Littérature scientifique sur le sujet « Lhcd »
Créez une référence correcte selon les styles APA, MLA, Chicago, Harvard et plusieurs autres
Sommaire
Consultez les listes thématiques d’articles de revues, de livres, de thèses, de rapports de conférences et d’autres sources académiques sur le sujet « Lhcd ».
À côté de chaque source dans la liste de références il y a un bouton « Ajouter à la bibliographie ». Cliquez sur ce bouton, et nous générerons automatiquement la référence bibliographique pour la source choisie selon votre style de citation préféré : APA, MLA, Harvard, Vancouver, Chicago, etc.
Vous pouvez aussi télécharger le texte intégral de la publication scolaire au format pdf et consulter son résumé en ligne lorsque ces informations sont inclues dans les métadonnées.
Articles de revues sur le sujet "Lhcd"
Shi, Bo, Zhen-Dong Yang, Bin Zhang, Cheng Yang, Kai-Fu Gan, Mei-Wen Chen, Jin-Hong Yang et al. « Heat Flux on EAST Divertor Plate in H-mode with LHCD/LHCD+NBI ». Chinese Physics Letters 34, no 9 (août 2017) : 095201. http://dx.doi.org/10.1088/0256-307x/34/9/095201.
Texte intégralHao, Xu, et Yi Yun Huang. « The Design of High Voltage DC Power Supply of 4.6GHZ/500MW LHCD ». Applied Mechanics and Materials 135-136 (octobre 2011) : 1027–36. http://dx.doi.org/10.4028/www.scientific.net/amm.135-136.1027.
Texte intégralSharma, P. K., D. Raju, S. K. Pathak, R. Srinivasan, K. K. Ambulkar, P. R. Parmar, C. G. Virani et al. « Current drive experiments in SST1 tokamak with lower hybrid waves ». Nuclear Fusion 62, no 5 (28 mars 2022) : 056020. http://dx.doi.org/10.1088/1741-4326/ac4297.
Texte intégralBing-ren, Shi. « Electron Heating in Tokamak LHCD Experiment ». Plasma Science and Technology 2, no 5 (octobre 2000) : 423–29. http://dx.doi.org/10.1088/1009-0630/2/5/001.
Texte intégralBibet, Ph, B. Beaumont, J. H. Belo, L. Delpech, A. Ekedahl, G. Granucci, F. Kazarian et al. « Toward a LHCD system for ITER ». Fusion Engineering and Design 74, no 1-4 (novembre 2005) : 419–23. http://dx.doi.org/10.1016/j.fusengdes.2005.06.014.
Texte intégralPi, Xiong, Lirong Tian, Huai-En Dai, Xiaochun Qin, Lingpeng Cheng, Tingyun Kuang, Sen-Fang Sui et Jian-Ren Shen. « Unique organization of photosystem I–light-harvesting supercomplex revealed by cryo-EM from a red alga ». Proceedings of the National Academy of Sciences 115, no 17 (9 avril 2018) : 4423–28. http://dx.doi.org/10.1073/pnas.1722482115.
Texte intégralEsterkin, A. R., et A. D. Piliya. « Fast ray tracing code for LHCD simulations ». Nuclear Fusion 36, no 11 (novembre 1996) : 1501–12. http://dx.doi.org/10.1088/0029-5515/36/11/i05.
Texte intégralDing, Bojiang, Erhua Kong, Miaohui Li, Yongliang Qin, Lei Zhang, Mao Wang, Handong Xu et al. « Recent Results of LHCD Experiments in EAST ». Plasma Science and Technology 13, no 2 (avril 2011) : 153–56. http://dx.doi.org/10.1088/1009-0630/13/2/05.
Texte intégralPark, S., H. Do, J. H. Jeong, W. Namkung, M. H. Cho, H. Park, Y. S. Bae et al. « Development status of KSTAR 5GHz LHCD system ». Fusion Engineering and Design 85, no 2 (avril 2010) : 197–204. http://dx.doi.org/10.1016/j.fusengdes.2009.12.004.
Texte intégralWu, Qiuran, Peng Lu, Yu Zheng, Hua Du, Liang Liu, Qingjun Zhu et Songlin Liu. « Neutronics assessments of LHCD antenna system for CFETR ». Fusion Engineering and Design 172 (novembre 2021) : 112877. http://dx.doi.org/10.1016/j.fusengdes.2021.112877.
