Abstract
The absence of frequency shifts in pulsed NMR experiments on the B-phase of 3He at tipping angles φ{symbol} 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)(ΩL2/γH) (1+4 cos φ{symbol}), where ΩL 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.
Original language | English (US) |
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Pages (from-to) | 43-44 |
Number of pages | 2 |
Journal | Physics Letters A |
Volume | 53 |
Issue number | 1 |
DOIs | |
State | Published - May 19 1975 |
Externally published | Yes |
All Science Journal Classification (ASJC) codes
- Physics and Astronomy(all)