Abstract
We search for 129Xe EDM by using an active nuclear spin maser. In this experiment, the amplitude of the maser oscillation signal is one of the most important parameters that eventually determine the frequency precision. The amplitude is proportional to the ratio of the transverse spin relaxation time T 2 to the effective longitudinal spin relaxation time \(T_{1}^{\ast }\). In particular, for a spin maser of 3He (a co-magnetometer) for which \(T_{1}^{\ast }\) typically reaches ∼50 h, a long T 2 is needed. T 2 depends on the homogeneity of the magnetic field which is applied with coils in order to keep the spins under precession. In the present report, we discuss on the design and construction of a new coil which provided a root-mean square (rms) field gradient of less than 5.0 μG/cm. The result of the field measurement has shown that the field gradient in the cell fulfills the target condition \(\sqrt {\langle {(\nabla B_{z})^{2}} \rangle } <5\; \mu \text {G/cm}\), and in fact T 2 of 3He has been measured to be as long as 11,000 s.
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Proceedings of the 5th Joint International Conference on Hyperfine Interactions and International Symposium on Nuclear Quadrupole Interactions (HFI/NQI 2014) Canberra, Australia, 21–26 September 2014
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Sakamoto, Y., Bidinosti, C.P., Ichikawa, Y. et al. Development of high-homogeneity magnetic field coil for 129Xe EDM experiment. Hyperfine Interact 230, 141–146 (2015). https://doi.org/10.1007/s10751-014-1109-5
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DOI: https://doi.org/10.1007/s10751-014-1109-5