Texte intégralThèses sur le sujet "Lhcd"
Liang, Anshu. « Understanding the low to high confinement transition in tokamak plasmas ». Electronic Thesis or Diss., Aix-Marseille, 2023. http://theses.univ-amu.fr.lama.univ-amu.fr/230112_LIANG_826zuy182lisgpn946fzpk544n_TH.pdf.
Texte intégralThe works presented in this thesis are devoted to understand the physical mechanism of the L-H transition. The driving mechanism of the velocity shear in the plasma edge has been studied using lower hybrid current drive (LHCD) power injection on the HL-2A tokamak in China. It has been shown that the increase of the velocity shear is mainly driven by the ion diamagnetic term of the radial electric field Er. During the L-H transition, it is observed that the ion diamagnetic term of the radial electric field Er plays a dominant role in the increase of velocity shear, while the contributions of the poloidal and toroidal velocity terms are negligible. The velocity shear must reach a critical value to allow the L-H transition to occur. This means that the critical value plays a role as a velocity shear threshold for the L-H transition. In addition, the stimulated effect of supersonic molecular beam injection (SMBI) on the L-H transition has also been investigated on HL-2A. The results suggest that SMBI could be a reliable method for reducing the L-H transition power threshold and controlling the L-H transition in future fusion reactors. Finally, efforts have been made on the optimization of LHCD coupling on the WEST tokamak in France and an analysis of the LH wave coupling in WEST plasmas has been carried out. The analysis shows that the toroidal reshaping of the fully-active-multijunction launcher carried out before its installation in WEST was successful. The experiments have also shown that the reshaping of the passive-active-multijunction launcher is necessary in order to avoid overheating on the launcher front in long pulses
Sierchio, Jennifer Marie. « The effect of ICRF and LHCD waveguide and launcher location on tritium breeding ratio and radiation damage in fusion reactors ». Thesis, Massachusetts Institute of Technology, 2016. http://hdl.handle.net/1721.1/103703.
Texte intégralCataloged from PDF version of thesis.
Includes bibliographical references (pages 73-76).
In most tokamak fusion reactor designs, ICRF (Ion Cyclotron Range of Frequencies) and LH (Lower Hybrid) radio frequency (RF) waves used to heat the plasma and drive current are launched from the low-field, outboard side where there is more access space. It has recently been proposed to launch these waves from the high-field side [1-3], which increases current-drive efficiency, allows for better wave penetration, and has favorable scrape-off-layer and plasma material interaction characteristics [4]. However the poloidal location and size of RF launchers will also affect important aspects of the neutronics of the tokamak fusion design, i.e. how the 14.1 MeV neutrons born out of the deuterium-tritium (D-T) fusion reaction interact with the surrounding blanket and structures. The goal of this thesis is to assess the dependence of RF launcher poloidal location on the important neutronics parameters of tritium fuel breeding, launcher damage and activation. To determine the effects of waveguide and antenna location on Tritium Breeding Ratio (TBR), damage, and activation, the MCNP Transport Code was used, as well as the EASY 2010 activation package to analyze the activation of the vacuum vessel components. A simple geometry was designed for MCNP, based on the original ARC model [1]. Seven locations for the waveguides and antenna were chosen: the inner and outer midplane, the inner and outer upper corners, two spaces between the midplane (inboard and outboard), and a central location directly above the vacuum vessel. TBR, DPA, and helium concentration were calculated at all seven points to find the optimal location for the waveguides and antenna. Four blanket materials were chosen: two liquid blankets (FliBe and Pb-17Li) and two solid blankets (Li4SiO4 and Li2TiO3). This was to test whether or not blanket material affects the optimal location of the launchers. We find that from the neutronics point of view the overall optimal location is the inboard upper corner, which minimizes DPA and helium concentration in the antenna and waveguide, and maximizes TBR. DPA in the waveguide was minimized when placed in the outboard upper corner, although the difference in DPA between the two locations was small. While TBR was maximized at the top of the vacuum vessel, the differences in TBR between all locations was less than 1%. These results reinforce the choice of inside, upper corner launch as the optimal location for current drive, launcher protection and neutronics. Activation was also assessed for the vacuum vessel, both without and with the waveguides and antenna, assuming irradiation times of one week, one month, and one year. Overall, activation was significant in the vacuum vessel, as expected, due to the use of Inconel 718. The IAEA recycling limit could be achieved, regardless of irradiation time. The dominant isotopes present after irradiation differed when the irradiation time was one week versus one month or one year. Activation was also assessed in the waveguides and antenna for the cases of the launchers being placed at the outboard midplane versus the inboard corner. The activation in the antenna was shown to be reduced by a factor of two and in the waveguides by a factor of four, when the launchers were placed in the inboard corner.
by Jennifer Marie Sierchio.
