Patent Number: 048045144
Section: claims

1. Apparatus for measuring intensity of a neutron flux comprising: (a) means exposed to said neutron flux for generating fission fragments at a rate proportional to said intensity;  (b) means exposed to a known fraction of said fission fragments for generating light signals in response to said known fraction of fission fragments, said light generating means being comprised of a solid layer of material having a thickness selected in accordance with a maximum range of said fission fragments in said light generating means;  (c) means, optically coupled to said light signal generating means, for generating electrical signals in response to said light signals; and  (d) means, electrically coupled to said electrical signal generating means, for processing said electrical signals to determine said intensity.  (a) second means exposed to said neutron flux for generating second fission fragments at a rate proportional to flux intensity of neutrons having an energy greater than a second fission energy threshold, said second fission energy threshold being different from said first fission energy threshold;  (b) means exposed to a second known fraction of said second fission fragments for generating second light signals in response to said second known fraction.  second means on a side of said fission fragment generating means opposite a side of said fission fragment generating means on which said means for generating light signals is positioned, and exposed to a second known fraction of fission fragments for generating second light signals in response to said second known fraction;  means, optically coupled to said second light signal generating means, for generating second electrical signals in response to said second light signals; and  means, electrically coupled to said first electrical signal generating means and said second electrical generating means, for detecting coincidences between said first electrical signals and said second electrical signals.  (a) generating fission fragments at a rate proportional to said intensity;  (b) exposing a solid material scintillator means of a thickness approximately on the order of a maximum penetration range of said fission fragments in the material of said scintillator means to said generated fission fragments whereby light signals are generated;  (c) generating electrical signals in response to said generated light signals; and  (d) processing said electrical signals to determine said intensity.  (e) generating fission fragments at a rate proportional to an intensity of neutrons having a second energy minimum energy level different from said first minimum energy level;  (f) generating light signals in response to a known fraction of said fission fragments generated in said step (e);  (g) generating electrical signals in response to said light signals generated in said step (f); and  (h) processing said second electrical signals generated in said step (g) together with said signals generated in said step (c) in order to determine a spectral distribution of said neutron flux.  (a) simultaneously generating a first and second fission fragment in response to one of said neutrons, said second fission fragment propagating in a direction opposite from the direction of propagation of said first fission fragment;  (b) generating a first light signal in response to said first fission fragment;  (c) generating a second light signal in response to said second fission fragment;  (d) detecting a coincidence between said first and second light signals; and  (e) generating a signal indicative of total energy liberated by first and second fission fragments corresponding to said coincidence.  (a) means disposed within said pressure vessel and exposed to the flux of neutrons from said core for generating fission fragments at a rate proportional to an intensity of said flux;  (b) light signal generating means exposed to a known fraction of said fission fragments for generating light signals in response to said known fraction, said light generating means having a thickness approximately on the order of a maximum penetration range of said fission fragments in said light generating means;  (c) means, optically coupled to said light signal generating means, for generating electrical signals in response to said light signals; and  (d) means, electrically coupled to said electrical signal generating means, for processing said electrical signals to determine intensity. 2. An apparatus as claimed in claim 1 wherein said means for generating fission fragments comprises a thin layer of fissile material. 3. An apparatus as claimed in claim 2 wherein said fissile material is selected from the group consisting of .sup.238 U, .sup.237 Np, .sup.235 U, and .sup.239 Pu. 4. An apparatus as claimed in claim 2 wherein said fissile layer has a thickness of approximately 5 microns. 5. An apparatus as claimed in claim 1 wherein said means for generating light comprises a scintillator. 6. An apparatus as claimed in claim 5 wherein said scintillator is comprised of a material selected from the group consisting of ZnS, NaI and CsI. 7. An apparatus as claimed in claim 1 wherein said means for generating electrical signals comprises a photomultiplier tube. 8. An apparatus as claimed in claim 1 wherein said light signal generating means and said electrical signal generating means are adjacent one another. 9. An apparatus as claimed in claim 1, further comprising means, optically coupled to said light generating means and said electrical signal generating means, for conducting light between said light signal generating means and said electrical signal generating means. 10. An apparatus as claimed in claim 9 wherein said means for conducting light comprises a plurality of optical fibers. 11. An apparatus as claimed in claim 9 wherein said light conducting means comprises a light pipe. 12. An apparatus as claimed in claim 1 wherein said means for generating fission fragments generates said fission fragments at a rate proportional to a flux intensity of neutrons having an energy above a first fission energy threshold, and further comprising: 13. An apparatus as claimed in claim 1 further comprising: 14. A method for measuring the intensity of a neutron flux comprising the steps of: 15. A method as claimed in claim 14 wherein said step (a) comprises exposing a fissile material to said neutron flux. 16. Apparatus according to claim 1, wherein said solid layer of material is of a thickness approximately on the order of a maximum penetration range of said fission fragments in the material of said solid layer. 17. A method as claimed in claim 15 wherein said step (a) is limited to generating fission fragments at a rate proportional to an intensity of neutrons having an energy greater than a first threshold, and further comprising the steps of 18. A method for measuring intensity of a flux of neutrons comprising the steps of: 19. A nuclear reactor having a pressure vessel, and a core within said pressure vessel for generating a flux of neutrons and comprising: