18 research outputs found
Effectiveness of the Live Births Information System in the Far-Western Brazilian Amazon
- Author
- Almeida M
- Barbosa L
- Cláudio Romero Farias Marinho
- Costa JMB da S
- Ferreira JSA
- Frias PG
- Guimarães EAA
- Jamille Gregório Dombrowski
- Luquetti DV
- Mascarenhas MDM
- Mello Jorge MHP
- Mello Jorge MHP
- Nhoncanse GC
- Paes NA
- Paiva NS
- Paola Marchesini
- Pedraza DF
- Predebon KM
- Ricardo Ataíde
- Rodrigo Medeiros de Souza
- Romero DE
- Silva CF
- Silva GF
- Silveira MF
- Theme Filha MM
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Visual illusion and line bisection: a bias hypothesis revisited
- Author
- AE Wilson
- AW Pressey
- D Bowers
- DJ Scarisbrick
- DS Geldmacher
- E Bisiach
- F Mancini
- F Mancini
- G Rizzolatti
- G Vallar
- J Chewning
- J Predebon
- J Predebon
- JB Mattingley
- JL Bradshaw
- JL Kashmere
- JM Baldwin
- KM Heilman
- ME Mundy
- MN Toba
- P Bartolomeo
- P Nichelli
- PA Shelton
- PW Halligan
- PW Halligan
- PW Halligan
- PW Halligan
- R Daini
- R Ricci
- RW Gardner
- S Chieffi
- S Chieffi
- S Chieffi
- S Chieffi
- S Chieffi
- S Coren
- S Savazzi
- S Suzuki
- Sergio Chieffi
- T Ro
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Pré-natal em mulheres usuárias do Sistema Único de Saúde em duas maternidades no Estado do Rio de Janeiro, Brasil: a cor importa?
- Author
- Andersen RM
- Andreucci CB
- Bailey SR
- Bairros FS
- Bassani DG
- Bernardes AC
- Bhutta ZA
- Chor D
- Dias-da-Costa JS
- Domingues RM
- Feijen-de Jong EI
- Fonseca SC
- Friche AA
- Gama SGN
- Kassar SB
- Katia Silveira da Silva
- Kotelchuck M
- Laurenti R
- Leal MC
- Leal MC
- Leite RM
- Matijasevich A
- Moraes AP
- Moubarac J
- Pacheco AJ
- Pauline Lorena Kale
- Predebon KM
- Sandra Costa Fonseca
- Victora CG
- Victora CG
- Viellas EF
- Wehby GL
- Woodhouse C
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Role of fast ion pressure in the isotope effect in JET L-mode plasmas
- Author
- Abduallev S
- Abhangi M
- Abreu P
- Afanasev V
- Afzal M
- Aggarwal KM
- Ahlgren T
- Aho-Mantila L
- Aiba N
- Airila M
- Alarcon T
- Albanese R
- Alegre D
- Aleiferis S
- Alessi E
- Aleynikov P
- Alkseev A
- Allinson M
- Alper B
- Alves E
- Ambrosino G
- Ambrosino R
- Amosov V
- Andrews R
- Angelone M
- Anghel M
- Angioni C
- Appel L
- Appelbee C
- Arena P
- Ariola M
- Arshad S
- Artaud J
- Arter W
- Asakura NN
- Ash A
- Ashikawa N
- Aslanyan V
- Asunta O
- Asztalos O
- Auriemma F
- Austin Y
- Avotina L
- Axton M
- Ayres C
- Baciero A
- Baiao D
- Balboa I
- Balden M
- Balshaw N
- Bandaru VK
- Banks J
- Baranov YF
- Barcellona C
- Barnard T
- Barnes M
- Barnsley R
- Baruzzo M
- Basiuk V
- Bassan M
- Bastow R
- Batista A
- Batistoni P
- Baumane L
- Bauvir B
- Baylor L
- Beaumont PS
- Beckers M
- Beckett B
- Bekris N
- Beldishevski M
- Bell K
- Belli F
- Belonohy E
- Benayas J
- Bergsaker H
- Bernardo J
- Bernert M
- Berry M
- Bertalot L
- Besiliu C
- Betar H
- Beurskens M
- Bielecki J
- Biewer T
- Bilato R
- Biletskyi O
- Bilkova P
- Binda F
- Birkenmeier G
- Bizarro JPS
- Bjorkas C
- Blackburn J
- Blackman TR
- Blanchard P
- Blatchford P
- Bobkov V
- Boboc A
- Bogar O
- Bohm P
- Bohm T
- Bolshakova I
- Bolzonella T
- Bonanomi N
- Bonanomi N
- Boncagni L
- Bonfiglio D
- Bonnin X
- Boom J
- Borba D
- Borodin D
- Borodkina I
- Boulbe C
- Bourdelle C
- Bowden M
- Bowman C