S.M.
McCarthy, James. « Search for rare baryonic b decays with the LHCb experiment at the LHC ». Thesis, University of Birmingham, 2015. http://etheses.bham.ac.uk//id/eprint/6247/.
Texte intégralManuzzi, Daniele. « Measure of the branching ratio of the B0→D∗−τ+ντ decay at LHCb : a preliminary study for RD∗(q2) in 3-prong τ decays ». Master's thesis, Alma Mater Studiorum - Università di Bologna, 2018. http://amslaurea.unibo.it/15841/.
Texte intégralMELONI, SIMONE. « Test of lepton flavour universality with the simultaneous measurement of R(D+) and R (D*+) with τ→ μνν decays at the LHCb experiment ». Doctoral thesis, Università degli Studi di Milano-Bicocca, 2022. http://hdl.handle.net/10281/364128.
Texte intégralIn the Standard Model of particle physics, the coupling of the electroweak gauge bosons to the leptons is independent of the lepton flavour. This property, known as Lepton Flavour Universality, is an accidental symmetry of the Standard Model, which can be tested in semileptonic b-meson decays. The variables used to test the Lepton Flavour Universality hypothesis are ratios of branching fractions between decays with the τ lepton and the ones with the μ lepton in the final state: R(Hc) = B(B → Hc τ ν) / B(B → Hc μν) with Hc a charmed meson produced in the decay. Any sign of deviation with respect to the Standard Model predictions in these variables could be a clear sign of New Physics effects. A tension at the level of 3σ with respect to the Standard Model predictions has been observed in the combination of the measurements of R(D) and R(D*) performed by the Belle, BaBar and LHCb collaborations. At the time of writing of this thesis, no measurement of the R(D) parameter has been performed by any hadron collider experiment. This thesis reports a simultaneous measurement of the R(D+) and R(D*+) parameters performed using B → D(*)lν decays. This measurement exploits leptonic decays of the τ lepton, τ → μνν , using a data sample corresponding to an integrated luminosity of 2.0 /fb collected in proton-proton collisions at a centre-of-mass energy of 13 TeV at the LHCb experiment during the 2015 and 2016 data taking years. All the steps of the analysis have been performed and all the main systematic uncertainties have been studied. The value of the measured parameters is still blinded and the analysis is in internal review within the LHCb collaboration. The expected uncertainty on the parameters of interest is given by R(D+) = xxx ± 0.033(stat.) ± 0.037(syst.), R(D*+)= xxx ± 0.040(stat.) ± 0.070(syst.).
Roselló, Canal Maria del Mar. « Control de l'escintil·lador SPD del calorímetre d'LHCb ». Doctoral thesis, Universitat Ramon Llull, 2009. http://hdl.handle.net/10803/9152.
Texte intégralL'LHC és un accelerador orientat a estudiar els constituents de la matèria on LHCb n'és un dels detectors. El calorímetre és aquella part del detector destinada a mesurar l'energia de les partícules que el travessen. En el nostre cas l'SPD discrimina entre partícules carregades i no carregades contribuint així en les decisions del calorímetre.
En l'electrònica de l'SPD trobareu diferenciades dues parts: l'electrònica en contacte directe amb el subdetector (Very Front End, VFE) i l'electrònica de gestió de l'SPD (la Control Board, CB). L'objectiu d'aquesta tesi és la descripció d'aquesta darrera així com la integració de l'SPD en el sistema de control del calorímetre.
El VFE realitza un primer processat de les dades del detector determinant un nivell digital el qual indica si s'ha rebut una partícula carregada o no. La CB és l'encarregada en canvi de la monitorització i el control del sistema SPD: és capaç d'enviar dades de configuració als VFE i a la vegada en monitoritza el correcte funcionament.
