Alexander Schnegg
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Alexander Schnegg has a total of 66 co-authors. Here are the top co-authors by number of shared publications:
K. Lips
Berlin Joint EPR Lab, Institut für Nanospektroskopie, Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Kékuléstr. 5, 12489 Berlin, Germany
6 shared publications- Joscha Nehrkorn
EPR Research Group MPI for Chemical Energy Conversion Stiftstrasse 34–36 45470 Mülheim Ruhr Germany
5 shared publications - Jan Behrends
Fachbereich Physik, Freie Universität Berlin, Berlin, Germany
4 shared publications Karsten Holldack
Institute Methods and Instrumentation for Synchrotron Radiation Research, Helmholtz-Zentrum Berlin für Materialien und Energie, Albert-Einstein-Straße 15, 12489 Berlin, Germany
3 shared publicationsM. Fehr
Berlin Joint EPR Lab, Institut für Silizium-Photovoltaik, Helmholtz Zentrum Berlin für Materialien und Energie, Germany
3 shared publicationsMatthias Fehr
Helmholtz-Zentrum Berlin für Materialien und Energie, Berlin Joint EPR Lab (BeJEL); Institut für Nanospektroskopie; Albert-Einstein-Str. 15 12489 Berlin Germany
3 shared publications
Latest Publications
- 1 August 2017
- Published by Elsevier in Journal of Magnetic Resonance
- Vol. 281, 17-25
Using rapid-scan EPR to improve the detection limit of quantitative EPR by more than one order of magnitude
- 1 August 2017
- Published by Elsevier in Journal of Magnetic Resonance
- Vol. 281, 17-25
Using rapid-scan EPR to improve the detection limit of quantitative EPR by more than one order of magnitude
- Open Access
- 1 July 2017
- Published by Elsevier in Journal of Magnetic Resonance
- Vol. 280, 10-19
Recent progress in synchrotron-based frequency-domain Fourier-transform THz-EPR
- 1 July 2017
- Published by Elsevier in Journal of Magnetic Resonance
- Vol. 280, 10-19
Open AccessRecent progress in synchrotron-based frequency-domain Fourier-transform THz-EPR
- 22 February 2017
- Published by American Chemical Society (ACS) in Inorganic Chemistry
- Vol. 56 (5) , 3102-3118
Magneto-Structural Correlations in Pseudotetrahedral Forms of the [Co(SPh)4]2– Complex Probed by Magnetometry, MCD Spectroscopy, Advanced EPR Techniques, and ab Initio Electronic Structure Calculations
The magnetic properties of pseudotetrahedral Co(II) complexes spawned intense interest after (PPh4)2[Co(SPh)4] was shown to be the first mononuclear transition-metal complex displaying slow relaxation of the magnetization in the absence of a direct current magnetic field. However, there are differing reports on its fundamental magnetic spin Hamiltonian (SH) parameters, which arise from inherent experimental challenges in detecting large zero-field splittings. There are also remarkable changes in the SH parameters of [Co(SPh)4]2– upon structural variations, depending on the counterion and crystallization conditions. In this work, four complementary experimental techniques are utilized to unambiguously determine the SH parameters for two different salts of [Co(SPh)4]2–: (PPh4)2[Co(SPh)4] (1) and (NEt4)2[Co(SPh)4] (2). The characterization methods employed include multifield SQUID magnetometry, high-field/high-frequency electron paramagnetic resonance (HF-EPR), variable-field variable-temperature magnetic circular dichroism (VTVH-MCD), and frequency domain Fourier transform THz-EPR (FD-FT THz-EPR). Notably, the paramagnetic Co(II) complex [Co(SPh)4]2– shows strong axial magnetic anisotropy in 1, with D = −55(1) cm–1 and E/D = 0.00(3), but rhombic anisotropy is seen for 2, with D = +11(1) cm–1 and E/D = 0.18(3). Multireference ab initio CASSCF/NEVPT2 calculations enable interpretation of the remarkable variation of D and its dependence on the electronic structure and geometry.