- Boyce T
- Boyer H
- Bradnam SC
- Braic V
- Bravanec R
- Breizman B
- Brennan D
- Breton S
- Brett A
- Brezinsek S
- Bright M
- Brix M
- Broeckx W
- Brombin M
- Broslawski A
- Brown B
- Brunetti D
- Bruno E
- Buch J
- Buchanan J
- Buckingham R
- Buckley M
- Bucolo M
- Budny R
- Bufferand H
- Buller S
- Bunting P
- Buratti P
- Burckhart A
- Burroughes G
- Buscarino A
- Busse A
- Butcher D
- Butler B
- Bykov I
- Cahyna P
- Calabro G
- Calacci L
- Callaghan D
- Callaghan J
- Calvo I
- Camenen Y
- Camp P
- Campling DC
- Cannas B
- Capat A
- Carcangiu S
- Card P
- Cardinali A
- Carman P
- Carnevale D
- Carr M
- Carralero D
- Carraro L
- Carvalho BB
- Carvalho DD
- Carvalho I
- Carvalho P
- Casiraghi I
- Casson FJ
- Castaldo C
- Catarino N
- Causa F
- Cavazzana R
- Cave-Ayland K
- Cavedon M
- Cecconello M
- Ceccuzzi S
- Cecil E
- Challis C
- Challis CD
- Chandra D
- Chang CS
- Chankin A
- Chapman B
- Chapman IT
- Chapman SC
- Chernyshova M
- Chiariello A
- Chitarin G
- Chmielewski P
- Chone L
- Cippo EP
- Ciraolo G
- Ciric D
- Citrin J
- Clairet F
- Clark E
- Clark M
- Clarkson R
- Clay R
- Clements C
- Coad JP
- Coates P
- Cobalt A
- Coccorese V
- Cocilovo V
- Coelho R
- Coenen JW
- Coffey I
- Colas L
- Colling B
- Collins S
- Conka D
- Conroy S
- Conway N
- Coombs D
- Cooper SR
- Corradino C
- Corre Y
- Corrigan G
- Cortes SDAR
- Coster D
- Craciunescu T
- Cramp S
- Crapper C
- Crisanti F
- Croci G
- Croft D
- Crombe K
- Cruz N
- Cseh G
- Cufar A
- Cullen A
- Curson P
- Curuia M
- Czarnecka A
- Czarski T
- Cziegler I
- Dabirikhah H
- Dal Molin A
- Dalgliesh P
- Dalley S
- Dankowski J
- Darrow D
- David P
- Davies A
- Davis W
- Dawson K
- Day C
- Day I
- de Aguilera AM
- De Bock M
- de Castro A
- De Dominici G
- de la Cal E
- de la Luna E
- De Masi G
- de Sa WP
- De Temmerman G
- De Tommasi G
- de Vries P
- Deane J
- Dejarnac R
- Del Sarto D
- Delabie E
- Delabie E
- Demerdzhiev V
- Dempsey A
- den Harder N
- Dendy RO
- Denis J
- Denner P
- Devaux S
- Devynck P
- Di Maio F
- Di Siena A
- Di Troia C
- Diaz FP
- Dickinson D
- Dinca P
- Dittmar T
- Dobrashian J
- Doerk H
- Doerner RP
- Domptail F
- Donne T
- Dorling SE
- dos Reis AP
- Douai D
- Dowson S
- Drenik A
- Dreval M
- Drewelow P
- Drews P
- Duckworth P
- Dumont R
- Dumortier P
- Dunai D
- Dunne M
- Duran I
- Durodie F
- Dutta P
- Duval BP
- Dux R
- Dylst K
- Edappala PV
- Edwards AM
- Edwards JS
- Eich T
- Eidietis N
- Eksaeva A
- Ellis R
- Ellwood G
- Elsmore C
- Emery S
- Enachescu M
- Ericsson G
- Eriksson F
- Eriksson J
- Eriksson LG
- Ertmer S
- Esquembri S
- Esquisabel AL
- Esser HG
- Ewart G
- Fable E
- Fable E
- Fagan D
- Faitsch M
- Falie D
- Fanni A
- Farahani A
- Fasoli A
- Faugeras B
- Fazinic S
- Felici F
- Felton RC
- Feng S
- Fernades A
- Fernandes H
- Fernandez DZ
- Ferreira DR
- Ferreira J
- Ferro G
- Fessey JA
- Ficker O
- Field A
- Fietz S
- Figini L
- Figueiredo A
- Figueiredo J
- Fil N
- Finburg P
- Fischer U
- Fittill L
- Fitzgerald M
- Flammini D
- Flanagan J
- Flinders K
- Foley S
- Fonnesu N
- Fontdecaba JM
- Formisano A
- Forsythe L
- Fortuna L
- Fransson E
- Frasca M
- Frassinetti L
- Freisinger M
- Fresa R
- Fridstrom R
- Frigione D
- Fuchs V
- Fusco V
- Futatani S
- Gal K
- Galassi D
- Galazka K
- Galeani S
- Gallart D
- Gallart D
- Galvao R
- Gao Y
- Garcia J
- Garcia-Carrasco A
- Garcia-Munoz M
- Gardener M