Veureu que el document es troba organitzat en 5 parts. A la primera part trobareu descrites les característiques principals del calorímetre, les seves funcions i la seva estructura. La part segona, tercera i quarta són dedicades integrament a la CB: a la part 2 tenim descrit el hardware, a la part 3 el sistema de control i a la quarta part hi trobarem comentats els diferents testos i proves realitzades tan sobre el hardware com amb el sistema de control. Finalment a la cinquena part hi trobarem resumits els objectius aconseguits amb el nostre disseny i les aportacions d'aquest en la globalitat de l'experiment.
En esta tesis se describe la electrónica y la gestión de la placa de control del SPD. SPD son las siglas correspondientes a Scintillator Pad Detector, parte del calorímetro de LHCb del acelerador LHC.
LHC es un acelerador orientado al estudio de los constituyentes de la materia donde LHCb es uno de los detectores. El calorímetro es aquella parte del detector destinada a medir la energía de las partículas que lo traviesan. En nuestro caso el SPD discrimina entre partículas cargadas y neutras contribuyendo así a las decisiones del calorímetro.
En la electrónica del SPD encontraréis diferenciadas dos partes: la electrónica en contacto directo con el detector (Very Front End, VFE) y la electrónica de gestión del SPD (la Control Board, CB). El objetivo de esta tesis es precisamente la descripción de esta última parte así como la integración del SPD en el sistema de control del calorímetro.
El VFE realiza un primer procesado de los datos del detector determinando un nivel digital el cual indica si la partícula detectada está cargada o no. La CB es en cambio la encargada de la monitorización y el control del sistema SPD: es capaz de enviar datos de configuración a los VFE y a la vez monitorizar su correcto funcionamiento.
Veréis que el documento se encuentra organizado en 5 partes. En la primera parte encontraréis descritas las características principales del calorímetro, sus funciones y su estructura. La segunda parte, la tercera y la cuarta están plenamente dedicadas a la CB: en la parte 2 tenemos descrito el hardware, en la parte 3 el sistema de control y en la cuarta encontraremos los diferentes tests y pruebas realizadas sobre el hardware y el sistema de control. Finalmente en la quinta parte tenemos resumidos los objetivos conseguidos con nuestro diseño y las aportaciones de este en la globalidad del experimento.
In this thesis you will have described the electronics and management of the SPD. SPD stands for Scintillator Pad Detector which is part of the LHCb calorimeter of the LHC accelerator.
LHC is an accelerator oriented to study the matter constitution and LHCb is one of the detectors designed for this challenge. The LHCb part oriented to measure the particles energy is the calorimeter. The SPD is designed to discriminate between charged and neutral particles contributing in the calorimeter decisions.
In the SPD electronics description we can distinguish between to parts: the electronics in contact with the subdetector (Very Front End, VFE) and the electronics in charge of the SPD management (the Control Board, CB). The goal of this thesis is the description of the last and also the integration of the SPD with the calorimeter control system.
The VFE captures the data from the detector and makes a first digital decision depending on if the particle detected is charged or not. The CB is in charge of the monitoring and control of the SPD system: is able to send configuration data to the VFE and also monitors parameters to assure a proper behaviour.
You will see that the document is divided in 5 parts. In the first, you will find described the calorimeter, its functionalities and its structure. Part 2, part 3 and part 4 are fully dedicated to the CB: in part 2 we will find the CB hardware, in part 3 the control system and finally in part 4 the different tests performed with the hardware and the control system. The document ends with part 5 where the main objectives of this work are summarized and also the contribution of the SPD design in the LHCb project.
Hopchev, Plamen. « Mesures de la luminosité absolue à l'expérience LHCb ». Phd thesis, Université de Grenoble, 2011. http://tel.archives-ouvertes.fr/tel-00684982.
Texte intégralAlessio, Federico. « Beam, Background and Luminosity Monitoring in LHCb and Upgrade of the LHCb Fast Readout Control ». Thesis, Aix-Marseille 2, 2011. http://www.theses.fr/2011AIX22044/document.
