- Alessi E
- Aleynikov P
- Alfier A
- Alkseev A
- Allinson M
- Alper B
- Alves E
- Ambrosino G
- Ambrosino R
- Amicucci L
- Amosov V
- Angelone M
- Anghel M
- Angioni C
- Appel L
- Appelbee C
- Arena P
- Ariola M
- Arnichand H
- Arshad S
- Asakura NN
- Ash A
- Ashikawa N
- Aslanyan V
- Asunta O
- Auriemma F
- Austin Y
- Avotina L
- Axton MD
- Ayres C
- Ayres CF
- Bacharis M
- Baciero A
- Baiao D
- Bailey S
- Baker A
- Balboa I
- Balden M
- Balshaw N
- Bament R
- Banks JW
- Baranov YF
- Barnard MA
- Barnes D
- Barnes M
- Barnsley R
- Baron-Wiechec A
- Baruzzo M
- Basiuk V
- Bassan M
- Bastow R
- Batista A
- Batistoni P
- Baughan R
- Bauvir B
- Baylor L
- Bazylev B
- Beal J
- Beaumont PS
- Beckers M
- Beckett B
- Becoulet A
- Bekris N
- Beldishevski M
- Bell K
- Belli F
- Bellinger M
- Belonohy E
- Ben Ayed N
- Benterman NA
- Bergsaker H
- Bernardo J
- Bernert M
- Berry M
- Bertalot L
- Besliu C
- Beurskens M
- Bieg B
- Bielecki J
- Biewer T
- Bigi M
- Bilkova P
- Binda F
- Bisoffi A
- Bizarro JPS
- Bjorkas C
- Blackburn J
- Blackman K
- Blackman TR
- Blanchard P
- Blatchford P
- Bobkov V
- Boboc A
- Bodnar G
- Bogar O
- Bolshakova I
- Bolzonella T
- Bonanomi N
- Bonelli F
- Boom J
- Booth J
- Borba D
- Borodin D
- Borodkina I
- Botrugno A
- Bottereau C
- Boulting P
- Bourdelle C
- Bowden M
- Bower C
- Bowman C
- Boyce T
- Boyd C
- Boyer HJ
- Bradshaw JMA
- Braic V
- Bravanec R
- Breizman B
- Bremond S
- Brennan PD
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- Brezinsek S
- Bright MDJ
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- Brombin M
- Broslawski A
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- Calvo I
- Camenen Y
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- Cane J
- Cannas B
- Capel AJ
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- Carralero D
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- Carvalho I
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- Chankin A
- Chapman IT
- Chapman SC
- Chernyshova M
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- Ciraolo G
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- Cortes S
- Cortes SDAR
- Coster D
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- Craciunescu T
- Cramp S
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- Crisanti F
- Croci G
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- Cseh G
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- Czarnecka A
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- Dankowski J
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- Davis W
- Day C
- Day IE
- de Aguilera AM
- De Backer A
- De Bock M
- de Castro A
- de la Cal E
- de la Luna E
- De Masi G
- de Pablos JL
- de Sa WWP
- De Temmerman G
- De Tommasi G
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- Deakin K
- Deane J
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- den Harder N
- Dendy RO
- Denis J
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- Devynck P
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- Ding B
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- Doerner RP
- Donne T
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- dos Reis AP
- Doswon S
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- Doyle PT
- Drenik A
- Drewelow P
- Drews P
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- Dumortier P
- Dunai D
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- Durodie F
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- Elsmore CG
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- Esposito B
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- Esser HG
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- Evans GE
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- Fasoli A
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- Fedorczak N
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- Geiger B
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- Gervasini G
- Gethins M
- Ghani Z
- Ghate M
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- Giacalone JC
- Giacomelli L
- Gibson CS
- Giegerich T
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- Gin D
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- Giruzzi G
- Gloggler S
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- Goloborod'ko V
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- Goncalves B
- Goniche M
- Goodliffe M
- Goodyear A
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- Gosk M
- Goulding R
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- Gowland R
- Graham B
- Graham ME
- Graves JP
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- Green NR
- Greuner H
- Grierson B
- Griph FS
- Grisolia C
- Grist D
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- Grundy CN
- Grzonka J
- Guard D
- Guerard C
- Guillemaut C
- Guirlet R
- Gurl C
- Hackett LJ
- Hacquin S
- Hagar A
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- Hakola A
- Halitovs M
- Hall SJ
- Hamlyn-Harris C
