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Solid State Electronic Devices

Ben G. Streetman, Sanjay Kumar Banerjee

Chapter 5

Junctions - all with Video Answers

Educators


Chapter Questions

01:55

Problem 1

A 900 -nm oxide is grown on (100) Si in wet oxygen at $1100^{\circ} \mathrm{C}$ (see Appendix VI). How long does it take to grow the first $200 \mathrm{~nm}$, the next $300 \mathrm{~nm}$, and the final $400 \mathrm{~nm} ?$
A square window $(1 \mathrm{~mm} \times 1 \mathrm{~mm})$ is etched in this oxide, and the wafer is reoxidized at $1150^{\circ} \mathrm{C}$ in wet oxygen such that the oxide thickness outside of the window region increases to $2000 \mathrm{~nm}$. Draw a cross section of the wafer and mark off all the thicknesses, dimensions, and oxide-Si interfaces relative to the original Si surface. Calculate the step heights in $\mathrm{Si}$ and in the oxide at the edge of the window.

David Collins
David Collins
Numerade Educator
05:43

Problem 2

When impurities are diffused into a sample from an unlimited source such that the surface concentration $N_{0}$ is held constant, the impurity distribution (profile) is given by
$$
N(x, t)=N_{0} \operatorname{erfc}\left(\frac{x}{2 \sqrt{D t}}\right)
$$
where $D$ is the diffusion coefficient for the impurity, $t$ is the diffusion time, and erfc is the complementary error function.

If a certain number of impurities are placed in a thin layer on the surface before diffusion, and if no impurities are added and none escape during diffusion, a gaussian distribution is obtained:
$$
N(x, t)=\frac{N_{s}}{\sqrt{\pi D t}} e^{-\left(x / 2 \sqrt{D_{t}}\right)^{2}}
$$
where $N_{s}$ is the quantity of impurity placed on the surface $\left(\right.$ atoms $\left./ \mathrm{cm}^{2}\right)$ prior to $t=0$. Notice that this expression differs from Eq. (4-44) by a factor of two. Why?
Figure P5-2 gives curves of the complementary error function and gaussian factors for the variable $u$, which in our case is $x / 2 \sqrt{D t}$. Assume that boron is diffused into $\mathrm{n}$ -type $\mathrm{Si}$ (uniform $\left.N_{d}=5 \times 10^{16} \mathrm{~cm}^{-3}\right)$ at $1000^{\circ} \mathrm{C}$ for 30 minutes. The diffusion coefficient for $\mathrm{B}$ in $\mathrm{Si}$ at this temperature is $D=3 \times 10^{-14} \mathrm{~cm}^{2} / \mathrm{s}$
(a) Plot $N_{a}(x)$ after the diffusion, assuming that the surface concentration is held constant at $N_{0}=5 \times 10^{20} \mathrm{~cm}^{-3} .$ Locate the position of the junction below the surface.
(b) Plot $N_{a}(x)$ after the diffusion, assuming that $\mathrm{B}$ is deposited in a thin layer on the surface prior to diffusion $\left(N_{s}=5 \times 10^{13} \mathrm{~cm}^{-2}\right)$, and no additional B atoms are available during the diffusion. Locate the junction for this case.
Hint: Plot the curves on five-cycle semilog paper, with an abscissa varying from zero to $\frac{1}{2} \mu \mathrm{m}$. In plotting $N_{a}(x)$, choose values of $x$ that are simple multiples of $2 \sqrt{D t}$.

Ameer Said
Ameer Said
Numerade Educator
01:37

Problem 3

Assuming a constant (unlimited) source diffusion of $\mathrm{P}$ at $1000^{\circ} \mathrm{C}$ into $\mathrm{p}$ -type $\mathrm{Si}$ $\left(N_{a}=2 \times 10^{16} \mathrm{~cm}^{-3}\right)$, calculate the time required to achieve a junction depth of 1 micron. See the equations in Prob. $5.2$ and data in Appendices VII and VIII.

