Wee Tse-Luen, Tzeng Yan-Kai, Han Chau-Chung, Chang Huan-Cheng, Fann Wunshain, Hsu Jui-Hung, Chen Kuan-Ming, Yu Yueh-Chung
Institute of Atomic and Molecular Sciences, Academia Sinica, Taipei 106, Taiwan.
J Phys Chem A. 2007 Sep 27;111(38):9379-86. doi: 10.1021/jp073938o. Epub 2007 Aug 18.
Two-photon fluorescence spectroscopy of negatively charged nitrogen-vacancy [(N-V)-] centers in type Ib diamond single crystals have been studied with a picosecond (7.5 ps) mode-locked Nd:YVO(4) laser operating at 1064 nm. The (N-V)- centers were produced by radiation damage of diamond using a 3 MeV proton beam, followed by thermal annealing at 800 degrees C. Prior to the irradiation treatment, infrared spectroscopy of the C-N vibrational modes at 1344 cm(-1) suggested a nitrogen content of 109 +/- 10 ppm. Irradiation and annealing of the specimen led to the emergence of a new absorption band peaking at approximately 560 nm. From a measurement of the integrated absorption intensity of the sharp zero-phonon line (637 nm) at liquid nitrogen temperature, we determined a (N-V)- density of (4.5 +/- 1.1) x 10(18) centers/cm3 (or 25 +/- 6 ppm) for the substrate irradiated at a dose of 1 x 1016) H(+)/cm(2). Such a high defect density allowed us to observe two-photon excited fluorescence and measure the corresponding fluorescence decay time. No significant difference in the spectral feature and fluorescence lifetime was observed between one-photon and two-photon excitations. Assuming that the fluorescence quantum yields are the same for both processes, a two-photon absorption cross section of sigma(TPA) = (0.45 +/- 0.23) x 10(-50) cm(4).s/photon at 1064 nm was determined for the (N-V)- center based on its one-photon absorption cross section of sigma(OPA) = (3.1 +/- 0.8) x 10(-17) cm2 at 532 nm. The material is highly photostable and shows no sign of photobleaching even under continuous two-photon excitation at a peak power density of 3 GW/cm(2) for 5 min.
利用一台工作波长为1064 nm的皮秒(7.5 ps)锁模Nd:YVO₄激光器,对Ib型金刚石单晶中带负电荷的氮空位[(N-V)⁻]中心进行了双光子荧光光谱研究。通过用3 MeV质子束对金刚石进行辐射损伤,随后在800℃下进行热退火,产生了(N-V)⁻中心。在辐照处理之前,1344 cm⁻¹处C-N振动模式的红外光谱表明氮含量为109±10 ppm。样品的辐照和退火导致出现一个新的吸收带,其峰值位于约560 nm处。通过测量液氮温度下尖锐零声子线(637 nm)的积分吸收强度,我们确定了在剂量为1×10¹⁶ H⁺/cm²下辐照的衬底中(N-V)⁻密度为(4.5±1.1)×10¹⁸个中心/cm³(或25±6 ppm)。如此高的缺陷密度使我们能够观察到双光子激发荧光并测量相应的荧光衰减时间。在单光子和双光子激发之间,未观察到光谱特征和荧光寿命的显著差异。假设两个过程的荧光量子产率相同,基于其在532 nm处的单光子吸收截面σ(OPA) =(3.1±0.8)×10⁻¹⁷ cm²,确定了(N-V)⁻中心在1064 nm处的双光子吸收截面σ(TPA) =(0.45±0.23)×10⁻⁵⁰ cm⁴·s/光子。该材料具有高度的光稳定性,即使在峰值功率密度为3 GW/cm²的连续双光子激发下持续5分钟,也没有光漂白的迹象。