Photon induced near field electron microscope and biological imaging system
A method of obtaining PINEM images includes providing femtosecond optical pulse, generating electron pulses, and directing the electron pulses towards a sample. The method also includes overlapping the femtosecond optical pulses and the electron pulses spatially and temporally at the sample and transferring energy from the femtosecond optical pulses to the electron pulses. The method further includes detecting electron pulses having an energy greater than a zero loss value, providing imaging in space and time.
1. A system for imaging a sample, the system comprising:
a chamber;
a stage assembly disposed in the chamber and adapted to receive the sample to be imaged;
a first laser, wherein the first laser is operable to emit an optical pulse along an optical path;
a second laser coupled to a cathode operable to emit an electron pulse having a predetermined energy;
a third laser coupled to the chamber, wherein the third laser is operable to emit clocking pulses;
a lens assembly operable to direct the electron pulse to impinge on the sample disposed on the stage assembly; and
a detector operable to capture the electron pulse passing through the sample, wherein the detector is a spectral detector, and wherein the electron pulse passing through the sample has a different energy than the predetermined energy.
2. The system of claim 1 wherein the chamber includes one or more optical ports.
3. The system of claim 1 wherein the chamber comprises a vacuum chamber.
4. The system of claim 1 further comprising a first frequency conversion stage disposed along the optical path and operable to produce a first frequency converted optical pulse.
5. The system of claim 4 wherein the cathode is optically coupled to the first frequency converted optical pulse.
6. The system of claim 1 wherein the lens assembly is an electron lens assembly.
7. The system of claim 1 wherein the electron pulse passing through the sample has an energy different than a predetermined energy.
8. A system comprising:
a chamber;
a stage assembly disposed in the chamber and adapted to receive a sample to be imaged;
a first laser, wherein the first laser is operable to emit an optical pulse along an optical path;
a second laser coupled to a cathode operable to emit an electron pulse having a predetermined energy;
a third laser coupled to the chamber, wherein the third laser is operable to emit clocking pulses;
a detector operable to capture the electron pulse passing through the sample, wherein the detector is a spectral detector, and wherein the electron pulse passing through the sample has a different energy than the predetermined energy;
a processor coupled to the detector; and
an output device coupled to the processor.
9. The system of claim 8 wherein the chamber including one or more optical ports.
10. The system of claim 8 further comprising:
a frequency conversion stage disposed along the optical path and operable to produce a frequency converted optical pulse.
11. The system of claim 10 wherein the cathode is optically coupled to the frequency converted optical pulse.
12. The system of claim 9 wherein the first laser is a femtosecond laser source.
13. The system of claim 8 further comprising a lens operable to direct the electron pulse to impinge on the sample disposed on the stage assembly.
14. The system of claim 8 wherein the processor comprises an energy filter operable to filter electron pulses having energies equal to the predetermined energy plus a number of quanta of a photon energy.
15. The system of claim 1 wherein the system is operable to obtain PINEM (photon-induced near-field electron microscopy) images.
16. The system of claim 8 wherein the system is operable to obtain PINEM (photon-induced near-field electron microscopy) images.
17. The system of claim 1 wherein the third laser is a clocking pulse laser and wherein the clocking pulse laser is operable to emit the clocking pulses to initiate a change in the sample.
18. The system of claim 8 wherein the third laser is a clocking pulse laser and wherein the clocking pulse laser is operable to emit the clocking pulses to initiate a change in the sample.
19. The system of claim 1 wherein the different energy is higher than the predetermined energy.
20. The system of claim 8 wherein the different energy is higher than the predetermined energy.
21. The system of claim 1 wherein a delay of the clocking pulses by the third laser enables measurements of the electron pulse and the optical pulse as the electron pulse and the optical pulse overlap temporally and spatially.
22. The system of claim 8 wherein a delay of the clocking pulses by the third laser enables measurements of the electron pulse and the optical pulse as the electron pulse and the optical pulse overlap temporally and spatially.