Chai Santi
Chai Santi
Numerade Educator
02:47

Problem 4

In an ion implanter, dopant implantation of energetic $\mathrm{B}$ ion is done into a Si substrate with $2 \mu \mathrm{m}$ oxide thickness, such that the peak B concentration becomes $5 \times 10^{18} / \mathrm{cm}^{3}$ at $0.4 \mu \mathrm{m}$ distance from the surface. For this projected range, what will be the energy and corresponding straggle? What will be the value of implant dose and beam current, if the scanning is done for $100 \mathrm{~cm}^{2}$ area with 30 sec implant time.

Chai Santi
Chai Santi
Numerade Educator
01:57

Problem 5

Silicon is implanted with $\mathrm{P}$ ions at $200 \mathrm{keV}$ to a dose of $2.1 \times 10^{14} \mathrm{~cm}^{-2}$. Calculate and plot the $\mathrm{P}$ distribution on a semilog plot as in Fig. $5-4 .$

Chai Santi
Chai Santi
Numerade Educator
00:58

Problem 6

We are interested in patterning the structure shown in Fig. P5-6. Design the mask aligner optics in terms of the numerical aperture of the lens and the wavelength of the source.

Farhanul Hasan
Farhanul Hasan
Numerade Educator
01:45

Problem 7

In a $\mathrm{p}^{+}$ -n Si junction, the $\mathrm{n}$ side has a donor concentration of $10^{16} \mathrm{~cm}^{-3} .$ If $n_{i}=10^{10} \mathrm{~cm}^{-3}$, relative dielectric constant $\epsilon_{r}=12$, calculate the depletion width at a reverse bias of $100 \mathrm{~V}$ ? What is the electric field at the mid-point of the depletion region on the $\mathrm{n}$ side? (Hint: Remember that $\mathrm{p}^{+}$ means very heavily doped!)

Chai Santi
Chai Santi
Numerade Educator
03:58

Problem 8

A semiconductor with a band gap of $0.8 \mathrm{eV}$ and an intrinsic carrier concentration of $10^{12} \mathrm{~cm}^{-3}$ is doped with $10^{18} \mathrm{~cm}^{-3}$ donors on the left half and $10^{17} \mathrm{~cm}^{-3}$ acceptors on the right half. Draw the equilibrium band diagram. Calculate the junction potential and the position of the Fermi level, and indicate them on the band diagram. Suppose an electron at the conduction band edge on the $\mathrm{p}$ side goes over the $\mathrm{n}$ side without scattering. Assuming parabolic band structure, calculate its wavevector there. The effective mass of the carriers is $0.2 m_{0}$.

Chai Santi
Chai Santi
Numerade Educator
03:17

Problem 9

An abrupt Si junction (area $=0.0001 \mathrm{~cm}^{2}$ ) has the following parameters:
n side $\quad \mathrm{p}$ side
$$
N_{d}=5 \times 10^{17} \mathrm{~cm}^{-3} \quad N_{a}=10^{17} \mathrm{~cm}^{-3}
$$
Draw and label the band diagram, and calculate the difference between the Fermi level and the intrinsic Fermi level on both sides. Calculate the built-in potential at the junction in equilibrium and the depletion width. What is the total number of exposed acceptors in the depletion region?

Chai Santi
Chai Santi
Numerade Educator
02:23

Problem 10

A p-n junction diode has a doping concentration of $10^{16} \mathrm{~cm}^{-3}$ on the $\mathrm{p}$ side. and is very highly doped on the $\mathrm{n}$ side. The intrinsic carrier concentration is $10^{9} \mathrm{~cm}^{-3}$, band gap is $2 \mathrm{eV}$, and $\epsilon_{r}=15 .$ Sketch the band diagram for a reverse bias of $2 \mathrm{~V}$, and calculate the values of band edges with respect to the quasiFermi levels far from the junction. Calculate the depletion charge per $\mathrm{cm}^{2}$ on the $\mathrm{n}$ side. If an electron at the conduction band edge on the $\mathrm{p}$ side goes over to the $\mathrm{n}$ side without scattering, calculate its velocity. Electron and hole effective masses $=0.4 m_{0}$.

