20 research outputs found

    Separated Kaon Electroproduction Cross Section and the Kaon Form Factor from 6 GeV JLab Data

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    The 1H^{1}H(e,eK+e,e^\prime K^+)Λ\Lambda reaction was studied as a function of the Mandelstam variable t-t using data from the E01-004 (FPI-2) and E93-018 experiments that were carried out in Hall C at the 6 GeV Jefferson Lab. The cross section was fully separated into longitudinal and transverse components, and two interference terms at four-momentum transfers Q2Q^2 of 1.00, 1.36 and 2.07 GeV2^2. The kaon form factor was extracted from the longitudinal cross section using the Regge model by Vanderhaeghen, Guidal, and Laget. The results establish the method, previously used successfully for pion analyses, for extracting the kaon form factor. Data from 12 GeV Jefferson Lab experiments are expected to have sufficient precision to distinguish between theoretical predictions, for example recent perturbative QCD calculations with modern parton distribution amplitudes. The leading-twist behavior for light mesons is predicted to set in for values of Q2Q^2 between 5-10 GeV2^2, which makes data in the few GeV regime particularly interesting. The Q2Q^2 dependence at fixed xx and t-t of the longitudinal cross section we extracted seems consistent with the QCD factorization prediction within the experimental uncertainty

    Charged pion form factor between Q^2=0.60 and 2.45 GeV^2. II. Determination of, and results for, the pion form factor

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    The charged pion form factor, Fpi(Q^2), is an important quantity which can be used to advance our knowledge of hadronic structure. However, the extraction of Fpi from data requires a model of the 1H(e,e'pi+)n reaction, and thus is inherently model dependent. Therefore, a detailed description of the extraction of the charged pion form factor from electroproduction data obtained recently at Jefferson Lab is presented, with particular focus given to the dominant uncertainties in this procedure. Results for Fpi are presented for Q^2=0.60-2.45 GeV^2. Above Q^2=1.5 GeV^2, the Fpi values are systematically below the monopole parameterization that describes the low Q^2 data used to determine the pion charge radius. The pion form factor can be calculated in a wide variety of theoretical approaches, and the experimental results are compared to a number of calculations. This comparison is helpful in understanding the role of soft versus hard contributions to hadronic structure in the intermediate Q^2 regime.Comment: 18 pages, 11 figure

    Charged pion form factor between Q2Q^2=0.60 and 2.45 GeV2^2. I. Measurements of the cross section for the 1{^1}H(e,eπ+e,e'\pi^+)nn reaction

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    Cross sections for the reaction 1{^1}H(e,eπ+e,e'\pi^+)nn were measured in Hall C at Thomas Jefferson National Accelerator Facility (JLab) using the CEBAF high-intensity, continous electron beam in order to determine the charged pion form factor. Data were taken for central four-momentum transfers ranging from Q2Q^2=0.60 to 2.45 GeV2^2 at an invariant mass of the virtual photon-nucleon system of WW=1.95 and 2.22 GeV. The measured cross sections were separated into the four structure functions σL\sigma_L, σT\sigma_T, σLT\sigma_{LT}, and σTT\sigma_{TT}. The various parts of the experimental setup and the analysis steps are described in detail, including the calibrations and systematic studies, which were needed to obtain high precision results. The different types of systematic uncertainties are also discussed. The results for the separated cross sections as a function of the Mandelstam variable tt at the different values of Q2Q^2 are presented. Some global features of the data are discussed, and the data are compared with the results of some model calculations for the reaction 1{^1}H(e,eπ+e,e'\pi^+)nn.Comment: 26 pages, 23 figure

    Separated Response Function Ratios in Exclusive, Forward pi^{+/-} Electroproduction

