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8/9/2019 Semicond Specimen
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Index Number: ___________________
Specimen Paper
TEL204/05 Semiconductor Device P!"ic"
Time: # $our"
In"truction" to candidate":
1. Please check that this question paper consists of six (6) printed pages beforeyou begin the examination.
2. Anser any ! questions in the anser booklet pro"ided.
#. $on%programmable electronic calculator may be used.
&. 'ou may refer to the Appendix for formulas and physical constants.
!. 'ou are not alloed to remo"e this question paper from the examination "enue.
opyright 2*1# +,-
2%
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TEL204/05
%ue"tion & '20 mar(")
(a) /ketch the crystal structure for simple cubic structure and body%centeredcubic structure. 0! marks
(b) he diamond lattice structure is the basic building block in silicon.(i) alculate the number of atoms in one cell of a diamond structure.0! marks
(ii) alculate the density of atoms in silicon in terms of atomsm#.0! marks
(c) he energy le"els in the hydrogen atom as proposed by 3ohr ha"ediscrete energy le"els ith principal quantum number n as shon in thefigure belo.
4igure 1
5i"en that the electron energy in the hydrogen atom 26.13n
En
= e7
8etermine the energy released hen an electron mo"es from energyle"els 9#to 91. 0! marks
%ue"tion 2 '20 mar(")
(a) 5i"en to doped silicon samples : and '. /ample : doped ith 1610
nitrogen atomscm 3 ; /ample ' doped ith 5 1013 aluminum atomscm3 .
(i) /tate the type of semiconductor for sample : and sample '.0& marks(ii) 4ind the ma
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%ue"tion # '20 mar(")
(a) A rectangular germanium block ith the dimensions as shon in the figure belohas a resisti"ity of 1*#m at 2*B.
4igure 1(i) 4ind the resistance beteen the square ends.
0& marks
(ii) 4ind the resistance beteen the rectangular ends.0& marks
(iii) A 1*mA current flos beteen the rectangular ends. 4ind the number ofelectrons passing the silicon block per second.
0& marks
(b) 3riefly explain the reason direct band gap semiconductor is more suitable to beused in optoelectronics applications. /ketch and label the energy band diagramof a direct band gap semiconductor and an indirect band gap
semiconductor.0> marks
%ue"tion 4 '20 mar(")(a) (i) +hat are the important points of CeisenbergDs uncertainty principleE
06 marks (ii) he uncertainty in the position of a particle ha"ing mass ?.11x1*%#1=g is >F
4ind the uncertainty in the momentum 02
hxp = of the particle.
0& marks (iii) An electron is mo"ing ith a "elocity of 1x1*Gcms. 8etermine its associated
de 3roglie a"elength 0Hhp here h is PlanckDs constant and p is
momentum. 0! marks
(b) 5i"en a sample of intrinsic silicon and a sample of intrinsic germanium ithsame dimensions for both samples. At room temperature hich sample hashigher resisti"ityE Iustify your anser.
0! marks
#
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TEL204/05
&
&%
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TEL204/05
%ue"tion 5 '20 mar(")
(a) 3riefly describe the particle in a box model in quantum mechanics. 02 marks
(b) Sketch the initial a"e functions for the first four energy states in a one%
dimensional particle in a box gi"en that 9*is the energy at ground state (nH1).
Label your diagram clearly. [8 marks]
(c) esium chloride (sl) is a typical body%centred cubic ionic structure ith the@adelung constant J H 1.G62G. Kt is gi"en that its aoH *.#!6 nm and n H 1*.!.4ind theL
(i) 3inding energy energy of sl in terms of e7. 0# marks(ii) @olar ohesi"e energy of sl in terms of kJ/mol. 0# marks
(d) he energy difference beteen the !d and 6s suble"els in gold accounts for its
color. Assuming this energy difference is about 2.G e7 explain hy gold has a
arm yello color.. [4 marks]
%ue"tion * '20 mar(")
(a) 4or an Al%/i,2%/i capacitor the doping of the substrate is $aH1*1&cm%# and the
oxide thickness is >2F. 5i"en that the flat band "oltage 743is M *.& 7 calculate
at strong in"ersion
(i) the surface potential
0& marks
(ii) the maximum depletion layer idth
02 marks
(iii) the gate "oltage
0& marks
(b) Nualitati"ely explain ho the oxide charges affect the threshold "oltage.
0& marks
(c)Oist to differences beteen ionic, covalent and metallic bonds. 06
marks
!
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+ppendix I
P!"ica, con"tant"
3oltmann constant k = 1 38 10 23. I=
Planck constant 341063.6
=h Is9lementary charge C1060.1 19=q
Permitti"ity in "acuum o =
8 85 10 12
. F / m
Permeability in "acuum o =
4 10 7
H / m
9lectron rest mass mo =
9 11 10 31
. kg
hermal "oltagekT
q = 0 0259. V (at T H #**=)
able 1L Properties of semiconductors and insulator (at #**= unless otherise noted)
Propert! -nit" Si .e .a+" Si2Lattice constant nm *.!*G *.!6!G! *.!6!#2 %
Density gcm# !.** Q 1*22 &.&2 Q 1*22 2.21 Q 1*222.2* Q1*22
Energy gap at300 K
e7 1.12& *.6G 1.&2 > M ?
Energy gap at 0K
e7 1.1G* *.G&& 1.!2 %
Relativepermittivity
% 11.G 16.* 1#.1 #.?
Intrinsic carrierconcentration cm# 1.&! Q 1*1* 2.& Q 1*1# ?.* Q 1*6 %Electron lattice
mobilitycm27s 1&1G #?** >>** 2*
Hole latticemobility
cm27s &G1 1?** &** 1*>
Effective densityof states in
conduction bandcm# 2.> Q 1*1? 1.*& Q 1*1? &.G Q 1*1G %
Effective densityof states in
valence bandcm# 1.*& Q 1*1? 6.* Q 1*1> G.* Q 1*1> %
Electroneffective mass
mn*mo 1.*> *.!! *.*6> %
Hole effectivemass
mp*mo *.>1 *.# *.! %
Electron affinity e7 &.*! &.** &.*G 1.*
6
G%
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+ppendix II
ormu,a" Seet
Binding energy )1
1)(4
(00
2
na
eB =
Molar cohesive energy C = B
(2NA
Kn the photoelectric effect the cutoff
a"elength
hc
c =
he maximum kinetic energy
K hhc
max = =
he stopping potentiale
KV
s
max=
he minimum frequency of photon
h
Ef
g=
he energy bandgap of /i
T
TEE gg
+
=
2)0(
Kntrinsic carrier concentration of
silicon ]exp[2kT
ENNn
g
vci
=
oncentration of ma