Real-time multidimensional terahertz imaging system and method
Real-time multidimensional terahertz imaging system and method, the method comprising method for imaging an object, comprising, in a laser pump line: patterning a laser pump beam with known patterns of a radiation beam and illuminating the object with the radiation beam; yielding a patterned pump beam; directing the patterned beam from the pump line and a laser probe beam from a laser probe line to a detection crystal; single-shot detection of the radiation beam waveform; and correlating the single-shot detection and the known patterns.
1. A system for imaging an object, comprising:
a laser source;
a beam splitter, dividing pulses emitted by the laser source into a pump beam in a pump line and a probe beam in a probe line;
in the pump line, a generator of a radiation beam; a pattern generator modulating the radiation beam in at least one of: amplitude and phase by preset patterns into a patterned radiation beam; and the object;
a focusing optics;
a detection crystal; said focusing optics focusing a patterned pump beam from said pump line and the probe beam from said probe line to said detection crystal; the probe beam sampling in said detection crystal different points in time of the radiation beam electric field waveform, each probe pulse spectral component or point along a spatial profile of the probe beam changing a polarization state thereof as a function of the strength of the radiation beam electric field;
a linear polarizer; said linear polarizer translating the changes in the polarization state into an intensity modulation of the probe beam;
a detector, said detector reading the intensity modulation of the probe beam in real-time; and
a computer reconstructing an image of the object from the preset patterns and corresponding readings at said detector.
2. The system of claim 1 , wherein the system comprises optics selected for spreading spectral components of the probe beam in time over a temporal window at least covering the entire duration of the radiation beam waveform; said linear polarizer translating the changes in the polarization state into intensity modulation of the probe beam spectrum and said detector is a real-time spectrometer.
3. The system of claim 1 , comprising in the probe line optics selected for nonlinear temporal dispersion and optics selected for linear temporal dispersion, said optics selected for nonlinear temporal dispersion inducing a nonlinear chirp in the probe beam, said optics selected for linear temporal dispersion spreading spectral components of a resulting chirped probe beam in time over a temporal window at least covering the entire duration of the radiation beam waveform; said linear polarizer translating the changes in the polarization state into intensity modulation of the probe beam spectrum and said detector is a real-time spectrometer.
4. The system of claim 1 , wherein the system comprises pulse front tilting optics in the probe line, said pulse front tilting optics tilting the probe pulse front in space over a temporal window at least covering the entire duration of the radiation beam waveform; said linear polarizer translating the changes in the polarization state into intensity modulation of the probe beam spatial profile and said detector is a detector array.
5. The system of claim 1 , wherein said laser source emits pulses of energies in a range between 0.1 and 100 nJ.
6. The system of claim 1 , wherein said laser source emits pulses of energies in a range between 1 μJ and 10 mJ.
7. The system of claim 1 , wherein said radiation generator generates radiation of in a frequency range between 0.1 and 230 THz.
8. The system of claim 1 , wherein said laser source emits pulses shorter than 1 picosecond.
9. The system of claim 1 , wherein said radiation generator generates pulses shorter than 1 picosecond of a frequency in a range between 0.1 and 10 THz.
10. The system of claim 1 , wherein said radiation generator generates THz broadband pulses by one of: i) optical rectification, ii) plasma generation, and iii) photoconductive antennas.
11. The system of claim 1 , wherein said radiation generator generates pulses of a frequency in a range between 10 and 230 THz.
12. The system of claim 1 , wherein said radiation generator is one of: i) an optical parametric amplifier and ii) an optical parametric oscillator, and generates pulses of a frequency in a range between 10 and 230 THz.
13. A method for imaging an object, comprising:
in a laser pump line: patterning a laser pump beam with known patterns of a radiation beam and illuminating the object with the radiation beam; yielding a patterned pump beam;
directing the patterned beam from the pump line and a laser probe beam from a laser probe line to a detection crystal;
single-shot detection of the radiation beam waveform;
correlating the single-shot detection and the known patterns.
14. The method of claim 13 , comprising:
dividing pulses emitted by a laser source into the pump beam and the probe beam;
in the pump line, generating the radiation beam and modulating the radiation beam in at least one of: amplitude and phase by the known patterns;
focusing the patterned pump beam from the pump line and the probe beam from the probe line to said detection crystal, the probe beam sampling in the detection crystal
different points in time of the radiation beam electric field waveform, each probe pulse spectral component or point along the spatial profile of the probe beam changing a polarization state thereof as a function of the strength of the radiation beam electric field;
translating the changes in the polarization state into an intensity modulation of the probe beam;
reading the intensity modulation of the probe beam in real-time; and
reconstructing an image of the object from the known patterns and corresponding readings.
15. The method of claim 13 , comprising:
in the probe line, spreading spectral components of the probe beam in time over a temporal window at least covering an entire duration of the radiation beam waveform;
said translating the changes in the polarization state into the intensity modulation of the probe beam comprising translating the changes in the polarization state into the intensity modulation of the probe beam spectrum; and
said reading the intensity modulation of the probe beam in real-time comprising detecting the intensity modulation of the probe beam spectrum.
16. The method of claim 13 , comprising:
in the probe line, tilting the probe pulse front in space over a temporal window at least covering an entire duration of the radiation beam waveform;
said translating the changes in the polarization state into the intensity modulation of the probe beam comprising translating the changes in the polarization state into the intensity modulation of the probe beam spatial profile; and
said reading the intensity modulation of the probe beam in real-time comprising detecting the intensity modulation of the probe beam profile.
17. The method of claim 13 , wherein the laser source emits pulses shorter than 1 picosecond.
18. The method of claim 13 , wherein the laser source emits pulses of energies in a range between 0.1 and 100 nJ.
19. The method of claim 13 , wherein the laser source emits pulses of energies in a range between 1 μJ and 10 mJ.
20. The method of claim 13 , wherein the radiation beam has a frequency in a range between 0.1 and 230 THz.