2011
DOI: 10.1016/j.tsf.2011.04.092
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Characterisation of thin film silicon films deposited by plasma enhanced chemical vapour deposition at 162MHz, using a large area, scalable, multi-tile-electrode plasma source

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Cited by 27 publications
(15 citation statements)
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“…Where the κ is regulation rate, {∆ε r, j } is the compensated sequence to the design variable sequence; and {s j } is the distributed sequence of {F CP,i }, the same as formula (17), and hence S = V −1Ũ F CP . Relative error (or non-uniformity) of the electron density profiles F C P (r ) on the probe line approximating to the expected profile F E P (r ) during the iterations.…”
Section: Profile Error Feedback (Pef) Methods Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…Where the κ is regulation rate, {∆ε r, j } is the compensated sequence to the design variable sequence; and {s j } is the distributed sequence of {F CP,i }, the same as formula (17), and hence S = V −1Ũ F CP . Relative error (or non-uniformity) of the electron density profiles F C P (r ) on the probe line approximating to the expected profile F E P (r ) during the iterations.…”
Section: Profile Error Feedback (Pef) Methods Modelmentioning
confidence: 99%
“…The first one is to do the multi-DOF design for the energy source. For instance, the solution that partitions the electrode into multi independently controllable sub-electrodes can achieve refined and flexible uniformity control of the plasma profile in the entire critical domain via regulating the power and phase of each sub-electrode, such as the multi-tile electrodes, [16][17][18] segmented electrodes, 19 and multi electrodes. 20 The other is to design the structure or material property of the medium in which the energy transfers.…”
Section: Introductionmentioning
confidence: 99%
“…14,15 To suppress this problem, VHF CCP discharges excited by segmented electrode are proposed and researched. [16][17][18][19] On the other hand, ICP discharges can overcome these limitations to some extent, i.e., the higher plasma density (up to 10 11 -10 12 cm À3 ) is maintained at a very low pressure (<10 mTorr), and fully independent control of the ion bombardment energy is possible using a separate bias onto the substrate. 20 However, controllability of plasma uniformity over a large area remains the major challenge.…”
Section: Introductionmentioning
confidence: 99%
“…One is to partition the energy source. For instance, the solution that the electrode is partitioned into multi independently controllable sub-electrodes can be refined and flexible regulate the uniformity of plasma profile with proper configuration of the power and phase of each sub-electrode, such as the multi-tile electrodes, [18][19][20] segmented electrodes, 21 and multi electrodes. 22 The other is to design the structure or material property of the media in which the energy transfers.…”
Section: Introductionmentioning
confidence: 99%