Chai Santi
Chai Santi
Numerade Educator
02:44

Problem 11

In a $\mathrm{p}-\mathrm{n}$ junction, the $\mathrm{n}$ -side doping is five times the p-side doping. The intrinsic carrier concentration $=10^{11} \mathrm{~cm}^{-3}$ and band gap is $2 \mathrm{eV}$ at $100^{\circ} \mathrm{C}$. If the builtin junction potential is $0.65 \mathrm{~V}$, what is the doping on the $\mathrm{p}$ side? If the relative
dielectric constant of this semiconductor is 10, what is the depletion capacitance at $2 \mathrm{~V}$ reverse bias for a diode of cross-sectional area of $0.5 \mathrm{~cm}^{2} ?$ Draw a qualitatively correct sketch of the band diagram and label the depletion widths and voltage drops for this bias.

Chai Santi
Chai Santi
Numerade Educator
00:49

Problem 12

For three $\mathrm{p}-\mathrm{n}$ junction diode samples $\mathrm{A}, \mathrm{B}$, and $\mathrm{C}$, acceptor and donor carrier concentrations are the same of $10^{15} / \mathrm{cm}^{3}$ and $10^{18} / \mathrm{cm}^{3}$, respectively. Find the contact potentials for these three devices at temp $300 \mathrm{~K}$. Intrinsic carrier concentrations for the three samples are $1.5 \times 10^{10} / \mathrm{cm}^{3}, 2 \times 10^{10} / \mathrm{cm}^{3}$, and $2 \times 10^{6} / \mathrm{cm}^{3}$. Comment on the comparison of estimated contact potentials.

Chai Santi
Chai Santi
Numerade Educator
01:56

Problem 13

In a $\mathrm{p}^{+}-\mathrm{n}$ junction the hole diffusion current in the neutral $\mathrm{n}$ material is given by Eq. (5-32). What are the electron diffusion and electron drift components of current at point $x_{n}$ in the neutral $\mathrm{n}$ region?

Chai Santi
Chai Santi
Numerade Educator
03:17

Problem 14

An abrupt Si p-n junction has $N_{a}=10^{17} \mathrm{~cm}^{-3}$ on the $\mathrm{p}$ side and $N_{d}=10^{16} \mathrm{~cm}^{-3}$ on the $\mathrm{n}$ side. At $300 \mathrm{~K},($ a) calculate the Fermi levels, draw an equilibrium band diagram, and find $V_{0}$ from the diagram; (b) compare the result from (a) with $V_{0}$ calculated from Eq. $(5-8) .$

Chai Santi
Chai Santi
Numerade Educator
04:12

Problem 15

Boron is implanted into an $\mathrm{n}$ -type Si sample $\left(N_{d}=10^{16} \mathrm{~cm}^{-3}\right)$, forming an abrupt junction of square cross section with area $=2 \times 10^{-3} \mathrm{~cm}^{2}$. Assume that the acceptor concentration in the p-type region is $N_{a}=4 \times 10^{18} \mathrm{~cm}^{-3}$. Calculate $V_{0}, x_{n 0}, x_{p 0}, Q_{+}$, and $E_{0}$ for this junction at equilibrium $(300 \mathrm{~K})$. Sketch $\mathscr{E}$ and the charge density to scale, as in Fig. $5-12$.

Narayan Hari
Narayan Hari
Numerade Educator
03:09

Problem 16

In a p-n junction diode acceptor, donor and intrinsic carrier concentrations are $10^{17} / \mathrm{cm}^{3}, 10^{18} / \mathrm{cm}^{3}$, and $10^{10} / \mathrm{cm}^{3}$, respectively. The relative dielectric constant for the material of the diode is 12 . The diffusion coefficients are $D_{n}=49 \mathrm{~cm}^{2} / \mathrm{sec}$ and $D_{p}=18 \mathrm{~cm}^{2} / \mathrm{sec}$, respectively. Electron and hole carrier lifetimes are the same, $25 \mathrm{~ns}$. Under forward bias of $0.2 \mathrm{~V}$, calculate the electron diffusion current density at a distance of twice of the diffusion length.

Chai Santi
Chai Santi
Numerade Educator
02:29

Problem 17

A Si n $^{+}$ p junction has an acceptor doping of $2 \times 10^{17} / \mathrm{cm}^{3}$ on the p side and crosssectional area of $10^{-2} \mathrm{~cm}^{2}$. If majority carrier lifetime is $10 \mathrm{~ns}$ and corresponding diffusion coefficient is $400 \mathrm{~cm}^{2} / \mathrm{sec}$, estimate the current density under a reverse bias of $0.3 \mathrm{~V}$ at $300 \mathrm{~K}$ temperature.