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- Harrison J
- Harting D
- Hasenbeck F
- Hatano Y
- Hatch DR
- Haupt TDV
- Hawes J
- Hawkes NC
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- Haydon PW
- Hayter N
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- Heesterman PJL
- Heinola K
- Heinola K
- Hellesen C
- Hellsten T
- Helou W
- Hemming ON
- Hender TC
- Henderson M
- Henderson SS
- Henriques R
- Hepple D
- Hermon G
- Hertout P
- Hidalgo C
- Highcock EG
- Hill M
- Hillairet J
- Hillesheim J
- Hillis D
- Hizanidis K
- Hjalmarsson A
- Hobirk J
- Hodille E
- Hogben CHA
- Hogeweij GMD
- Hollingsworth A
- Hollis S
- Homfray DA
- Horacek J
- Hornung G
- Horton AR
- Horton LD
- Horvath L
- Hoshino KK
- Hotchin SP
- Hough MR
- Howarth PJ
- Hubbard A
- Huber A
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- Huddleston TM
- Hughes M
- Huijsmans GTA
- Hunter CL
- Huynh P
- Hynes AM
- Iglesias D
- Imazawa N
- Imbeaux F
- Imrisek M
- Incelli M
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- Irishkin M
- Ivanova-Stanik I
- Jachmich S
- Jacobsen AS
- Jacquet P
- Jansons J
- Jardin A
- Jarvinen A
- Jaulmes F
- Jednorog S
- Jenkins I
- Jeong C
- Jepu I
- Jepu I
- Joffrin E
- Johnson R
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- Joita L
- Jones G
- Jones TTC
- Jun DT
- Kallenbach A
- Kamiya K
- Kaniewski J
- Kantor A
- Kappatou A
- Karhunen J
- Karkinsky D
- Karnowska I
- Kaufman M
- Kaveney G
- Kazakov Y
- Kazantzidis V
- Keeling DL
- Keenan T
- Keep J
- Kempenaars M
- Kennedy C
- Kenny D
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- Kim HS
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- Kinch A
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- Kinna DJ
- Kiptily V
- Kirk A
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- Kirschner A
- Kizane G
- Klepper C
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- Kodeli I
- Kogan L
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- Kominis Y
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- Koskela T
- Koslowski HR
- Koubiti M
- Kovari M
- Kowalska-Strzeciwilk E
- Krasilnikov A
- Krasilnikov V
- Krawczyk N
- Kresina M
- Krieger K
- Krivska A
- Kruezi U
- Ksiazek I
- Kukushkin A
- Kundu A
- Kurki-Suonio T
- Kwak S
- Kwiatkowski R
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- Lahtinen A
- Laing A
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- Lennholm M
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- Weisen H
- Weiszflog M
- Wellstood C
- West AT
- Wheatley MR
- Whetham S
- Whitehead AM
- Whitehead BD
- Widdowson A
- Widdowson AM
- Wiechec AB
- Wiesen S
- Wilkinson J
- Williams J
- Williams M
- Wilson AR
- Wilson DJ
- Wilson HR
- Wilson J
- Wischmeier M
- Withenshaw G
- Withycombe A
- Witts DM
- Wood D
- Wood R
- Woodley C
- Wray S
- Wright J
- Wright JC
- Wu J
- Wukitch S
- Wynn A
- Xu T
- Yadikin D
- Yanling W
- Yao L
- Yavorskij V
- Yoo MG
- Young C
- Young D
- Young ID
- Young R
- Zacks J
- Zagorski R
- Zaitsev FS
- Zanino R
- Zarins A
- Zastrow KD
- Zerbini M
- Zhang W
- Zhou Y
- Zilli E
- Zoita V
- Zoletnik S
- Zychor I
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
Selected set of samples from JET ITER-Like Wall (JET-ILW) divertor tiles exposed in 2015-2016 has been analysed using Thermal Desorption Spectrometry (TDS). The deuterium (D) amounts obtained with TDS were compared with Nuclear Reaction Analysis (NRA). The highest amount of D was found on the top part of inner divertor which has regions with the thickest deposited layers as for divertor tiles removed in 2014. This area resides deep in the scrape-off layer and plasma configurations for the second (ILW-2, 2013-2014) and the third (ILW-3, 2015-2016) JET-ILW campaigns were similar. Agreement between TDS and NRA is good on the apron of Tile 1 and on the upper vertical region whereas on the lower vertical region of Tile 1 the NRA results are clearly smaller than the TDS results. Inner divertor Tile 3 has somewhat less D than Tiles 0 and 1, and the D amount decreases towards the lower part of the tile. The D retention at the divertor inner and outer corner regions is not symmetric as there is more D retention poloidally at the inner than at the outer divertor corner. In most cases the TDS spectra for the ILW-3 samples are different from the corresponding ILW-2 spectra because HD and D-2 release occurs at higher temperatures than from the ILW-2 samples indicating that the low energy traps have been emptied during the plasma operations and that D is either in the energetically deep traps or located deeper in the sample
Overview of the JET results
- Author
- Abel I
- Afanesyev V
- Aftanas M
- Agarici G
- Aggarwal KM
- Aho-Mantila L
- Ahonen E
- Aints M
- Airila M
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- Alarcon T
- Albanese R
- Alexeev A
- Alfier A
- Allan P
- Almaviva S
- Alonso A
- Alper B
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- Alves D
- Ambrosino G
- Amosov V
- Andersson F.
