Kiadtisak Saenboonruang

Prof. Dr. Kiadtisak Saenboonruang

Applied Radiation and Isotopes, Kasetsart University, Bangkok, Krung Thep Maha Nakhon, Thailand
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Research Focus & Metrics

Academic Career Length

15Years (2012-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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15 March 2012 in Physical Review Letters
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Journal Article
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SAS. Abrahamyan
S. Abrahamyan
ZAZ. Ahmed
Z. Ahmed
HAH. Albataineh
H. Albataineh
KAK. Aniol
K. Aniol
DAD. S. Armstrong
D. S. Armstrong
PCPREX Collaboration
PREX Collaboration
We report the first measurement of the parity-violating asymmetry APV in the elastic scattering of polarized electrons from Pb208. APV is sensitive to the radius of the neutron distribution (Rn). The result APV=0.656±0.060(stat)±0.014(syst)  ppm corresponds to a difference between the radii of the neutron and proton distributions Rn−Rp=0.33−0.18+0.16  fm and provides the first electroweak observation of the neutron skin which is expected in a heavy, neutron-rich nucleus.

26 March 2012 in Physical Review C
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CHC. J. Horowitz
C. J. Horowitz
ZAZ. Ahmed
Z. Ahmed
CJC. -M. Jen
C. -M. Jen
ARA. Rakhman
A. Rakhman
PSP. A. Souder
P. A. Souder
GUG. M. Urciuoli
G. M. Urciuoli
We use distorted wave electron scattering calculations to extract the weak charge form factor FW(q¯), the weak charge radius RW, and the point neutron radius Rn of 208Pb from the Lead Radius Experiment (PREX) parity-violating asymmetry measurement. The form factor is the Fourier transform of the weak charge density at the average momentum transfer q¯=0.475 fm−1. We find FW(q¯)=0.204±0.028(exp)±0.001(model). We use the Helm model to infer the weak radius from FW(q¯). We find RW=5.826±0.181(exp)±0.027(model)fm. Here the experimental error includes PREX statistical and systematic errors, while the model error describes the uncertainty in RW from uncertainties in the surface thickness σ of the weak charge density. The weak radius is larger than the charge radius, implying a “weak charge skin” where the surface region is relatively enriched in weak charges compared to (electromagnetic) charges. We extract the point neutron radius Rn=5.751±0.175(exp)±0.026(model)±0.005(strange)fm from RW. Here there is only a very small error (strange) from possible strange quark contributions. We find Rn to be slightly smaller than RW because of the nucleon's size. Finally, we find a neutron skin thickness of Rn−Rp=0.302±0.175(exp)±0.026 (model) ± 0.005 (strange) fm, where Rp is the point proton radius.

1 December 2018 in Radiation Physics and Chemistry
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Journal Article
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WPWorawat Poltabtim
Worawat Poltabtim
EWEkachai Wimolmala
Ekachai Wimolmala
Kiadtisak SaenboonruangKiadtisak Saenboonruang
Kiadtisak Saenboonruang

5 March 2012 in Physical Review Letters
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ZAZ. Ahmed
Z. Ahmed
KAK. Allada
K. Allada
KAK. A. Aniol
K. A. Aniol
DAD. S. Armstrong
D. S. Armstrong
JAJ. Arrington
J. Arrington
HCHAPPEX Collaboration
HAPPEX Collaboration
The parity-violating cross-section asymmetry in the elastic scattering of polarized electrons from unpolarized protons has been measured at a four-momentum transfer squared Q2=0.624  GeV2 and beam energy Eb=3.48  GeV to be APV=−23.80±0.78(stat)±0.36(syst) parts per million. This result is consistent with zero contribution of strange quarks to the combination of electric and magnetic form factors GEs+0.517GMs=0.003±0.010(stat)±0.004(syst)±0.009(ff), where the third error is due to the limits of precision on the electromagnetic form factors and radiative corrections. With this measurement, the world data on strange contributions to nucleon form factors are seen to be consistent with zero and not more than a few percent of the proton form factors.

10 November 2017 in Nature Communications
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MDM. Defurne
M. Defurne
AJA. Martí Jiménez-Argüello
A. Martí Jiménez-Argüello
ZAZ. Ahmed
Z. Ahmed
HAH. Albataineh
H. Albataineh
KAK. Allada
K. Allada
PZP. Zhu
P. Zhu
The internal structure of nucleons (protons and neutrons) remains one of the greatest outstanding problems in modern nuclear physics. By scattering high-energy electrons off a proton we are able to resolve its fundamental constituents and probe their momenta and positions. Here we investigate the dynamics of quarks and gluons inside nucleons using deeply virtual Compton scattering (DVCS)—a highly virtual photon scatters off the proton, which subsequently radiates a photon. DVCS interferes with the Bethe-Heitler (BH) process, where the photon is emitted by the electron rather than the proton. We report herein the full determination of the BH-DVCS interference by exploiting the distinct energy dependences of the DVCS and BH amplitudes. In the regime where the scattering is expected to occur off a single quark, measurements show an intriguing sensitivity to gluons, the carriers of the strong interaction.

16 November 2017 in Iranian Polymer Journal
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Donruedee ToyenDonruedee Toyen
Donruedee Toyen
ARAnawat Rittirong
Anawat Rittirong
WPWorawat Poltabtim
Worawat Poltabtim
Kiadtisak SaenboonruangKiadtisak Saenboonruang
Kiadtisak Saenboonruang