Chai Santi
Chai Santi
Numerade Educator
02:51

Problem 18

Estimate the expressions for developed electric field of a p-n junction where the space charge profile at depletion region is given as $\mathrm{p}(x)=\mathrm{q} \cdot \mathrm{h}(2 x+3)$, where $x$ is a distance of the device from physical contact at $x=0$ and $h$ is a constant.

Narayan Hari
Narayan Hari
Numerade Educator
01:31

Problem 19

(a) $\mathrm{A}$ Si $\mathrm{p}^{+}-\mathrm{n}$ junction $10^{-2} \mathrm{~cm}^{2}$ in area has $N_{d}=10^{15} \mathrm{~cm}^{-3}$ doping on the $\mathrm{n}$ side. Calculate the junction capacitance with a reverse bias of $10 \mathrm{~V}$.
(b) An abrupt $\mathrm{p}^{+}-\mathrm{n}$ junction is formed in $\mathrm{Si}$ with a donor doping of $N_{d}=10^{15} \mathrm{~cm}^{-3} .$ What is the depletion region thickness $W$ just prior to avalanche breakdown?

Chai Santi
Chai Santi
Numerade Educator
01:41

Problem 20

In a p $^{+} n$ junction diode, which side penetration depth will be larger? Estimate and compare the ratio of the penetration depths on both sides of the junction if the acceptor concentration is twice than that for the donor concentration. Compare the generated electric fields on both sides also.

Aman Kumar
Aman Kumar
Numerade Educator
01:52

Problem 21

For a Si $\mathrm{p}^{+} \mathrm{n}$ junction of area $2 \times 10^{-4} \mathrm{~cm}^{2}$, calculate the depletion width, the peak electric field, and the depletion capacitance under $60 \mathrm{~V}$ of reverse bias with the following diode specifications:
s side $\quad \mathrm{n} \mathrm{sig}$
$$
\begin{aligned}
N_{a} &=10^{19} / \mathrm{cm}^{3} & & N_{d}=10^{16} / \mathrm{cm}^{3} \\
\tau_{p} &=10 \mathrm{~ns} & & \tau_{n}=0.1 \mathrm{~ns} \\
\mu_{p} &=800 \mathrm{~cm}^{2} / \mathrm{V}-\mathrm{sec} & & \mu_{\mathrm{n}}=1250 \mathrm{~cm}^{2} / \mathrm{V}-\mathrm{sec} \\
\mu_{\mathrm{n}} &=200 \mathrm{~cm}^{2} / \mathrm{V}-\mathrm{sec} & & \mu_{\mathrm{p}}=1400 \mathrm{~cm}^{2} / \mathrm{V}-\mathrm{sec}
\end{aligned}
$$

Chai Santi
Chai Santi
Numerade Educator
04:32

Problem 22

In a simple p-n diode, if the diffusion coefficent for holes is twice than that for the electrons, the minority carrier concentration at $\mathrm{n}$ side is twice than that in $\mathrm{p}$ side, and the diffusion coefficent for holes is also twice of that for the electrons, calculate the injection efficiency for this diode at $x_{n}=0$.

Chai Santi
Chai Santi
Numerade Educator
03:29

Problem 23

An abrupt Si $\mathrm{p}-\mathrm{n}$ junction diode with area $=10^{-4} \mathrm{~cm}^{2}$ has $N_{a}=10^{17} / \mathrm{cm}^{3}$ and $N_{d}=10^{18} / \mathrm{cm}^{3}$. The diode has FB of 1 V. The mobility's for electrons and holes are $\mu \mathrm{n}=1350 \mathrm{~cm}^{2} / \mathrm{v}-\mathrm{sec}, \mu_{p}=400 \mathrm{~cm}^{2} / \mathrm{v}-\mathrm{sec}$, and $\tau_{p}=\tau_{n}=10 \mathrm{~ns}$.
(a) Find the excess carrier concentration.
(b) Find the electron and hole concentration at $x=2 L_{n}$ and $2 L_{p}$