- Andreev V
- Andrew Y
- Angelone M
- Anghel A
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- Angioni C
- Apruzzese G
- Arcis N
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- Argouarch A
- Ariola M
- Armitano A
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- Arshad S
- Artaserse G
- Artaud JF
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- Asp E
- Asunta O
- Atanasiu CV
- Atkins G
- Avotina L
- Axton MD
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- Baciero A
- Bailescu V
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- Balboa I
- Balden M
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- Beaumont PS
- Beausang K
- Becoulet M
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- Hamilton DT
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- Harling JDW
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- Hawkes NC
- Hawryluk R
- Hay JH
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- Haydon PW
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- Hazel S
- Heesterman PJL
- Heidbrink W
- Heinola K
- Hellesen C
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- Hemming ON
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- Horn BA
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- Horton LD
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- Howell DF
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- Huddleston TM
- Hudson Z
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- Wilson DJ
- Wilson HR
- Wischmeier M
- Witts DM
- Wolf RC
- Wolowski J
- Woscov P
- Wright J
- Xu GS
- Yavorskij V
- Yerashok V
- Yoo M
- Yorkshades J
- Young C
- Young D
- Young ID
- Yuhong X
- Yun S
- Zabeo L
- Zabolotny W
- Zaccarian L
- Zagorski R
- Zaitsev FS
- Zakharov L
- Zanino R
- Zaroschi V
- Zastrow KD
- Zatz I
- Zefran B
- Zeidner W
- Zerbini M
- Zhang T
- Zhitlukin A
- Zhu Y
- Zimmermann O
- Zoita V
- Zoletnik S
- Zwingman W
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2011
- Field of study
Since the last IAEA Conference JET has been in operation for one year with a programmatic focus on the qualification of ITER operating scenarios, the consolidation of ITER design choices and preparation for plasma operation with the ITER-like wall presently being installed in JET. Good progress has been achieved, including stationary ELMy H-mode operation at 4.5 MA. The high confinement hybrid scenario has been extended to high triangularity, lower ρ*and to pulse lengths comparable to the resistive time. The steady-state scenario has also been extended to lower ρ*and ν*and optimized to simultaneously achieve, under stationary conditions, ITER-like values of all other relevant normalized parameters. A dedicated helium campaign has allowed key aspects of plasma control and H-mode operation for the ITER non-activated phase to be evaluated. Effective sawtooth control by fast ions has been demonstrated with3He minority ICRH, a scenario with negligible minority current drive. Edge localized mode (ELM) control studies using external n = 1 and n = 2 perturbation fields have found a resonance effect in ELM frequency for specific q95values. Complete ELM suppression has, however, not been observed, even with an edge Chirikov parameter larger than 1. Pellet ELM pacing has been demonstrated and the minimum pellet size needed to trigger an ELM has been estimated. For both natural and mitigated ELMs a broadening of the divertor ELM-wetted area with increasing ELM size has been found. In disruption studies with massive gas injection up to 50% of the thermal energy could be radiated before, and 20% during, the thermal quench. Halo currents could be reduced by 60% and, using argon/deuterium and neon/deuterium gas mixtures, runaway electron generation could be avoided. Most objectives of the ITER-like ICRH antenna have been demonstrated; matching with closely packed straps, ELM resilience, scattering matrix arc detection and operation at high power density (6.2 MW m-2) and antenna strap voltages (42 kV). Coupling measurements are in very good agreement with TOPICA modelling. \ua9 2011 IAEA, Vienna
Overview of the JET results
- Author
- Abel I
- Afanesyev V
- Aftanas M
- Agarici G
- Aggarwal KM
- Aho-Mantila L
- Ahonen E
- Aints M
- Airila M
- Akers R
- Alarcon T
- Albanese R
- Alexeev A
- Alfier A
- Allan P
- Almaviva S