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    The study of exclusive π±\pi^{\pm} electroproduction on the nucleon, including separation of the various structure functions, is of interest for a number of reasons. The ratio RL=σLπ/σLπ+R_L=\sigma_L^{\pi^-}/\sigma_L^{\pi^+} is sensitive to isoscalar contamination to the dominant isovector pion exchange amplitude, which is the basis for the determination of the charged pion form factor from electroproduction data. A change in the value of RT=σTπ/σTπ+R_T=\sigma_T^{\pi^-}/\sigma_T^{\pi^+} from unity at small t-t, to 1/4 at large t-t, would suggest a transition from coupling to a (virtual) pion to coupling to individual quarks. Furthermore, the mentioned ratios may show an earlier approach to pQCD than the individual cross sections. We have performed the first complete separation of the four unpolarized electromagnetic structure functions above the dominant resonances in forward, exclusive π±\pi^{\pm} electroproduction on the deuteron at central Q2Q^2 values of 0.6, 1.0, 1.6 GeV2^2 at WW=1.95 GeV, and Q2=2.45Q^2=2.45 GeV2^2 at WW=2.22 GeV. Here, we present the LL and TT cross sections, with emphasis on RLR_L and RTR_T, and compare them with theoretical calculations. Results for the separated ratio RLR_L indicate dominance of the pion-pole diagram at low t-t, while results for RTR_T are consistent with a transition between pion knockout and quark knockout mechanisms.Comment: 6 pages, 3 figure

    Assessing the potential for sea-based macroalgae cultivation and its application for nutrient removal in the Baltic Sea

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    Marine eutrophication is a pervasive and growing threat to global sustainability. Macroalgal cultivation is a promising circular economy solution to achieve nutrient reduction and food security. However, the location of production hotspots is not well known. In this paper the production potential of macroalgae of high commercial value was predicted across the Baltic Sea region. In addition, the nutrient limitation within and adjacent to macroalgal farms was investigated to suggest optimal site-specific configuration of farms. The production potential of Saccharina latissima was largely driven by salinity and the highest production yields are expected in the westernmost Baltic Sea areas where salinity is >23. The direct and interactive effects of light availability, temperature, salinity and nutrient concentrations regulated the predicted changes in the production of Ulva intestinalis and Fucus vesiculosus. The western and southern Baltic Sea exhibited the highest farming potential for these species, with promising areas also in the eastern Baltic Sea. Macroalgal farming did not induce significant nutrient limitation. The expected spatial propagation of nutrient limitation caused by macroalgal farming was less than 100–250 m. Higher propagation distances were found in areas of low nutrient and low water exchange (e.g. offshore areas in the Baltic Proper) and smaller distances in areas of high nutrient and high water exchange (e.g. western Baltic Sea and Gulf of Riga). The generated maps provide the most sought-after input to support blue growth initiatives that foster the sustainable development of macroalgal cultivation and reduction of in situ nutrient loads in the Baltic Sea.</p

    Exclusive π+ electroproduction off the proton from low to high -t

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    Background: Measurements of exclusive meson production are a useful tool in the study of hadronic structure. In particular, one can discern the relevant degrees of freedom at different distance scales through these studies. Purpose: To study the transition between nonperturbative and perturbative quantum chromodynamics as the square of four-momentum transfer to the struck proton, -t, is increased. Method: Cross sections for the H1(e,e′π+)n reaction were measured over the -t range of 0.272 to 2.127 GeV2 with limited azimuthal coverage at fixed beam energy of 4.709 GeV, Q2 of 2.4 GeV2, and W of 2.0 GeV at the Thomas Jefferson National Accelerator Facility (JLab) Hall C. Results: The -t dependence of the measured π+ electroproduction cross section generally agrees with prior data from JLab Halls B and C. The data are consistent with a Regge amplitude-based theoretical model but show poor agreement with a generalized parton distribution-based model. Conclusion: The agreement of cross sections with prior data implies small contribution from the interference terms, and the confirmation of the change in t slopes between the low- and high - t regions previously observed in photoproduction indicates the changing nature of the electroproduction reaction in our kinematic regime

    Determination of the pion charge form factor at Q[superscript 2] = 1.60 and 2.45 (GeV/c)[superscript 2]

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    Publisher's version/PDFThe [superscript 1]H(e, e'[pi][superscript +])n cross section was measured at four-momentum transfers of Q[superscript 2] = 1.60 and 2.45 GeV[superscript 2] at an invariant mass of the photon nucleon system of W = 2.22 GeV. The charged pion form factor (F[subscript pi]) was extracted from the data by comparing the separated longitudinal pion electroproduction cross section to a Regge model prediction in which F[subscript pi] is a free parameter. The results indicate that the pion form factor deviates from the charge-radius constrained monopole form at these values of Q[superscript 2] by one sigma, but is still far from its perturbative quantum chromodynamics prediction
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