Abstract
We consider a method for optimizing the tunnel effect for low-energy particles by using coherent correlated states formed under controllable pulsed action on these particles. Typical examples of such actions are the effect of a pulsed magnetic field on charged particles in a gas or plasma. Coherent correlated states are characterized most comprehensively by the correlation coefficient r(t); an increase of this factor elevates the probability of particle tunneling through a high potential barrier by several orders of magnitude without an appreciable increase in their energy. It is shown for the first time that the formation of coherent correlated states, as well as maximal |r(t)|max and time-averaged 〈|r(t)|〉 amplitudes of the correlation coefficient and the corresponding tunneling probability are characterized by a nonmonotonic (oscillating) dependence on the forming pulse duration and amplitude. This result makes it possible to optimize experiments on the realization of low-energy nuclear fusion and demonstrates the incorrectness of the intuitive idea that the tunneling probability always increases with the amplitude of an external action on a particle. Our conclusions can be used, in particular, for explaining random (unpredictable and low-repeatability) experimental results on optimization of energy release from nuclear reactions occurring under a pulsed action with fluctuations of the amplitude and duration. We also consider physical premises for the observed dependences and obtain optimal relations between the aforementioned parameters, which ensure the formation of an optimal coherent correlated state and optimal low-energy tunneling in various physical systems with allowance for the dephasing action of a random force. The results of theoretical analysis are compared with the data of successful experiments on the generation of neutrons and alpha particles in an electric discharge in air and gaseous deuterium.
Similar content being viewed by others
References
V. V. Dodonov, E. V. Kurmishev, and V. I. Manko, Phys Lett. A 79, 150 (1980).
V. V. Dodonov and V. I. Man’ko, Transactions of FIAN (Russia) 183, 71 (1987).
V. V. Dodonov, A. B. Klimov, and V. I. Man’ko, Transactions of FIAN (Russia) 200, 56 (1991).
V. V. Dodonov, A. B. Klimov, and V. I. Man’ko, Phys Lett. A 220, 41 (1996).
V. I. Vysotskii and S. V. Adamenko, Tech Phys. 55, 613 (2010).
V. I. Vysotskii, M. V. Vysotskyy, and S. V. Adamenko, J. Exp. Theor. Phys. 114, 243 (2012).
V. I. Vysotskii, S. V. Adamenko, and M. V. Vysotskyy, J. Exp. Theor. Phys. 115, 551 (2012).
V. I. Vysotskii and M. V. Vysotskyy, Eur Phys. J. A 49, 99 (2013). doi 10.1140/epja/i2013-13099-2
V. I. Vysotskii, S. V. Adamenko, and M. V. Vysotskyy, Ann Nucl. Energy 62, 618 (2013).
V. I. Vysotskii and M. V. Vysotskyy, J. Exp. Theor. Phys. 118, 534 (2014).
V. V. Dodonov and A. V. Dodonov, J. Russ. Laser Res. 35, 39 (2014).
A. V. Dodonov and V. V. Dodonov, Phys Lett. A 35, 1071 (2014).
V. I. Vysotskii and M. V. Vysotskyy, J. Exp. Theor. Phys. 121, 559 (2015).
V. I. Vysotskii and M. V. Vysotskyy, Curr Sci. 108, 524 (2015).
E. Schrödinger, Ber. Kgl. Akad. Wiss., Berlin S24, 296 (1930).
H. P. Robertson, Phys Rev. A 35, 667 (1930).
V. V. Dodonov and A. V. Dodonov, Phys Scripta 90, 074049 (2015).
V. I. Vysotskii, S. V. Adamenko, and M. V. Vysotskii, J. Surf. Invest.: X-ray, Synchrotron Neutron Tech. 6, 369 (2012).
V. I. Vysotskii, M. V. Vysotskyy, and S. Bartalucci, Ann Nucl. Energy 62, 613 (2013).
V. I. Vysotskii and A. A. Kornilova, Ann Nucl. Energy 62, 626 (2013).
V. I. Vysotskii and A. A. Kornilova, Curr Sci. 108, 636 (2015).
V. N. Chernega, J. Russ. Laser Res. 34, 168 (2013).
D. Letts, D. Cravens, and P. I. Hagelstein, Low-Energy Nuclear Reactions Sourcebook (Am. Chem. Soc., Washington, DC, 2009), Vol. 2, p. 81.
V. I. Vysotskii and M. V. Vysotskyy, J. Exp. Theor. Phys. 120, 246 (2015).
V. I. Dubinko, Lett Mater. 5, 87 (2015).
S. Adamenko, and F. Selleri, and A. van der Merwe, Fundam. Theor. Phys. 156 (2007).
S. V. Adamenko and V. I. Vysotskii, Found Phys. 34, 1801 (2004).
S. V. Adamenko and V. I. Vysotskii, Found Phys. Lett. 17, 203 (2004).
S. V. Adamenko and V. I. Vysotskii, Found Phys. Lett. 19, 21 (2006).
L. I. Urutskoev, V. I. Liksonov, and V. G. Tsinoev, Ann Found. Louis de Broglie 27, 701 (2002).
M. I. Lomaev and B. A. Nechaev, V. N. Padalko, S. I. Kuznetsov, D. A. Sorokin, V. F. Tarasenko, and A. P. Yalovets, Tech Phys. 57, 124 (2012).
A. V. Agafonov, A. V. Bagulya, O. D. Dalkarov, et al., Phys Rev. Lett. 111, 115003 (2013).
R. Mills, http://brilliantlightpower.com.
P. Caldirola, Nuovo Cim. 18, 393 (1941).
E. Kanai, Progr Theor. Phys. 3, 440 (1948).
E. M. Bazylyan and Yu. P. Raizer, Lightning Physics and Lightning Protection (Fizmatlit, Moscow, 2001; CRC, Boca Raton, FL, 2000).
A. V. Gurevich, V. P. Antonova, A. P. Chubenko, et al., Phys Rev. Lett. 108, 125001 (2012).
B. Zh. Zalikhanov, Phys Part. Nucl. 47, 108 (2016).
Author information
Authors and Affiliations
Corresponding author
Additional information
Original Russian Text © V.I. Vysotskii, M.V. Vysotskyy, 2017, published in Zhurnal Eksperimental’noi i Teoreticheskoi Fiziki, 2017, Vol. 152, No. 2, pp. 234–251.
Rights and permissions
About this article
Cite this article
Vysotskii, V.I., Vysotskyy, M.V. Formation of correlated states and tunneling for a low energy and controlled pulsed action on particles. J. Exp. Theor. Phys. 125, 195–209 (2017). https://doi.org/10.1134/S106377611707024X
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1134/S106377611707024X