- Garzotti L
- Gaspar J
- Gaudio P
- Gear D
- Gebhart T
- Gee S
- Geiger B
- Gelfusa M
- George R
- Gerasimov S
- Gervasini G
- Gethins M
- Ghani Z
- Ghate M
- Gherendi M
- Ghezzi F
- Giacalone JC
- Giacomelli L
- Giacometti G
- Gibson K
- Giegerich T
- Gil L
- Gilbert MR
- Gin D
- Giovannozzi E
- Giroud C
- Giroud C
- Gloggler S
- Goff J
- Gohil P
- Goloborod'ko V
- Gomes R
- Goncalves B
- Goniche M
- Goodyear A
- Gorini G
- Gorler T
- Goulding R
- Goussarov A
- Graham B
- Graves JP
- Greuner H
- Grierson B
- Griffiths J
- Griph S
- Grist D
- Groth M
- Grove R
- Gruca M
- Guard D
- Guerard C
- Guillemaut C
- Guirlet R
- Gulati S
- Gurl C
- Gutierrez-Milla A
- Hackett L
- Hacquin S
- Hager R
- Hakola A
- Halitovs M
- Hall S
- Hallworth-Cook S
- Ham C
- Hamed M
- Hamilton N
- Hamlyn-Harris C
- Hammond K
- Hancu G
- Harrison J
- Harting D
- Hasenbeck F
- Hatano Y
- Hatch DR
- Haupt T
- Hawes J
- Hawkes NC
- Hawkins J
- Hawkins P
- Hazel S
- Heesterman P
- Heinola K
- Hellesen C
- Hellsten T
- Helou W
- Hemming O
- Hender TC
- Henderson M
- Henderson SS
- Henriques R
- Hepple D
- Herfindal J
- Hermon G
- Hidalgo C
- Higginson W
- Highcock EG
- Hillesheim J
- Hillis D
- Hizanidis K
- Hjalmarsson A
- Ho A
- Hobirk J
- Hogben CHA
- Hogeweij GMD
- Hollingsworth A
- Hollis S
- Holzl M
- Honore JJ
- Hook M
- Hopley D
- Horacek J
- Hornung G
- Horton A
- Horton LD
- Horvath L
- Hoshino KK
- Hotchin SP
- Howell R
- Hubbard A
- Huber A
- Huber V
- Huddleston TM
- Hughes J
- Hughes M
- Huijsmans GTA
- Huynh P
- Hynes A
- Igaune I
- Iglesias D
- Imazawa N
- Imrisek M
- Incelli M
- Innocente P
- Ivanova-Stanik I
- Ivings E
- Jachmich S
- Jackson A
- Jackson T
- Jacquet P
- Jansons J
- Jaulmes F
- Jednorog S
- Jenkins I
- Jepu I
- Johnson R
- Johnson T
- Johnston J
- Joita L
- Joly J
- Jonasson E
- Jones C
- Jones G
- Jones L
- Jones N
- Jones T
- Jun DT
- Juvonen M
- Kallenbach A
- Kalsey M
- Kaltiaisenaho T
- Kamiya K
- Kaniewski J
- Kantor A
- Kappatou A
- Karhunen J
- Karkinsky D
- Kaufman M
- Kaveney G
- Kazakov Y
- Kazantzidis V
- Keeling DL
- Keenan FP
- Kempenaars M
- Kent J
- Kent O
- Keogh K
- Khilkevich E
- Kim HT
- Kim HT
- King D
- King R
- Kinna DJ
- Kiptily V
- Kirk A
- Kirov K
- Kirschner A
- Kizane G
- Klas M
- Klepper C
- Klix A
- Knight M
- Knight P
- Knipe S
- Knott S
- Kobuchi T
- Kochl F
- Kocsis G
- Kodeli I
- Koechl F
- Kogut D
- Koivuranta S
- Kolesnichenko Y
- Kollo Z
- Kominis Y
- Koppen M
- Korolczuk S
- Kos B
- Koslowski HR
- Kotschenreuther M
- Koubiti M
- Kovaldins R
- Kovanda O
- 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
- Kwon OJ
- Laguardia L
- Lahtinen A
- Laing A
- Lalousis P
- Lam N
- Lamb C
- Lambertz HT
- Lang PT
- Lanthaler S
- Laszynska E
- Lawless R
- Lawson KD
- Lazaros A
- Lazzaro E
- Leach R
- Learoyd G
- Leerink S
- Lefebvre X
- Leggate HJ
- Lehmann J
- Lehnen M
- Leichauer P
- Leichtle D
- Leipold F
- Lengar I
- Lennholm M
- Lepiavko B
- Leppanen J
- Lerche E
- Lerche E
- Lescinskis A
- Lescinskis B
- Lesnoj S
- Leyland M
- Leysen W
- Li L
- Li Y
- Liang Y
- Likonen J
- Linke J
- Linsmeier C
- Lipschultz B
- Litaudon X
- Liu G
- Lloyd B
- Lo Schiavo VP
- Loarer T
- Loarte A
- Lomanowski B
- Lomas P
- Lomas PJ
- Lonnroth J
- Lopez JM
- Lorenzini R
- Losada U
- Loughlin M
- Lowry C
- Luce T
- Lucock R
- Lukin A
- Luna C
- Lungaroni M
- Lungu CP
