Low-pump sum frequency generation of frequency-stabilized 453 nm blue laser for photonic quantum interface

Jian Wang; Yuhao Pan; Yunfeng Huang; Chuanfeng Li; Guangcan Guo

doi:doi:10.3788/COL201715.122701

Chinese Optics Letters, 2017, 15 (12): 122701, Published Online: Jul. 18, 2018

Low-pump sum frequency generation of frequency-stabilized 453 nm blue laser for photonic quantum interface

Jian Wang ^1,2Yuhao Pan ^1,2Yunfeng Huang ^1,2,*Chuanfeng Li ^1,2Guangcan Guo ^1,2

Author Affiliations

¹ CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China

² Synergetic Innovation Centre in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei 230026, China

Figures & Tables

Fig. 1. (Color online) Experimental setup. BS, beam splitter; DM, dichroic mirror; IF, interference filter; A-lens, aspheric lens; PM, power meter; WG, waveguide. The red line represents the 880 nm laser, the gray line represents the 935 nm laser, and the blue line represents the 453 nm pump laser. DMs are used here to combine the 935 nm laser and the 880 nm laser together.

下载图片查看原文

Fig. 2. Relation between the 453 nm laser output and the temperature of the PPLN waveguide.

下载图片查看原文

Fig. 3. Relation between the output power of the generated 453 nm laser with input power of the 935 nm laser. Here, the input power of the 880 nm laser is 12 mW, and the biggest power of the 935 nm laser is 48 mW.

下载图片查看原文

Fig. 4. Relation between the conversion efficiency and the input power of the 935 nm laser.

下载图片查看原文

Fig. 5. Measurement of the long-term stability of the generated blue laser.

下载图片查看原文

Jian Wang, Yuhao Pan, Yunfeng Huang, Chuanfeng Li, Guangcan Guo. Low-pump sum frequency generation of frequency-stabilized 453 nm blue laser for photonic quantum interface[J]. Chinese Optics Letters, 2017, 15(12): 122701.

Low-pump sum frequency generation of frequency-stabilized 453 nm blue laser for photonic quantum interface

Fig. 2. Relation between the 453 nm laser output and the temperature of the PPLN waveguide.

Fig. 3. Relation between the output power of the generated 453 nm laser with input power of the 935 nm laser. Here, the input power of the 880 nm laser is 12 mW, and the biggest power of the 935 nm laser is 48 mW.

Fig. 4. Relation between the conversion efficiency and the input power of the 935 nm laser.

Fig. 5. Measurement of the long-term stability of the generated blue laser.

关于本站 Cookie 的使用提示

全站搜索

Low-pump sum frequency generation of frequency-stabilized 453 nm blue laser for photonic quantum interface

Fig. 2. Relation between the 453 nm laser output and the temperature of the PPLN waveguide.

Fig. 3. Relation between the output power of the generated 453 nm laser with input power of the 935 nm laser. Here, the input power of the 880 nm laser is 12 mW, and the biggest power of the 935 nm laser is 48 mW.

Fig. 4. Relation between the conversion efficiency and the input power of the 935 nm laser.

Fig. 5. Measurement of the long-term stability of the generated blue laser.

相关论文

相关资讯

关于本站 Cookie 的使用提示

全站搜索