首页> 外文会议>Advanced Devices and Materials for Laser Remote Sensing >LUMINESCENCE OF RARE EARTH DOPED Si/ZrO_2 CO-SPUTTERED FILMS
【24h】

LUMINESCENCE OF RARE EARTH DOPED Si/ZrO_2 CO-SPUTTERED FILMS

机译:稀土掺杂Si / ZrO_2共溅射薄膜的发光强度

获取原文
获取原文并翻译 | 示例

摘要

Er~(3+), Nd~(3+) and Tm~(3+) doped Si/ZrO_2 thin films have been prepared by rf co-sputtering. The films are 5 inches long and divided into 50 sections or positions, labeled from P1 to P50. The target configuration is such that the main target is ZrO_2 (181.46 cm~2), the rare earth (RE) oxide pellet (1.43 cm~2) is placed on the main target below the middle of section of the film and the Si chip (6.67 cm~2 or 6.00 cm~2) is placed on the main target below one end of the film (P40 to P50). The films were annealed to 700℃. The Er~(3+) ~4I_(13/2) → ~4I_(15/2) emission was detected but no ~4I_(11/2) → ~4I_(15/2) emission was detected. The ~4I_(13/2) → ~4I_(15/2) emision shows a narrow peak at 1527 nm (FWHM = 6.5 nm for P20) with two weaker side bands from 1430 nm to 1500 nm and from 1550 nm to 1600 nm. The Nd~(3+) ~4I_(3/2) → ~4I_(9/2), ~4I_(3/2) → ~4I_(11/2), and ~4I_(3/2) → ~4I_(13/2) emissions were detected being the ~4I_(3/2) → ~4I_(11/2) peaked at 1065 nm (FWHM = 39.5 nm for P30) the strongest. The ~4I_(3/2) → ~4I_(9/2) emission is relatively weak, less than one-fourth the peak intensity of the ~4I_(3/2) → ~4I_(11/2) emission but is broad (FWHM = 92 nm for P30). No Er~(3+) ~4I_(13/2) → ~4I_(15/2) emission or Nd~(3+) ~4F_(3/2) emissions were detected for the Si rich ends of the respective films, being the emission stronger from the Si poor end of the film towards the middle of the film. The maximum Er~(3+) ~4I_(13/2) → ~4I_(15/2) emission is for P20 and the maximum peak intensity for the Nd~(3+) ~4I_(3/2) → ~4I_(11/2) emission is for P30. The excitation wavelength dependence behavior for the Nd~(3+) ~4I_(3/2) → ~4I_(11/2) emission is that typical of energy transfer from the Si nanoparticles to the emitting Nd~(3+) ions. The excitation wavelength behavior for the Er~(3+) ~4I_(13/2) → ~4I_(15/2) emission reflects a mix of energy transfer from the Si nanoparticles and strong absorption for excitation wavelengths of 488.0 nm and 514.5 nm. The Tm~(3+) doped Si/ZrO_2 thin film does not exhibit infrared (IR) PL from the ~3H_4 → ~3F_4 emission or the ~3F_4 → ~3H_6 emission. The intense band from 500 nm to 800 nm observed for all of the RE doped Si/ZrO_2 films, due to defects in ZrO_2, barely permits the detection of the Tm~(3+) ~3H_4 → ~3H_6 emission which is best observed for P35.
机译:通过射频共溅射制备了Er〜(3 +),Nd〜(3+)和Tm〜(3+)掺杂的Si / ZrO_2薄膜。胶片长5英寸,分为50个部分或位置,标记为P1至P50。靶材的配置应使主要靶材为ZrO_2(181.46 cm〜2),将稀土(RE)氧化物颗粒(1.43 cm〜2)放置在膜和硅片中间的下方的主要靶材上将(6.67 cm〜2或6.00 cm〜2)(6.67 cm〜2)放置在胶片一端(P40至P50)下方的主要目标上。将膜退火至700℃。检测到Er〜(3+)〜4I_(13/2)→〜4I_(15/2)发射,但未检测到〜4I_(11/2)→〜4I_(15/2)发射。 〜4I_(13/2)→〜4I_(15/2)表示在1527 nm处出现一个窄峰(对于P20,FWHM = 6.5 nm),其中有两个较弱的边带,分别为1430 nm至1500 nm和1550 nm至1600 nm。 。 Nd〜(3+)〜4I_(3/2)→〜4I_(9/2),〜4I_(3/2)→〜4I_(11/2)和〜4I_(3/2)→〜4I_检测到(13/2)的发射是〜4I_(3/2)→〜4I_(11/2)在1065 nm处达到峰值(对于P30,FWHM = 39.5 nm)最强。 〜4I_(3/2)→〜4I_(9/2)发射相对较弱,不到〜4I_(3/2)→〜4I_(11/2)发射的峰值强度的四分之一,但较宽(对于P30,FWHM = 92 nm)。对于各膜的富Si端,未检测到Er〜(3+)〜4I_(13/2)→〜4I_(15/2)发射或Nd〜(3+)〜4F_(3/2)发射,从薄膜的Si不良端到薄膜中间的发射强度更大。最大的Er〜(3+)〜4I_(13/2)→〜4I_(15/2)发射是针对P20,最大的峰值强度是针对Nd〜(3+)〜4I_(3/2)→〜4I_ (11/2)发射用于P30。 Nd〜(3+)〜4I_(3/2)→〜4I_(11/2)发射的激发波长依赖性行为是典型的从Si纳米粒子到发射Nd〜(3+)离子的能量转移。 Er〜(3+)〜4I_(13/2)→〜4I_(15/2)发射的激发波长行为反映了Si纳米粒子的能量转移和对488.0 nm和514.5 nm激发波长的强吸收的混合。掺杂有Tm〜(3+)的Si / ZrO_2薄膜在〜3H_4→〜3F_4发射或〜3F_4→〜3H_6发射时不显示红外(IR)PL。由于ZrO_2中的缺陷,所有掺稀土的Si / ZrO_2薄膜在500 nm至800 nm处观察到了很强的谱带,几乎无法检测到Tm〜(3+)〜3H_4→〜3H_6发射,这对于P35。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号