Abstract
The absence of frequency shifts in pulsed NMR experiments on the B-phase of 3He at tipping angles ϕ less than 104° is explained on the basis of Leggett's resonance equations. At tipping angles greater than 104° and large magnetic fields we find the frequency shift δω = ( 4 15 )(Ω L 2/γH) (1+4 cos ϕ) , where Ω L is the longitudinal resonance frequency of the B-phase and H is the magnetic field. The consistency with the observed nuclear free precision signal is pointed out.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