- 22 February 2017
- Published by American Chemical Society (ACS) in Inorganic Chemistry
- Vol. 56 (5) , 3102-3118
Magneto-Structural Correlations in Pseudotetrahedral Forms of the [Co(SPh)4]2– Complex Probed by Magnetometry, MCD Spectroscopy, Advanced EPR Techniques, and ab Initio Electronic Structure Calculations
The magnetic properties of pseudotetrahedral Co(II) complexes spawned intense interest after (PPh4)2[Co(SPh)4] was shown to be the first mononuclear transition-metal complex displaying slow relaxation of the magnetization in the absence of a direct current magnetic field. However, there are differing reports on its fundamental magnetic spin Hamiltonian (SH) parameters, which arise from inherent experimental challenges in detecting large zero-field splittings. There are also remarkable changes in the SH parameters of [Co(SPh)4]2– upon structural variations, depending on the counterion and crystallization conditions. In this work, four complementary experimental techniques are utilized to unambiguously determine the SH parameters for two different salts of [Co(SPh)4]2–: (PPh4)2[Co(SPh)4] (1) and (NEt4)2[Co(SPh)4] (2). The characterization methods employed include multifield SQUID magnetometry, high-field/high-frequency electron paramagnetic resonance (HF-EPR), variable-field variable-temperature magnetic circular dichroism (VTVH-MCD), and frequency domain Fourier transform THz-EPR (FD-FT THz-EPR). Notably, the paramagnetic Co(II) complex [Co(SPh)4]2– shows strong axial magnetic anisotropy in 1, with D = −55(1) cm–1 and E/D = 0.00(3), but rhombic anisotropy is seen for 2, with D = +11(1) cm–1 and E/D = 0.18(3). Multireference ab initio CASSCF/NEVPT2 calculations enable interpretation of the remarkable variation of D and its dependence on the electronic structure and geometry.
- 4 March 2016
- Published by Wiley in Physica Status Solidi (a)
- Vol. 213 (7) , 1747-1750
Multifrequency EPR study of HWCVD μc-SiC:H for photovoltaic applications
- 4 March 2016
- Published by Wiley in Physica Status Solidi (a)
- Vol. 213 (7) , 1747-1750
Multifrequency EPR study of HWCVD μc-SiC:H for photovoltaic applications
- Open Access
- 25 February 2016
- Published by Forschungszentrum Julich, Zentralbibliothek in Journal of large-scale research facilities JLSRF
- Vol. 2, A51
THz Electron Paramagnetic Resonance / THz Spectroscopy at BESSY II
THz Electron Paramagnetic Resonance / THz Spectroscopy at BESSY II
- 25 February 2016
- Published by Forschungszentrum Julich, Zentralbibliothek in Journal of large-scale research facilities JLSRF
- Vol. 2, A51
Open AccessTHz Electron Paramagnetic Resonance / THz Spectroscopy at BESSY II
THz Electron Paramagnetic Resonance / THz Spectroscopy at BESSY II
- 7 January 2016
- Published by American Chemical Society (ACS) in The Journal of Physical Chemistry C
- Vol. 120 (2) , 853-861
Probing the Fate of Mn Complexes in Nafion: A Combined Multifrequency EPR and XAS Study
- 7 January 2016
- Published by American Chemical Society (ACS) in The Journal of Physical Chemistry C
- Vol. 120 (2) , 853-861
Probing the Fate of Mn Complexes in Nafion: A Combined Multifrequency EPR and XAS Study
- 1 August 2015
- Published by Elsevier in Journal of Magnetic Resonance
- Vol. 257, 94-101
CW and pulsed electrically detected magnetic resonance spectroscopy at 263 GHz/12 T on operating amorphous silicon solar cells
- 1 August 2015
- Published by Elsevier in Journal of Magnetic Resonance
- Vol. 257, 94-101
CW and pulsed electrically detected magnetic resonance spectroscopy at 263 GHz/12 T on operating amorphous silicon solar cells
- 24 July 2015
- Published by American Chemical Society (ACS) in The Journal of Physical Chemistry B
- Vol. 119 (43) , 13816-13824
Simulating Frequency-Domain Electron Paramagnetic Resonance: Bridging the Gap between Experiment and Magnetic Parameters for High-Spin Transition-Metal Ion Complexes
We present a comparison of experimental and simulated frequency- and field-domain electron paramagnetic resonance (EPR) spectra of integer and half-integer high-spin transition-metal ion complexes. For the simulation of EPR spectra a new tool within the EPR simulation software EasySpin is introduced, which allows for field- and frequency-domain EPR simulations with the same theoretical model and the same set of spin Hamiltonian parameters. The utility of this approach is demonstrated on the integer-spin complexes NiBr2(PPh3)2 and [Tp2Mn]SbF6 (both S = 1) and the half-integer-spin Fe(III) porphyrins, hemin (Fe(PPIX)Cl) and Fe(TPP)Cl (both S = 5/2). We demonstrate that the combination of field- and frequency-domain EPR techniques allows the determination of spin Hamiltonian parameters, in particular large zero-field splittings, with high accuracy.
