Nucleons after pion absorption

We calculate energy spectra and angular distributions of single and correlated spectra after the absorption of stopped pions in nuclei. We assume: The pion is abosrbed by a pair of nucleons; these primary nucleons may leave the nucleus directly or only after one or more collisions with other nucleons. We propose a multiple scattering expansion for the intranuclear cascade after pion absorption. Various experimental data are successfully described in shape and absolute magnitude. The ratio R_np = R(π^?np → nn)/R (π^? pp → np) is determined from the experimental proton spectra: R_np = 13 ± 6.     

Direct processes in chaotic microwave cavities in the presence of absorption

We quantify the presence of direct processes in the S matrix of chaotic microwave cavities with absorption in the one-channel case. To this end the full distribution P(S)(S) of the S matrix, i.e., S=sqrt[R]e(itheta), is studied in cavities with time-reversal symmetry for different antenna coupling strengths T(a) or direct processes. The experimental results are compared with random-matrix calculations and with numerical simulations including absorption. The theoretical result is a generalization of the Poisson kernel. The experimental and the numerical distributions are in excellent agreement with theoretical predictions for all cases.     

A model for pion absorption in nuclei

To describe pion absorption in nuclei, we introduce a model which assumes that incident pion is absorbed by the row of target nucleons along the beam direction. The momentum distribution of these nucleons after absorbing the pion is assumed to be determined by the phase space. The experimental data on the inclusive proton cross section are well reproduced.     

Direct observation of switching processes in permalloy rings with lorentz microscopy

To achieve a deeper understanding of the switching process of magnetic Permalloy rings, Lorentz electron microscopy (LTEM) is used for the first time to image the magnetic configuration of such rings under applied external field conditions. Because of the exceptionally high lateral resolution we find two clearly distiguishable wall configurations present in the so-called "onion state." Furthermore, we show that a bias field present during a remagnetization cycle prevents the rings from transforming into a flux closure state, in which case remagnetization is a pure domain wall motion process.     

Quasi-two-body pion absorption on helium-3

We examine the pion absorption process on a deuteron-like pair in ³He. It is shown that the effective increase in the density of the “deuteron” leads to an interesting signature in the proton polarisation, P_y. Suggestions are made concerning the best energies and angles at which to perform the corresponding measurements.     

Amplitude ambiguities in pion absorption on the diproton

A classification is given of, and intra-relationships are derived between amplitudes which yield identical spin-summed differential cross sections and vector polarizations for one of the nucleons emitted in pion absorption on the diproton. To accomplish this, a formal correspondence is established between the amplitude for pion absorption on the diproton and the amplitude for pion nucleon elastic scattering, and the well-known Minami ambiguity for the latter is generalized.Paper dedicated to the memory of Michael Moravcsik, whose untimely death terminated a very useful exchange of ideas onamplitude ambiguities, a subject on which he had been a leading authority. His remarks and observations provided me with a better, deeper insight into the topic of this paper     

Angular distribution in neutrino-induced single pion production processes

A partial wave decomposition of \({v \mathord{\left/ {\vphantom {v {\bar v}}} \right. \kern-0em} {\bar v}}\) single pion production is used for studying resonant and nonresonant contributions. The dominant resonance excitation is dynamically described by a semirelativistic quark model. Nonresonant background is considered to arise from Born-terms diminuished by the lowest order partial waves (which are determined by resonances alone.) The method permits evaluation of interferences between resonance and background amplitudes as well as, more importantly, among resonances themselves. Predicted interference patterns are reflected by the pion angular distribution coefficients which compare well with recent data. Results obtained this way are also in agreement with momentum transfer measurements if higher resonance excitation form factors are chosen to resemble those tested in pion photoproduction, rendering simultaneously any nonresonant background small.     

Formation of primary particles in stopped pion absorption reactions

The results from analyzing the yields of protons (p), deuterons (d), and tritons (t) formed in the absorption of stopped π^– mesons by intranuclear clusters are presented. The contributions from cluster absorption to the production of hydrogen isotopes in stopped pion absorption reactions are determined. Phenomenological formulas are proposed for describing the mass number (A) dependences of the yields of the primary protons with ～15% precision in the mass number range of 6 < A < 209 (and of the primary deuterons and tritons in the mass number range of 59 < A < 209). Evidence is observed of the constancy of the ratio between the elemental absorption widths for the absorption of pions by pp and pn pairs over the investigated range of mass numbers.     