- Lungu M
- Lunniss A
- Lunt T
- Lupelli I
- Lutsenko V
- Lyssoivan A
- Macheta P
- Macusova E
- Magesh B
- Maggi C
- Maggiora R
- Mahesan S
- Maier H
- Mailloux J
- Maingi R
- Makwana R
- Malaquias A
- Malinowski K
- Malizia A
- Manas P
- Manduchi G
- Manso ME
- Mantica P
- Mantica P
- Mantsinen M
- Manzanares A
- Maquet P
- Marandet Y
- Marcenko N
- Marchetto C
- Marchuk O
- Marconato N
- Mariani A
- Marin M
- Marinelli M
- Marinucci M
- Markovic T
- Marocco D
- Marot L
- Marsh J
- Martin A
- Martin-Solis JR
- Martone R
- Martynova Y
- Maruyama S
- Maslov M
- Matejcik S
- Mattei M
- Matthews GF
- Matveev D
- Matveeva E
- Mauriya A
- Maviglia F
- May-Smith T
- Mayer M
- Mayoral ML
- Mazon D
- Mazzotta C
- McAdams R
- McCarthy PJ
- McClements KG
- McCormack O
- McCullen PA
- McDonald D
- McHardy M
- McKean R
- McKehon J
- McNamee L
- Meadowcroft C
- Meakins A
- Medley S
- Meigh S
- Meigs AG
- Meisl G
- Meiter S
- Meitner S
- Meneses L
- Menmuir S
- Menmuir S
- Mergia K
- Merle A
- Merriman P
- Mertens P
- Meshchaninov S
- Messiaen A
- Meyer H
- Michling R
- Milanesio D
- Militello F
- Militello-Asp E
- Milocco A
- Miloshevsky G
- Mink F
- Minucci S
- Miron I
- Mistry S
- Miyoshi Y
- Mlynar J
- Moiseenko V
- Monaghan P
- Monakhov I
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- Mooney R
- Moradi S
- Morales J
- Moran J
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- Moreira L
- Moro F
- Morris J
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- Mosher S
- Moulton D
- Mrowetz T
- Muir A
- Muraglia M
- Murari A
- Muraro A
- Murphy S
- Muscat P
- Muthusonai N
- Myers C
- N'Konga B
- Nabais F
- Naish J
- Naish R
- Nakano T
- Napoli F
- Nardon E
- Naulin V
- Nave MFF
- Nedzelskiy I
- Nemtsev G
- Nesenevich V
- Nespoli F
- Neto A
- Neto EL
- Neu R
- Neverov VS
- Newman M
- Ng S
- Nicassio M
- Nielsen AH
- Nina D
- Nishijima D
- Noble C
- Nobs CR
- Nocente M
- Nodwell D
- Nordlund K
- Nordman H
- Normanton R
- Noterdaeme JM
- Nowak S
- Nunes I
- O'Gorman T
- O'Mullane M
- Oberkofler M
- Oberparleiter M
- Odupitan T
- Ogawa MT
- Okabayashi M
- Olivares PV
- Oliver H
- Olney R
- Omoregie L
- Ongena J
- Orsitto F
- Orszagh J
- Orte LB
- Osborne T
- Otin R
- Owen A
- Owen T
- Paccagnella R
- Packer LW
- Pajuste E
- Pamela S
- Panja S
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- Parail V
- Pardanaud C
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- Parsons M
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- Pasqualotto R
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- Patten H
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- Pautasso G
- Pavlichenko R
- Pavone A
- Pawelec E
- Peackoc A
- Pehkonen SP
- Peluso E
- Penot C
- Penzo J
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- Pericoli V
- Peruzzo S
- Peterka M
- Petersson P
- Petravich G
- Petre A
- Petrzilka V
- Philipps V
- Pigatto L
- Pillon M
- Pinches S
- Pintsuk G
- Piovesan P
- Piron C
- Piron L
- Pironti A
- Pisano F
- Pitts R
- Plyusnin V
- Poli FM
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- Pompilian OG
- Pool P
- Popovichev S
- Poradzinski M
- Porfiri MT
- Porosnicu C
- Porton M
- Possnert G
- Potzel S
- Poulipoulis G
- Powell T
- Prajapati V
- Prakash R
- Predebon I
- Prestopino G
- Price D
- Price M
- Price R
- Primetzhofer D
- Prior P
- Pucella G
- Puglia P
