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Here, for excitation via the pump beam, precisely the same scheme as in TRFE is used, but with linear polarization. The pump is amplitude modulated by a photograph-elastic modulator at 100 kHz. The linearly polarized, unmodulated probe beam is divided right into a reference beam, which happens to be routed around the cryostat plus the take a look at beam, which can be transmitted throughout the sample.
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The oriented provider spins precess at the Larmor frequency around the magnetic discipline utilized within the Voigt geometry BV (B⊥k). The coherent spin dynamics is then detected through the Faraday ellipticity on the linearly-polarized probe pulses.
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In This method nuclear magnetic resonances are measured by way of resonant lessen of dynamic nuclear polarization by radio frequency (RF) radiation. For that optical detection with the TRFE amplitude at fastened magnetic subject is utilised. A small RF coil of about 5 mm diameter owning 5 turns is positioned near to the sample surface area, similar to ref. 49. The coil is mounted flat within the sample surface and the laser beam is transmitted throughout the bore with the coil. The RF induced magnetic area course is perpendicular to its area and parallel to k.
The atoms (black circle) are localized near the centre of the cavity. The Raman lasers enter the vacuum chamber at a 45° angle for the cavity axis. The reflected gentle within the probe laser is Utilized in the homodyne detection.
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The information on which the plots On this paper are primarily based as well as other conclusions of the examine can be found from the corresponding authors on justified request.
T = 1.6 K and BV = 1 T. c Scheme demonstrates spins precessing at 5 least expensive PSC mode frequencies. Black curve at the bottom shows sum sign of such modes, weighted assuming an ensemble with a Gaussian distribution of amplitudes, as shown in panel d from the crimson vertical traces. d Illustration of your pumped provider spin polarizations in inhomogeneous NC ensemble issue to a magnetic field. Green line exhibits the distribution of carrier precession frequencies due to dispersion of your Larmor frequency. It is actually modeled by Gaussian with width Δω. PSC modes for the one-pump protocol, satisfying the ailment ωL = NωR = twoπN/TR, are revealed because of the pink vertical traces. e Zoom on the TRFE signal in The 2-pumps protocol from b, indicated via the box. Higher scale offers hold off in units of separation, TD, among two pumps. The bursts inside the signal are associated with the electron spins with Larmor frequencies that are commensurate with the frequency: ωD = twoπM/TD.