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Dive into the research topics where Fukun Liu is active.

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Featured researches published by Fukun Liu.


Nuclear Fusion | 2013

Experimental investigations of LHW?plasma coupling and current drive related to achieving H-mode plasmas in EAST

B. J. Ding; E.H. Kong; M. H. Li; Lei Zhang; W. Wei; M. Wang; Handong Xu; Y. C. Li; Bili Ling; Qing Zang; Gang Xu; Xiang Han; H.L. Zhao; Ling Zhang; L.M. Zhao; Huaichuan Hu; Yitao Yang; L. Liu; A. Ekedahl; M. Goniche; R. Cesario; Y. Peysson; J. Decker; V. Basiuk; P. Huynh; J. Artaud; F. Imbeaux; Jiafang Shan; Fukun Liu; Yanping Zhao

Aimed at high-confinement (H-mode) plasmas in the Experimental Advanced Superconducting Tokamak (EAST), the effect of local gas puffing from electron and ion sides of a lower hybrid wave (LHW) antenna on LHW?plasma coupling and high-density experiments with lower hybrid current drive (LHCD) are investigated in EAST. Experimental results show that gas puffing from the electron side is more favourable to improve coupling compared with gas puffing from the ion side. Investigations indicate that LHW?plasma coupling without gas puffing is affected by the density near the LHW grill (grill density), hence leading to multi-transition of low?high?low (L?H?L) confinement, with a correspondingly periodic characteristic behaviour in the plasma radiation. High-density experiments with LHCD suggest that strong lithiation gives a significant improvement on current drive efficiency in the higher density region than 2???1019?m?3. Studies indicate that the sharp decrease in current drive efficiency is mainly correlated with parametric decay instability.Using lithium coating and gas puffing from the electron side of the LHW antenna, an H-mode plasma is obtained by LHCD in a wide range of parameters, whether LHW is deposited inside the half-minor radius or not, implying that a central and large driven current is not a necessary condition for the H-mode plasma. H-mode is investigated with CRONOS.


Nuclear Fusion | 1999

Lower hybrid current drive experiments and improved performance on the HT-7 superconducting tokamak

Guangli Kuang; Yuexiou Liu; Jiafang Shan; W. Xu; Xiangqin Zhang; Dengcheng Liu; Fukun Liu; Yubao Zhu; Cheng Zhang; Guanghua Zheng; J.H. Wu; Jianan Lin; Bojiang Ding; Handong Xu; Yude Fang; Jiangang Li; Jiarong Luo; Xiaodong Zhang; Baonian Wan; Qingchu Zhao; Jianshan Mao; X. Gao; Shouyin Zhang; Chengfu Li; Xuemao Gu; Pinjian Qing; Hengyu Fan; S. Liu; Bili Ling; B. J. Ding

The feedback control system to control plasma current and position on the HT-7 superconducting tokamak was greatly improved in early 1998. Lower hybrid current drive (LHCD) experiments with the improved control system were performed to sustain long pulse discharges and to improve plasma confinement. Partial non-inductive current drive and full non-inductive current drive for several seconds by means of LHCD were demonstrated. It was observed that plasma confinement could be considerably improved by LHCD. Experimental evidence suggests that this improvement during the LHCD phase could be due to the modification of the current profile in the outer region of the plasma. MHD modes (especially m = 2) seem unstable with such a current profile. The EFIT code was modified for the reconstruction of the magnetic surfaces in HT-7 and a test computation was performed.


Physics of Plasmas | 2011

Investigation of lower hybrid wave coupling and current drive experiments at different configurations in experimental advanced superconducting tokamak

B J Ding; Y. L. Qin; Wentao Li; M. H. Li; E. H. Kong; Ling-yu Zhang; A. Ekedahl; Y Peysson; J. Decker; M. Wang; Handong Xu; H C Hu; G. Xu; Jiafang Shan; Fukun Liu; Yanping Zhao; Baonian Wan; J.G. Li

Using a 2 MW 2.45 GHz lower hybrid wave (LHW) system installed in experimental advanced superconducting tokamak, we have systematically carried out LHW-plasma coupling and lower hybrid current drive experiments in both divertor (double null and lower single null) and limiter plasma configuration with plasma current (Ip) ∼ 250 kA and central line averaged density (ne) ∼ 1.0–1.3 × 1019 m−3 recently. Results show that the reflection coefficient (RC) first is flat up to some distance between plasma and LHW grill, and then increases with the distance. Studies indicate that with the same plasma parameters, the best coupling is obtained in the limiter case (with plasma leaning on the inner wall), followed by the lower single null, and the one with the worst coupling is the double null configuration, explained by different magnetic connection length. The RCs in the different poloidal rows show that they have different coupling characteristics, possibly due to local magnetic connection length. Current drive effici...


