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首页> 外文期刊>Thin Solid Films >A Comparative Study Of Crn_x Coatings Synthesized By Dc And Pulsed Dc Magnetron Sputtering
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A Comparative Study Of Crn_x Coatings Synthesized By Dc And Pulsed Dc Magnetron Sputtering

机译:直流磁控和脉冲直流磁控溅射制备Crn_x涂层的比较研究

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Chromium nitride (CrN_x) coatings were prepared by reactively sputtering chromium metal target with various nitrogen flow rate percentages (f_(N2)) using a closed field unbalanced magnetron sputtering system operated in dc and middle frequency pulsed condition (100 kHz and 50% duty cycle). In this study, plasma examination proved that a large amount of ions with a wide range of ion energies (up to 65 eV and mainly from 10-30 eV region) was identified in the pulsed plasma compared to the low ion flux and energy (0-10 eV) in a dc discharged plasma. The results showed that the phase structure of CrN_x coatings was changed from nitrogen doped Cr(N) to pure β-VCr_2N, and to a mixture of β-Cr_2N and c-CrN and then to pure c-CrN phases with an increase in the f_(N2) in both dc and pulsed conditions. However, the pulsed CrN_x coatings exhibit lower N concentrations than dc CrN_x coatings prepared under the same f_(N2), which leads to the existing of β-Cr_2N phase within a wide range of f_(N2) (30-50%). In comparison with the typical large columnar structure in the dc sputtered coatings, the pulsed CrN_x coatings exhibit dramatic microstructure improvements which benefited from the improved plasma density and ion bombardment from the pulsed plasma, where the super dense and nearly equi-axial structures were observed in a wide range of f_(N2). The microstructure improvements contributed to the enhancements in the hardness and wear resistance of pulsed CrN_x coatings. In the pulsed CrN_x coatings, the hardness values were above 30 GPa when the f_(N2) is in the range of 30-40%, which is related to the formation of the β-Cr_2N phase. With the formation of a mixture of β-Cr_2N and c-CrN phases in the coatings deposited with 40-50% f_(N2), a low COF of 0.36 and wear rate of 1.66× 10~(-6) mm~3N~(-1) m~(-1) can be achieved.
机译:氮化铬(CrN_x)涂层是通过使用在直流和中频脉冲条件(100 kHz和50%占空比)下运行的封闭场不平衡磁控溅射系统通过以各种氮气流量百分比(f_(N2))反应性溅射铬金属靶材来制备的)。在这项研究中,等离子体检查证明,与低离子通量和低能量(0相比)相比,在脉冲等离子体中可以识别出大量具有广泛离子能量的离子(高达65 eV,主要来自10-30 eV区域)。 -10 eV)在直流放电等离子体中。结果表明,CrN_x涂层的相结构从掺杂氮的Cr(N)变为纯的β-VCr_2N,再由β-Cr_2N和c-CrN的混合物转变为纯c-CrN的相,且相变增加。在直流和脉冲条件下均为f_(N2)。但是,脉冲CrN_x涂层的N浓度低于在相同f_(N2)下制备的dc CrN_x涂层的N浓度,这导致在宽范围的f_(N2)(30-50%)中存在β-Cr_2N相。与直流溅射镀膜中典型的大柱状结构相比,脉冲CrN_x镀膜具有显着的微观结构改善,这得益于改善的等离子体密度和脉冲等离子体的离子轰击,其中观察到了超致密和近等轴结构。 f_(N2)的范围很广。微观结构的改善有助于提高脉冲CrN_x涂层的硬度和耐磨性。在脉冲CrN_x涂层中,当f_(N2)在30%至40%的范围内时,硬度值高于30 GPa,这与β-Cr_2N相的形成有关。在沉积有40-50%f_(N2)的涂层中形成β-Cr_2N和c-CrN相的混合物时,低COF为0.36,磨损率为1.66×10〜(-6)mm〜3N〜可以达到(-1)m〜(-1)

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