- Puiatti ME
- Purahoo K
- Pusztai I
- Putterich T
- Rachlew E
- Rack M
- Ragona R
- Rainford M
- Raj P
- Rakha A
- Ramogida G
- Ranjan S
- Rapson CJ
- Rasmussen D
- Rasmussen JJ
- Rathod K
- Ratta G
- Ratynskaia S
- Ravera G
- Rebai M
- Reed A
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- Regana J
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- Reimold F
- Reinhart M
- Reinke M
- Reiser D
- Rendell D
- Reux C
- Reynolds S
- Ricci D
- Richiusa M
- Rigamonti D
- Rimini FG
- Rinati GV
- Risner J
- Riva M
- Rivero-Rodriguez J
- Roach C
- Robins R
- Robinson S
- Robson D
- Rodionov R
- Rodrigues P
- Rodriguez J
- Rohde V
- Romanelli F
- Romanelli M
- Romanelli S
- Romazanov J
- Rowe S
- Rubel M
- Rubinacci G
- Rubino G
- Ruchko L
- Ruset C
- Rzadkiewicz J
- Saarelma S
- Sabot R
- Saez X
- Safi E
- Sahlberg A
- Saibene G
- Saleem M
- Salewski M
- Salmi A
- Salmon R
- Salzedas F
- Samm U
- Sandiford D
- Santa P
- Santala MIK
- Santos B
- Santucci A
- Sartori F
- Sartori R
- Sauter O
- Scannell R
- Schluck F
- Schlummer T
- Schmid K
- Schmuck S
- Schopf K
- Schweinzer J
- Schworer D
- Scott SD
- Sergienko G
- Sertoli M
- Shabbir A
- Sharapov SE
- Shaw A
- Sheikh H
- Shepherd A
- Shevelev A
- Shiraki D
- Shumack A
- Sias G
- Sibbald M
- Sieglin B
- Silburn S
- Silva A
- Silva C
- Silva J
- Silvagni D
- Simmons P
- Simpson J
- Sinha A
- Sipila SK
- Sips ACC
- Siren P
- Sirinelli A
- Sjostrand H
- Skiba M
- Skilton R
- Skvara V
- Slade B
- Smith P
- Smith R
- Smith SF
- Snoj L
- Soare S
- Solano ER
- Soldan CP
- Somers A
- Sommariva C
- Sonato P
- Sos M
- Sousa J
- Sozzi C
- Spagnolo S
- Sparapani P
- Spelzini T
- Spineanu F
- Sprada D
- Sridhar S
- Stables G
- Staebler GM
- Stallard J
- Stamatelatos I
- Stamp MF
- Stan-Sion C
- Stancar Z
- Staniec P
- Stankunas G
- Stano M
- Stavrou C
- Stefanikova E
- Stepanov I
- Stephen AV
- Stephen M
- Stephens J
- Stevens B
- Stober J
- Stokes C
- Strachan J
- Strand P
- Strauss HR
- Strom P
- Studholme W
- Subba F
- Suchkov E
- Summers HP
- Sun H
- Sunden EA
- Sutton N
- Suzuki TT
- Svensson J
- Sytnykov D
- Szabolics T
- Szepesi G
- Tabares F
- Tadic T
- Tal B
- Tala T
- Taliercio C
- Tallargio A
- Tanaka K
- Tang W
- Tardocchi M
- Tatali R
- Taylor D
- Taylor D
- Tegnered D
- Telesca G
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- Weiland M
- Weisen H
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- Whittaker D
- Widdowson AM
- Wiechec AB
- Wiesen S
- Wilkie G
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- Willoughby D
- Wilson HR
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- Wilson J
- Wischmeier M
- Withycombe A
- Witts D
- Wolfrum E
- Wood R
- Woodley C
- Woodley R
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- Wright JC
- Wright P
- Wukitch S
- Wynn A
- Xiang L
- Xu T
- Xue Y
- Yadikin D
- Yakovenko Y
- Yanling W
- Yavorskij V
- Young D
- Young I
- Young R
- Zacks J
- Zagorski R
- Zaitsev FS
- Zakharov L
- Zanino R
- Zarins A
- Zarins R
- Zastrow KD
- Zerbini M
- Zhang W
- Zhou Y
- Zilli E
- Zocco A
- Zoita V
- Zoletnik S
- Zwingmann W
- Zychor I
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
