Lecture #12 OUTLINE • Metal-semiconductor contacts (cont.) – I-V characteristics Reading: Finish 14.2 Spring 2007 EE130 Lecture 12, Slide 1 Current Flow in a Schottky Diode FORWARD BIAS REVERSE BIAS Spring 2007 • Current is determined by majority-carrier flow across the MS junction: – Under forward bias, majority-carrier diffusion from the semiconductor into the metal dominates – Under reverse bias, majority-carrier diffusion from the metal into the semiconductor dominates EE130 Lecture 12, Slide 2 Voltage Drop across the MS Diode • Under equilibrium conditions (VA = 0), the voltage drop across the semiconductor depletion region is the built-in voltage Vbi. • If VA 0, the voltage drop across the semiconductor depletion region is Vbi - VA. Spring 2007 EE130 Lecture 12, Slide 3 Depleted Layer Width, W, for VA 0 Last time, we found that V x qN D W x 2 2K S 0 At x = 0, V = - (Vbi - VA) 2 s (Vbi VA ) W qN D • W increases with increasing –VA • W decreases with increasing ND - (Vbi - VA) Spring 2007 EE130 Lecture 12, Slide 4 W for p-type Semiconductor V x qN A W x 2 2 K S 0 At x = 0, V = Vbi + VA 2 s (VA Vbi ) W qN A • W increases with increasing VA • W decreases with increasing NA Spring 2007 EE130 Lecture 12, Slide 5 Thermionic Emission Theory • Electrons can cross the junction into the metal if 1 2 K.E. x mvx qVbi VA 2 2q Vbi VA vx vmin * mn • Thus the current for electrons at a given velocity is: I s M , v x qAvx n(vx ) • So, the total current over the barrier is: v min I s M qA v n(v )dv x Spring 2007 EE130 Lecture 12, Slide 6 x x Schottky Diode I - V • For a nondegenerate semiconductor, it can be shown that 4kTm*2 * 2 nv x n h3 EF Ec / kT mn / 2 kT v x e e • We can then obtain 4qmn* k 2 2 F B / kT qVA / kT I S M AT e e 3 h * m AJ S e qVA / kT , where J S 120 n T 2 e F B / kT A/cm 2 m0 • In the reverse direction, the electrons always see the same barrier FB, so I M S I S M VA 0 • Therefore Spring 2007 I I S (e qVA / kT 1) where I S AJ S EE130 Lecture 12, Slide 7 Applications of Schottky Diodes • IS of a Schottky diode is 103 to 108 times larger than that of a pn junction diode, depending on FB . Schottky diodes are preferred rectifiers for lowvoltage, high-current applications. Spring 2007 EE130 Lecture 12, Slide 8 Summary • In a Schottky contact, charge is stored on either side of the MS junction – The applied bias VA modulates this charge and thus the voltage drop across the semiconductor depletion region Flow of majority carriers into the metal varies exponentially with VA J J S (e qVA / kT 1) mn* 2 qF B / kT where J S 120 T e A/cm 2 m0 Spring 2007 EE130 Lecture 12, Slide 9