热电材料可以将热能直接转化为电能,在回收利用废热发电领域有巨大潜力。相比于无机热电材料,有机热电材料具有机械柔性,适用于智能穿戴设备。利用具有优良平面性的噻吩基异靛青(TIIG)和含有烷氧噻吩侧链的苯并[1,2-b:4,5-b']二噻吩...热电材料可以将热能直接转化为电能,在回收利用废热发电领域有巨大潜力。相比于无机热电材料,有机热电材料具有机械柔性,适用于智能穿戴设备。利用具有优良平面性的噻吩基异靛青(TIIG)和含有烷氧噻吩侧链的苯并[1,2-b:4,5-b']二噻吩(BDT-TO)分别为电子受体和电子给体,设计合成了一种新型给受体(D-A)共轭聚合物。该聚合物有优良的溶解性和热稳定性以及较窄的带隙。聚合物薄膜经过FeCl_(3)/CH_(3)NO_(2)氧化掺杂后,电导率最高可达1.80 S cm^(-1),最优热电性能0.23μW m^(-1) K^(-2)。展开更多
In this paper, a self-mode-locked Nd:YVO_4 picosecond vortex laser is demonstrated, which can operate on the different Laguerre-Gaussian(LG) modes at 1 064 nm. A π/2 mode converter is utilized to realize the picoseco...In this paper, a self-mode-locked Nd:YVO_4 picosecond vortex laser is demonstrated, which can operate on the different Laguerre-Gaussian(LG) modes at 1 064 nm. A π/2 mode converter is utilized to realize the picosecond vortex laser with LG mode transformed from the high-order Hermite-Gaussian(HG) mode. For the proposed laser, the mode-locked pulse repetition rate is 1.81 GHz. The average output powers of LG_(12) mode and LG_(02) mode are 1.241 W and 1.27 W, respectively, and their slope efficiencies are 23.2% and 24%, respectively.展开更多
文摘热电材料可以将热能直接转化为电能,在回收利用废热发电领域有巨大潜力。相比于无机热电材料,有机热电材料具有机械柔性,适用于智能穿戴设备。利用具有优良平面性的噻吩基异靛青(TIIG)和含有烷氧噻吩侧链的苯并[1,2-b:4,5-b']二噻吩(BDT-TO)分别为电子受体和电子给体,设计合成了一种新型给受体(D-A)共轭聚合物。该聚合物有优良的溶解性和热稳定性以及较窄的带隙。聚合物薄膜经过FeCl_(3)/CH_(3)NO_(2)氧化掺杂后,电导率最高可达1.80 S cm^(-1),最优热电性能0.23μW m^(-1) K^(-2)。
基金supported by the National Natural Science Foundation of China(No.61108021)the Fundamental Research Funds for the Central Universities(Nos.2013JBM091 and S16JB00010)
文摘In this paper, a self-mode-locked Nd:YVO_4 picosecond vortex laser is demonstrated, which can operate on the different Laguerre-Gaussian(LG) modes at 1 064 nm. A π/2 mode converter is utilized to realize the picosecond vortex laser with LG mode transformed from the high-order Hermite-Gaussian(HG) mode. For the proposed laser, the mode-locked pulse repetition rate is 1.81 GHz. The average output powers of LG_(12) mode and LG_(02) mode are 1.241 W and 1.27 W, respectively, and their slope efficiencies are 23.2% and 24%, respectively.