This paper presents results of JET ITER-like wall L-mode experiments in hydrogen and deuterium (D) plasmas, dedicated to the study of the isotope dependence of ion heat transport by determination of the ion critical gradient and stiffness by varying the ion cyclotron resonance heating power deposition. When no strong role of fast ions in the plasma core is expected, the main difference between the two isotope plasmas is determined by the plasma edge and the core behavior is consistent with a gyro-Bohm scaling. When the heating power (and the fast ion pressure) is increased, in addition to the difference in the edge region, also the plasma core shows substantial changes. The stabilization of ion heat transport by fast ions, clearly visible in D plasmas, appears to be weaker in H plasmas, resulting in a higher ion heat flux in H with apparent anti-gyro-Bohm mass scaling. The difference is found to be caused by the different fast ion pressure between H and D plasmas, related to the heating power settings and to the different fast ion slowing down time, and is completely accounted for in non-linear gyrokinetic simulations. The application of the TGLF quasi-linear model to this set of data is also discussed
First principles and integrated modelling achievements towards trustful fusion power predictions for JET and ITER
- Author
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- Abhangi M
- Abreu P
- Afanasev V
- Afzal M
- Aggarwal KM
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- Zakharov L
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- Zoletnik S
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- Zychor I
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
Predictability of burning plasmas is a key issue for designing and building credible future fusion devices. In this context, an important effort of physics understanding and guidance is being carried out in parallel to JET experimental campaigns in H and D by performing analyses and modelling towards an improvement of the understanding of DT physics for the optimization of the JET-DT neutron yield and fusion born alpha particle physics. Extrapolations to JET-DT from recent experiments using the maximum power available have been performed including some of the most sophisticated codes and a broad selection of models. There is a general agreement that 11-15 MW of fusion power can be expected in DT for the hybrid and baseline scenarios. On the other hand, in high beta, torque and fast ion fraction conditions, isotope effects could be favourable leading to higher fusion yield. It is shown that alpha particles related physics, such as TAE destabilization or fusion power electron heating, could be studied in ITER relevant JET-DT plasmas
Ion cyclotron resonance heating scenarios for DEMO
- Author
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- Zagorski R
- Zaitsev FS
- Zakharov L
- Zanino R
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- Zerbini M
- Zhang W
- Zhou Y
- Zilli E
- Zocco A
- Zoita V
- Zoletnik S
- Zwingmann W
- Zychor I
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