- 24 July 2015
- Published by American Chemical Society (ACS) in The Journal of Physical Chemistry B
- Vol. 119 (43) , 13816-13824
Simulating Frequency-Domain Electron Paramagnetic Resonance: Bridging the Gap between Experiment and Magnetic Parameters for High-Spin Transition-Metal Ion Complexes
We present a comparison of experimental and simulated frequency- and field-domain electron paramagnetic resonance (EPR) spectra of integer and half-integer high-spin transition-metal ion complexes. For the simulation of EPR spectra a new tool within the EPR simulation software EasySpin is introduced, which allows for field- and frequency-domain EPR simulations with the same theoretical model and the same set of spin Hamiltonian parameters. The utility of this approach is demonstrated on the integer-spin complexes NiBr2(PPh3)2 and [Tp2Mn]SbF6 (both S = 1) and the half-integer-spin Fe(III) porphyrins, hemin (Fe(PPIX)Cl) and Fe(TPP)Cl (both S = 5/2). We demonstrate that the combination of field- and frequency-domain EPR techniques allows the determination of spin Hamiltonian parameters, in particular large zero-field splittings, with high accuracy.
- Open Access
CW and pulsed electrically detected magnetic resonance spectroscopy at 263 GHz/12 T on operating amorphous silicon solar cells
Here we describe a new high frequency/high field continuous wave and pulsed electrically detected magnetic resonance (CW EDMR and pEDMR) setup, operating at 263 GHz and resonance fields between 0 and 12 T. Spin dependent transport in illuminated hydrogenated amorphous silicon p-i-n solar cells at 5 K and 90 K was studied by in operando 263 GHz CW and pEDMR alongside with complementary X-band CW EDMR. Benefiting from the superior resolution at 263 GHz, we were able to better resolve EDMR signals originating from spin dependent hopping and recombination processes. 5 K EDMR spectra were found to be dominated by conduction and valence band tale states involved in spin dependent hopping, with additional contributions from triplet exciton states. 90 K EDMR spectra could be assigned to spin pair recombination involving conduction band tail states and dangling bonds as dominating spin dependent transport process, with additional contributions from valence band tail and triplet exciton states.
Open AccessCW and pulsed electrically detected magnetic resonance spectroscopy at 263 GHz/12 T on operating amorphous silicon solar cells
Here we describe a new high frequency/high field continuous wave and pulsed electrically detected magnetic resonance (CW EDMR and pEDMR) setup, operating at 263 GHz and resonance fields between 0 and 12 T. Spin dependent transport in illuminated hydrogenated amorphous silicon p-i-n solar cells at 5 K and 90 K was studied by in operando 263 GHz CW and pEDMR alongside with complementary X-band CW EDMR. Benefiting from the superior resolution at 263 GHz, we were able to better resolve EDMR signals originating from spin dependent hopping and recombination processes. 5 K EDMR spectra were found to be dominated by conduction and valence band tale states involved in spin dependent hopping, with additional contributions from triplet exciton states. 90 K EDMR spectra could be assigned to spin pair recombination involving conduction band tail states and dangling bonds as dominating spin dependent transport process, with additional contributions from valence band tail and triplet exciton states.
- 12 February 2014
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 112 (6) , 066403
Metastable Defect Formation at Microvoids Identified as a Source of Light-Induced Degradation inLight-induced degradation of hydrogenated amorphous silicon (), known as the Staebler-Wronski effect, has been studied by time-domain pulsed electron-paramagnetic resonance. Electron-spin echo relaxation measurements in the annealed and light-soaked state revealed two types of defects (termed type I and II), which can be discerned by their electron-spin echo relaxation. Type I exhibits a monoexponential decay related to indirect flip-flop processes between dipolar coupled electron spins in defect clusters, while the phase relaxation of type II is dominated by nuclear spin dynamics and is indicative for isolated spins. We propose that defects are either located at internal surfaces of microvoids (type I) or are isolated and uniformly distributed in the bulk (type II). The concentration of both defect type I and II is significantly higher in the light-soaked state compared to the annealed state. Our results indicate that in addition to isolated defects, defects on internal surfaces of microvoids play a role in light-induced degradation of device-quality .- 12 February 2014
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 112 (6) , 066403
Metastable Defect Formation at Microvoids Identified as a Source of Light-Induced Degradation inLight-induced degradation of hydrogenated amorphous silicon (), known as the Staebler-Wronski effect, has been studied by time-domain pulsed electron-paramagnetic resonance. Electron-spin echo relaxation measurements in the annealed and light-soaked state revealed two types of defects (termed type I and II), which can be discerned by their electron-spin echo relaxation. Type I exhibits a monoexponential decay related to indirect flip-flop processes between dipolar coupled electron spins in defect clusters, while the phase relaxation of type II is dominated by nuclear spin dynamics and is indicative for isolated spins. We propose that defects are either located at internal surfaces of microvoids (type I) or are isolated and uniformly distributed in the bulk (type II). The concentration of both defect type I and II is significantly higher in the light-soaked state compared to the annealed state. Our results indicate that in addition to isolated defects, defects on internal surfaces of microvoids play a role in light-induced degradation of device-quality .