Near-infrared free carrier absorption enhancement of heavily doped silicon in all-dielectric metasurface

2020 ◽  
Vol 117 (13) ◽  
pp. 134101
Author(s):  
Honghao Yu ◽  
Qing Xiong ◽  
Hong Wang ◽  
Ye Zhang ◽  
Yi Wang ◽  
...  
2014 ◽  
Vol 116 (6) ◽  
pp. 063106 ◽  
Author(s):  
Simeon C. Baker-Finch ◽  
Keith R. McIntosh ◽  
Di Yan ◽  
Kean Chern Fong ◽  
Teng C. Kho

2004 ◽  
Vol 84 (13) ◽  
pp. 2265-2267 ◽  
Author(s):  
Joerg Isenberg ◽  
Wilhelm Warta

1991 ◽  
Vol 69 (6) ◽  
pp. 3687-3690 ◽  
Author(s):  
S. C. Jain ◽  
A. Nathan ◽  
D. R. Briglio ◽  
D. J. Roulston ◽  
C. R. Selvakumar ◽  
...  

2021 ◽  
Vol 8 ◽  
Author(s):  
Di Sun ◽  
Yu Fang ◽  
Xiaoyan Yan ◽  
Wen Shan ◽  
Wenjun Sun ◽  
...  

Transition metal-doped Sb2Se3 has become a heated topic caused by the strong nonlinear optical response and the ultrafast response time at high laser excitation. In this paper, the Co-doped Sb2Se3 with different doping amount (0.5, 1.0, and 1.5 W) nanofilms were prepared by magnetron sputtering technology, and the nonlinear behavior of Co-doped Sb2Se3 nanofilms at near infrared were systematically studied. The results of the femtosecond Z-Scan experiment indicate that the Co-doped Sb2Se3 nanofilms exhibit broadband nonlinear response properties owing to the free carrier absorption, the Kerr refraction, the two-photon absorption, and the free carrier refraction. The nonlinear absorption coefficients of Co-doped Sb2Se3 nanofilms are from 3.0 × 10−9 to 2.03 × 10−8 m/ W under excitation at 800, 980, and 1,030 nm, and the nonlinear refractive index of the Co-doped Sb2Se3 nanofilms is from 4.0 × 10−16 to -3.89 × 10−15 m2/ W at 800, 980, and 1,030 nm. More importantly, Co-doped Sb2Se3 (1.5 W) nanofilm exhibits ultrafast carrier absorption (<1 ps) and a stronger transient absorption intensity of ΔOD > 6.3. The Co-doping content can controllably tune the crystalline degree, the ultrafast carrier absorption, the intensity of the reverse saturation absorption, the broadband nonlinear optical response, and the carrier relaxation time of Co-doped Sb2Se3 nanofilms. These results are sufficient to support their applications in broadband nonlinear photonic devices.


2013 ◽  
Vol 60 (7) ◽  
pp. 2156-2163 ◽  
Author(s):  
Marc Rudiger ◽  
Johannes Greulich ◽  
Armin Richter ◽  
Martin Hermle

ACS Photonics ◽  
2018 ◽  
Vol 5 (9) ◽  
pp. 3472-3477 ◽  
Author(s):  
Mehbuba Tanzid ◽  
Arash Ahmadivand ◽  
Runmin Zhang ◽  
Ben Cerjan ◽  
Ali Sobhani ◽  
...  

2009 ◽  
Vol 34 (21) ◽  
pp. 3397 ◽  
Author(s):  
Rohan D. Kekatpure ◽  
Mark L. Brongersma

1985 ◽  
Vol 59 ◽  
Author(s):  
R. J. Bleiler ◽  
R. S. Hockett ◽  
P. Chu ◽  
E. Strathman

ABSTRACTOxygen precipitation in CZ silicon is known to provide beneficial yield improvements in integrated circuit processing if the location and amount of precipitation can be properly controlled. The concentration of oxygen in the unprocessed silicon substrate is one of the most important variables to control for achieving these improvements. Fourier Transform Infrared Spectroscopy (FTIR) has successfully been used to measure [0] in silicon when the silicon resistivity is greater than about 0.1 Ω-cm. At lower resistivities typical of p+ and n+ substrates used for epi-wafers as free carrier absorption interferes with the FTIR measurement of bulk [0].This work will focus on how to quantitatively measure oxygen in heavily-doped silicon by Secondary Ion Mass Spectrometry (SIMS) with a high sample thruput, low background signal, and tight σ/x distribution. SIMS calibration is performed against FTIR-calibrated substrates with resistivity higher than 0.1Ωcm. Typical background signals as measured in FZ are a factor of 20 below signals in CZ, and the 160− signal in CZ is over 105 count/sec. resulting in an excellent signal-to-noise ratio for each single measurement. Typical thruput is 18 samples per day where each sample is analyzed four to five times to obtain a σ/x of 3% for an oxygen level of 15 ppma (ASTM F121−80).


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