TY - JOUR
T1 - X-ray beam induced current measurements for multi-modal x-ray microscopy of solar cells
AU - Ossig, Christina
AU - Nietzold, Tara
AU - West, Bradley
AU - Bertoni, Mariana
AU - Falkenberg, Gerald
AU - Schroer, Christian G.
AU - Stuckelberger, Michael E.
N1 - Funding Information:
We greatly acknowledge J. Garrevoet, M. Seyrich, A. Schropp, D. Brückner, J. Hagemann, K. Spiers, and T. Boese from the Deutsches Elektronen-Synchrotron (DESY) and A. Kolditz, J. Siebels, J. Flügge, C. Strelow, T. Kipp, and A. Mews from the University of Hamburg for supporting measurements at beamline P06 at PETRA III, DESY; M. Holt, Z. Cai, M. Cherukara, and V. Rose from the Argonne National Laboratory (ANL) for supporting measurements at beamline 26-ID-C at the Advanced Photon Source (APS) at ANL; D. Salomon and R. Tucoulou from the European Synchrotron Radiation Facility (ESRF) for supporting measurements at beamline ID16B at ESRF; R. Farshchi, D. Poplavkyy, and J. Bailey from MiaSolé Hi-Tech Corp., and E. Avancini, Y. Romanyuk, S. Bücheler, and A. Tiwari from the Swiss Federal Laboratories for Materials Science and Technology (EMPA) for providing solar cells. We acknowledge DESY (Hamburg, Germany), a member of the Helmholtz Association HGF, for the provision of experimental facilities. We acknowledge the European Synchrotron Radiation Facility (Grenoble, France) for provision of synchrotron radiation facilities. This research used resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357.
Funding Information:
We greatly acknowledge J. Garrevoet, M. Seyrich, A. Schropp, D. Br?ckner, J. Hagemann, K. Spiers, and T. Boese from the Deutsches Elektronen-Synchrotron (DESY) and A. Kolditz, J. Siebels, J. Fl?gge, C. Strelow, T. Kipp, and A. Mews from the University of Hamburg for supporting measurements at beamline P06 at PETRA III, DESY; M. Holt, Z. Cai, M. Cherukara, and V. Rose from the Argonne National Laboratory (ANL) for supporting measurements at beamline 26-ID-C at the Advanced Photon Source (APS) at ANL; D. Salomon and R. Tucoulou from the European Synchrotron Radiation Facility (ESRF) for supporting measurements at beamline ID16B at ESRF; R. Farshchi, D. Poplavkyy, and J. Bailey from MiaSol? Hi-Tech Corp., and E. Avancini, Y. Romanyuk, S. B?cheler, and A. Tiwari from the Swiss Federal Laboratories for Materials Science and Technology (EMPA) for providing solar cells. We acknowledge DESY (Hamburg, Germany), a member of the Helmholtz Association HGF, for the provision of experimental facilities. We acknowledge the European Synchrotron Radiation Facility (Grenoble, France) for provision of synchrotron radiation facilities. This research used resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357.
Publisher Copyright:
© 2019 Journal of Visualized Experiments.
PY - 2019/8
Y1 - 2019/8
N2 - X-ray beam induced current (XBIC) measurements allow mapping of the nanoscale performance of electronic devices such as solar cells. Ideally, XBIC is employed simultaneously with other techniques within a multi-modal X-ray microscopy approach. An example is given herein combining XBIC with X-ray fluorescence to enable point-by-point correlations of the electrical performance with chemical composition. For the highest signal-to-noise ratio in XBIC measurements, lock-in amplification plays a crucial role. By this approach, the X-ray beam is modulated by an optical chopper upstream of the sample. The modulated X-ray beam induced electrical signal is amplified and demodulated to the chopper frequency using a lock-in amplifier. By optimizing low-pass filter settings, modulation frequency, and amplification amplitudes, noise can efficiently be suppressed for the extraction of a clear XBIC signal. A similar setup can be used to measure the X-ray beam induced voltage (XBIV). Beyond standard XBIC/XBIV measurements, XBIC can be measured with bias light or bias voltage applied such that outdoor working conditions of solar cells can be reproduced during in-situ and operando measurements. Ultimately, the multi-modal and multi-dimensional evaluation of electronic devices at the nanoscale enables new insights into the complex dependencies between composition, structure, and performance, which is an important step towards solving the materials' paradigm.
AB - X-ray beam induced current (XBIC) measurements allow mapping of the nanoscale performance of electronic devices such as solar cells. Ideally, XBIC is employed simultaneously with other techniques within a multi-modal X-ray microscopy approach. An example is given herein combining XBIC with X-ray fluorescence to enable point-by-point correlations of the electrical performance with chemical composition. For the highest signal-to-noise ratio in XBIC measurements, lock-in amplification plays a crucial role. By this approach, the X-ray beam is modulated by an optical chopper upstream of the sample. The modulated X-ray beam induced electrical signal is amplified and demodulated to the chopper frequency using a lock-in amplifier. By optimizing low-pass filter settings, modulation frequency, and amplification amplitudes, noise can efficiently be suppressed for the extraction of a clear XBIC signal. A similar setup can be used to measure the X-ray beam induced voltage (XBIV). Beyond standard XBIC/XBIV measurements, XBIC can be measured with bias light or bias voltage applied such that outdoor working conditions of solar cells can be reproduced during in-situ and operando measurements. Ultimately, the multi-modal and multi-dimensional evaluation of electronic devices at the nanoscale enables new insights into the complex dependencies between composition, structure, and performance, which is an important step towards solving the materials' paradigm.
KW - CIGS
KW - Engineering
KW - Issue 150
KW - Lock-in amplification
KW - Multi-modal
KW - Photovoltaics
KW - Solar cell
KW - Synchrotron radiation
KW - X-ray beam induced current
KW - X-ray beam induced voltage
KW - X-ray microscopy
KW - XBIC
KW - XBIV
UR - http://www.scopus.com/inward/record.url?scp=85071969835&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85071969835&partnerID=8YFLogxK
U2 - 10.3791/60001
DO - 10.3791/60001
M3 - Article
C2 - 31498310
AN - SCOPUS:85071969835
SN - 1940-087X
VL - 2019
JO - Journal of Visualized Experiments
JF - Journal of Visualized Experiments
IS - 150
M1 - e60001
ER -