Texte intégralThere are two main central topics in the thesis: the LHCb beam, background and luminosity monitoring systems and the LHCb optimization systems of experimental conditions. These systems are heavily connected to each other, as improving the machine beam, background and luminosity conditions will automatically improve global operation by maximizing the ratio of luminosity recorded over signal background. At the same time, improving the operation of the experiment will help improve luminosity, by studying more accurately the beam and background conditions and therefore improving the LHC machine settings. In this thesis, the systems to accomplish the requirements of these two main topics are described in detail
Kochebina, Olga. « Study of Rare Charm Decays with the LHCb Detector at CERN ». Thesis, Paris 11, 2014. http://www.theses.fr/2014PA112208/document.
Texte intégralRare charm decays proceed mostly through the c -> u Flavor Changing Neutral Current (FCNC), which is possible only at loop level in the Standard Model (SM). In charmed decays, FCNCs are subject to a very efficient GIM suppression, leading to very rare processes. Consequently, rare charm decays are good tools to probe to New Physics (NP) beyond the SM. NP particles could become detectable by causing observables such as branching ratios and CP or angular asymmetries to deviate from the SM predictions. The main subject of this thesis is the measurement of the branching ratio of the D0 -> K-π+ ρ/ω (->µ+µ-) mode. It will be precious in the future, in particular as a normalization mode in the study of all: D0 -> h-h’+ µ+µ- decays D0 -> K-π+µ+µ-, D0 -> π+π-µ+µ-, D0 -> K+K-µ+µ- and D0 -> K+π-µ+µ-. Using 2/fb of 2012 LHCb data we find: B(D0 -> K-π+ ρ/ω (->µ+µ-)) = (4.37± 0.12(stat.) ±0.53(syst.)) ×10^-6. This is the first measurement of this mode. We also determined sensitivities to total and partial branching fractions and asymmetries in D0 -> h-h’+ µ+µ- decays with future LHCb datasets. In addition, the systematic uncertainties affecting the searches for the 3-body decays, D+(s) -> π+µ+µ- and D+(s) -> π-µ+µ+, carried out by LHCb based on the data collected in 2011 (1/fb). Finally, the results of the tests of front-end electronic board for the Upgrade of LHCb are presented
Laubser, J. « Conception et réalisation de l'unité de décision du système de déclenchement de premier niveau du détecteur LHCb au LHC ». Phd thesis, Université Blaise Pascal - Clermont-Ferrand II, 2007. http://tel.archives-ouvertes.fr/tel-00283775.
Texte intégralLivres sur le sujet "Lhcd"
Gardi, Einan, Nigel Glover et Aidan Robson, dir. LHC Phenomenology. Cham : Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-05362-2.
Texte intégralBinoth, T. LHC physics. Boca Raton, FL : Taylor & Francis, 2012.
Trouver le texte intégralGiudice, Gian Francesco. Odyssee im Zeptoraum : Eine Reise in die Physik des LHC. Berlin : Springer Berlin, 2011.
Trouver le texte intégralBrüning, O. LHC design report. Sous la direction de European Organization for Nuclear Research. Geneva : European Organization for Nuclear Research, 2004.
Trouver le texte intégralZla-ba-tshe-riṅ. Lhad med g'yu loʼi rṅul thigs. Dharamsala, H.P : Bod-kyi Dgu-chu-sum Las-ʼgul Tshogs-pa, 2007.
Trouver le texte intégralBzo mchog lhad mo kun mthoṅ. Chʼang-tu : Si-khron mi rigs dpe skrun khaṅ, 2000.
Trouver le texte intégralPlehn, Tilman. Lectures on LHC physics. Heidelberg : Springer, 2012.
Trouver le texte intégralPlehn, Tilman. Lectures on LHC Physics. Berlin, Heidelberg : Springer Berlin Heidelberg, 2012. http://dx.doi.org/10.1007/978-3-642-24040-9.
Texte intégralPlehn, Tilman. Lectures on LHC Physics. Cham : Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-05942-6.
Texte intégralL, Kane G., et Pierce Aaron, dir. Perspectives on LHC physics. Hackensack, NJ : World Scientific, 2008.
Trouver le texte intégralChapitres de livres sur le sujet "Lhcd"
Quagliani, Renato. « The LHCb Detector at the LHC ». Dans Springer Theses, 29–65. Cham : Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-030-01839-9_2.
Texte intégralGandini, Paolo. « The LHCb Experiment at the LHC ». Dans Observation of CP Violation in B± → DK± Decays, 25–53. Cham : Springer International Publishing, 2013. http://dx.doi.org/10.1007/978-3-319-01029-8_2.
