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| ==Mechanism== | ==Mechanism== | ||
| In all fusion processes, the ] sets the requisite energy which interacting ] need to fuse. Since nuclei are always positively charged the ] is always repulsive. One way to avoid this problem is to use ] since they have no charge, the Coulomb barrier for such interactions is nil. Since isolated neutrons are unstable, the neutrons themselves must be created through other nuclear reactions. The O-P process allows for similar sorts of nuclear reactions to take place with naturally occurring stable deuterium. | In all fusion processes, the ] sets the requisite energy which interacting ] need to fuse. Since nuclei are always positively charged the ] is always repulsive. One way to avoid this problem is to use ] since they have no charge, the Coulomb barrier for such interactions is nil. Since isolated neutrons are unstable, the neutrons themselves must be created through other nuclear reactions. The O-P process allows for similar sorts of nuclear reactions to take place with naturally occurring stable deuterium. | ||
| During the O-P process, the deuteron's positive charge is spatially polarized, as if at one end of a ], the proton end. As the deuteron approaches the target nucleus, it is repelled by the ], converting ] to ] until, assuming the energy is not sufficient for it to surmount the barrier, the deuteron approaches to a minimum distance. Fusion proceeds when the unstable deuterated nucleus decays into daughter nuclei, normally a proton being one of the products. | During the O-P process, the deuteron's positive charge is spatially polarized, as if at one end of a ], the proton end. As the deuteron approaches the target nucleus, it is repelled by the ], converting ] to ] until, assuming the energy is not sufficient for it to surmount the barrier, the deuteron approaches to a minimum distance. Fusion proceeds when the unstable deuterated nucleus decays into daughter nuclei, normally a proton being one of the products. | ||
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The Oppenheimer–Phillips process or strip reaction is a type of deuteron-induced nuclear reaction.
In this process the neutron half of an energetic deuteron fuses with a target nucleus, transmuting it to a heavier isotope, while the proton half is ejected. An example would be the nuclear transmutation of carbon-12 to carbon-13.
The process is considered important because the cross section for the interaction is enhanced over that expected from the Bohr model due to a polarization of the deuteron where the proton-end faces away from the incident nucleus and the neutron-end faces towards the incident nucleus during most energetically favorable arrangement for the reaction.
History
Explanation of this effect was published by J. Robert Oppenheimer and Melba Phillips in 1935, considering experiments with the Berkeley cyclotron showing that some elements became radioactive under deuteron bombardment.
Mechanism
In all fusion processes, the Coulomb barrier sets the requisite energy which interacting atomic nuclei need to fuse. Since nuclei are always positively charged the electrostatic force is always repulsive. One way to avoid this problem is to use neutrons since they have no charge, the Coulomb barrier for such interactions is nil. Since isolated neutrons are unstable, the neutrons themselves must be created through other nuclear reactions. The O-P process allows for similar sorts of nuclear reactions to take place with naturally occurring stable deuterium.
During the O-P process, the deuteron's positive charge is spatially polarized, as if at one end of a barbell, the proton end. As the deuteron approaches the target nucleus, it is repelled by the electrostatic field, converting kinetic energy to potential energy until, assuming the energy is not sufficient for it to surmount the barrier, the deuteron approaches to a minimum distance. Fusion proceeds when the unstable deuterated nucleus decays into daughter nuclei, normally a proton being one of the products.
As the neutron is drawn to the target nucleus, the binding force exerted by it pulls the proton closer than it would otherwise have approached on its own. If the neutron is captured, the proton is stripped from it and is ejected by the electrostatic field, and since it has half the mass of the deuteron, it can recoil with more than double the incident velocity, and may carry away more than the incident kinetic energy of the deuteron, leaving the transmuted nucleus in a state as if it had fused with a neutron of negative kinetic energy.
References
- ^ Friendlander, 2008, p. 68-69
- Oppenheimer, 1995, page 192 cf. Note on the transmutation function for deuterons, J. Robert Oppenheimer and Melba Phillips, Phys. Rev. 48, September 15, 1935, 500-502, received July 1, 1935.
- Blatt, 1991, pp. 508-509
- Blatt, 1991, pp. 508-509
- J. Robert Oppenheimer (1995). Alice Kimball Smith, Charles Weiner (ed.). Robert Oppenheimer: Letters and Recollections (reimpressed, illustrated ed.). Stanford University Press. ISBN 0804726205, 9780804726207.
{{cite book}}: Check|isbn=value: invalid character (help) - Gerhart Friedlander (1949). Introduction to Radiochemistry. John Wiley And Sons. ISBN 1443723096, 9781443723091.
{{cite book}}: Check|isbn=value: invalid character (help) - M. Blatt, John (1991). Theoretical Nuclear Physics (illustrated ed.). Courier Dover Publications. pp. 505–516. ISBN 0486668274, 9780486668277.
{{cite book}}: Check|isbn=value: invalid character (help); Unknown parameter|coauthor=ignored (|author=suggested) (help)
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