The vector (P z) and tensor (P zz) polarizations of a deuteron beam have been measured
using elastic deuteron–carbon scattering at 75.6 MeV and deuteron-proton scattering at 270 …

Time-reversal breaking and parity-conserving millistrong interactions, suggested in 1965,
still remain a viable mechanism of CP-violation beyond the Standard Model. One of its …

Stored beams of polarized protons, electrons, or deuterons can be spin flipped by sweeping
an rf dipole's or solenoid's frequency through an rf spin resonance. Fitting such data to the …

We recently analyzed all available data on spin-flipping stored beams of polarized protons,
electrons, and deuterons. Fitting the modified Froissart-Stora equation to the measured …

Spin-resonance strength produced by a localized rf field has been a focus of recent
publications<? format?>[VS Morozov, Phys. Rev. ST Accel. Beams 7, 024002 (2004) …

In order to measure the mass of the η meson with high accuracy using the dp→ He 3 η
reaction, the momentum of the circulating deuteron beam in the Cooler Synchrotron COSY …

The Chao matrix formalism allows analytic calculations of a beam's polarization behavior
inside a spin resonance. We recently tested its prediction of polarization oscillations …

We recently tested a new spin resonance crossing technique, Kondratenko Crossing (KC),
by sweeping an rf-solenoid's frequency through an rf-induced spin resonance with both the …

We used an rf solenoid to study the widths of rf spin resonances with both bunched and
unbunched beams of 1.85 GeV/c polarized deuterons stored in the COSY synchrotron. With …

A measurement of the spin observables in external target and storage ring experiments
requires a comparison of interactions of oppositely polarized beams. The ideal way to …