Texte intégralBastianin, Andrea. « Findings from the LHC/HL-LHC Programme ». Dans The Economics of Big Science, 71–77. Cham : Springer International Publishing, 2020. http://dx.doi.org/10.1007/978-3-030-52391-6_10.
Texte intégralFrühwirth, Rudolf, et Are Strandlie. « LHC Experiments ». Dans Pattern Recognition, Tracking and Vertex Reconstruction in Particle Detectors, 169–79. Cham : Springer International Publishing, 2020. http://dx.doi.org/10.1007/978-3-030-65771-0_10.
Texte intégralHeinemeyer, Sven. « Higgs/Electroweak in the SM and the MSSM ». Dans LHC Phenomenology, 3–34. Cham : Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-05362-2_1.
Texte intégralGrossman, Yuval. « Introduction to Flavour Physics ». Dans LHC Phenomenology, 35–80. Cham : Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-05362-2_2.
Texte intégralCacciapaglia, Giacomo. « Beyond the Standard Model Phenomenology and the ElectroWeak Symmetry Breaking ». Dans LHC Phenomenology, 81–121. Cham : Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-05362-2_3.
Texte intégralMättig, Peter. « Probing the Standard Model at Hadron Colliders ». Dans LHC Phenomenology, 125–72. Cham : Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-05362-2_4.
Texte intégralMurray, William. « Higgs Boson Searches ». Dans LHC Phenomenology, 173–202. Cham : Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-05362-2_5.
Texte intégralGershon, Tim. « Flavour Physics in the LHC Era ». Dans LHC Phenomenology, 203–37. Cham : Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-05362-2_6.
Texte intégralActes de conférences sur le sujet "Lhcd"
Feng, Jianqiang, Jiafang Shan et Mao Wang. « A Fault Diagnosis Expert System for LHCD System on EAST ». Dans 18th International Conference on Nuclear Engineering. ASMEDC, 2010. http://dx.doi.org/10.1115/icone18-29346.
Texte intégralLu, B., X. Y. Bai, Y. Peysson, Y. P. Zhang, D. Mazon, G. L. Xiao, X. L. Zou et al. « Recent LHCD experiments on HL-2A and LHCD system development on HL-2M ». Dans THE 6TH INTERNATIONAL CONFERENCE ON BIOLOGICAL SCIENCE ICBS 2019 : “Biodiversity as a Cornerstone for Embracing Future Humanity”. AIP Publishing, 2020. http://dx.doi.org/10.1063/5.0013734.
Texte intégralBibet, Ph, B. Beaumont, J. Belo, J. P. S. Bizarro, L. Delpech, A. Ekedahl, G. Granucci et al. « ITER LHCD Plans and Design ». Dans 21st IEEE/NPS Symposium on Fusion Engineering SOFE 05. IEEE, 2005. http://dx.doi.org/10.1109/fusion.2005.252946.
Texte intégralBai, X. Y., J. Liang, K. Feng, B. Lu, H. Zeng, C. Wang, J. Q. Wang et al. « HL-2M LHCD antenna development ». Dans THE 6TH INTERNATIONAL CONFERENCE ON BIOLOGICAL SCIENCE ICBS 2019 : “Biodiversity as a Cornerstone for Embracing Future Humanity”. AIP Publishing, 2020. http://dx.doi.org/10.1063/5.0013732.
Texte intégralBibet, Ph, C. Portafaix, G. Agarici, L. Cogneau-Garampon, C. Deck, Ph Froissard, M. Goniche et al. « New launchers for Tore Supra LHCD ». Dans The twelfth topical conference on radio frequency power in plasmas. AIP, 1997. http://dx.doi.org/10.1063/1.53401.
Texte intégralRimini, F. G., B. Alper, Y. F. Baranov, J. C. De Haas, J. A. Dobbing, A. C. Ekedahl, L. G. Eriksson et al. « High power LHCD experiments in JET ». Dans The 11th topical conference on radio frequency power in plasmas. AIP, 1996. http://dx.doi.org/10.1063/1.49563.