- Alonso A
- Alper B
- Altmann H
- Alves D
- Ambrosino G
- Amosov V
- Andersson F.
- Andreev V
- Andrew Y
- Angelone M
- Anghel A
- Anghel M
- Angioni C
- Apruzzese G
- Arcis N
- Arena P
- Argouarch A
- Ariola M
- Armitano A
- Arnoux G
- Arshad S
- Artaserse G
- Artaud JF
- Ash A
- Asp E
- Asunta O
- Atanasiu CV
- Atkins G
- Avotina L
- Axton MD
- Ayres C
- Baciero A
- Bailescu V
- Baiocchi B
- Baker RA
- Balboa I
- Balden M
- Balorin C
- Balshaw N
- Banks JW
- Baranov YF
- Barbier D
- Barlow IL
- Barnard MA
- Barnsley R
- Barrena L
- Barrera L
- Baruzzo M
- Basiuk V
- Bateman G
- Batistoni P
- Baumgarten N
- Baylor L
- Bazylev B
- Beaumont PS
- Beausang K
- Becoulet M
- Bekris N
- Beldishevski M
- Bell AC
- Belli F
- Bellinger M
- Bellizio T
- Belo PSA
- Belonohy E
- Bennett PE
- Benterman NA
- Berger-By G
- Bergsaker H
- Berk H
- Bernardo J
- Bernert M
- Bertrand B
- Beurskens MNA
- Bieg B
- Bienkowska B
- Biewer TM
- Bigi M
- Bilkova P
- Bin W
- Bird J
- Bizarro J
- Bjorkas C
- Blackman TR
- Blanchard P
- Blanco E
- Blum J
- Bobkov V
- Boboc A
- Boilson D
- Bolshakova I
- Bolzonella T
- Boncagni L
- Bonheure G
- Bonnin X
- Borba D
- Borthwick A
- Botrugno A
- Boulbe C
- Bouquey F
- Bourdelle C
- Bowden M
- Boyce T
- Boyer HJ
- Bozhenkov A
- Brade RJ
- Bradshaw JMA
- Braet J
- Braic V
- Braithwaite GC
- Brault C
- Breizman B
- Bremond S
- Brennan PD
- Brett A
- Breue J
- Brezinsek S
- Bright MDJ
- Briscoe F
- Brix M
- Brombin M
- Brown BC
- Brown DPD
- Brzozowski J
- Bucalossi J
- Buckley MA
- Budd T
- Budny RV
- Bunting P
- Buratti P
- Burcea G
- Burckhart A
- Butcher PR
- Buttery RJ
- Cahyna P
- Calabro G
- Callaghan CP
- Caminade JP
- Camp PG
- Campling DC
- Caniello R
- Canik J
- Cannas B
- Capel AJ
- Carannante G
- Card PJ
- Cardinali A
- Carlstrom T
- Carman P
- Carralero D
- Carraro L
- Carter T
- Carvalho BB
- Carvalho I
- Carvalho P
- Casati A
- Castaldo C
- Caughman J
- Cavazzana R
- Cavinato M
- Cecconello M
- Cecil E
- Cecil FE
- Cenedese A
- Centioli C
- Cesario R
- Challis CD
- Chandler M
- Chang C
- Chankin A
- Chapman IT
- Chektybayev B
- Chernyshova M
- Child DJ
- Chiru P
- Chitarin G
- Chugonov I
- Ciric D
- Clairet F
- Clarke RH
- Clay R
- Clever M
- Coad JP
- Coates PA
- Cocilovo V
- Coda S
- Coelho R
- Coenen J
- Coffey I
- Colas L
- Cole M
- Collins S
- Combs S
- Compan J
- Conboy JE
- Conroy S
- Cook N
- Cook SP
- Cook SPH
- Coombs D
- Cooper SR
- Corre Y
- Corrigan G
- Cortes S
- Coster D
- Counsell GF
- Courtois X
- Cox M
- Craciunescu T
- Cramp S
- Crisanti F
- Croci G
- Croft O
- Crombe K
- Crowley BJ
- Cruz N
- Cseh G
- Cupido L
- Curuia M
- Cusack RA
- Czarnecka A
- Czarski T
- Dalley S
- Daly ET
- Dalziel A
- Daniel R
- Darrow D
- David O
- Davies JJ
- Davies N
- Davies W
- Day C
- Day IE
- De Angelis R
- de Arcas G
- de Baar MR
- de la Cal E
- de la Luna E
- de Pablos JL
- De Tommasi G
- de Vicente SMG
- de Vries PC
- De-Angelis R
- Degli Agostini F
- del-Castillo-Negrete D
- Delabie E
- Delpech L
- Denisov G
- Denyer AJ
- Denyer RF
- Devaux S
- Devynck P
- Di Matteo L
- Di Pace L
- Dirken PJ
- Dittmar T
- Dnestrovskiy A
- Dodt D
- Doerner R
- Doldatov S
- Dominiczak K
- Dooley P
- Dorling SE
- Douai D
- Down AP
- Doyle PT
- Drake JR
- Dreischuh T
- Drozdov V
- Dumortier P
- Dunai D
- Duran I
- Durodie F
- Dutta P
- Dux R
- Dylst K
- Eaton R
- Edlington T
- Edwards AM
- Edwards DT
- Edwards PK
- Eich T
- Ekedahl A
- Elevant T
- Ellingboe B
- Elsmore CG
- Emmoth B
- Erdei G
- Ericsson G
- Eriksson Annika
- Eriksson LG
- Esposito B
- Esser HG
- Estrada T
- Evangelidis EA
- Evans GE
- Ewart GD
- Ewers DT
- Falchetto G
- Falie D
- Fanthome JGA
- Farthing JW
- Fasoli A
- Faugeras B
- Fedorczak N
- Felton RC
- Fenzi C
- Fernades A
- Fernandes H
- Ferreira J
- Ferreira JA
- Ferron J
- Fessey JA
- Figini L
- Figueiredo A
- Figueiredo J
- Finburg P
- Finken KH
- Fischer U
- Fitzgerald N
- Flanagan J
- Fleming C
- Forbes AD
- Ford O
- Formisano A
- Fraboulet D
- Francis RJ
- Frassinetti L
- Fresa R
- Friconneau JP
- Frigione D
- Fullard K
- Fundamenski W
- Gal K
- Gao X
- Garavaglia S
- Garbet X
- Garcia J
- Gardner W
- Garibaldi P
- Garnier D
- Garzotti L
- Gaudio P
- Gauthier E
- Gaze JW
- Gear DF
- Gedney J
- Gee SJ
- Gelfusa M
- Genangeli E
- Gerasimov S
- Geraud A
- Gerbaud T
- Gherendi M
- Ghirelli N
- Giacalone JC
- Giacomelli L
- Gibson CS
