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Intense 1.54 μm fluorescence of Er~(3+)/Yb~(3+) codoped phosphate glass and the three-photon phenomenon of near infrared upconversion luminescence

机译:Er〜(3 +)/ Yb〜(3+)共掺杂磷酸盐玻璃的1.54μm强烈荧光和近红外上转换发光的三光子现象

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摘要

Transparent P_2O_5-CaO-Na_2O glasses codoped with Er~(3+) and Yb~(3+) ions were fabricated by high-temperature melting technique. Strong near infrared and visible upconversion luminescence were observed under 975 nm laser diode excitation, and the luminescence processes were explained in details. For 1.54 μm band, the calculated peak emission cross sections is 1.04×10~(-20) cm~2, and it is better than that in germinate, tellurite, silicate, and other phosphate glasses. The near infrared upconversion emission around 828 nm contains two-photon and three-photon processes, and it is attributed to the transition ~4S_(3/2)→~4I_(13/2), which enhances the population of the upper level for 1.54 μm laser emission and reduces the energy loss due to upconversion. Efficient near infrared fluorescence indicates Er~(3+)/Yb~(3+) codoped phosphate glass is a promising laser and amplifier material.
机译:通过高温熔融技术制备了掺有Er〜(3+)和Yb〜(3+)离子的透明P_2O_5-CaO-Na_2O玻璃。在975nm激光二极管激发下观察到强的近红外和可见的上转换发光,并且详细解释了发光过程。在1.54μm波段,计算出的峰值发射截面为1.04×10〜(-20)cm〜2,优于发芽,亚碲酸盐,硅酸盐及其他磷酸盐玻璃。 828 nm附近的近红外上转换发射包含两个光子和三个光子过程,这归因于〜4S_(3/2)→〜4I_(13/2)跃迁,从而增加了高能级的数量。 1.54μm激光发射并减少了由于上变频引起的能量损失。有效的近红外荧光表明Er〜(3 +)/ Yb〜(3+)共掺杂磷酸盐玻璃是一种很有前途的激光器和放大器材料。

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  • 来源
    《Journal of Applied Physics》 |2010年第3期|033110.1-033110.5|共5页
  • 作者单位

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

    Photonics Center, College of Physical Science, Nankai University, Tianjin 300071, People's Republic of China The Key Laboratory of Weak Light Nonlinear Photonics, Ministry of Education, Nankai University, Tianjin 300457, People's Republic of China;

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