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Esr 900

Manufactured by Bruker
Sourced in United Kingdom

The ESR 900 is an electron spin resonance (ESR) spectrometer designed for laboratory use. It is a scientific instrument used to detect and analyze the magnetic properties of materials by measuring the absorption of microwave radiation by unpaired electrons in a sample. The ESR 900 provides a means to study the electronic structure and chemical environment of paramagnetic species within a sample.

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6 protocols using esr 900

1

Optically Detected Magnetic Resonance Spectroscopy

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Optically detected magnetic resonance experiments were carried out using a modified X-band spectrometer (Bruker E300) equipped with a continuous-flow helium cryostat (Oxford ESR 900) and a microwave cavity (Bruker ER4104OR, approximately 9.43 GHz) with optical access. Optical irradiation was performed with a 532 nm continuous-wave laser (Cobolt Samba CW 532 nm DPSSL) from one side-opening of the cavity. PL was detected with a silicon photodiode (Hamamatsu S2281) on the opposite opening, using a 561 nm long-pass filter to reject excitation light. The PL signal was amplified by a current/voltage amplifier (Femto DHPCA-100). For continuous-wave ODMR, PL was recorded by a lock-in detector (Ametek SR 7230) referenced by on–off modulation of microwaves with a frequency of 547 Hz. Microwaves were generated with a microwave signal generator (Anritsu MG3694C), amplified to 3 W (Microsemi) and guided into the cavity. For trODMR, PL was recorded by a digitizer card (GaGe Razor Express 1642 CompuScope) whereby a pulse blaster card (PulseBlasterESR-PRO) triggered the digitizer card and produced microwave pulses for a set length. Microwaves were generated with the same microwave signal generator as in continuous-wave ODMR, whereby they were amplified to 5 W by a travelling wave tube amplifier (Varian VZX 6981 K1ACDK) and guided into the cavity.
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2

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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3

EPR Spectroscopy of Dry Powder Samples

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EPR spectra were recorded using the Bruker ELEXSYS E500 (Bremen, Germany) with helium cryostat ESR 900 (Abingdon, United Kingdom). Previously calibrated 2,2-diphenyl-1-picrylhydrazyl (DPPH) was used as a standard. Temperature was controlled using the ITC4 503S Oxford thermostat (Abingdon, United Kingdom). Spectra were always recorded with a modulation amplitude at least eight times lower than the line width with a microwave power low enough to avoid saturation. The last strongly over modulated spectrum was recorded at 5 K with 0.64 mW of microwave power and modulation amplitude set to 2 G to enhance the background signals. About 11 mg of dry brown powder were used.
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4

CW-EPR Spectroscopy of Paramagnetic Samples

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CW-EPR spectra were
recorded on a Varian spectrometer with a Bruker super-High Q cavity
(ER 4122SHQE) coupled to a He-flow ESR900 cryostat. The measurements
were taken with the following experimental parameters. Microwave frequency:
9.4 GHz, microwave power: 2 mW, magnetic field modulation amplitude:
0.2 mT, magnetic field modulation frequency: 100 kHz, time constant:
300 ms, magnetic field step: 0.005 mT, and temperature T = 15 and 298 K.
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5

Characterization of TmQueH by EPR

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Anaerobically reconstituted TmQueH (as described above, 150 μL, 10 mg/mL) was mixed with 1 mM sodium dithionite and transferred into a sealed EPR tube in an anaerobic glovebox. Samples were removed from the glovebox and flash frozen in liquid nitrogen before EPR analysis. EPR spectra were acquired with a Bruker Elexsys E500 system utilizing an Oxford ESR900 cryostat at a frequency of 9.644 GHz, in the perpendicular setting of a Bruker ER4116-DM dual mode resonator. The field modulation frequency was set at 100 kHz, modulation amplitude at 10 G, and the microwave power at 2 mW at 10 K. All spectra were baseline-corrected by subtraction of the EPR signal of a blank. For the oxidized sample, the tube was thawed and exposed to air for 30 minutes before being frozen in liquid nitrogen.
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6

CW-EPR Spectroscopy of Frozen Samples

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Continuous wave (CW) electron paramagnetic resonance (EPR) measurements were performed at X-band frequency (~9.65 GHz) using a Bruker EMXplus spectrometer equipped with a Bruker high-sensitivity cavity (ER4119HS) and a nitrogen-flow cryostat (ESR 900). A high-sensitivity Bruker Premium-X bridge with an integrated microwave frequency counter was employed along with a magnetic field controller (ER083CS) that was calibrated using a Bruker NMR field probe (ER035M). All measurements utilized a 4 G modulation amplitude with a 100 kHz modulation frequency, an 80.92 ms time constant, and a 1 mW microwave power. All spectra were recorded on frozen solutions held at 85 K. All spectra were processed and analyzed using the software package EasySpin (version 6.0.0),55 (link) as implemented in Matlab (version R2022b). Spin quantification of samples presented for UV/vis measurements was performed using a 1 mM CuSO4 standard.
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