- Gil C
- Gilligan SJ
- Gimblett CG
- Gin D
- Giovannozzi E
- Giroud C
- Giruzzi G
- Godwin J
- Goff JK
- Gohil P
- Gojska A
- Goloborod\u27ko V
- Goncalves B
- Goniche M
- Gonzales S
- Goodyear A
- Gorelenkov N
- Gorini G
- Goulding R
- Graham B
- Graham D
- Graham ME
- Graves J
- Green NR
- Greuner H
- Grigore E
- Griph FS
- Grisolia C
- Gros G
- Groth M
- Grunhagen S
- Gryaznevich MP
- Guirlet R
- Gunn J
- Gupta A
- Guzdar P
- Hackett LJ
- Hacquin S
- Haist B
- Hakola A
- Halitovs M
- Hall SJ
- Hamilton DT
- Han H
- Handley RC
- Harding S
- Harling JDW
- Harting D
- Harvey MJ
- Haupt TDV
- Hawkes NC
- Hawryluk R
- Hay JH
- Hayashi N
- Haydon PW
- Hayward IR
- Hazel S
- Heesterman PJL
- Heidbrink W
- Heinola K
- Hellesen C
- Hellsten T
- Hemming ON
- Hender TC
- Henderson M
- Hennion V
- Hidalgo C
- Higashijima S
- Hill JW
- Hill K
- Hill M
- Hillairet J
- Hillis D
- Hirai T
- Hitchin M
- Hobirk J
- Hogan C
- Hogben CHA
- Hogeweij GMD
- Hollingham IC
- Holyaka R
- Homfray DA
- Honeyands G
- Hong JH
- Hong SH
- Horacek J
- Horn BA
- Horton AR
- Horton LD
- Hotchin SP
- Hough MR
- Houlberg W
- Howell DF
- Huber A
- Huddleston TM
- Hudson Z
- Hughes M
- Huhnerbein M
- Hume CC
- Hunt AJ
- Hunter CL
- Hutchinson TS
- Huygen S
- Huysmans G
- Ide S
- Illescas C
- Imbeaux F
- Ivanova D
- Ivanova-Stanik I
- Ivings E
- Jachmich S
- Jackson G
- Jacquet P
- Jakubowska K
- James PV
- Janky F
- Jarvinen A
- Jednorog S
- Jenkins I
- Jennison MAC
- Jeskins C
- Joffrin E
- Johnson MF
- Johnson MG
- Johnson R
- Johnson T
- Jolovic D
- Jonauskas V
- Jones EM
- Jones G
- Jones HD
- Jones TTC
- Jouvet M
- Jun DT
- Jupen C
- Kachtchouk I
- Kaczmarczyk J
- Kallenbach A
- Kallne J
- Kalupin D
- Kalvin S
- Kamelander G
- Kamendje R
- Kamiya K
- Kappatou A
- Kasparek W
- Kasprowicz G
- Katramados I
- Kaveney G
- Kaye AS
- Kear MJ
- Keeling DL
- Kelliher D
- Kempenaars M
- Khilar P
- Khilkevich E
- Kidd NG
- Kiisk M
- Kim H
- Kim KM
- King RF
- Kinna DJ
- Kiptily V
- Kirnev G
- Kirneva N
- Kirov K
- Kirschner A
- Kisielius R
- Kislov D
- Kiss G
- Kizane G
- Klein A
- Klepper C
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- Klix A
- Knaup M
- Kneuper K
- Kneupner H
- Knight PJ
- Knipe SJ
- Kocan M
- Koch R
- Kochl F
- Kocsis G
- Koivuranta S
- Koppitz T
- Korotkov A
- Koskela T
- Koslowski HR
- Kotov V
- Kovari MD
- Kramer G
- Krasilnikov A
- Krasilnikov V
- Kraus S
- Kreter A
- Krieger K
- Kritz A
- Krivchenkov Y
- Kruezi U
- Krylov S
- Ksiazek I
- Kuhn S
- Kuhnlein W
- Kukushkin A
- Kundu A
- Kurki-Suonio Taina
- Kurowski A
- Kuteev B
- Kuyanov A
- Kwon OJ
- Kyrytsya V
- La Haye R
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- Labate C
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- Laguardia L
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- Lasa A
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- Last JR
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- Lennholm M
- Lerche E
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- Li Puma A
- Li Y
- Liang Y
- Likonen J
- Lin Y
- Lindholm V
- Linke J
- Linstead SA
- Lipshultz B
- Litaudon X
- Litvak AG
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- Lomas PJ
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- Looker DJ
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- Loughlin MJ
- Loving AB
- Lowry C
- Luce T
- Lucock RMA
- Lukanitsa A
- Lukin A
- Lungu AM
- Lungu CP
- Lyssoivan A
- Macheta P
- Mackenzie AS
- Macrae M
- Maddaluno G
- Maddison GP
- Madsen J
- Magesh B
- Maget P
- Maggi CF
- Maier H
- Mailloux J
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- Makowski M
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- Widdowson AM
- Wiegmann C
- Wiesen S
- Wilson A
- Wilson D
- Wilson DJ
- Wilson HR
- Wischmeier M
- Witts DM
- Wolf RC
- Wolowski J
- Woscov P
- Wright J
- Xu GS
- Yavorskij V
- Yerashok V
- Yoo M
- Yorkshades J
- Young C
- Young D
- Young ID
- Yuhong X
- Yun S
- Zabeo L
- Zabolotny W
- Zaccarian L
- Zagorski R
- Zaitsev FS
- Zakharov L
- Zanino R
- Zaroschi V
- Zastrow KD
- Zatz I
- Zefran B
- Zeidner W
- Zerbini M
- Zhang T
- Zhitlukin A
- Zhu Y
- Zimmermann O
- Zoita V
- Zoletnik S
- Zwingman W
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2011
- Field of study
