dipole form factor
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2020 ◽  
Vol 29 (08) ◽  
pp. 2050066
Author(s):  
P. K. Rath ◽  
B. Shukla ◽  
K. Chaturvedi ◽  
V. K. Nautiyal ◽  
R. Chandra ◽  
...  

Within the squark-neutrino mechanism of [Formula: see text]-violating SUSY, sets of 12 nuclear transition matrix elements (NTMEs) are calculated for the neutrinoless double-[Formula: see text] decay [Formula: see text] of [Formula: see text]Zr, [Formula: see text]Mo, [Formula: see text]Pd, [Formula: see text]Te and [Formula: see text]Nd isotopes. Specifically, four sets of HFB wave functions generated with four different parametrizations of the pairing plus multipolar two-body interactions, dipole form factor and three different parametrizations of the Jastrow short-range correlations are employed in the calculation of NTMEs with two possible prescriptions for the hadronization, namely the two-nucleon mode and the pionic mode. Without (with) Miller–Spencer parametrization of short-range correlation, uncertainties in average NTMEs [Formula: see text] (QBM), [Formula: see text] (NRQM), [Formula: see text] (FF3) and [Formula: see text] turn out be 11–18% (29–37%), 11–16% (27–31%), 5–12% (13–17%) and 3–13% (9–15%), respectively.


2019 ◽  
Vol 2019 ◽  
pp. 1-6 ◽  
Author(s):  
Zhen-Yang Wang ◽  
Jing-Juan Qi ◽  
Xin-Heng Guo

In this work, we study the BK¯ molecule in the Bethe-Salpeter (BS) equation approach. With the kernel containing one-particle-exchange diagrams and introducing two different form factors (monopole form factor and dipole form factor) in the vertex, we solve the BS equation numerically in the covariant instantaneous approximation. We investigate the isoscalar and isovector BK¯ systems, and we find that X5568 cannot be a BK¯ molecule.


2015 ◽  
Vol 24 (02) ◽  
pp. 1550008 ◽  
Author(s):  
L. Syukurilla ◽  
T. Mart

We have phenomenologically investigated the kaon photoproduction process γp → K+Λ by combining different types of hadronic form factors (HFFs) inside a covariant isobar model. We obtained the best model with the smallest χ2/N by using the dipole form factor in the Born terms and a combination of the dipole, Gaussian, as well as generalized dipole form factors in the hadronic vertices of the nucleon, kaon and hyperon resonances. By utilizing this model we found that the experimental data used in the analysis are internally consistent, whereas the behavior of differential cross-section at forward angles is not significantly affected by the variation of hadronic coupling constants (CCs) and form factor cutoffs in the model.


2013 ◽  
Vol 28 (24) ◽  
pp. 1350115 ◽  
Author(s):  
M. HAGHIGHAT ◽  
I. MOTIE ◽  
Z. REZAEI

We consider the Lorentz violated extension of the standard model. In this framework, there are terms that explicitly violate CP-symmetry. We examine the CPT-even dμν-term to find the electric dipole moment of charged leptons. We show that the form factors besides the momentum transfer, depend on a new Lorentz-scalar, constructing by dμν and the four momenta of the lepton, as well. Such an energy dependence of the electric dipole form factor leads to an enhancement of the lepton electric dipole moment at high energy, even at the zero momentum transfer. We show that at [Formula: see text] the electric dipole moment of the charged lepton can be as large as 10-14 e cm .


2011 ◽  
Vol 695 (1-4) ◽  
pp. 268-274 ◽  
Author(s):  
J. de Vries ◽  
E. Mereghetti ◽  
R.G.E. Timmermans ◽  
U. van Kolck

2011 ◽  
Vol 696 (1-2) ◽  
pp. 97-102 ◽  
Author(s):  
E. Mereghetti ◽  
J. de Vries ◽  
W.H. Hockings ◽  
C.M. Maekawa ◽  
U. van Kolck

2007 ◽  
Vol 70 (2) ◽  
pp. 349-357 ◽  
Author(s):  
J. Kuckei ◽  
C. Dib ◽  
A. Faessler ◽  
T. Gutsche ◽  
S. G. Kovalenko ◽  
...  

2006 ◽  
Vol 32 (4) ◽  
pp. 547-564 ◽  
Author(s):  
Claudio Dib ◽  
Amand Faessler ◽  
Thomas Gutsche ◽  
Sergey Kovalenko ◽  
Jan Kuckei ◽  
...  

2005 ◽  
Vol 605 (3-4) ◽  
pp. 273-278 ◽  
Author(s):  
W.H. Hockings ◽  
U. van Kolck

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