A measurement of the K + total cross sections on carbon and deuterium and their ratios from 450 to 740 MeV/c has been carried out at the Brookhaven Alternating Gradient Synchrotron. The observed ratios depart significantly from those expected from conventional nuclear physics calculations. The data are compared with models of nucleon "swelling," which ascribe the effect to quark deconfinement or, alternatively, to vector-meson exchange with density-dependent masses.PACS numbers: 25.80.Nv, 12.40.Aa, 13.75.Jz The low-momentum AT + holds a very special position as the weakest of any available strongly interacting probes. It has a mean free path in the nucleus larger than 6 fm. Thus the K + is capable of probing the entire volume of the nucleus. l Single scattering of the K + with a nucleon in the nucleus dominates scattering, and only small and calculable higher-order corrections are needed. These properties make the K + the ideal hadronic probe of nuclear-medium effects, and a useful complement to leptonic or electromagnetic probes. The nucleon is a dynamical entity and its internal structure can, in principle, be altered by its surrounding nuclear environment. This work reports an experiment in which the K + is used to compare the nucleon in the nucleus with a free nucleon.Siegel, Kaufmann, and Gibbs, 2 recognizing the special properties of the K + probe and its analogy to the leptonic probes of the European Muon Collaboration (EMC) effect, argued that if the nucleons in the nucleus "swell" (partial deconfinement), the effect could be detected by measuring the ratio of the K + total cross section on carbon to that on deuterium. At low momenta ( < 800 MeV/c) the K*N interaction is dominated by the S\\ channel. The authors predicted that a 10% increase in nucleon size carries with it a (5-10)% increase in Ss n . Such an increase would be consistent with that of the quark-confinement scale predicted by Close et al. 3 Siegel, Kaufmann, and Gibbs calculated the abovementioned ratio in an optical model and concluded that an increase of 10% in the S\\ K*N phase shift would result in ratios significantly higher than the upper limits of the calculation with free K~*~N phase shifts and conventional medium corrections which do not include nucleon "swelling."Brown, Dover, Siegel, and Weise 4 took another view of the swelling effect and pointed out that in mesonexchange models of the K + N interaction, p and co exchanges play a dominant role. The vector-meson mass is density dependent which in turn implies a densitydependent K + N scattering amplitude. The elastic scattering and reaction cross sections were then calculated in an optical potential derived from the scattering amplitude. They also calculated the ratio of total cross sections of K*C to K*d, with the result that a reasonable density parameter produced an increase in the ratio similar to the predictions of Siegel, Kaufmann, and Gibbs. Weise 5 has compared these alternative models and discussed their interpretation in terms of nucleon swelling. In this paper, the ...
1. Until recently studies of intestinal aluminium absorption used pharmacological amounts of stable 27Al. 2. To examine the intestinal absorption of trace amounts of different chemical compounds of aluminium, in the present study we have employed the long half-life isotope of aluminium, 26Al, and accelerator mass spectrometry. Trace amounts of 26Al (2.7-12.1 ng) as the hydroxide, citrate, citrate plus 1 mmol/kg sodium citrate, or maltolate respectively, were administered to four groups of rats (n = 9 per group) by gavage. Blood and urine samples were collected for 5 h and the 26Al content (as a percentage of the administered dose) determined by accelerator mass spectrometry. 3. The 5 h urinary 26Al excretion amounted to 0.1 +/- 0.02, 0.7 +/- 0.2, 5.1 +/- 1.5 and 0.1 +/- 0.1% of administered dose in the four groups respectively. There was a strong positive correlation between peak plasma 26Al (r = 0.98) and urinary 26Al excretion in individual animals (P < 0.001). 4. We conclude that the fractional intestinal absorption of trace oral doses of aluminium hydroxide is at least 0.1% (compared with the previous estimate of 0.01% using large 27Al oral loads). Absorption of aluminium citrate given alone is significantly greater (0.7%) and is further increased to 5% by the accompanying sodium citrate, consistent with an enhancing effect of added citrate upon mucosal aluminium permeability. Aluminium maltolate absorption approximates that of aluminium hydroxide (0.1%).