Since the last IAEA Conference JET has been in operation for one year with a programmatic focus on the qualification of ITER operating scenarios, the consolidation of ITER design choices and preparation for plasma operation with the ITER-like wall presently being installed in JET. Good progress has been achieved, including stationary ELMy H-mode operation at 4.5 MA. The high confinement hybrid scenario has been extended to high triangularity, lower ρ*and to pulse lengths comparable to the resistive time. The steady-state scenario has also been extended to lower ρ*and ν*and optimized to simultaneously achieve, under stationary conditions, ITER-like values of all other relevant normalized parameters. A dedicated helium campaign has allowed key aspects of plasma control and H-mode operation for the ITER non-activated phase to be evaluated. Effective sawtooth control by fast ions has been demonstrated with3He minority ICRH, a scenario with negligible minority current drive. Edge localized mode (ELM) control studies using external n = 1 and n = 2 perturbation fields have found a resonance effect in ELM frequency for specific q95values. Complete ELM suppression has, however, not been observed, even with an edge Chirikov parameter larger than 1. Pellet ELM pacing has been demonstrated and the minimum pellet size needed to trigger an ELM has been estimated. For both natural and mitigated ELMs a broadening of the divertor ELM-wetted area with increasing ELM size has been found. In disruption studies with massive gas injection up to 50% of the thermal energy could be radiated before, and 20% during, the thermal quench. Halo currents could be reduced by 60% and, using argon/deuterium and neon/deuterium gas mixtures, runaway electron generation could be avoided. Most objectives of the ITER-like ICRH antenna have been demonstrated; matching with closely packed straps, ELM resilience, scattering matrix arc detection and operation at high power density (6.2 MW m-2) and antenna strap voltages (42 kV). Coupling measurements are in very good agreement with TOPICA modelling. \ua9 2011 IAEA, Vienna
Overview of the JET results
- Author
- Abel I
- Afanesyev V
- Aftanas M
- Agarici G
- Aggarwal KM
- Aho-Mantila L
- Ahonen E
- Aints M
- Airila M
- Akers R
- Alarcon T
- Albanese R
- Alexeev A
- Alfier A
- Allan P
- Almaviva S
- Alonso A
- Alper B
- Altmann H
- Alves D
- Ambrosino G
- Amosov V
- Andersson F.
- Andreev V
- Andrew Y
- Angelone M
- Anghel A
- Anghel M
- Angioni C
- Apruzzese G
- Arcis N
- Arena P
- Argouarch A
- Ariola M
- Armitano A
- Arnoux G
- Arshad S
- Artaserse G
- Artaud JF
- Ash A
- Asp E
- Asunta O
- Atanasiu CV
- Atkins G
- Avotina L
- Axton MD
- Ayres C
- Baciero A
- Bailescu V
- Baiocchi B
- Baker RA
- Balboa I
- Balden M
- Balorin C
- Balshaw N
- Banks JW
- Baranov YF
- Barbier D
- Barlow IL
- Barnard MA
- Barnsley R
- Barrena L
- Barrera L
- Baruzzo M
- Basiuk V
- Bateman G
- Batistoni P
- Baumgarten N
- Baylor L
- Bazylev B
- Beaumont PS
- Beausang K
- Becoulet M
- Bekris N
- Beldishevski M
- Bell AC
- Belli F
- Bellinger M
- Bellizio T
- Belo PSA
- Belonohy E
- Bennett PE
- Benterman NA
- Berger-By G
- Bergsaker H
- Berk H
- Bernardo J
- Bernert M
- Bertrand B
- Beurskens MNA
- Bieg B
- Bienkowska B
- Biewer TM
- Bigi M
- Bilkova P
- Bin W
- Bird J
- Bizarro J
- Bjorkas C
- Blackman TR
- Blanchard P
- Blanco E
- Blum J
- Bobkov V
- Boboc A
- Boilson D
- Bolshakova I
- Bolzonella T
- Boncagni L
- Bonheure G
- Bonnin X
- Borba D
- Borthwick A
- Botrugno A
- Boulbe C
- Bouquey F
- Bourdelle C
- Bowden M
- Boyce T
- Boyer HJ
- Bozhenkov A
- Brade RJ
- Bradshaw JMA
- Braet J
- Braic V
- Braithwaite GC
- Brault C
- Breizman B
- Bremond S
- Brennan PD
- Brett A
- Breue J
- Brezinsek S
- Bright MDJ
- Briscoe F
- Brix M
- Brombin M
- Brown BC
- Brown DPD
- Brzozowski J
- Bucalossi J
- Buckley MA
- Budd T
- Budny RV
- Bunting P
- Buratti P
- Burcea G
- Burckhart A
- Butcher PR
- Buttery RJ
- Cahyna P
- Calabro G
- Callaghan CP
- Caminade JP
- Camp PG
- Campling DC
- Caniello R
- Canik J
- Cannas B
- Capel AJ
- Carannante G
- Card PJ
- Cardinali A
- Carlstrom T
- Carman P
- Carralero D
- Carraro L
- Carter T
- Carvalho BB
- Carvalho I
- Carvalho P
- Casati A
- Castaldo C
- Caughman J
- Cavazzana R
- Cavinato M
- Cecconello M
- Cecil E
- Cecil FE
- Cenedese A
- Centioli C
- Cesario R
- Challis CD
- Chandler M
- Chang C
- Chankin A
- Chapman IT
- Chektybayev B
- Chernyshova M
