Isotopic imaging via nuclear resonance fluorescence with laser-based Thomson radiation
View Patent ↗The present invention utilizes novel laser-based, high-brightness, high-spatial-resolution, pencil-beam sources of spectrally pure hard x-ray and gamma-ray radiation to induce resonant scattering in specific nuclei, i.e., nuclear resonance fluorescence. By monitoring such fluorescence as a function of beam position, it is possible to image in either two dimensions or three dimensions, the position and concentration of individual isotopes in a specific material configuration. Such methods of the present invention material identification, spatial resolution of material location and ability to locate and identify materials shielded by other materials, such as, for example, behind a lead wall. The foundation of the present invention is the generation of quasimonochromatic high-energy x-ray (100's of keV) and gamma-ray (greater than about 1 MeV) radiation via the collision of intense laser pulses from relativistic electrons. Such a process as utilized herein, i.e., Thomson scattering or inverse-Compton scattering, produces beams having diameters from about 1 micron to about 100 microns of high-energy photons with a bandwidth of ΔE/E of approximately 10E −3 .
1. A Nuclear Resonance Fluorescence detection method, comprising:
directing a beam of Thomson radiation comprising a fractional bandwidth of about 10 −3 at a target region so as to probe for one or more suspect materials;
resonantly exciting nuclei of said one or more suspect materials within said target region with said beam of Thomson radiation;
resonantly exciting nuclei of a reference scatterer with said beam transmitted through said suspect material, said reference scatterer comprising one or more predetermined nuclear species of interest; and
measuring an energy spectrum of photons resulting from said resonantly excited reference scatterer, wherein a disparity between the attenuation measured for resonant and non-resonant photons indicates a detected said suspect material.
2. The method of claim 1 , wherein said beam of Thomson radiation comprises a beam diameter from about 1 micron to about 100 microns.
3. The method of claim 2 , wherein said beam of Thomson radiation comprises a beam diameter of about 10 microns.
4. The method of claim 1 , wherein said beam of Thomson radiation comprises beams of relativistic electrons having a narrow relative kinetic energy spread, Δγ/γ of less than about 10 −3 .
5. The method of claim 1 , wherein said measured disparity between resonant and non-resonant photons comprises an attenuation width, ΔE/E, of less than about 10 −6 .
6. The method of claim 1 , wherein said beam of Thomson radiation comprises a beam divergence of less than about 1 mrad.
7. The method of claim 1 , wherein a detector array is configured to measure the rate of resonant scattering so as to determine the flux of resonant photons exiting said target region.
8. The method of claim 1 , wherein said target having said suspect material is imaged by moving the beam, the target, or both, and/or by controlling the angular distribution of the electrons in the interaction region of said Thomson radiation source so as to scan said beam over the extent of said target.
9. The method of claim 1 , wherein said Thomson radiation can be tuned to a resonant energy by changing the electron beam energy or by changing the laser interaction wavelengths.
10. A Nuclear Resonance Fluorescence apparatus, comprising:
a Thomson radiation source comprising a fractional bandwidth of about 10 −3 ;
means for directing said Thomson radiation source at a target region;
one or more reference resonance scatterers, said reference resonance scatterers comprising one or more predetermined nuclear species of interest and wherein said one or more reference resonance scatterers are further configured to receive transmitted radiation resulting from said Thomson radiation source through said target; and
means for measuring a predetermined nuclear species of interest by measuring the energies of photons scattered from said reference scatterers, wherein a disparity between the attenuation measured for resonant and non-resonant photons indicates a detected suspect material.
11. The apparatus of claim 10 , wherein said Thomson radiation source comprises a beam diameter from about 1 micron to about 100 microns.
12. The apparatus of claim 11 , wherein said Thomson radiation source comprises a beam diameter of about 10 microns.
13. The apparatus of claim 10 , wherein said Thomson radiation source comprises relativistic electrons having a narrow relative kinetic energy spread Δγ/γ, of less than about 10 −3 .
14. The apparatus of claim 10 , wherein said measured disparity between resonant and non-resonant photons comprises an attenuation width, ΔE/E, of less than about 10 −6 .
15. The apparatus of claim 10 , wherein said Thomson radiation source comprises a beam divergence of less than about 1 mrad.
16. The apparatus of claim 10 , wherein a detector array is configured to measure the rate of resonant scattering so as to determine the flux of resonant photons exiting said target region.
17. The apparatus of claim 10 , wherein said target having said suspect material is imaged by moving the beam, the target, or both, and/or by controlling the angular distribution of the electrons in the interaction region of said Thomson radiation source so as to scan said beam over the extent of said target.
18. The apparatus of claim 10 , wherein said Thomson radiation source comprises a resonant energy tuned by changing an electron beam energy or an interaction lasing wavelength so that a predetermined fraction of the photons has the right energy to excite a resonance in a nuclear species of interest.
19. The apparatus of claim 18 , wherein said interaction lasing wavelengths are obtained by a lasing material selected from Neodymium(Nd)-doped glass, Neodymium-doped yttrium lithium fluoride, Yb:YAG, Ti:Sapphire, Yb:glass, KGW, KYW, YLF, S-FAP, YALO, YCOB, Cr:forsterite, and GdCOB.
20. The apparatus of claim 18 , wherein said interaction lasing wavelengths are obtained by utilizing an optical parametric oscillator.
21. The apparatus of claim 10 , wherein said means for measuring comprises at least one detector selected from: an Aluminum Antimonide radiation detector, a Germanium radiation detector, a high-purity Germanium (HPGe) radiation detector, and a cryo-cooled Germanium radiation detector.