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. 2011 Mar 8;6(1):199. doi: 10.1186/1556-276X-6-199

Table 1.

Summary of representative experimental results showing the important relationship between the LSPR energy and emission energy in order to attain the best enhancement

Emitting materials and configurations Peak emission energy (nm) Metal used Optical properties of metal layer Enhancement References
InGaN/GaN multiple QW 463 Ag Transmittance exhibits absorption from 396 to 455 nm 32.2% with an 100-mA current Kwon et al. [33]
Alq3 thin film 525 Au A peak in absorption at 510 nm 20-fold Fujiki et al. [34]
InGaN/GaN QW 550 Ag A dip in transmission at about 550 nm 150% in peak intensity with a 20-mA current Yeh et al. [36]
InGaN/GaN QW 465 Au A dip in transmission in 511 nm 180% with a 20-mA current Sung et al. [37]
Organic poly 575 Ag Large absorption from 330 to 500 nm Sixfold Qiu et al. [41]
Si QD 600 Ag A peak in absorption at 535 nm Reaches maximum at 530 nm Kim et al. [42]
ZnMgO alloys 357 Pt Extinction band near 350 nm Sixfold You et al. [44]
ZnO film 380 Ag Extinction band near 370 nm Threefold Cheng et al. [45]
Si-on-insulator 1,140 Ag A dip in transmission at about 520 nm 2.5-fold in peak intensity Pillai et al. [48]
CdSe/ZnS nanocrystals 580 Au A peak in absorption at about 600 nm 30-fold Pompa et al. [53]
Si QD 775 Ag A dip in transmission at 710 nm Twofold, with the peak blue shifts Biteen et al. [54]
GaN 440 Ag A dip in transmission at about 440 nm Twofold Mak et al. [62]