- Child DJ
- Chiru P
- Chitarin G
- Chugonov I
- Ciric D
- Clairet F
- Clarke RH
- Clay R
- Clever M
- Coad JP
- Coates PA
- Cocilovo V
- Coda S
- Coelho R
- Coenen J
- Coffey I
- Colas L
- Cole M
- Collins S
- Combs S
- Compan J
- Conboy JE
- Conroy S
- Cook N
- Cook SP
- Cook SPH
- Coombs D
- Cooper SR
- Corre Y
- Corrigan G
- Cortes S
- Coster D
- Counsell GF
- Courtois X
- Cox M
- Craciunescu T
- Cramp S
- Crisanti F
- Croci G
- Croft O
- Crombe K
- Crowley BJ
- Cruz N
- Cseh G
- Cupido L
- Curuia M
- Cusack RA
- Czarnecka A
- Czarski T
- Dalley S
- Daly ET
- Dalziel A
- Daniel R
- Darrow D
- David O
- Davies JJ
- Davies N
- Davies W
- Day C
- Day IE
- De Angelis R
- de Arcas G
- de Baar MR
- de la Cal E
- de la Luna E
- de Pablos JL
- De Tommasi G
- de Vicente SMG
- de Vries PC
- De-Angelis R
- Degli Agostini F
- del-Castillo-Negrete D
- Delabie E
- Delpech L
- Denisov G
- Denyer AJ
- Denyer RF
- Devaux S
- Devynck P
- Di Matteo L
- Di Pace L
- Dirken PJ
- Dittmar T
- Dnestrovskiy A
- Dodt D
- Doerner R
- Doldatov S
- Dominiczak K
- Dooley P
- Dorling SE
- Douai D
- Down AP
- Doyle PT
- Drake JR
- Dreischuh T
- Drozdov V
- Dumortier P
- Dunai D
- Duran I
- Durodie F
- Dutta P
- Dux R
- Dylst K
- Eaton R
- Edlington T
- Edwards AM
- Edwards DT
- Edwards PK
- Eich T
- Ekedahl A
- Elevant T
- Ellingboe B
- Elsmore CG
- Emmoth B
- Erdei G
- Ericsson G
- Eriksson Annika
- Eriksson LG
- Esposito B
- Esser HG
- Estrada T
- Evangelidis EA
- Evans GE
- Ewart GD
- Ewers DT
- Falchetto G
- Falie D
- Fanthome JGA
- Farthing JW
- Fasoli A
- Faugeras B
- Fedorczak N
- Felton RC
- Fenzi C
- Fernades A
- Fernandes H
- Ferreira J
- Ferreira JA
- Ferron J
- Fessey JA
- Figini L
- Figueiredo A
- Figueiredo J
- Finburg P
- Finken KH
- Fischer U
- Fitzgerald N
- Flanagan J
- Fleming C
- Forbes AD
- Ford O
- Formisano A
- Fraboulet D
- Francis RJ
- Frassinetti L
- Fresa R
- Friconneau JP
- Frigione D
- Fullard K
- Fundamenski W
- Gal K
- Gao X
- Garavaglia S
- Garbet X
- Garcia J
- Gardner W
- Garibaldi P
- Garnier D
- Garzotti L
- Gaudio P
- Gauthier E
- Gaze JW
- Gear DF
- Gedney J
- Gee SJ
- Gelfusa M
- Genangeli E
- Gerasimov S
- Geraud A
- Gerbaud T
- Gherendi M
- Ghirelli N
- Giacalone JC
- Giacomelli L
- Gibson CS
- Gil C
- Gilligan SJ
- Gimblett CG
- Gin D
- Giovannozzi E
- Giroud C
- Giruzzi G
- Godwin J
- Goff JK
- Gohil P
- Gojska A
- Goloborod\u27ko V
- Goncalves B
- Goniche M
- Gonzales S
- Goodyear A
- Gorelenkov N
- Gorini G
- Goulding R
- Graham B
- Graham D
- Graham ME
- Graves J
- Green NR
- Greuner H
- Grigore E
- Griph FS
- Grisolia C
- Gros G
- Groth M
- Grunhagen S
- Gryaznevich MP
- Guirlet R
- Gunn J
- Gupta A
- Guzdar P
- Hackett LJ
- Hacquin S
- Haist B
- Hakola A
- Halitovs M
- Hall SJ
- Hamilton DT
- Han H
- Handley RC
- Harding S
- Harling JDW
- Harting D
- Harvey MJ
- Haupt TDV
- Hawkes NC
- Hawryluk R
- Hay JH
- Hayashi N
- Haydon PW
- Hayward IR
- Hazel S
- Heesterman PJL
- Heidbrink W
- Heinola K
- Hellesen C
- Hellsten T
- Hemming ON
- Hender TC
- Henderson M
- Hennion V
- Hidalgo C
- Higashijima S
- Hill JW
- Hill K
- Hill M
- Hillairet J
- Hillis D
- Hirai T
- Hitchin M
- Hobirk J
- Hogan C
- Hogben CHA
- Hogeweij GMD
- Hollingham IC
- Holyaka R
- Homfray DA
- Honeyands G
- Hong JH
- Hong SH
- Horacek J
- Horn BA
- Horton AR
- Horton LD
- Hotchin SP
- Hough MR
- Houlberg W
- Howell DF
- Huber A
- Huddleston TM
- Hudson Z
- Hughes M
- Huhnerbein M
- Hume CC
- Hunt AJ
- Hunter CL
- Hutchinson TS
- Huygen S
- Huysmans G
- Ide S
- Illescas C
- Imbeaux F
- Ivanova D
- Ivanova-Stanik I
- Ivings E
- Jachmich S
- Jackson G
- Jacquet P
- Jakubowska K
- James PV
- Janky F
- Jarvinen A
- Jednorog S
- Jenkins I
- Jennison MAC
- Jeskins C
- Joffrin E
- Johnson MF
- Johnson MG
- Johnson R
- Johnson T
- Jolovic D
- Jonauskas V
- Jones EM
- Jones G
- Jones HD
- Jones TTC
- Jouvet M
- Jun DT
- Jupen C
- Kachtchouk I
- Kaczmarczyk J
- Kallenbach A
- Kallne J
- Kalupin D
- Kalvin S
- Kamelander G
- Kamendje R
- Kamiya K
- Kappatou A
- Kasparek W
- Kasprowicz G
- Katramados I
- Kaveney G
- Kaye AS
- Kear MJ
- Keeling DL
- Kelliher D
- Kempenaars M
- Khilar P
- Khilkevich E
- Kidd NG
- Kiisk M
- Kim H
- Kim KM
- King RF
- Kinna DJ
- Kiptily V
- Kirnev G
- Kirneva N
- Kirov K
- Kirschner A
- Kisielius R
- Kislov D
- Kiss G
- Kizane G
- Klein A
- Klepper C
