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7 protocols using simfonia

1

Characterization of DNA and RNA Radicals

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As per our ongoing studies on DNA and RNA-radicals,7 , 8 (link), 23 (link) – 35 (link) a Varian Century Series X-band (9.3 GHz) ESR spectrometer with an E-4531 dual cavity, 9-inch magnet, and a 200 mW Klystron was used and Fremy’s salt (gcenter = 2.0056, A(N) = 13.09 G) was employed for the field calibration. All ESR spectra have been recorded at 77 K and at 40 dB (20 µ W). Spectral recording at 77 K maximizes signal height and allows for comparison of signal intensities.
Following our works on DNA and RNA-radicals,7 , 8 (link), 23 (link) – 35 (link) the anisotropic simulations of the experimentally recorded ESR spectra were carried out by employing the Bruker programs (WIN-EPR and SimFonia). The ESR parameters (e.g., hyperfine coupling constant (HFCC) values, linwidth, etc.) were adjusted to obtain the “best fit” simulated spectrum that matched the experimental ESR spectrum well (see supporting information Figure S1 and our works26 (link), 28 (link), 29 , 35 (link)).
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2

Electron Spin Resonance Spectrometry Protocol

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Following our works,22 (link)–29 (link), 31 , 36 (link)–38 (link) a Varian Century Series X-band (9.3 GHz) ESR spectrometer with an E-4531 dual cavity, 9-inch magnet, and a 200 mW Klystron was used for the ESR studies. For the field calibration, Fremy’s salt (gcenter = 2.0056, A(N) = 13.09 G) was employed. All ESR spectra were recorded at 77 K and at microwave power of 40 dB (20 μW). Recording of ESR spectra at 77 K maximizes the signal height and allows for comparison of signal intensities. For recording and digital storage of EPR spectra and for spectral analyses, we used our in-house developed programs (ESRTAK and ESRADSUB). To obtain a simulated spectrum that matches the corresponding experimentally recorded spectrum, we employed the Bruker programs (WIN-EPR, SIMFONIA).22 (link)–29 (link), 31 , 36 (link)–38 (link)
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3

Characterization of CYP125A13 by EPR

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To record the CYP125A13 electron paramagnetic resonance (EPR) spectra, a Bruker X-band spectrometer (9.5 GHz) equipped with a continuous supply of helium cryostat ESR 900 and an ITC 4 temperature controller used to achieve a base temperature of 5 K, was used. The microwave frequency and modulation frequency used were 9.647GHz and 100 kHz, respectively. The data were recorded and analyzed at The Korea Basic Science Research Institute, Western Seoul Center. Before the measurement, the oxidized form of 180 μM CYP12A13 in 10 mM potassium phosphate buffer (pH 7.4) was frozen in liquid nitrogen in EPR quartz tubes (Wilmad). The spectral data comprising the g-tensor and line width of the heme centers were acquired by the accumulation of spectra in the Simfonia or Xsophe (Bruker) programs.
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4

EPR Spectroscopy of Cu-Zeolites

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The EPR spectra of Cu-containing zeolites were recorded as the first derivative of the absorption signal of a EMXplus EPR spectrometer (Bruker, Karlsruhe, Germany) in the X-band (9.4 GHz). A variable temperature unit ER4141VTM was used for temperature variation. The EPR spectra were simulated by the program SimFonia (Bruker) and the quantitative analysis was performed by the licensed program SpinCount (Bruker).
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5

EPR Spectroscopy of Radical Formation

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EPR spectra were obtained at X-band and at room temperature on a Bruker EMX-8/2.7 (9.86 GHz) equipped with a high-sensitivity cavity (4119/HS 0205) and a gaussmeter (Bruker, Wissembourg, France). A flat quartz cell (FZKI160–5 × 0.3 mm, Magnettech, Berlin, Germany) was used to measure radical formation. WINEPR and SIMFONIA software (Bruker, Wissembourg, France) were used for data processing and spectrum computer simulation. Typical scanning parameters were: scan rate, 1.2 G/s; scan number, 5; modulation amplitude, 1 G; modulation frequency, 100 kHz; microwave power, 20 mW; sweep width, 100 G; sweep time, 83.88 s; time constant, 40.96 ms; magnetic field 3460–3560 G.
EPR experiments were carried out using the spin-trapping agent DMPO (5,5-dimethyl-1-pyrroline N-oxide). The analyses were performed by adding DMPO (final concentration 50 mM) on 106 CHO cells in PBS buffer. When needed, H2O contained in the PBS buffer was replaced by D20. The illumination was performed directly though the quartz flat cell containing the sample.
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6

EPR Spectroscopy of 1,4-Naphthoquinone Radicals

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X-band EPR spectra were recorded at 295 K on a Bruker EMX spectrometer (Billerica, MA, USA). The instrument parameters were frequency, 9.30 GHz; MW power, 1 or 4 mW; range, 20 G; modulation frequency, 100 kHz; modulation amplitude, 0.1 or 0.2 G; and time constant, 0.17 s.
EPR samples were prepared by diluting 16 mM 1,4-NQ DMSO stocks in PBS buffer (pH 7.4, final 1,4-NQ concentration 4 mM) and reacted with GSH, Cys, or H2S prepared in PBS buffer. H2S stock was prepared by dissolving Na2S in PBS. For hypoxia reactions, 1,4-NQs were diluted into N2-sparged PBS buffer and the solutions were further sparged with N2 while H2S was prepared by dissolving Na2S into N2-sparged PBS. Reaction solutions were then transferred into capillary tubes for EPR measurements. To prepare 1,4-NQ semiquinone radical, 4 mM 1,4-NQs were reacted with 0.15–0.25× sodium borohydride (NaBH4).
The simulation of EPR spectra was conducted using Simfonia (Bruker). The parameters used in the simulation were g = 2.0044 and hyperfine splitting of 3.21 G for protons 2 and 3 and 0.63 G for protons 5, 6, 7, and 8. The parameters for simulating the spectrum of the SH-substituted 1,4-NQ were g = 2.0044 and hyperfine splitting of 0.69 G for protons 5, 6, 7, and 8.
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7

EPR Spectroscopy of Indolone Radicals

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All experiments were performed with hQR2 (20 µg/mL), DMPO (125 mM), the indolone substrates (125 µM), and BNAH (3 mM); for some assays, we added S29434 (5 µM). EPR spectra were acquired with a Bruker EMX-8/2.7 (9.86 GHz) equipped with a high-sensitivity cavity (4119/HS 0205) and a gaussmeter (Bruker, Wissembourg, France), at X-band and at room temperature. For analyses, we used a flat quartz cell, FZKI160-5 × 0.3 mm (Magnettech, Berlin, Germany). We performed data processing and spectrum simulation with WINEPR and SIMFONIA software (Bruker). Scanning parameters were: microwave power, 20 mW; sweep width, 100 G; sweep time, 83.88 s; time constant, 40.96 ms; magnetic field, 3460–3560 G; scan rate, 1.2 G/s; scan number, 5; modulation amplitude, 1 G; and modulation frequency, 100 kHz. We conducted the EPR spectra analysis as reported previously [20 (link)]. Each EPR spectrum comprises the intensity of the peaks on the y-axis in arbitrary units (a.u.), and the magnetic field on the x-axis in gauss (g). The scale of the magnetic field is not included for reasons of simplicity because it is not used in this study. The features used are the signal intensity measured by integrating the area under all peaks and the signal shape with the number of peaks.
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