Chai Santi
Chai Santi
Numerade Educator
01:56

Problem 24

A Si $\mathrm{p}-\mathrm{n}$ junction with cross-sectional area $A=0.001 \mathrm{~cm}^{2}$ is formed with $N_{a}=10^{15} \mathrm{~cm}^{-3}$ and $N_{d}=10^{20} \mathrm{~cm}^{-3} .$ Calculate:
(a) Contact potential, $V_{0}$.
(b) Space-charge width at equilibrium (zero bias).
(c) Current with a forward bias of $0.7 \mathrm{~V}$. Assume that the current is diffusion dominated. Assume $\mu_{n}=1500 \mathrm{~cm}^{2} / \mathrm{V}-\mathrm{s}, \mu_{p}=450 \mathrm{~cm}^{2} / \mathrm{V}-\mathrm{s}$, and
$\tau_{n}=\tau_{q}=2.5 \mathrm{~ms}$. Which carries most of the current, electrons or holes, and why? If you wanted to double the electron current, what should you do?

Chai Santi
Chai Santi
Numerade Educator
01:57

Problem 25

Suppose in a p'n diode the $\mathrm{n}$ region and the $\mathrm{p}$ region thickness are $20 \mu \mathrm{m}$ and $5 \mu \mathrm{m}$, respectively. What will be the $\mathrm{RB}$ applied to obtain a breakdown for this diode? [Given: $\left.\in=11.8, N d=10^{15} / \mathrm{cm}^{3}\right]$

Narayan Hari
Narayan Hari
Numerade Educator
01:01

Problem 26

In a p-n junction diode operating under certain reverse bias $V_{r}$, if $V_{r}$ is increased to $3 V_{r}$, what will be the impact on the following parameters?
(a) Depletion width
(b) Contact potential
(c) Junction capacitance
(d) Probability of breakdown

Narayan Hari
Narayan Hari
Numerade Educator
02:23

Problem 27

We make a Si bar with a p-type doping of $2 \times 10^{16} \mathrm{~cm}^{-3}$ on the left half and a p-type doping of $10^{18} \mathrm{~cm}^{-3}$ on the right side. Sketch the equilibrium band diagram, with precise values marked off, far from the doping transition at $600 \mathrm{~K}$ when the intrinsic carrier concentration is $10^{16} \mathrm{~cm}^{-3} .$ (Note: This is p type on both sides. Such a junction is known as a high-low junction rather than a $\mathrm{p}-\mathrm{n}$ junction. Observe that the doping level is comparable to $n_{i}$ on the left side! Do not worry about the exact details right near the doping transition!)

Chai Santi
Chai Santi
Numerade Educator
01:32

Problem 28

Assume that an abrupt Si $\mathrm{p}-\mathrm{n}$ junction with area $10^{-4} \mathrm{~cm}^{2}$ has $N_{a}=10^{17} \mathrm{~cm}^{-3}$ on the $\mathrm{p}$ side and $N_{d}=10^{17} \mathrm{~cm}^{-3}$ on the $\mathrm{n}$ side. The diode has a forward bias of $0.7 \mathrm{~V}$. Using mobility values from Fig. 3-23 and assuming that $\tau_{n}=\tau_{p}=1 \mu s$, plot $I_{p}$ and $I_{n}$ vs. distance on a diagram such as Fig. 5-17, including both sides of the junction. Neglect recombination within $W$.

Chai Santi
Chai Santi
Numerade Educator
02:37

Problem 29

In a p $\mathrm{n}$ diode reverse biased at $5 \mathrm{~V}$, the generated capacitance is $20 \mathrm{pF}$. If the doping of the $\mathrm{p}$ side is doubled and the bias is change to $20 \mathrm{~V}$, what will be the change in capacitance? If now the bias is changed to $100 \mathrm{~V}$, then what will be the change?

Keshav Singh
Keshav Singh
Numerade Educator
01:02

Problem 30

A Ge $\mathrm{p}^{+} \mathrm{n}$ junction diode has donor doping of $2 \times 10^{15} / \mathrm{cm}^{3}$ and relative permittivity 16. What will be the minimum thickness of $\mathrm{n}$ region that will ensure avalanche breakdown at $300 \mathrm{~V}$ reverse bias voltage?

