In a quantum dot made of an indirect gap material such as Si, the electron–hole Coulomb interaction alone can give rise to “dark” excitons even in the absence of exchange interaction. We present the predicted excitonic spectra for hydrogen-passivated Si dots and find very good agreement with the recent experiment of Wolkin, Jorne, Fauchet, Allan, and Delerue [Phys. Rev. Lett. 82, 197 (1999)]. The calculated splitting between dark and bright excitons, arising from Coulomb and exchange interactions, agrees very well with the optical data of Calcott, Nash, Canham, Kane, and Brumhead [J. Phys Condens. Matter 5, L91 (1993)].

1.
A.
Franceschetti
,
L. W.
Wang
,
H.
Fu
, and
A.
Zunger
,
Phys. Rev. B
58
,
R13367
(
1998
), and references therein.
2.
M. V.
Wolkin
,
J.
Jorne
,
P. M.
Fauchet
,
G.
Allan
, and
C.
Delerue
,
Phys. Rev. Lett.
82
,
197
(
1999
).
3.
P. D.
Calcott
,
K. J.
Nash
,
L. T.
Canham
,
M. J.
Kane
, and
D.
Brumhead
,
J. Phys.: Condens. Matter
5
,
L91
(
1993
).
4.
S. B.
Zhang
,
C. Y.
Yeh
, and
A.
Zunger
,
Phys. Rev. B
48
,
11204
(
1993
).
5.
L. W. Wang and A. Zunger, in Semiconductor Nanostructures, edited by P. V. Kamat and D. Meisel (Elsevier Science, New York, 1996), Vol. 103, p. 161.
6.
A.
Franceschetti
,
H.
Fu
,
L. W.
Wang
, and
A.
Zunger
,
Phys. Rev. B
60
,
1819
(
1999
).
7.
H.
Fu
and
A.
Zunger
,
Phys. Rev. B
57
,
R15064
(
1998
).
8.
L. W.
Wang
and
A.
Zunger
,
Phys. Rev. B
53
,
9579
(
1996
).
9.
K.
Leung
and
K. B
Whaley
,
Phys. Rev. B
56
,
7455
(
1997
).
10.
E.
Martin
,
C.
Delerue
,
G.
Allan
, and
M.
Lannoo
,
Phys. Rev. B
50
,
18258
(
1994
).
11.
S.
Öḡüt
,
J.
Chelikowsky
, and
S.
Louie
,
Phys. Rev. Lett.
79
,
1770
(
1997
).
12.
A.
Franceschetti
,
L.-W.
Wang
, and
A.
Zunger
,
Phys. Rev. Lett.
83
,
1269
(
1999
).
This content is only available via PDF.
You do not currently have access to this content.