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- In field B apply RF field to material at Larmor frequency ω_0
- Coil of L_0 perpendicular to B_0 to induce spin flip
- LCR circuit (so that ω_0=1/√LC ) to observe change in impedance with frequency
- As frequency changes: circuit response to Q-curve and polarization signal
- Sweep frequency around ω_0 to integrate in ω.
Microwave setup
Dynamic Nuclear Polarization System
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- nλ/2 cable length: leads to steeper Q-curve, making smaller polarized signals much more difficult to analyze using traditional background subtraction and signal extraction methods.
- Q-meter configurations (calibration constant)
- Changes in Radiofrequency Radio frequency (RF) environment
- Temperature Change
- Statistical errors dependent on DAQ
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5. Plot the residuals (Difference between Polynomial fit and the Baseline-RawSignal plot). Apply Apply a cut for both sides of the wings and calculate the area under the curve.
