| Page |
Location |
Currently Reads |
Should Read |
| XIII |
9.4.1 |
by Confined Acoustic |
by Folded Acoustic |
| 14 |
third line from bottom |
conversion factor for various units can be be found at the end of this book |
conversion factor from eV to frequency can be found inside the front cover of this book |
| 28 |
Fig. 2.6 |
Red sphere = F, Shaded sphere = Ca |
Red sphere = Ca, Shaded sphere = F |
| 41 |
last |
change only by 0 or ± 1 |
change only by ± 1 |
| 46 |
Table 2.13 |
{md
} xyz |
{md} xzy |
| 74 |
Eq.(2.60) |
H12 '2+H13'2 |
|H12'|2+|H13'|2 |
|
Eq.(2.61) |
[(H11'+H12')2-4(H11'H12'-H12'2-H13'2)]1/2 |
[(H11'+H22')2-4(H11'H22'-|H12'|2-|H13'|2)]1/2 |
| 88 |
Fig. 2.25b |
(the vertical axis passes through "X1c") |
(axis should be broken as with "X4c") |
| 93 |
Problem 2.8 a |
 |
 |
| 108 |
Fig. 3.5 (first two pictures) |
A is shaded light red |
A is shaded black |
| 113 |
Fig. 3.11 caption |
solid circles |
circles |
| 116 |
text box |
 |
 |
| 132 |
Problem 3.4b |
(shear tensors are shown as determinants) |
(shear tensors should be shown as matrices) |
| 182 |
4.3.3 heading |
An Application |
Another Application |
| 224 |
first line |
sum of ... plus ... |
sum of ... and ... |
| 235 |
second paragraph |
is real imples that … |
is real implies that … |
| 236 |
second paragraph |
is not importance … |
is not important … |
| 242 |
fourth paragraph |
By symplifying this … |
By simplifying this … |
| 249 |
eqn. (6.39) |
 |
 |
| 252 |
third paragraph |
… band separation Eev. |
… band separation Ecv. |
| 252 |
third paragraph |
doubly degenerate band [eqn. 6.55] |
degenerate band is given by [eqn. 6.55] |
| 268 |
Fig. 6.20b |
(the two black dots in exciton pictures are not aligned with the dot above) |
(align all three black dots) |
|
| 277 |
Fig. 6.25 |
- |
(remove gray lines) |
| 278 |
Fig. 6.26 |
x-axis: 17.100 17.200 etc. |
x-axis: 17100 17200 etc. |
| 284 |
first line |
much higher that the … |
much higher than the … |
| 284 |
fourth paragraph |
in order than (6.107) be satisfied |
in order that (6.107) be satisfied |
| 284 |
fifth paragraph |
E is not necessary zero |
E is not necessarily zero |
| 285 |
last paragraph |
… and longitudinal resonance … |
… and longitudinal resonances … |
| 285 |
last paragraph |
… transverse of longitudinal vibrations … |
… transverse or longitudinal vibrations … |
| 312 |
second line from the top |
shown in (3.20) |
shown in (2.48) |
| 379 |
first paragraph |
… given by (6.115b). |
… given by (6.114b). |
| 390 |
last paragraph |
energy denominator in (7.59) diverges |
energy dependent term in (7.59) diverges |
| 439 |
third line from bottom |
zinc blende |
zinc-blende |
| 575 |
Ref. 5.31 |
D.K. Kim |
D.S. Kim |
| Page |
Location |
Currently Reads |
Should Read |
| 11 |
SUMMARY
second line |
and and |
and |
| 14 |
(2.1) |
rj |
ri' |
| 16 |
4 lines below (2.7) |
H 1e |
H1e |
| 24 |
line 5 from top |
R is a group (and therefore a sbugroup of G) the space |
then R is a group (and therefore a sbugroup of G) while the space |
| 25 |
first line of Fig. 2.4 caption |
(c) a gilde plane. |
(c) a glide plane. |
| 27 |
line 17 |
(a/4)(0,1,1) |
(a/4)[0,1,1] |
|
Fig.2.5 |
a and a/4 for distance between atoms (red solid circles) |
(3)1/2a and (3)1/2a/4 |
| 47 |
4 lines below Table 2.14 |
reciprocal lattice vector (2p/a)(0,0,2) |
reciprocal lattice vector (2 p/a)(2,0,0) |
| 49 |
5 lines from top of second paragraph |
( T sx>)2=T(1/2,1/2,0) |
(Tsx)2=T(0,1/2,1/2) |
| 59 |
second line of Fig. 2.21 caption |
the sign ov V1a |
the sign of Via |
| 61 |
three lines above 2.5.2 |
X1 conduction band state in Ge is split into two X6 spin doublets |
X1 conduction band state in Ge is split into two states X 6
and X7 |
| 65 |
line 14 from bottom of page |
positive term to m* |
positive term to 1/m* |
| 74 |
Eq.(2.60) |
H12'2+H13'2 |
|H12'|2+|H13'|2 |
|
Eq.(2.61) |
