TY - JOUR
T1 - The DKP equation in presence of a Woods–Saxon potential
T2 - Transmission resonances and bound states
AU - Garzón, Alexis
AU - Fernández, Ricardo
AU - Arévalo, Vicente A.
AU - Laroze, David
AU - Pérez, Laura M.
AU - de Zayas, Benjamín
AU - Rojas, Clara
N1 - Publisher Copyright:
© 2025 World Scientific Publishing Company.
PY - 2025/8/20
Y1 - 2025/8/20
N2 - In this paper, we solve the Duffin–Kemmer–Petiau (DKP) equation in the presence of the Woods–Saxon potential barrier and well for spin-one particles. We derive the scattering solution in terms of the Gaussian hypergeometric function 2F1(a, b; c; z), the regularized Gaussian hypergeometric function 2F̃1(a,b;c;z), and the Gamma function Γ(x). Our analysis reveals the presence of transmission resonances. To observe these resonances, we calculate and plot the transmission T and reflection R coefficients for various parameters of the Woods–Saxon potential barrier. Our results are compared with those obtained for the square potential barrier and the cusp potential barrier, which represent limiting cases of the Woods–Saxon potential barrier. Furthermore, we investigate the bound state solutions, determining the critical turning point Vcr to study particle–antiparticle creation and compute the norm N. Finally, we also compare our results with those obtained for the square potential well and the cusp potential well, confirming that pair creation occurs in both potential wells.
AB - In this paper, we solve the Duffin–Kemmer–Petiau (DKP) equation in the presence of the Woods–Saxon potential barrier and well for spin-one particles. We derive the scattering solution in terms of the Gaussian hypergeometric function 2F1(a, b; c; z), the regularized Gaussian hypergeometric function 2F̃1(a,b;c;z), and the Gamma function Γ(x). Our analysis reveals the presence of transmission resonances. To observe these resonances, we calculate and plot the transmission T and reflection R coefficients for various parameters of the Woods–Saxon potential barrier. Our results are compared with those obtained for the square potential barrier and the cusp potential barrier, which represent limiting cases of the Woods–Saxon potential barrier. Furthermore, we investigate the bound state solutions, determining the critical turning point Vcr to study particle–antiparticle creation and compute the norm N. Finally, we also compare our results with those obtained for the square potential well and the cusp potential well, confirming that pair creation occurs in both potential wells.
KW - DKP equation
KW - Woods–Saxon potential
KW - bound states
KW - transmission resonances
UR - https://www.scopus.com/pages/publications/105009108412
U2 - 10.1142/S0217751X25500782
DO - 10.1142/S0217751X25500782
M3 - Article
AN - SCOPUS:105009108412
SN - 0217-751X
VL - 40
JO - International Journal of Modern Physics A
JF - International Journal of Modern Physics A
IS - 23
M1 - 2550078
ER -