Pion absorption in He was studied at T =62.5 and 82.8 MeV using nucleon-nucleon coincidences, For~+ absorption on proton-neutron pairs the differential cross section is the same as that for n. ++d~p+p except for an increase by a factor of about 1.5. For m absorption on the proton-proton pair, the differential cross section is asymmetric about 90', indicating possible isospin mixing. The total cross sections Op, (m+) are 10.2%0.9 mb and 13.5+1.3 mb at 62.5 and 82.8 MeV and for opp(~) are 0 70%0 07 mb and 0 92+0 10 mb at 62 5 and 82 8 MeV The three body absorption cross sections for m+ and n are found to be comparable to each other and show no strong energy dependence. The three-body absorption cross section 03(m+) is 6.7%2.5 mb and 5.7+2.3 mb and for m, a3(m ) is 8.7+1.4 mb and 6.5+2.0 mb at 62.5 and 82.8 MeV, respectively.
Total cross sections for the H(/r + ,;r + /r + )/2 reaction have been measured at pion kinetic energies of 180, 184, 190, and 200 MeV. The threshold value for the matrix element ain^K*) and the s-wave, isospin-2, nn scattering length a® were determined. The results were found to be in agreement with chiral perturbation theory and inconsistent with the model of dominance by quark loop anomalies.PACS numbers: 13.75.Gx, 1 UO. Rd, 25.80.Fm Investigations of the underlying symmetries of quantum chromodynamics (QCD) have led to the belief that the chiral-symmetry-breaking formalism developed by Weinberg 1 is the low-energy manifestation of QCD. 2 Chiral perturbation theory (ChPT) extends the original Weinberg theory by including rescattering effects between interacting mesons. For the KK system Gasser and Leutwyler 3 have made ChPT predictions for the ^y-wave, isospin-0 and isospin-2 scattering lengths, namely, a § = (0.20 ± 0.01 )m~x and a\ =( -0.042 ±0.002)m~]. Ivanov and Troitskaya 4 have used the model of dominance by quark loop anomalies (QLAD) to predict a § =0.20m~* and a\ = -0.060™*"'. This model attributes KK rescattering effects to a exchange.Experimental data for a\ are very sparse. The most precise value to date was obtained from a measurement of the A^4 decay parameters by Rosselet et al. 5 and was found to be a 2° -(-0.028 ±0.012)m,T l (a 43% uncertainty). Near threshold, the angular momentum barrier limits the significant Feynman diagrams for the H(/r + , K + K + )n reaction to virtual KK scattering and the contact interaction since these are the only possible 5-wave processes. As a result, at threshold the total cross section is determined by the s-wave isospin-2 scattering length a® and the contact interaction.Olsson and co-workers 6 have derived the following relationship between a2 and CI(K^K + ) by means of an effective-Lagrangian model which relates the total cross section at threshold to a\ (with /* = 93.3 MeV): a(K + K + )=20.%a$ -0.243m*" 1 , where CI(K + K + ) is the reduced matrix element of the threshold value of the cross section (cr) for H(K + ,K + K + )n and is given by a = tf(/r + /r + ) 2 xl.28xl0" 5 r* 2 /> c . m . fib, where T* is the energy above threshold in the center of mass and Pc.m. is the center-of-mass momentum of the incident pion.In this formalism the strength of the KK interaction is characterized by the chiral-symmetry-breaking parameter £ as derived by Olsson and Turner. 6 Then a$ and a2 can be determined from £ via the relations a § = (0.156 -0.0560£)m ;r " 1 and a% =( -0.045 -0.0224$)m*~1, with /*=93.3 MeV. When £=0, the theory is equivalent to lowest-order ChPT. Olsson and Turner believed that a single value of £ would determine ao and a 2 uniquely; however, they ignored the KK rescattering effects incorporated in the ChPT and QLAD approaches. 3,4 Since KK scattering in the H{K +
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.
hi@scite.ai
10624 S. Eastern Ave., Ste. A-614
Henderson, NV 89052, USA
Copyright © 2024 scite LLC. All rights reserved.
Made with 💙 for researchers
Part of the Research Solutions Family.