TRANSIENT ABSORPTION FOR CHARACTERIZATION
OF INTERMEDIATE BAND SOLAR CELLS
P. Kolla
1
, A. Norman
2
, and S. Smith
1
1
Nanoscience and Nanoengineering,
South Dakota School of Mines and Technology
Rapid City, SO 57701
2
National Renewable Energy Laboratory
Golden, CO 80401
ABSTRACT
We use transient absorption methods to charaterize the
sequential two-photon absorption in a quantum-dot super
latt
.
ice ba
�
ed intermediate band solar cell (QD-IBSC).
USing collinear, orthogonally polarized beams generated
f
�
om an Optical Parametric Oscillator (OPO) at varying
time delay, tuned stepwise from 1050nm to 1250nm, we
use the solar cell photocurrent as a diret measure of the
transient absorption by measuring the diferential photo
current as a function of time delay between two
energetically degenerate, - 100fs pulses. For comparison,
we measure the pulse autocorrelation in the same
geometry using a GaAsP photodiode, where all obseved
photocurrent is derived from instantaneous two-photon
absorption. Our measurements show that at high intensity,
the measurement is dominated by instantaneous two
photon absorption, with a simultaneous sequential two
photon photocurrent which persists beyond the pulse
overlap. Our measurements demonstrate the method can
reveal carrier dynamics in a working QD-IBSC, and their
dep
�
ndence on energy. The method could potentially give
details of the band structure formed in the QD-IBSC. Such
knowledge may benefit device development and future
designs of IBSCs based on QD superlattices or alternative
intermediate band materials or device strutures.
INTRODUCTION
The intermediate band solar cell (IBSC) allows sequential
absorption of low-energy photons which would otherwise
not be absorbed by a single junction solar cell [1). Based
on thermodynamic arguments, the IBSC has a theoretical
eficiency as high as 63%, well above current state of the
art �ande
�
cells
.
[2]. However, the details of realizing a
device which satisfies the contingencies upon which such
eficiency is theoretically possible have not been achieved.
The Quantum Dot IBSC (QD-IBSC), conSisting of a
superlattice of self-assembled quantum dots embedded in
a higher band-gap absorber, has been proposed as a
means of achieving a working IBSC, and has been studied
both experimentally and theoretically [3-5).While evidence
of the sequential absorption process has been confirmed
[4], significant improvements in eficiency have not been
realized, Further, such measurements generally do not
reveal the mechanisms which limit the device, and many
details of the electronic structure of the QD superlattice
IBSC remain unknown.
978-1-4244-5892-9/10/$26.00 ©2010 IEEE
In this work, we report our adaptation of transient
absorption methods to investigate the dynamics of the
carrier populations associated with the below-gap QD
states in a QD-IBSC, with the intention of revealing details
of the intermediate band which are inaccessible to purely
time-integrated methods.
SAMPLES STUDIED
As shown in figure 1, the QD-IBSCs used in our
experiments consist of 50 periods of self-assembled
InxGa
1
-xAs quantum dots grown by MOCVD under
Stranski-Krastanov growth conditions, and embedded in a
GaAs
1
-xPx p-i-n diode structure. These devices were
developed at NREL, characterized by photoluminescence
and I-V measurements, and were shown to be good
working diodes with a room temperature QD luminescence
peak energy around 1.04lm. This was confirmed by
tuning our laser excitation near 1.05lm where strong
absorption and corresponding photocurrent was obseved.
Au grid bar
200 nm n+ GaAs
n - 2 x 10'9
30 nm n GalnP, n - 2 X 10'9
100 nm p GaAs, P- 2 x 10
18
P+ GaAs (311)8 substrate
P - 8 X 10'8
Au contact
}SO x 10nm Gas•.•8SP•.• ,l
6.1 Mlln •.41Ga.... As QDs
Figure 1 Representative QD-IBSC device structure
used in our experiments. A 50 period quantum dot
superlatice is embedded in a p-i-n diode.
EXPERIMENTAL METHODS
Under pulsed illumination, absorption and transmission of
light is proportional to the occupation of carriers within the
available density of states. Femtosecond lasers can
produce intense pulses of light much shorter than the
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