The $pd \to \eta \,^3$He Reaction and $\eta \,^3$He Bound State? The $B^* \bar B^* \rho $ System

Vortex-free state of 3He-B in a rotating cylinder.

Measurement of the eta b(1S) mass and the branching fraction for Gamma(3S) -> gamma eta b(1S)

G. Bonvicini, D. Cinabro, A. Lincoln, M. J. Smith, P. Zhou, J. Zhu, P. Naik, J. Rademacker, D. M. Asner, K. W. Edwards, J. Reed, A. N. Robichaud, G. Tatishvili, E. J. White, R. A. Briere, H. Vogel, P. U. E. Onyisi, J. L. Rosner, J. P. Alexander, D. G. Cassel, R. Ehrlich, L. Fields, R. S. Galik, L. Gibbons, S. W. Gray, D. L. Hartill, B. K. Heltsley, J. M. Hunt, D. L. Kreinick, V. E. Kuznetsov, J...

Ferromagneticlike Resonance Behavior in Superfluid 3He-B

Measurements of the pair-breaking edge in superfluid 3He-B.

The dynamics of vortex generation in superfluid 3He-B

A profound change occurs in the stability of quantized vortices in externally applied flow of superfluid 3He-B at temperatures . 0.6Tc, owing to the rapidly decreasing damping in vortex motion with decreasing temperature. At low damping an evolving vortex may become unstable and generate a new independent vortex loop. This single-vortex instability is the generic mechanism for creating the requ...