text: In oxygen: 
  * the Hopfield bands, very strong, between about 67 and 100 nanometres in the ultraviolet (named after John J. Hopfield);
  * a diffuse system between 101.9 and 130 nanometres;
  * the Schumann–Runge continuum, very strong, between 135 and 176 nanometres;
  * the Schumann–Runge bands between 176 and 192.6 nanometres (named for Victor Schumann and Carl Runge);
  * the Herzberg bands between 240 and 260 nanometres (named after Gerhard Herzberg);
  * the atmospheric bands between 538 and 771 nanometres in the visible spectrum; including the oxygen δ (~580 nm), γ (~629 nm), B (~688 nm), and A-band (~759-771 nm)
  * a system in the infrared at about 1000 nanometres.
  In ozone:
  * the Hartley bands between 200 and 300 nanometres in the ultraviolet, with a very intense maximum absorption at 255 nanometres (named after Walter Noel Hartley);
  * the Huggins bands, weak absorption between 320 and 360 nanometres (named after Sir William Huggins);
  * the Chappuis bands (sometimes misspelled "Chappius"), a weak diffuse system between 375 and 650 nanometres in the visible spectrum (named after J. Chappuis); and
  * the Wulf bands in the infrared beyond 700 nm, centered at 4,700, 9,600 and 14,100 nanometres, the latter being the most intense (named after Oliver R. Wulf).
  In nitrogen:
  * The Lyman–Birge–Hopfield bands, sometimes known as the Birge–Hopfield bands, in the far ultraviolet: 140&ndash; 170 nm (named after Theodore Lyman, Raymond T. Birge, and John J. Hopfield)