Plasma Physics and Controlled Fusion | 2006

Dynamics of runaway electrons in lower hybrid current drive plasmas in the HT-7 tokamak

Z. Y. Chen; Baonian Wan; S. Y. Lin; Yuejiang Shi; Liqun Hu; J Younis; X.Z. Gong; Jiafang Shan; Fukun Liu; B. J. Ding; X. Gao; Ht Team

In lower hybrid current drive (LHCD) plasmas with non-zero loop voltage, the fast electron tail can act as a seed population of runaways. The runaways are found to be enhanced in the presence of lower hybrid (LH) waves when the fast electron tail extends above the critical velocity for electrons to run away. In runaway discharges, the LH waves may suppress runaway electrons due to the drop in the electric field linked to the non-inductive current drive. In this paper, the behaviour of runaway electrons in an extensive range of LHCD plasmas is presented.


Materials Research Innovations | 2015

Advanced graphene nanomaterials for electrochemical energy storage

Fukun Liu; Dongfeng Xue

Abstract The application of graphene in the field of electrochemical energy storage devices has been intensively investigated due to its many promising physical and chemical properties. The purpose of the current review paper is to introduce some latest advances in this area. At the beginning, the advantages of graphene as electrode materials and some existing problems will be discussed. In the following parts, we focus on three factors that can significantly influence the performance when graphene based materials are used for energy storage, including preventing the nanosheets from restacking, doping by foreign elements and compositing with other active materials. To illustrate such factors, some examples regarding the development of electrode materials for batteries and supercapacitors based on graphene have been reviewed. At the end, prospects and further developments for graphene based electrochemical energy storage will be also proposed.


Nuclear Fusion | 2007

Quasi-steady-state ac plasma current operation in HT-7 tokamak

Jiangang Li; Jiarong Luo; Shaojie Wang; Peng Fu; Biao Shen; Fukun Liu; Baonian Wan; Jiafang Shan; Guosheng Xu; Juan Huang; Jun Yu; Jiansheng Hu; Qiping Yuan; Yeming Hu; Ht Team

A quasi-steady-state alternating current operation assisted by lower hybrid wave (LHW) was achieved on a HT-7 superconducting tokamak with plasma current of Ip = 125 kA, line-averaged density of 1.5 × 1019 m−3, electron temperature of Te = 500 eV and 30–50 s plasma duration. Plasma current was sustained and smoothly transferred from one direction to the other without loss of ionization. Plasma position control, LHW assistance, strong gas puffing and good wall condition are the key issues to have a smooth transition of plasma current. Our modelling results show that current reversal equilibrium configuration with two oppositely flowing currents in the high-field-side and the low-field-side during current reversal exists. This is in agreement with experimental measurements.


Nuclear Fusion | 2015

First results of LHCD experiments with 4.6 GHz system toward steady-state plasma in EAST

Fukun Liu; B. J. Ding; J.G. Li; Baonian Wan; Jiafang Shan; M. Wang; L. Liu; L.M. Zhao; M. H. Li; Y. C. Li; Ying Yang; Z.G. Wu; J.Q. Feng; Huaichuan Hu; H. Jia; Y.Y. Huang; W. Wei; M. Cheng; Liuwei Xu; Qing Zang; B. Lyu; S. Y. Lin; Yanmin Duan; J.H. Wu; Y. Peysson; J. Decker; J. Hillairet; A. Ekedahl; Z.P. Luo; J. Qian

A 4.6 GHz lower-hybrid current drive (LHCD) system has been firstly commissioned in EAST in the 2014 campaign. The first LHCD results with 4.6 GHz show that LHW can be coupled to plasma with a low reflection coefficient, drive plasma current and plasma rotation, modify the plasma current profile, and heat plasma effectively. By means of configuration optimization and local gas puffing near the LHW antenna, good LHW–plasma coupling with a reflection coefficient less than 5% is obtained. The maximum LHW power coupled to plasma is up to 3.5 MW. The current drive (CD) efficiency is up to 1.1 × 1019 A m−2 W−1 and the central electron temperature is above 4 keV, suggesting that LH power could be mainly deposited in the core region, which is in agreement with code simulation. Experiments show that the current profile is effectively modified and toroidal rotation in the co-current direction is driven by the LHCD. Also, the CD efficiency and current profile depend on the launched wave spectrum, suggesting the possibility of controlling the current profile by changing the phase difference. Repeatable H-mode plasma is obtained by either the 4.6 GHz LHCD system alone, or together with a 2.45 GHz LHCD system, the NBI (neutral beam injection) system. The different ELM features of H-mode between the different heating methods are under investigation.


