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The influence of film-to-substrate characteristics on the electron field emission behavior of the diamond films

机译:膜对衬底特性对金刚石膜电子发射特性的影响

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Diamond films possessing large electron field emission properties were obtained usingB(OCH{sub}3){sub}3 as dopants in chemical vapor deposition process. TheCH{sub}4:B(OCH{sub}3){sub}3 ratio and total gas flow rate markedly influenced the emissioncurrent density (J{sub}e) without significantly altering the turn-on electric field (E{sub}0) andeffective work function (Φ{sub}e) of the films. The emission current density attainable is(J{sub}e){sub}(Si) =280μA/cm{sup}2 (at 20 V/μm) with (E{sub}0){sub}(Si) = 10.2 V/μm and(Φ{sub}e){sub}(Si) = 0.0934 eV for the films deposited usingCH{sub}4:B(OCH{sub}3){sub}3:H{sub}2= 18:6:300 sccm. Analysis using Raman spectroscopyrevealed that the improvement of the J{sub}e value could be attributed to the modification on thedefect concentration of the films. Precoating an Au layer on Si substrates pronouncedly lowered theturn-on electric field to [(E{sub}0){sub}(Au/Si = 7.1 V/μm] without markedly altering the effectivework function [(Φ{sub}e)(Au/Si)=0.0534 eV]. This is ascribed to a modification on the film-to-substrate interface which reduced the conduction barrier for electrons to transport from substrates tothe emission sites, i.e. the diamond surfaces. The emission current density attainable is(J{sub}e)(Au/Si)=700μA/cm{sup}2 (at 20 V/μm).
机译:以B(OCH {sub} 3){sub} 3为掺杂剂,在化学气相沉积工艺中获得了具有较大电子场发射性能的金刚石薄膜。 CH {sub} 4:B(OCH {sub} 3){sub} 3的比率和总气体流量显着影响发射电流密度(J {sub} e),而不会显着改变开启电场(E {sub} 0)和胶片的有效功函数(Φ{sub} e)。在(E {sub} 0){sub}(Si)= 10.2的情况下,可获得的发射电流密度为(J {sub} e){sub}(Si)=280μA/ cm {sup} 2(在20 V /μm时)对于使用CH {sub} 4:B(OCH {sub} 3){sub} 3:H {sub} 2 = 18沉积的薄膜,V /μm和(Φ{sub} e){sub}(Si)= 0.0934 eV :6:300 sccm。利用拉曼光谱分析表明,J e值的提高可以归因于膜缺陷浓度的改变。在Si基板上预涂Au层可显着降低开启电场至[(E {sub} 0){sub}(Au / Si = 7.1 V /μm],而不会显着改变有效功函数[(Φ{sub} e) (Au / Si)= 0.0534 eV]。这归因于膜-基底界面上的修饰,该修饰降低了电子从基底传输到发射位置(即金刚石表面)的传导势垒。 (J {sub} e)(Au / Si)=700μA/ cm {sup} 2(在20 V /μm时)。

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