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- Klix A
- Knaup M
- Kneuper K
- Kneupner H
- Knight PJ
- Knipe SJ
- Kocan M
- Koch R
- Kochl F
- Kocsis G
- Koivuranta S
- Koppitz T
- Korotkov A
- Koskela T
- Koslowski HR
- Kotov V
- Kovari MD
- Kramer G
- Krasilnikov A
- Krasilnikov V
- Kraus S
- Kreter A
- Krieger K
- Kritz A
- Krivchenkov Y
- Kruezi U
- Krylov S
- Ksiazek I
- Kuhn S
- Kuhnlein W
- Kukushkin A
- Kundu A
- Kurki-Suonio Taina
- Kurowski A
- Kuteev B
- Kuyanov A
- Kwon OJ
- Kyrytsya V
- La Haye R
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- Labate C
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- Laguardia L
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- Lasa A
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- Last JR
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- Lennholm M
- Lerche E
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- Li Puma A
- Li Y
- Liang Y
- Likonen J
- Lin Y
- Lindholm V
- Linke J
- Linstead SA
- Lipshultz B
- Litaudon X
- Litvak AG
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- Lomas PJ
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- Looker DJ
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- Loughlin MJ
- Loving AB
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- Lucock RMA
- Lukanitsa A
- Lukin A
- Lungu AM
- Lungu CP
- Lyssoivan A
- Macheta P
- Mackenzie AS
- Macrae M
- Maddaluno G
- Maddison GP
- Madsen J
- Magesh B
- Maget P
- Maggi CF
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- Weulersse JM
- Wheatley MR
- Whiteford AD
- Whitehead AM
- Whitehurst AG
- Widdowson AM
- Wiegmann C
- Wiesen S
- Wilson A
- Wilson D
- Wilson DJ
- Wilson HR
- Wischmeier M
- Witts DM
- Wolf RC
- Wolowski J
- Woscov P
- Wright J
- Xu GS
- Yavorskij V
- Yerashok V
- Yoo M
- Yorkshades J
- Young C
- Young D
- Young ID
- Yuhong X
- Yun S
- Zabeo L
- Zabolotny W
- Zaccarian L
- Zagorski R
- Zaitsev FS
- Zakharov L
- Zanino R
- Zaroschi V
- Zastrow KD
- Zatz I
- Zefran B
- Zeidner W
- Zerbini M
- Zhang T
- Zhitlukin A
- Zhu Y
- Zimmermann O
- Zoita V
- Zoletnik S
- Zwingman W
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2011
- Field of study
Since the last IAEA Conference JET has been in operation for one year with a programmatic focus on the qualification of ITER operating scenarios, the consolidation of ITER design choices and preparation for plasma operation with the ITER-like wall presently being installed in JET. Good progress has been achieved, including stationary ELMy H-mode operation at 4.5 MA. The high confinement hybrid scenario has been extended to high triangularity, lower ρ*and to pulse lengths comparable to the resistive time. The steady-state scenario has also been extended to lower ρ*and ν*and optimized to simultaneously achieve, under stationary conditions, ITER-like values of all other relevant normalized parameters. A dedicated helium campaign has allowed key aspects of plasma control and H-mode operation for the ITER non-activated phase to be evaluated. Effective sawtooth control by fast ions has been demonstrated with3He minority ICRH, a scenario with negligible minority current drive. Edge localized mode (ELM) control studies using external n = 1 and n = 2 perturbation fields have found a resonance effect in ELM frequency for specific q95values. Complete ELM suppression has, however, not been observed, even with an edge Chirikov parameter larger than 1. Pellet ELM pacing has been demonstrated and the minimum pellet size needed to trigger an ELM has been estimated. For both natural and mitigated ELMs a broadening of the divertor ELM-wetted area with increasing ELM size has been found. In disruption studies with massive gas injection up to 50% of the thermal energy could be radiated before, and 20% during, the thermal quench. Halo currents could be reduced by 60% and, using argon/deuterium and neon/deuterium gas mixtures, runaway electron generation could be avoided. Most objectives of the ITER-like ICRH antenna have been demonstrated; matching with closely packed straps, ELM resilience, scattering matrix arc detection and operation at high power density (6.2 MW m-2) and antenna strap voltages (42 kV). Coupling measurements are in very good agreement with TOPICA modelling. \ua9 2011 IAEA, Vienna
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