Spectroscopy of 7Li in stopped pion absorption reactions

The structure of excited levels in the ⁷Li isotope is studied via inclusive and correlation measurements in the stopped π^? meson absorption reactions ¹⁰B(π^?, t)X and ¹²C(π^?, dt)X, respectively. The experiment is conducted using a low-energy pion beam at the LAMPF meson factory. Analysis of the missing mass spectra reveals ⁷Li states with the resonance parameters (E _x , Γ) (4.7, 0.1), (6.6, 0.9), (7.3, 0.1), (9.1, 2.8), and (9.6, 0.4) MeV. A highly excited state with E _x ≈ 11.2 MeV (i.e., an isobar analog of ⁷He) is observed in the ¹⁰B(π^?,t)X reaction. An excited state with E _x = 10.3 ± 0.1 MeV and γ = 1.8 ± 0.4 Mev is observed for the first time in the ¹²C(π^?,dt)X reaction.     

Two nucleon emission following bound pion absorption

The absorption of a bound 2p pion in¹⁶O with the emission of two fast nucleons leading to low excitation of the residual nucleus has been studied. In our calculation, the following important effects have been considered simultaneously: (i) correlations in the initial nuclear wave function are treated on the basis of the Brueckner theory, (ii) the mutual final state scattering of the emitted pair and (iii) the nucleon-nucleus scattering are taken into account by the use of eikonal model wave function. Results are compared with other calculations and experiments. It is found that inspite of our elaborate treatments serious discrepancies between theory and experiments still remain. A more careful study of the absorption mechanism is emphasized.     

Direct observation of split-off exciton and phonon structures in absorption spectrum of silicon

The split-off band exciton of silicon has been observed in the absorption spectrum by using a wavelength modulation technique. The spin-orbit splitting of the valence band is determined to be 44.1 ± 0.3 meV at 1.8 °K. The structures associated with some two-phonon indirect transitions have also been observed in the absorption spectrum.     

Effects of meson exchange currents on pion absorption

The effect of the π exchange current on the pion absorption process π⁺ + d → p + p has been investigated. The absorption cross section is significantly enhanced particularly in the energy region above the 33 resonance.     

Microscopic description of bound 2p pion absorption

The p-wave bound pion absorption in ¹⁶O has been studied in detail. The role of rescattering terms in conjunction with initial and final state nucleon-nucleon correlations are investigated and found to be necessary to explain the reason that nn emission is favored over np emission. These terms are included using a phenomenological model for the πN interaction and a microscopic one where an intermediate isobar is excited. The angular distributions and recoil momentum distributions are also calculated and compared with experiments.     

Search for light neutron-rich isotopes in stopped pion absorption

The results based on the spectroscopy of superheavy hydrogen isotopes (^4?7H), heavy helium isotopes (^6,7He), and heavy lithium isotopes (^7?12Li) produced in stopped pion absorption by light nuclei were analyzed. Search for nuclear states was performed in inclusive and correlation measurements of missing mass spectra. A broad range of excitation energies studied in correlation measurements provided the possibility of search for isobaric analog states and cluster resonances. A comparison with experimental and theoretical results of other authors was conducted.     

Search for superheavy hydrogen isotopes in pion absorption reactions

Review of the experimental results on the search for and the spectroscopy of the superheavy hydrogen isotopes ^4–7H obtained in stopped π^?-meson absorption by ⁹Be and ¹¹Be nuclei is presented. Study of light neutron-rich nuclei is a principal line in developing modern views on the properties of nuclear forces and determination of nuclear properties near the drip line. The present method of investigation relies on precision measurements of energy of charged particles emitted after pion absorption by nuclei. Important advantages of this method are the practically accurate initial state energy and momentum, as well as the possibility to study a wide range of excitation energy. In the frames of this method new results were obtained on level structures of the isotopes ^4–6H and indications on ⁷H production. Comparison with other experimental and theoretical results is performed.