Diffraction dissociation of nuclei in 450 GeV/c proton-nucleus collisions

Diffractive dissociation of nuclei (Be, Al, W) in collisions with 450 GeV/c protons,pApX, has been measured with the HELIOS spectrometer at the CERN Super Proton synchrotron. The dependence of the single-diffraction cross-section on the nuclear massA can be parametrized as _SD mb×A ^0.35±0.02, showing the peripheral nature of the process. The differential cross-section d_SD=(3.8±0.3)mb ×A ^0.35±0.02, is exponential with the slope parameter, increasing from 6.2±0.4 (GeV/c)^–2 for beryllium to 7.9±0.5 (GeV/c)^–2 for tungsten. The slope parameter also increases with increasing massM _X of the diffractively produced state. The rapidity, multiplicity, and transverse-momentum distributions of the particles of the diffractively produced stateX show a longitudinal phase-space population and are remarkably insensitive to the nuclear mass. This, together with theA ^1/3 dependence of _SD, suggests that the dominant process of nuclear diffractive excitation is the dissociation of single nucleons.Deceased     

Extinction, scattering, and absorption of anomalous radar-reflected emission in a cloud and atmosphere

For the anomalous radar reflection from the oversized water drops originating in water-ice phase transition observable in the submillimeter band transparency window of ice [1] we consider the process of extinction, scattering, and absorption in a cloud and atmosphere. Our calculations, which are based on experimental results, show that in the situation when the convective cloud is illuminated from nadir by a narrow-beam submillimeter radar (carried on board an airplane or a satellite), the total extinction and absorption in the cloud and atmosphere is nearby 20dB in the long-wave transparency window of atmosphere. In the central part of submillimeter band these losses may be as high as 40dB.However,the level of losses has no effect on a difference between the radar reflection coefficients for overcooled water and ice existing due to phase transition, and this difference may be over 20dB in the 0.3 to 0.8mm ice transparency window.     

Spin-phonon coupling in intermediate valency: exactly solvable models

Two exactly solvable models are presented to describe the dynamic coupling of magnetic transitions within Kramer's degenerate multiplets and lattice vibrations. The magnetic susceptibilities are calculated. It is shown that the spin-boson coupling can reduce the single ion Curic constant at low temperature. For special symmetries the Curie constant may vanish, yielding a temperature independent susceptibility at lowT.     

Incommensurate and commensurate magnetic long-range order in metallic REPd3 compounds of rare earths (RE=Nd,Tb, Dy,Er, Tm,Yb)

Compared to previous bulk magnetic measurements unusual magnetic ordering phenomena were detected by systematic neutron scattering experiments performed in the temperature range of 7 mKT300 K on the series of cubic metallic compounds REPd₃ of the rare earths RE=Nd, Tb, Dy, Er, Tm and Yb. Except for ErPd₃ withT _N =3 K the observed critical temperatures are compatible with the de Gennes scaling. The complexity of long-range magnetic ordering increases with decreasing 4f ⁿ occupancy, ranging from ferro- or ferrimagnetism in YbPd₃ and DyPd₃ via commensurate antiferromagnetic ordering in ErPd₃ and TmPd₃ [k=(1/2, 1/2, 0)] to incommensurate antiferromagnetic ordering of modulated type in TbPd₃ and NdPd₃. Both RKKY interactions, crystalline electric field, hybridization with 4d states of Pd as well as nuclear spin polarization in the case of RE=Nd appear to be of importance for the magnetic properties of REPd₃ systems.     

Sound propagation in metallic glasses—a new look at the tunneling model

A variety of amorphous metals exhibit a characteristic behavior in their acoustic properties at low frequencies which differs from the predictions of the standard tunneling model. We point out that a lower cut-off _min for the tunnel matrix element, which is needed for consistency of the tunneling model, leads to an upper bound on relaxation times induced by the conduction electrons. We derive explicit expressions for the velocity shift and internal friction for the normalconducting and superconducting case. It is shown that a maximum relaxation time plays an essential role at audio frequencies. The corresponding change of the acoustic properties is in qualitative agreement with vibrating reed experiments.