Chai Santi
Chai Santi
Numerade Educator
01:02

Problem 31

Calculate the capacitance for the following Ge $\mathrm{p}^{+} \mathrm{n}$ junction for two reverse bias voltages of 1 and 3 V. [Given: $N_{d}=10^{16} / \mathrm{cm}^{3}, N_{a}=10^{18} / \mathrm{cm}^{3}$, area $=10^{-4} \mathrm{~cm}^{2}, n i$, $\left.\mathrm{Ge}=2 \times 10^{10} / \mathrm{cm}^{3}\right]$

Chai Santi
Chai Santi
Numerade Educator
02:00

Problem 32

We assumed in Section $5.2 .3$ that carriers are excluded within $W$ and that the semiconductor is neutral outside $W$. This is known as the depletion approximation. Obviously, such a sharp transition is unrealistic. In fact, the space charge varies over a distance of several Debye lengths, given by
$L_{D}=\left[\frac{\epsilon_{s} k T}{q^{2} N_{d}}\right]^{1 / 2}$ on the n side.
Calculate the Debye length on the $\mathrm{n}$ side for $\mathrm{Si}$ junctions having $N_{a}=10^{18} \mathrm{~cm}^{-3}$ on the $\mathrm{p}$ side and $N_{d}=10^{14}, 10^{16}$, and $10^{18} \mathrm{~cm}^{-3}$ on the $\mathrm{n}$ side and compare with the size of $W$ in each case.

Chai Santi
Chai Santi
Numerade Educator
02:56

Problem 33

A Si p-n junction diode with area $=10^{4} \mathrm{~cm}^{2}$ has $N_{a}=10^{17} / \mathrm{cm}^{3}$ and $N_{d}=10^{17} / \mathrm{cm}^{3}$.
(a) Find the reverse saturation current, given $\mu \mathrm{n}=1500 \mathrm{~cm}^{2} / \mathrm{v}-\mathrm{sec}, \mu \mathrm{p}=$
$450 \mathrm{~cm}^{2} / \mathrm{v}-\mathrm{sec}$, and $\tau_{p}=\tau_{n}=2 \mathrm{~ns} .$
(b) With the ideality factor $\mathrm{n}=1.5$ and $\mathrm{FB}$ of $0.2 \mathrm{~V}$, calculate the forward current.

Kratika Bhadauria
Kratika Bhadauria
Numerade Educator
01:37

Problem 34

Holes are injected in a $\mathrm{p}^{+} \mathrm{n}$ diode with an $\mathrm{n}$ region width similar to hole diffusion length $L_{p}$. Excess holes at $n$ side varies linearly from $\triangle p_{n}\left(\right.$ at $\left.x_{n}=0\right)$ to zero (at $x_{n}=L_{p}$ ). Solve the diffusion equation to find the excess hole concentration.

Chai Santi
Chai Santi
Numerade Educator
02:23

Problem 35

Solve for the electron carrier concentration and current density at the p region for narrow base diode with high recombination at the edges of depletion $\mathrm{n}$ region.

Chai Santi
Chai Santi
Numerade Educator
01:15

Problem 36

Consider an $\mathrm{n}^{+} \mathrm{p}$ junction under reverse bias of $5 \mathrm{~V}$. Let $N_{a}=5 \times 10^{17} \mathrm{~cm}^{-3}$. Find the reverse current density due to diffusion. [Given: $D_{n}=10 \mathrm{~cm}^{2} / \mathrm{sec}$, $\left.L_{n}=45 \mu \mathrm{m}\right]$

Chai Santi
Chai Santi
Numerade Educator
01:11

Problem 37

The diode of Fig. $5-23 \mathrm{c}$ is used in a simple half-wave rectifier circuit in which the diode is placed in series with a load resistor. Assume that the diode offset voltage $E_{0}$ is $0.4 \mathrm{~V}$ and that $R=d v / d i=400 \Omega .$ For a load resistor of $1 k \Omega$ and a sinusoidal input of $2 \sin \omega t$, sketch the output voltage (across the load resistor) over two cycles.

