The built-in strain in self-assembled quantum dots has large impact on their physical properties, but both its average value and degree of anisotropy are often unknown. The authors demonstrate that the pressure coefficient of optical phonons might be used as probe for the strain status of the dots. This method was applied to the case of Ge dots capped with Si layers of different thicknesses. The authors observe a transition from a strictly biaxial stress situation for uncapped dots to a status of quasihydrostatic strain for cap-layer thicknesses larger than a critical value of the order of the dot height.

1.
Nano-Optoelectronics
, edited by
M.
Grundmann
(
Springer
,
Berlin
,
2002
), pp.
299
428
.
2.
J.
Stangl
,
V.
Holý
, and
G.
Bauer
,
Rev. Mod. Phys.
76
,
725
(
2004
).
3.
E.
Anastassakis
and
M.
Cardona
,
Semicond. Semimetals
55
,
117
(
1998
) and references therein.
4.
F.
Cerdeira
,
A.
Pinczuk
,
L. C.
Bean
,
B.
Batlogg
, and
B. A.
Wilson
,
Appl. Phys. Lett.
45
,
1138
(
1984
).
5.
M.
Stoehr
,
D.
Aubel
,
S.
Juillaguet
,
J. L.
Bischoff
,
L.
Kubler
,
D.
Bolmont
,
F.
Hamdani
,
B.
Fraisse
, and
R.
Fourcade
,
Phys. Rev. B
53
,
6923
(
1996
).
6.
P. H.
Tan
,
K.
Brunner
,
D.
Bougeard
, and
G.
Abstreiter
,
Phys. Rev. B
68
,
125302
(
2003
).
7.
K. L.
Teo
,
L.
Qin
,
Z. X.
Shen
, and
O. G.
Schmidt
,
Appl. Phys. Lett.
80
,
2919
(
2002
).
8.
P. H.
Tan
,
D.
Bougeard
,
G.
Abstreiter
, and
K.
Brunner
,
J. Appl. Phys.
98
,
113517
(
2005
).
9.
A. V.
Baranov
,
A. V.
Fedorov
,
T. S.
Perova
,
R. A.
Moore
,
S.
Solosin
,
V.
Yam
,
D.
Bouchier
, and
V.
Le Thanh
,
J. Appl. Phys.
96
,
2857
(
2004
).
10.
A. V.
Baranov
,
A. V.
Fedorov
,
T. S.
Perova
,
R. A.
Moore
,
V.
Yam
,
D.
Bouchier
,
V.
Le Thanh
, and
K.
Berwick
,
Phys. Rev. B
73
,
075322
(
2006
).
11.
M.
Ya. Valakh
,
V. O.
Yukhymchuk
,
V. M.
Dzhagan
,
O. S.
Lytvyn
,
A. G.
Milekhin
,
A. I.
Nikiforov
,
O. P.
Pchelyakov
,
F.
Alsina
, and
J.
Pascual
,
Nanotechnology
16
,
1464
(
2005
).
12.
V. A.
Volodin
,
M. D.
Efremov
,
A. S.
Deryabin
, and
L. V.
Sokolov
,
Semiconductors
40
,
1314
(
2006
).
13.
A.
Bernardi
,
M. I.
Alonso
,
A. R.
Goñi
,
J. O.
Ossó
, and
M.
Garriga
,
Appl. Phys. Lett.
89
,
101921
(
2006
).
14.
A.
Bernardi
,
J. O.
Ossó
,
M. I.
Alonso
,
A. R.
Goñi
, and
M.
Garriga
,
Nanotechnology
17
,
2602
(
2006
).
15.
A.
Bernardi
,
M. I.
Alonso
,
A. R.
Goñi
,
J. O.
Ossó
, and
M.
Garriga
,
Surf. Sci.
601
,
2783
(
2007
).
16.
H. K.
Mao
,
J.
Xu
, and
P. M.
Bell
,
J. Geophys. Res.
91
,
4673
(
1986
).
17.

At ambient pressure the frequency of the second-order Raman feature associated to scattering by two transverse acoustic phonons of Si (2TA) is similar to that of the Ge–Ge mode. Nevertheless, for our dots the Ge peak is about ten times more intense than the 2TA feature, thus, having no influence on the determination of the pressure coefficient of the Ge mode. Moreover, both peaks shift with pressure in opposite directions, leading to an increased peak separation with pressure.

18.
A.
Bernardi
,
J. S.
Reparaz
,
A. R.
Goñi
,
M. I.
Alonso
, and
M.
Garriga
,
Phys. Status Solidi B
244
,
76
(
2007
).
19.
C.
Ulrich
,
E.
Anastassakis
,
K.
Syassen
,
A.
Debernardi
, and
M.
Cardona
,
Phys. Rev. Lett.
78
,
1283
(
1997
).
20.
Numerical Data and Functional Relationships in Science and Technology
,
Landolt-Börnstein
, New Series Vol.
17
, edited by
O.
Madelung
,
H.
Weiss
, and
M.
Schulz
(
Springer
,
Heidelberg
,
1982
), Sec. 2, p.
64
and p.
107
.
21.
K. L.
Teo
,
L.
Qin
,
I. M.
Noordin
,
G.
Karunasiri
,
Z. X.
Shen
,
O. G.
Schmidt
,
K.
Eberl
, and
H. J.
Queisser
,
Phys. Rev. B
63
,
121306
(
2001
).
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