[(H11'+H12')2-4(H11'H12'-H12'2-H13'2)]1/2 |
[(H11'+H22')2-4(H11'H22'-|H12'|2-|H13'|2)]1/2 |
| 84 |
line 13 from bottom |
four phase vectors exp(ik.d a) |
four phase factors exp(ik.da |
| 85 |
The matrix element for <X2|Hint|Y1 in Table 2.25 |
Vxx g4* |
Vxyg4* |
| 88 |
Fig. 2.25(b) |
G25'c |
G25'v |
|
|
X4c |
X4v |
| 93 |
line 1 from top |
Characters of C3V and C2V Point Groups |
Characters of C3v and C2v Point Groups |
| 95 |
Footnote 1 first line |
implicitely |
implicitly |
| 118 |
Table 3.1 |
a(G1c-a(G15v) |
a(G1c)-a(G15v) |
| 126 |
6th line from bottom |
calculatd |
calculated |
| 129 |
Prob.3.1(b) |
G=2G1++G1-+G4+ |
G=2G1++G2-+G5+ |
|
Prob.3.1(c) |
the 18 zone-center phonon modes in Cu2O have the symmetriesG1-+G3-+3G4- +G5-+G4+ |
the 18 zone-center phonon modes in Cu2O have the symmetriesG2-+G3-+3G4-+G5-+G5+ |
|
second line above Fig. 3.12 |
The G4+ mode is Raman-active |
The G5+ mode is Raman-active |
| 131 |
line 6 |
Syzyz=Szyzy |
Syzyz=Szyzy=Sxyyx...=Syzzy |
| 132 |
Prob.3.4(c) |
off-diagonal matrix elements of the strain tensor are all equal to S44 |
off-diagonal matrix elements of the strain tensor should all be equal to S44/2 |
|
Problem 3.4(b) and (c) |
diagonal |
|
| 134 |
Problem 3.6(d)
second last line |
The quantized two transverse |
The two quantized transverse |
| 137 |
Problem 3.8 The last sentence before part (a) |
In Problems 3.11 and 3.12 we will perform theoretical calculation of b and d. |
In Problems 3.10 and 3.11 we will perform theoretical calculation of b* and d*. |
| 138 |
Prob.3.9 first line of second paragraph |
and G15 valence band |
and G25' valence band |
|
Problem 3.10 line before the matrix |
a diagonal matrix.. |
a unit matrix.. |
| 140 |
Problem 3.11 two lines before the matrix |
a diagonal tensor |
a unit tensor |
| 141 |
Prob. 3.11(c) second line above table |
|Z2 with |X2 |
|Y1 with |X2 |
| 143 |
Prob.3.11(c)first line after second equation |
the bonding (G15 conduction band) and antibonding (G'25 valence band) |
the antibonding (G15conduction band) and
bonding (G'25 valence band) |
| 146 |
Problem 3.16(b) |
H ep=(|e|/.. |
Hep=(4 p|e|/.. |
| 147 |
six lines from top |
based on which of these; force constants |
based on which; these force constants |
| 152 |
last paragraph |
one way to solve (4.3) |
one way to solve (4.2) |
| 156 |
6th line after 4.2.2 |
solutions of (4.2).. |
solutions of (4.22).. |
| 157 |
Fig.4.1 |
there is a small gap between the valence band and the k-axis |
there should be no gap between the valence band and the k-axis |
| 165 |
end of page (Table 4.3) |
more recent data [2.70]. |
more recent data. |
| 167 |
4th line below (4.45) |
labeld |
labeled |
| 168 |
Table 4.4 |
Experimental values for Si (45), InP(31), ZnTe(30) and CdTe(30) are all in normal style |
Experimental values for Si (45), InP(31), ZnTe(30) and CdTe(30) should all be in italics |
| 170 |
first line of Table 4.5 caption |
theoretical values of.. |
theoretical energies of.. |
| 175 |
one line below (4.57) |
Det[G] |
DetG |
| 176 |
3rd line below b) Resonant State Solutions |
DOS n(E) |
DOS no(E) |
|
(4.68) |
Some k's are in bold-type while two are not |
All k's should be in bold-type: k |
|
2nd line below (4.68) |
[to be denoted as no(E)] |
[i.e. no(E)] |
| 177 |
(4.72) |
n(r,E)=(-1/p)Im{TrG(r,r')} |
n(r,E)=(-1/p)Im{G(r,r)} |
|
(4.73) |
|
Below the summation sign k should be in bold-type: k |
| 178 |
line above (4.85) |
Substituting (4.83) and (4.60) into.. |
Substituting (4.83) and (4.59) into.. |
| 180 |
4th line from top |
to be equal pNd(Es).. |
to be equal -pNd (Es).. |
| 182 |
5th line from bottom |
|
Remove entire sentence: Since N has attracted…exciton.. |
| 183 |
third to last line |
vary important |
very important |
| 185 |
second line from top |
energies of N in the GaAsP.. |
energies of an electron bound to N in the GaAsP.. |
| 186 |
(4.95) |
E0k |
Replace all E0k in this equation with E0,k |