Chai Santi
Chai Santi
Numerade Educator
01:32

Problem 38

The ideality factor $\mathbf{n}$ can be used to describe the relative importance of recombination within the transition region and the neutral region. Calculate and plot the $I-V$ characteristics of a diode, using Eq. (5-74) for values of the ideality factor of $1.0,1.2,1.4,1.6,1.8$, and $2.0 .$
$$
\begin{aligned}
A &=100 \mu \mathrm{m}^{2}, N_{a}=10^{19} \mathrm{~cm}^{-3}, \text { and } \\
N_{d} &=10^{19} \mathrm{~cm}^{-3} ; \tau_{n}=\tau_{p}=\mu \mathrm{s}
\end{aligned}
$$

Chai Santi
Chai Santi
Numerade Educator
01:56

Problem 39

Assume holes are injected from a $\mathrm{p}^{+}-\mathrm{n}$ junction into a short $\mathrm{n}$ region of length $l$ If $\delta p\left(x_{n}\right)$ varies linearly from $\Delta \mathrm{p} n$ at $x_{n}=0$ to zero at the ohmic contact $\left(x_{n}=l\right)$, find the steady state charge in the excess hole distribution $Q_{p}$ and the current $I$.

Chai Santi
Chai Santi
Numerade Educator
04:32

Problem 40

Assume that a $\mathrm{p}^{+}$ -n diode is built with an $\mathrm{n}$ region width $l$ smaller than a hole diffusion length $\left(l<L_{p}\right)$. This is the so-called narrow base diode. Since for this case holes are injected into a short $\mathrm{n}$ region under forward bias, we cannot use the assumption $\delta p\left(x_{n}=\infty\right)=0$ in Eq. (4-35). Instead, we must use as a boundary condition the fact that $\delta p=0$ at $x_{n}=l$.
(a) Solve the diffusion equation to obtain
$$
\delta p\left(x_{n}\right)=\frac{\Delta p_{n}\left[e^{\left(l-x_{n}\right) / L_{p}}-e^{\left(x_{n}-l\right) / L_{p}}\right]}{e^{l / L_{p}}-e^{-l / L_{p}}}
$$
(b) Show that the current in the diode is
$$
I=\left(\frac{q A D_{p} p_{n}}{L_{p}} \operatorname{ctnh} \frac{l}{L_{p}}\right)\left(e^{q V / k T}-1\right)
$$

Chai Santi
Chai Santi
Numerade Educator
02:26

Problem 41

Given the narrow base diode result (Prob. 5.40), (a) calculate the current due to recombination in the $\mathrm{n}$ region, and (b) show that the current due to recombination at the ohmic contact is
$$
I(\text { ohmic contact })=\left(\frac{q A D_{p} p_{n}}{L_{p}} \operatorname{csch} \frac{l}{L_{p}}\right)\left(e^{q V / k T}-1\right)
$$

Narayan Hari
Narayan Hari
Numerade Educator
01:39

Problem 42

Assume that a $\mathrm{p}^{+}-\mathrm{n}$ junction is built with a graded $\mathrm{n}$ region in which the doping is described by $N_{d}(x)=G x^{m} .$ The depletion region $\left(W \cong x_{n 0}\right)$ extends from essentially the junction at $x=0$ to a point $W$ within the $n$ region. The singularity at $x=0$ for negative $\mathbf{m}$ can be neglected.
(a) Integrate Gauss's law across the depletion region to obtain the maximum value of the electric field $\mathscr{E}_{0}=-q G W^{(\mathbf{m}+1)} / \boldsymbol{\epsilon}(\mathbf{m}+1)$.
(b) Find the expression for $(x)$, and use the result to obtain $V_{0}-V=$ $q G W^{(\mathbf{m}+2)} / \epsilon(\mathbf{m}+2)$
(c) Find the charge $Q$ due to ionized donors in the depletion region; write $Q$ explicitly in terms of $\left(V_{0}-V\right)$.
(d) Using the results of $(\mathrm{c})$, take the derivative $d Q / d\left(V_{0}-V\right)$ to show that the capacitance is
$$
C_{j}=A\left[\frac{q G \epsilon^{(m+1)}}{(m+2)\left(V_{0}-V\right)}\right]^{1 /(\mathbf{m}+2)}
$$

Chai Santi
Chai Santi
Numerade Educator
00:58

Problem 43

We deposit a metal with a work function of $4.6 \mathrm{eV}$ on $\mathrm{Si}$ (electron affinity of $4 \mathrm{eV}$ ) and acceptor doping level of $10^{18} \mathrm{~cm}^{-3}$. Draw the equilibrium band diagram and mark off the Fermi level, the band edges, and the vacuum level. Is this a Schottky or ohmic contact, and why? By how much should the metal work function be altered to change the type of contact? Explain with reference to the band diagram.

