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REVISTA DE LA UNIVERSIDAD DEL ZULIA. 3ª época. Año 15, N° 42, 2024
C. Sandoval-Ruiz // ZPF para arreglo de Proyección de Onda: φ-LFSR en Modelado Fp[x]/f(x)…281-305
DOI: https://doi.org/10.46925//rdluz.42.16
Camarda, M. (2021). La secuencia de Fibonacci y los mecanismos de eficiencia energética: hacia
un uso racional y eficiente de la energía a nivel macroscópico.
Revista de la Escuela de
Perfeccionamiento en Investigación Operativa, 29(50), 49-67.
https://revistas.unc.edu.ar/index.php/epio/article/view/35544
Casado, A., & Guerra, S. (2023). Partial Bell-State Measurement with Type-II Parametric
Down Conversion: Extracting Phase Information from the Zeropoint Field (I). Entropy, 25(3),
393. https://doi.org/10.3390/e25030393
Chen, B., Huang, K., Raghupathi, S., Chandratreya, I., Du, Q., & Lipson, H. (2022). Automated
discovery of fundamental variables hidden in experimental data. Nature Computational Science,
2(7), 433-442. https://doi.org/10.1038/s43588-022-00281-6
Deleito, A. (2001) La generalización de la sucesión de Fibonacci permite describir cualquier
sistema lineal mediante el uso de una sola función. Phin, 5(27).
Falcón, N., Williams, P., & Muñoz, A. Nader, D. (2000). Microfísica del relámpago del
Catatumbo.
Revista Ingeniería UC
, 7(1).
Figueroa, C., Castro, L., Fox, J. R., & Lozano, M. (2013). La secuencia de Fibonacci y el número
de oro en ingeniería eléctrica y análisis numérico.
Formación Universitaria
, 6(2), 23-32.
http://dx.doi.org/10.4067/S0718-50062013000200004
French, A. P. (1974). Vibraciones y Ondas. Curso de Física del M.I.T. Primera Edición. Editorial
Reverté.
Haisch, B., & Rueda, A. (2000). On the relation between a zero-point-field-induced inertial
effect and the Einstein–de Broglie formula
. Physics Letters A
, 268(4-6), 224-227.
https://doi.org/10.1016/S0375-9601(00)00186-9
Martín, Á. (2021). Desarrollo de un prototipo para medidas de electroluminiscencia en paneles
solares. En: https://uvadoc.uva.es/bitstream/handle/10324/47990/TFG-I-
1974.pdf?sequence=1&isAllowed=y
Mills, B., Shaeffer, R., Yue, L., & Ho, C. K. (2020). Improving next generation falling particle
receiver designs subject to anticipated operating conditions. In Energy Sustainability, 83631,
V001T02A013. American Society of Mechanical Engineers.
https://asmedigitalcollection.asme.org/ES/proceedings-abstract/ES2020/1086846
Molina, S. (2006). Función de onda en cadena de Fibonacci incluyendo correlación electrónica.
Peña, L., Cetto, A. M., & Valdés-Hernándes, A. (2014). The zero-point field and the emergence
of the quantum.
International Journal of Modern Physics E
, 23(09), 1450049.
https://doi.org/10.1142/S0218301314500499