
OPTIMIZACIÓN DE LA CAPTURA DE IMÁGENES SWIR GÓMEZ-LÓPEZ et al.
ties within the cells, especially under partial shading or early-
stage degradation scenarios (Zhang y cols., 2022; Matusz-
Kalász y cols., 2025). These limitations have led to a gro-
wing interest in alternative diagnostic tools that leverage non-
visible spectra for enhanced fault identification.
Electroluminescence (EL) imaging has gained widespread
use in PV diagnostics due to its capacity to reveal structu-
ral anomalies at the cell level. By applying a forward bias
to the module, EL enables the visualization of current path-
ways and inactive areas through near-infrared emissions. Ho-
wever, conventional EL imaging using silicon-based CCD or
CMOS sensors typically operates within the 300–1000 nm
range, which limits its sensitivity to low-intensity emissions
and restricts the contrast in cells affected by subtle mecha-
nical or electrical degradation (Qin y cols., 2021; Redondo-
Plaza y cols., 2025).
To address these limitations, imaging in the Short-Wave
Infrared (SWIR) band—specifically between 900 and 1700
nm—has been explored as a more effective approach. SWIR
cameras equipped with Indium Gallium Arsenide (InGaAs)
sensors offer improved detection of internal cell structures
and enable imaging under low-excitation conditions, facili-
tating defect localization with higher contrast and better pe-
netration through encapsulant layers (Mei y cols., 2020; Li
y cols., 2022). This spectral advantage becomes particularly
useful in detecting faint or diffuse electroluminescent signals
that arise in micro-cracked or PID-affected regions.
Nonetheless, the practical implementation of SWIR-based
EL imaging poses its own challenges. Image quality depends
heavily on the calibration of capture parameters such as ex-
posure time, digital gain, and polarization current. In ad-
dition, captured images often suffer from geometric distor-
tions, fixed-pattern noise, and uneven background illumina-
tion. To extract diagnostically relevant information, it is ne-
cessary to apply a robust preprocessing pipeline that inclu-
des background subtraction, perspective correction, and lo-
cal contrast enhancement methods such as Contrast Limited
Adaptive Histogram Equalization (CLAHE).
Despite the growing availability of advanced imaging
techniques, there remains a limited number of studies that
integrate hardware optimization with tailored image proces-
sing methods for SWIR-based EL diagnostics. Moreover, cu-
rrent literature often focuses on either experimental valida-
tion or post-processing algorithms in isolation, leaving a gap
in holistic approaches that combine acquisition and analy-
sis within a single workflow (Chen y cols., 2021; Rehman y
cols., 2023).
This study proposes and validates a complete methodo-
logy that combines optimized SWIR image acquisition with
a systematic preprocessing framework to support the early
detection of structural defects in PV modules. The metho-
dology involves the experimental configuration of polariza-
tion currents and exposure parameters, followed by the im-
plementation of automated image corrections to improve de-
fect visibility. The ultimate goal is to enable cost-effective,
high-resolution diagnostics that support predictive mainte-
nance and lifecycle extension of PV systems, especially in
environments where standard inspection methods fall short.
MATERIALS AND METHODS
Experimental Setup
Experimental evaluations were conducted at the Microgrid
Laboratory of the University of Cuenca (Espinoza y cols.,
2017). The image acquisition system comprised an OWL 640
M camera equipped with a 16 mm focal length lens and an In-
GaAs sensor. This setup enabled the capture of SWIR images
in the 900–1700 nm wavelength range, which is well-suited
for detecting internal structural features in crystalline silicon
PV modules (Mei y cols., 2020).
The test samples included both monocrystalline and
polycrystalline PV panels, selected to represent configura-
tions commonly found in utility-scale and distributed gene-
ration systems. To induce electroluminescence emissions, a
programmable Chroma DC power supply was used to apply
polarization currents ranging from 2 A to 8 A.
Image acquisition was performed using the XCAP-Std
software, which provided precise control over exposure ti-
me, gain, and frame rate parameters. Experimental runs were
conducted to assess the influence of these parameters on ima-
ge contrast, uniformity, and the visibility of structural anoma-
lies.
PV Panel
Dark Chamber
PC
Power Supply
EL Image
SWIR Camera
Fig. 1: Experimental setup showing the OWL 640 M camera,
Chroma power supply, and PV panel under inspection.
Image Acquisition Procedure
The electrical excitation applied to the PV panels directly
affects the quality and clarity of the resulting EL images. To
determine an appropriate polarization current (IEL), experi-
mental tests were conducted using a Heckert Solar NeMo 60
P260 13 polycrystalline module. This panel, with an open-
circuit voltage (VOC ) of 39.4 V and a short-circuit current
(ISC) of 8.97 A, was placed inside a dark chamber during
acquisition. For practical purposes, VOC and ISC were appro-
ximated to 40 V and 9 A, respectively.
Current levels ranging from 1
6ISC to ISC were applied to
assess their impact on image quality. Figure 2 displays EL
images obtained under these varying conditions. The analysis
showed that although IEL =ISC resulted in the most intense
emission, structural features could already be distinguished
from 1
2ISC, allowing the use of lower excitation while limiting
thermal stress on the panel.
For preventive maintenance applications, using a current
equal to or greater than 3
6ISC was found to provide sufficient
EL signal intensity without introducing excessive thermal
stress on the module. This observation is consistent with the
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