Chai Santi
Chai Santi
Numerade Educator
04:16

Problem 44

Design an ohmic contact for n-type GaAs using InAs, with an intervening graded InGaAs region (see Fig. 5-44).

Chai Santi
Chai Santi
Numerade Educator
00:45

Problem 45

A Schottky barrier is formed between a metal having a work function of $4.3 \mathrm{eV}$ and p-type Si (electron affinity $=4 \mathrm{eV}$ ). The acceptor doping in the $\mathrm{Si}$ is $10^{17} \mathrm{~cm}^{-3}$
(a) Draw the equilibrium band diagram, showing a numerical value for $q V_{0}$.
(b) Draw the band diagram with $0.3 \mathrm{~V}$ forward bias. Repeat for $2 \mathrm{~V}$ reverse bias.

Chai Santi
Chai Santi
Numerade Educator
00:58

Problem 46

We want to make a Schottky diode on one surface of an n-type semiconductor, and an ohmic contact on the other side. The electron affinity is $5 \mathrm{eV}$, band gap is $1.5 \mathrm{eV}$, and the Fermi potential is $0.25 \mathrm{eV} ?$ What should be values of work functions of the two metals? (Give your answer as greater than or less than certain values.) Sketch the band diagram of the structure.

Chai Santi
Chai Santi
Numerade Educator
03:10

Problem 47

A semiconductor heterojunction is made between the following materials, A and $\mathrm{B}$, with the following parameters:
$$
\begin{array}{cccccccc}
& & & \begin{array}{c}
\text { Doping } \\
\left(\mathrm{cm}^{-3}\right)
\end{array} & \begin{array}{c}
\text { Length } \\
(\mu \mathrm{m})
\end{array} & \begin{array}{c}
\mathrm{L}_{n, p} \\
(\mu \mathrm{m})
\end{array} & \begin{array}{c}
n_{i} \\
\left(\mathrm{~cm}^{-3}\right)
\end{array} & \begin{array}{c}
\tau_{n, p} \\
(\mu \mathrm{s})
\end{array} \\
\mathrm{A}: & 2 & 4 & N_{A}=10^{20} & 0.5 & 10 & 10^{8} & 10 \\
\mathrm{~B}: & 1 & 5 & N_{D}=10^{16} & 0.1 & 100 & 10^{10} & 1
\end{array}
$$
Draw the equilibrium band diagram, marking off the band edge energies and $E_{F}$, with respect to the vacuum level.

Calculate the current density if the junction is forward biased such that the minority concentrations are increased by a factor of $10^{6}$.
(Hint: Use appropriate approximations. There is a lot of extraneous information here; the answer is very simple. Remember that this is a $\mathrm{p}^{+}-\mathrm{n}$ junction, and the length of the semiconductors is $\ll$ diffusion length; the minority carrier concentration is zero at the ohmic contacts at both ends of the device.)

Chai Santi
Chai Santi
Numerade Educator
04:14

Problem 48

A p-n junction diode has a doping concentration of $10^{17} \mathrm{~cm}^{-3}$ on the p- side, and double that on the $\mathrm{n}$ side. The intrinsic carrier concentration is $10^{11} \mathrm{~cm}^{-3}$, band gap is $2 \mathrm{eV}$, and $\epsilon_{r}=15 .$ Sketch the band diagram in equilibrium, and mark off the values of band edges with respect to the Fermi level and the depletion widths on both sides.

Repeat the above for a heterojunction, where the band gap on the $\mathrm{n}$ side is reduced to $1 \mathrm{eV}$, and the electron affinity on the $\mathrm{n}$ side is $4 \mathrm{eV}$. Other parameters are kept the same. Band offsets are the same for conduction and valence bands across the heterojunction.

Chai Santi
Chai Santi
Numerade Educator