|
last 3 lines from end |
,then <Eo-2>is positive. In order that E |
Since <Eo-2>is positive, in order that E |
| 191 |
Fig. 4.10 caption |
(b) Im{F(E)} |
(b) -Im{F(E)} |
| 195 |
line above (5.6) |
|
Add the following phrase after the word zero: " and denoting the electronic
charge -e asq" |
| 196 |
line after (5.14) |
(..Fermi energy) |
(..Fermi energy when T~0) |
| 199 |
below (5.33) |
|
add phrase:
where summation is over all k' not equal to k. |
| 202 |
(5.46) |
q o =Ne2/(epsilon)skBT |
q o=4(pi)Ne2/(epsilon)skBT see
[6.9 p.497] |
| 203 |
end of first paragraph |
(5.45) |
(5.43) |
| 206 |
7 lines below the figure caption |
the Brillouin zone length along |
the Brillouin zone length measured from the zone center along |
| 242 |
first paragraph |
replacing (epsilon) r and (epsilon)i by n and k |
replacing (epsilon)r and (epsilon)i by n and (kappa) |
| 205 |
2nd line from bottom |
valley |
valleys |
| 220 |
2nd line in section 5.4.3 |
..higher voltage |
..high voltage |
| 275 |
(2.85b) |
HeRc |
HeR |
| 258 |
Table 6.3 |
energy of E1+(Delta)1 in InP=3.835 eV |
energy of E1+(Delta)1 in InP=3.28 eV while
energy of E1 +(Delta)1 in GaP=3.835 eV |
| 259 |
(6.58a) |
(epsilon) i=A(x-1)1/2 for x1 where
A=2e2(2mu)3/2 (/Pcv/2 )Eg1/2/[m2(omega) 2(hbar) 3] |
(epsilon)i=Ax-1/2(x-1)1/2 for x1 where A=2e2(2mu) 3/2(/Pcv/2)E g-3/2/[m2(hbar)] |
| 275 |
second line |
both kc and ke by k |
both kv and ke by k |
| 284 |
Case 2 (Longitudianl Field) |
When epsilon = 0. E is not |
When epsilon = 0, E is not |
| 287 |
Figure 6.30 vertical axis label |
w/w0 |
w/wT |
| 297 |
first paragraph |
in (6.10) and expression in (6.123) we obtain |
in (6.10) and expression in (6.126b) we obtain |
| 300 |
Fig. 6.37 caption |
calculated with (6.8) and (6.123) |
calculated with (6.8) and (6.126b) |
| 336 |
third line from top |
Roosbroek-Schockley relation |
Roosbroeck-Shockley relation |
| 340 |
5 lines above (7.9) |
n=ne=np |
n=ne=nh |
| 348 |
line above (7.19) |
E' is proportional to 1/r |
E' is proportional to 1/R |
| 355 |
3 lines above (7.23) |
In the (D oh) picture |
In the (D+X) picture |
| 369 |
3 lines from end of second paragraph |
and the red sunset; |
and the red sunset. |
| 383 |
second line from bottom of page |
(7.48). when there is |
(7.48). When there is |
| 384 |
last line |
(Problem 7.7) |
(Problem 7.8) |
| 391 |
(7.62) |
e(wi> )-e(ws |2 |
e(wi )-e(ws )|2 |
| 398 |
second line from bottom |
denominator in (7.70) an be |
denominator in (7.70) can be |
| 399 |
x-axis label of inset of Fig.7.35 |
qao |
qaB |
| 415 |
6 line from bottom |
vacuum ultraviolet(UV) |
vacuum ultraviolet (VUV) |
| 416 |
first line from top |
see [8.1,2]. |
see [8.1,2]). |
| 418 |
line 5 from top of second paragraph |
(process 2) |
(prcoess 2 with circle around 2) |
|
line 7 from top of second paragraph |
(process 3) |
(process 3 with circle around 3) |
| 436 |
8 lines below (8.10) |
incidence. ARPES data |
emission ARPES data |
| 441 |
lines 2 and 3 below Fig. 8.21 |
referenced to the vacuum level. |
referenced to the top of the valence band. |
| 509 |
(9.54b) |
sin (../..)-(C../..) |
sin(../..)+(C../..) |
| 517 |
3rd line from bottom |
for a positive bias and 4.8 for a negative voltage |
for a negative bias and 3.8 for a positive voltage |
| 518 |
3rd line above Fig. 9.35 |
In0.35Ga0.47As |
In0.53Ga0.47As |
| 528 |
second line from end of second paragraph |
the carrier mangetic field |
the mangetic field |
| 530 |
7th line from top of page |
As a matter of fact, r xy/(e2h) acts |
As a matter of fact, rxy/(e2/h) acts |
| 560 |
middle of page |
Rk=hbar/e2=(25812.807..) |
Rk=h/e2=(25812.807..) |
| 587 |
7.81 |
(1957) |
(1976) |
| 615 |
left column, 13 lines from bottom |
splin-polarized |
spin-polarized |
| Inside bottom cover |
Table of Units Heading |
Si--CGS |
SI--CGS |
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