1 5 Ju l 2 00 5 Antimatter induced fusion and thermonuclear explosions
نویسندگان
چکیده
The feasibility of using antihydrogen for igniting inertial confinement fusion pellets or triggering large scale thermonuclear explosions is investigated. The number of antiproton annihilations required to start a thermonuclear burn wave in either DT or Li2DT is found to be about 10/k, where k is the compression factor of the fuel to be ignited. In the second part, the technologies for producing antiprotons with high energy accelerator systems and the means for manipulating and storing microgram amounts of antihydrogen are examined. While there seems to be no theoretical obstacles to the production of 10 antiprotons per day (the amount required for triggering one thermonuclear bomb), the construction of such a plant involves several techniques which are between 3 and 4 orders of magnitude away from present day technology. Considering the financial and energy investments needed to produce antimatter, applications will probably remain confined to the military domain. Since antihydrogen-triggered thermonuclear explosives are very compact and have extremely reduced fall-out, we conclude that such devices will enhance the proliferation of nuclear weapons and further diffuse the distinction between low-yield nuclear weapons and conventional explosives.
منابع مشابه
The physics of antimatter induced fusion and thermonuclear explosions
The possibility of using antihydrogen for igniting inertial confinement fusion pellets or triggering large scale thermonuclear explosions is investigated. The number of antiproton annihilations required to start a thermonuclear burn wave in either D or Li2DT is found to be about 10/k, where k is the compression factor of the fuel to be ignited. We conclude that the financial and energy investme...
متن کامل1 8 Ju l 2 00 5 Antimatter weapons ( 1946 - 1986 ) : From Fermi and Teller ’ s speculations to the first open scientific publications ∗
We recall the early theoretical speculations on the possible explosive uses of antimatter, from 1946 to the first production of antiprotons, at Berkeley in 1955, and until the first capture of cold antiprotons, at CERN on July 17–18, 1986, as well as the circumstances of the first presentation at a scientific conference of the correct physical processes leading to the ignition of a large scale ...
متن کاملAntimatter Induced Fusion and Thermonuclear Explosions *
The feasibility of using antihydrogen for igniting inertial confinement fusion pellets or triggering large-scale thermonuclear explosions is investigated. The number of antiproton annihilations required to start a thermonuclear burn wave in either DT or Li2DT is found to be about 10/κ, where κ is the compression factor of the fuel to be ignited. In the second part, the technologies for producin...
متن کاملar X iv : h ep - p h / 05 07 14 1 v 1 1 2 Ju l 2 00 5 Volkov solution for two laser beams and ITER Miroslav
We find the solutions of the Dirac equation for two plane waves (laser beams) and we determine the modified Compton formula for the scattering of two photons on an electron. The practical meaning of the two laser beams is, that two laser beams impinging on a target which is constituted from material in the form a foam, can replace 100-200 laser beams impinging on a normal target and it means th...
متن کاملThe 1908 Tunguska cosmic body (TCB) explosion: Role of hydrogen thermonuclear explosion in support of cometary hypothesis
If the 1908 Tunguska cosmic body (TCB) explosion involved a comet, compressional heating of the comet was expected to create hydrogen and deuterium plasma. The velocity distribution of protons and deuterons in this plasma is not expected to be the Maxwell-Boltzmann distribution. It is shown that the use of a generalized momentum distribution leads to substantial increases of deuteron fusion rat...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2008