One-click electromagnetism at the nanoscale
The extinction (UV-vis), absorption and scattering spectrum of silver nanospheres of any size, in any solvent, with or without a shell: in one click, from exact Mie theory. Set the diameter and press Calculate.
Spheres in water, from exact Mie theory with this site's solver (the calculator above gives the full spectrum for any size, solvent or coating).
| Diameter | Plasmon peak (λmax) | Molar extinction coefficient at λmax | Scattering share |
|---|---|---|---|
| 5 nm | 384 nm | 3.19 × 108 M−1 cm−1 | < 1 % |
| 10 nm | 385 nm | 2.52 × 109 M−1 cm−1 | 2 % |
| 15 nm | 386 nm | 8.06 × 109 M−1 cm−1 | 8 % |
| 20 nm | 388 nm | 1.75 × 1010 M−1 cm−1 | 17 % |
| 30 nm | 393 nm | 4.36 × 1010 M−1 cm−1 | 41 % |
| 40 nm | 400 nm | 6.89 × 1010 M−1 cm−1 | 62 % |
| 50 nm | 408 nm | 8.84 × 1010 M−1 cm−1 | 76 % |
| 60 nm | 419 nm · 2nd peak 374 nm | 1.04 × 1011 M−1 cm−1 | 86 % |
| 70 nm | 431 nm · 2nd peak 377 nm | 1.18 × 1011 M−1 cm−1 | 92 % |
| 80 nm | 446 nm · 2nd peak 380 nm | 1.29 × 1011 M−1 cm−1 | 94 % |
| 90 nm | 461 nm · 2nd peak 385 nm | 1.39 × 1011 M−1 cm−1 | 95 % |
| 100 nm | 481 nm · 2nd peak 390 nm | 1.50 × 1011 M−1 cm−1 | 96 % |
| 125 nm | 533 nm · 2nd peak 406 nm | 1.82 × 1011 M−1 cm−1 | 97 % |
| 150 nm | 601 nm · 2nd peak 427 nm | 2.20 × 1011 M−1 cm−1 | 98 % |
| 200 nm | 759 nm · 2nd peak 485 nm | 3.19 × 1011 M−1 cm−1 | 99 % |
Silver optical constants: Johnson & Christy (1972); water: Hale & Querry (1973). Plasmon peak: the dipole (longest-wavelength) extinction maximum; the second, shorter-wavelength peak of large particles is the quadrupole. Molar extinction coefficient ε = NA Cext / (1000 ln 10), so the particle concentration is c = A / (ε ℓ). Scattering share: Csca / Cext at the peak. Below about 10 nm real particles show broader, weaker peaks (electron surface scattering) than bulk optical constants give.