Nanostructures – density of states Faculty of Physics UW
[email protected] Local density of states Gęstość stanów (ogólnie) można zdefiniować jako: 푁 퐸 = 훿 퐸 − 휀푛 푛 Jak widać po scałkowaniu: 퐸2 퐸2 퐸2 න 푁 퐸 푑퐸 = න 훿 퐸 − 휀푛 푑퐸 = න 훿 퐸 − 휀푛 푑퐸 퐸1 퐸1 푛 푛 퐸1 Przykładowo: 1 1 1 2푚 푁1퐷 퐸 = 훿 퐸 − 휀 푘 = න 훿 푘 − 푘′ 2 푑푘 = 2π 퐸′ 푘 휋 퐸 푘 1 1 푚 푁2퐷 퐸 = 훿 퐸 − 휀 푘 = න 훿 푘 − 푘′ 2휋푘 푑푘 = 2π 2 퐸′ 푘 휋ℏ2 푘 3/2 1 1 1 2푚 푁3퐷 퐸 = 훿 퐸 − 휀 푘 = න 훿 푘 − 푘′ 4휋푘2 푑푘 = 퐸 2π 3 퐸′ 푘 2휋2 ℏ2 푘 2017-06-05 2 Electrons statistics in crystals The case of a semiconductor, in which both the electron gas and hole gas are far from the degeneracy: the probability of filling of the electronic states: 퐸 퐸 휉 − 퐺 − 푒 + 퐸퐺 푓 ≈ 푒 2푘퐵푇 푘퐵푇 푘퐵푇 퐸 = + 퐸 퐸푒 푒 2 푒 퐸푐 and of holes 푓ℎ = 1 − 푓푒 퐸 퐸 휉 − 퐺 − ℎ − 2푘 푇 푘 푇 푘 푇 푓ℎ ≈ 푒 퐵 퐵 퐵 ∞ 휋 න 푥푒−푥 푑푥 = 2 0 퐸푣 퐸퐺 Thus: 퐸 = − − 퐸ℎ 퐸ℎ ∗ 3/2 퐸 휉 − 퐸 −휉 2 푚푒푘퐵푇 − 퐺 푐 푛 휉 = 2 푒 2푘퐵푇 ⋅ 푒푘퐵푇 = 푁 푇 푒 푘퐵푇 2휋ℏ2 푐 ∗ 3/2 퐸 휉 − 휉−퐸 푚ℎ푘퐵푇 − 퐺 − 푣 푝 휉 = 2 푒 2푘퐵푇 ⋅ 푒 푘퐵푇 = 푁 푇 푒 푘퐵푇 2휋ℏ2 푣 2017-06-05 3 Electrons statistics in crystals What is the concentration of carriers for T>0? In the thermodynamic equilibrium for an intrinsic semiconductors (półprzewodniki samoistne), the concentration of electrons in the conduction band is equal to the concnetration of holes in the valence band (because they appear only as a result of excitation from the valence band).