For CW-EPR measurements, each EPR sample was approximately 10 μL with the spin-labeled RNA concentrations being 50–120 μM, and was loaded into a borosilicate glass capillary (1.0 mm ID × 1.2 mm OD, Fiber Optic Center, Inc.) sealed at one end. CW-EPR spectra were obtained on a Bruker EMX X-band spectrometer equipped with an ER-041X microwave Bridge and a high sensitivity cavity (ER-4119HS, Bruker Biospin, Inc). All CW-EPR spectra were acquired at room temperature with an incident microwave power of 2 mW, a modulation frequency of 100 kHz, and a modulation amplitude of 1 G. For each sample, 10 scans were collected and accumulated. The spectra were background corrected and normalized following a previously reported procedure.51 (link) Spin counting was performed based on the 2nd integral values of the baseline-corrected but not normalized CW-EPR spectra,51 (link) and the details are described in Fig. S5 and Table S5.
Er 041x microwave bridge
The ER-041X microwave Bridge is a laboratory instrument designed for electron paramagnetic resonance (EPR) spectroscopy. Its core function is to generate and control microwave signals, which are used to excite and detect the resonant behavior of unpaired electron spins within a sample. The ER-041X provides the necessary microwave signal generation and processing capabilities to enable EPR measurements in a research or analytical laboratory setting.
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2 protocols using er 041x microwave bridge
CW-EPR Spectroscopy for RNA Folding
For CW-EPR measurements, each EPR sample was approximately 10 μL with the spin-labeled RNA concentrations being 50–120 μM, and was loaded into a borosilicate glass capillary (1.0 mm ID × 1.2 mm OD, Fiber Optic Center, Inc.) sealed at one end. CW-EPR spectra were obtained on a Bruker EMX X-band spectrometer equipped with an ER-041X microwave Bridge and a high sensitivity cavity (ER-4119HS, Bruker Biospin, Inc). All CW-EPR spectra were acquired at room temperature with an incident microwave power of 2 mW, a modulation frequency of 100 kHz, and a modulation amplitude of 1 G. For each sample, 10 scans were collected and accumulated. The spectra were background corrected and normalized following a previously reported procedure.51 (link) Spin counting was performed based on the 2nd integral values of the baseline-corrected but not normalized CW-EPR spectra,51 (link) and the details are described in Fig. S5 and Table S5.
EPR Spectroscopy Protocol for Material Characterization
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