The present paper offers an overview of the potential of ion cyclotron resonance heating (ICRH) or radio frequency heating for the DEMO machine. It is found that various suitable heating schemes are available. Similar to ITER and in view of the limited bandwidth of about 10 MHz that can be achieved to ensure optimal functioning of the launcher, it is proposed to make core second harmonic tritium heating the key ion heating scheme, assisted by fundamental cyclotron heating He-3 in the early phase of the discharge; for the present design of DEMO-with a static magnetic field strength of B-o = 5.855 T-that places the T and 3He layers in the core for f = 60 MHz and suggests centering the bandwidth around that main operating frequency. In line with earlier studies for hot, dense plasmas in large-size magnetic confinement machines, it is shown that good single pass absorption is achieved but that the size as well as the operating density and temperature of the machine cause the electrons to absorb a non-negligible fraction of the power away from the core when core ion heating is aimed at. Current drive and alternative heating options are briefly discussed and a dedicated computation is done for the traveling wave antenna, proposed for DEMO in view of its compatibility with substantial antenna-plasma distances. The various tasks that ICRH can fulfill are briefly listed. Finally, the impact of transport and the sensitivity of the obtained results to changes in the machine parameters is commented on
Control of the hydrogen:deuterium isotope mixture using pellets in JET
- Author
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
Deuterium pellets are injected into an initially pure hydrogen H-mode plasma in order to control the hydrogen: deuterium (H:D) isotope mixture. The pellets are deposited in the outer 20% of the minor radius, similar to that expected in ITER, creating transiently hollow electron density profiles. A H: D isotope mixture of approximately 45%:55% is obtained in the core with a pellet fuelling throughput of Phi(pel) = 0.045P(aux)/T-e,T-ped similar to previous pellet fuelling experiments in pure deuterium. Evolution of the H: D mix in the core is reproduced using a simple model, although deuterium transport could be higher at the beginning of the pellet train compared with the flat-top phase
Recurrence Plots for Dynamic Analysis of Type-I ELMs at JET With a Carbon Wall
- Author
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- Zocco A
- Zoita V
- Zoletnik S
- Zwingmann W
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- Publication venue
- 'Institute of Electrical and Electronics Engineers (IEEE)'
- Publication date
- 01/01/2019
- Field of study
In this paper, the dynamic characteristics of type-I edge-localized modes (ELM) time series from the JET tokamak, the world's largest magnetic confinement plasma physics experiment, have been investigated through recurrence plots (RPs). The analysis has been focused on RPs of pedestal temperature, line averaged electron density, and outer divertor D-alpha time series during experiments with a carbon wall. The analysis of RPS shows the patterns similar to those characteristics of signals exhibiting type-2 intermittency, in particular, a characteristic kite-like shape; this gives useful hints to model the temperature signal as well as the D-alpha radiation time series, with simple nonlinear maps capturing the nearly periodic behavior of type-I ELMs
A new mechanism for increasing density peaking in tokamaks: improvement of the inward particle pinch with edge E x B shearing
- Author
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