Texte intégralTakase, Y., P. T. Bonoli, A. Ejiri, T. Oosako, J. C. Wright, Philip M. Ryan et David Rasmussen. « LHCD Scenarios for Spherical Tokamak Plasmas ». Dans RADIO FREQUENCY POWER IN PLASMAS : 17th Topical Conference on Radio Frequency Power in Plasmas. AIP, 2007. http://dx.doi.org/10.1063/1.2800502.
Texte intégralShcherbinin, O. N., E. Z. Gusakov, V. V. Dyachenko, M. A. Irzak, S. A. Khitrov, Volodymyr Bobkov et Jean-Marie Noterdaeme. « Proposal on LHCD Experiments in Spherical Tokamaks ». Dans RADIO FREQUENCY POWER IN PLASMAS : Proceedings of the 18th Topical Conference. AIP, 2009. http://dx.doi.org/10.1063/1.3273784.
Texte intégralMirizzi, F., A. Cardinali, R. Cesario, L. Panaccione, V. Pericoli Ridolfini, G. L. Ravera et A. A. Tuccillo. « FAST and its LHCD System. Work in progress ». Dans 2009 23rd IEEE/NPSS Symposium on Fusion Engineering - SOFE. IEEE, 2009. http://dx.doi.org/10.1109/fusion.2009.5226418.
Texte intégralCôté, A., C. Côté, Y. Demers, V. Fuchs, X. Litaudon, G. Abel, J. L. Lachambre et al. « Current profile control experiments with LHCD on TdeV ». Dans The twelfth topical conference on radio frequency power in plasmas. AIP, 1997. http://dx.doi.org/10.1063/1.53375.
Texte intégralRapports d'organisations sur le sujet "Lhcd"
Ko, Jinseok, Steve Scott, Syun'ichi Shiraiwa, Martin Greenwald, Ronald Parker et Gregory Wallace. Intra-shot MSE Calibration Technique For LHCD Experiments. Office of Scientific and Technical Information (OSTI), novembre 2009. http://dx.doi.org/10.2172/969308.
Texte intégralJ. Hosea, D. Beals, W. Beck, S. Bernabei, W. Burke, R. Childs, R. Ellis et al. The LHCD Launcher for Alcator C-Mod - Design, Construction, Calibration and Testing. Office of Scientific and Technical Information (OSTI), juin 2005. http://dx.doi.org/10.2172/841200.
Texte intégralJones, S. E., J. Kesner, S. Luckhardt, F. Paoletti, S. von Goeler, S. Bernabei, R. Kaita et F. Rimini. Fast electron current density profile and diffusion studies during LHCD in PBX-M. Office of Scientific and Technical Information (OSTI), août 1993. http://dx.doi.org/10.2172/10183503.
Texte intégralJames, A., D. Brunner, B. LaBombard, C. Lau, B. Lipschultz, D. Miller, M. Reinke et al. Imaging of molybdenum erosion and thermography at visible wavelengths in Alcator C-Mod ICRH and LHCD discharges. Office of Scientific and Technical Information (OSTI), juin 2013. http://dx.doi.org/10.2172/1088479.
Texte intégralArtuso, M. Tests of LHCb Silicon Detectors. Office of Scientific and Technical Information (OSTI), décembre 2007. http://dx.doi.org/10.2172/1985128.
Texte intégralCartiglia, N., et C. Royon. LHC forward physics. Office of Scientific and Technical Information (OSTI), octobre 2015. http://dx.doi.org/10.2172/1222458.
Texte intégralBartl, A., J. Soederqvist et F. Paige. Supersymmetry at LHC. Office of Scientific and Technical Information (OSTI), novembre 1996. http://dx.doi.org/10.2172/425352.
Texte intégralAmbrosio, G., F. M. Ametrano, F. Broggi, N. Andreev, K. Artoos, M. Begg, G. Bellomo et al. EPAC/LHC Magnet Papers. Office of Scientific and Technical Information (OSTI), juin 1996. http://dx.doi.org/10.2172/1119495.
Texte intégralDippo, James L., Tim Erikson et Kris Hess. Fuelcell-Hybrid Mine loader (LHD). Office of Scientific and Technical Information (OSTI), juillet 2009. http://dx.doi.org/10.2172/990290.
Texte intégralPelaez, Jose R. Strong WW Interaction at LHC. Office of Scientific and Technical Information (OSTI), décembre 1998. http://dx.doi.org/10.2172/9985.
Texte intégral