Abstract
We consider the electric and magnetic polarisabilities of the proton including the valence quark as well as pion dressing effects in an independent quark model with an effective scalar-vector harmonic potential which renders the solvability of relativistic Dirac equations for confined quarks, and has in fact acted as an alternative to the cloudy bag model (CBM). This model which has been applied successfully to a variety of hadronic problems is also observed here to yield the electromagnetic polarisabilities of the proton satisfactorily without any free parameters. The electric and magnetic polarisabilities, including valence quark core and pion cloud effects, obtained here as anti {alpha}{sub P}=14.074.10{sup -4} fm{sup 3} and anti {beta}{sub P}=3.155.10{sup -4} fm{sup 3}, are well within the uncertainties of their experimental measurements of (10.9{+-}2.2{+-}1.4).10{sup -4} fm{sup 3} and (3.3{+-}2.2{+-}1.4).10{sup -4} fm{sup 3}, respectively and are also in agreement with other model estimations. (orig.).
Barik, N;
[1]
Dash, B K;
[1]
Das, P;
[2]
Panda, A R
[2]
- Utkal Univ., Bhubaneswer (India). P.G. Dept. of Phys.
- Department of Physics, Kendrapara College, Kendrapara-754211 (India)
Citation Formats
Barik, N, Dash, B K, Das, P, and Panda, A R.
Electromagnetic polarisabilities of the proton in an independent particle potential model.
Netherlands: N. p.,
1996.
Web.
doi:10.1016/0375-9474(96)00103-0.
Barik, N, Dash, B K, Das, P, & Panda, A R.
Electromagnetic polarisabilities of the proton in an independent particle potential model.
Netherlands.
https://doi.org/10.1016/0375-9474(96)00103-0
Barik, N, Dash, B K, Das, P, and Panda, A R.
1996.
"Electromagnetic polarisabilities of the proton in an independent particle potential model."
Netherlands.
https://doi.org/10.1016/0375-9474(96)00103-0.
@misc{etde_385053,
title = {Electromagnetic polarisabilities of the proton in an independent particle potential model}
author = {Barik, N, Dash, B K, Das, P, and Panda, A R}
abstractNote = {We consider the electric and magnetic polarisabilities of the proton including the valence quark as well as pion dressing effects in an independent quark model with an effective scalar-vector harmonic potential which renders the solvability of relativistic Dirac equations for confined quarks, and has in fact acted as an alternative to the cloudy bag model (CBM). This model which has been applied successfully to a variety of hadronic problems is also observed here to yield the electromagnetic polarisabilities of the proton satisfactorily without any free parameters. The electric and magnetic polarisabilities, including valence quark core and pion cloud effects, obtained here as anti {alpha}{sub P}=14.074.10{sup -4} fm{sup 3} and anti {beta}{sub P}=3.155.10{sup -4} fm{sup 3}, are well within the uncertainties of their experimental measurements of (10.9{+-}2.2{+-}1.4).10{sup -4} fm{sup 3} and (3.3{+-}2.2{+-}1.4).10{sup -4} fm{sup 3}, respectively and are also in agreement with other model estimations. (orig.).}
doi = {10.1016/0375-9474(96)00103-0}
journal = []
issue = {4}
volume = {605}
journal type = {AC}
place = {Netherlands}
year = {1996}
month = {Aug}
}
title = {Electromagnetic polarisabilities of the proton in an independent particle potential model}
author = {Barik, N, Dash, B K, Das, P, and Panda, A R}
abstractNote = {We consider the electric and magnetic polarisabilities of the proton including the valence quark as well as pion dressing effects in an independent quark model with an effective scalar-vector harmonic potential which renders the solvability of relativistic Dirac equations for confined quarks, and has in fact acted as an alternative to the cloudy bag model (CBM). This model which has been applied successfully to a variety of hadronic problems is also observed here to yield the electromagnetic polarisabilities of the proton satisfactorily without any free parameters. The electric and magnetic polarisabilities, including valence quark core and pion cloud effects, obtained here as anti {alpha}{sub P}=14.074.10{sup -4} fm{sup 3} and anti {beta}{sub P}=3.155.10{sup -4} fm{sup 3}, are well within the uncertainties of their experimental measurements of (10.9{+-}2.2{+-}1.4).10{sup -4} fm{sup 3} and (3.3{+-}2.2{+-}1.4).10{sup -4} fm{sup 3}, respectively and are also in agreement with other model estimations. (orig.).}
doi = {10.1016/0375-9474(96)00103-0}
journal = []
issue = {4}
volume = {605}
journal type = {AC}
place = {Netherlands}
year = {1996}
month = {Aug}
}