78 CHAPTER 2. ELECTRONIC LEVELS IN SEMICONDUCTORS
E 2Ec (bulk)–W/ 2 0 +W/ 2zE 1E 2
E 1k 11E = h^2 k// + E 2
2 m*EnergyP arabol i c two- di mensi onal subbandsΔEcE = h^2 k// + E 1
2m*E 1 (HH)
E 1 (L H)
E 2 (HH)
E 2 (L H)
L i ght hol e
subbandsHeavy hole
subbandsValence
bandC onducti on
bandEv (bulk)Density of statesE ffective gap
Well gapQ uantum wel l E vs k 1122Figure 2.33: Schematic of density of states in a 3–, 2– and 1–dimensional system. The subband
structure is shown.