Nuclear Fusion | 2004

Experimental investigation of the interaction of IBW and LHCD in the HT-7 tokamak

Baonian Wan; Yuejiang Shi; Guosheng Xu; X.Z. Gong; Yanping Zhao; Jiafang Shan; Junyu Zhao; Yubao Zhu; Jiangang Li; Guangli Kuang; Fukun Liu; Yuzhou Mao; Yanxin Jie; Haiqing Liu

Experiments of simultaneous injection of LHWs and IBWs into plasmas have been conducted in the HT-7 tokamak. Evidence that IBW can control the plasma pressure profile was observed in LHCD plasmas. It was found that electron Landau damping (ELD) of IBWs occurred around the maxima of parallel refractive index, n||, and that the ion cyclotron resonant layer can enhance off-axis LHW power deposition and create a localized fast electron current channel. But the global LHCD efficiency during an IBW pulse was not improved obviously. As a result of the localization of LHCD during an IBW pulse, the global current density profile was modified, which was indicated by the internal inductance, li. Optimization of this operation mode utilizing the features of the interaction of IBWs and LHCD provides a new way of obtaining a high performance plasma under steady-state conditions.


Nuclear Fusion | 2015

Investigations of LHW-plasma coupling and current drive at high density related to H-mode experiments in EAST

B. J. Ding; Y. C. Li; L. Zhang; M. H. Li; W. Wei; E.H. Kong; M. Wang; Handong Xu; Shouxin Wang; Guosheng Xu; L.M. Zhao; H C Hu; H. Jia; M. Cheng; Yitao Yang; L. Liu; H.L. Zhao; Y. Peysson; J. Decker; M. Goniche; L. Amicucci; R. Cesario; A. A. Tuccillo; S. G. Baek; R.R. Parker; P.T. Bonoli; F. Paoletti; C. Yang; Jiafang Shan; Fukun Liu

Two important issues in achieving lower hybrid current drive (LHCD) high confinement plasma in EAST are to improve lower hybrid wave (LHW)-plasma coupling and to drive the plasma current at a high density. Studies in different configurations with different directions of toroidal magnetic field (Bt) show that the density near the antenna is affected by both the radial electric field induced by plasma without a LHW (Er_plasma) in the scrape off layer (SOL), and the radial electric field induced by LHW power (Er_LH) near the grill. Investigations indicate that Er × Bt in the SOL leads to a different effect of configuration on the LHW-plasma coupling and Er_LH × Bt accounts for the asymmetric density behaviour in the SOL observed in the experiments, where Er is the total radial electric field in the SOL. Modelling of parametric instability (PI), collisional absorption (CA) and scattering from density fluctuations (SDF) in the edge region, performed considering the parameters of high density LHCD experiments in EAST, has shown that these mechanisms could be responsible for the low current drive (CD) efficiency at high density. Radiofrequency probe spectra, useful for documenting PI occurrence, show sidebands whose amplitude in the case of the lithiated vacuum chamber is smaller than in the case of poor lithiation, consistently with growth rates from PI modeling of the respective reference discharges. Since strong lithiation is also expected to diminish the parasitic effect on the LHCD of the remaining possible mechanisms, this appears to be a useful method for improving LHCD efficiency at a high density.


Physics of Plasmas | 2016

Lower hybrid current drive experiments with different launched wave frequencies in the EAST tokamak

M. H. Li; B. J. Ding; Fukun Liu; Jiafang Shan; M. Wang; Handong Xu; Li Liu; H C Hu; Xiaotao Zhang; Y. C. Li; W. Wei; Z. G. Wu; W. D. Ma; Y. Yang; J. Q. Feng; H. Jia; Xin Wang; D. J. Wu; M. Chen; L. Xu; J. W. Wang; S. Y. Lin; J. Z. Zhang; J. Qian; Zhengping Luo; Qing Zang; Xiao Feng Han; H.L. Zhao; Y. Peysson; J. Decker

EAST has been equipped with two high power lower hybrid current drive (LHCD) systems with operating frequencies of 2.45 GHz and 4.6 GHz. Comparative LHCD experiments with the two different frequencies were performed in the same conditions of plasma for the first time. It was found that current drive (CD) efficiency and plasma heating effect are much better for 4.6 GHz LH waves than for the one with 2.45 GHz. High confinement mode (H-mode) discharges with 4.6 GHz LHCD as the sole auxiliary heating source have been obtained in EAST and the confinement is higher with respect to that produced previously by 2.45 GHz. A combination of ray-tracing and Fokker-Planck calculations by using the C3PO/LUKE codes was performed in order to explain the different experimental observations between the two waves. In addition, the frequency spectral broadening of the two LH wave operating frequencies was surveyed by using a radio frequency probe.

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Jiafang Shan

Chinese Academy of Sciences

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Handong Xu

Chinese Academy of Sciences

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M. H. Li

Chinese Academy of Sciences

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M. Wang

Chinese Academy of Sciences

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B. J. Ding

Chinese Academy of Sciences

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X.Z. Gong

Chinese Academy of Sciences

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Huaichuan Hu

Chinese Academy of Sciences

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Y. C. Li

Chinese Academy of Sciences

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W. Wei

Chinese Academy of Sciences

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