Developing successful tokamak operation scenarios, as well as confident extrapolation of present-day knowledge requires a rigorous understanding of plasma turbulence, which largely determines the quality of the confinement. In particular, accurate particle transport predictions are essential due to the strong dependence of fusion power or bootstrap current on the particle density details. Here, gyrokinetic turbulence simulations are performed with physics inputs taken from a JET power scan, for which a relatively weak degradation of energy confinement and a significant density peaking is obtained with increasing input power. This way physics parameters that lead to such increase in the density peaking shall be elucidated. While well-known candidates, such as the collisionality, previously found in other studies are also recovered in this study, it is furthermore found that edge E x B shearing may adopt a crucial role by enhancing the inward pinch. These results may indicate that a plasma with rotational shear could develop a stronger density peaking as compared to a non-rotating one, because its inward convection is increased compared to the outward diffusive particle flux as long as this rotation has a significant on E x B flow shear stabilization. The possibly significant implications for future devices, which will exhibit much less torque compared to present day experiments, are discussed
Modification of the Alfven wave spectrum by pellet injection
- Author
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2019
- Field of study
Alfven eigenmodes driven by energetic particles are routinely observed in tokamak plasmas. These modes consist of poloidal harmonics of shear Alfven waves coupled by inhomogeneity in the magnetic field. Further coupling is introduced by 3D inhomogeneities in the ion density during the assimilation of injected pellets. This additional coupling modifies the Alfven continuum and discrete eigenmode spectrum. The frequencies of Alfven eigenmodes drop dramatically when a pellet is injected in JET. From these observations, information about the changes in the ion density caused by a pellet can be inferred. To use Alfven eigenmodes for MHD spectroscopy of pellet injected plasmas, the 3D MILD codes Stellgap and AE3D were generalised to incorporate 3D density profiles. A model for the expansion of the ionised pellet plasmoid along a magnetic field line was derived from the fluid equations. Thereby, the time evolution of the Alfven eigenfrequency is reproduced. By comparing the numerical frequency drop of a toroidal Alfven eigenmode (TAE) to experimental observations, the initial ion density of a cigar-shaped ablation region of length 4cm is estimated to be n(*) = 6.8 x 10(22) m(-3) at the TAE location (r/a approximate to 0.75). The frequency sweeping of an Alfven eigenmode ends when the ion density homogenises poloidally. Modelling suggests that the time for poloidal homogenisation of the ion density at the TAE position is tau(h) = 18 +/- 4 ms for inboard pellet injection, and tau(h) = 26 +/- 2 ms for outboard pellet injection. By reproducing the frequency evolution of the elliptical Alfven eigemnode (EAE), the initial ion density at the EAE location (r/a approximate to 0.9) can be estimated to be n(*) = 4.8 x 10(22) m(-3). Poloidal homogenisation of the ion density takes 2.7 times longer at the EAE location than at the TAE location for both inboard and outboard pellet injection