Multipulse-induced spectroscopy method and device based on femtosecond plasma grating
A multipulse-induced spectroscopy method based on a femtosecond plasma grating includes: pre-exciting a sample on a stage by providing a femtosecond pulse to form the femtosecond plasma grating; providing a post-pulse on the sample at an angle to excite the sample to generate a plasma, wherein the post-pulse comprises one or more femtosecond pulses, there is a time interval between the femtosecond pulse and the post-pulse, and the time interval is less than a lifetime of the femtosecond plasma grating; and receiving and analyzing a fluorescence emitted from the plasma to determine element information of the sample.
1. A multipulse-induced spectroscopy method based on a femtosecond plasma grating, comprising:
pre-exciting a sample on a stage by providing a femtosecond pulse to form the femtosecond plasma grating;
providing a post-pulse on the sample at an angle to excite the sample to generate a plasma, wherein the post-pulse comprises one or more femtosecond pulses, there is a time interval between the femtosecond pulse and the post-pulse, and the time interval is less than a lifetime of the femtosecond plasma grating; and
receiving and analyzing a fluorescence emitted from the plasma to determine element information of the sample;
wherein the method further comprises:
splitting the femtosecond pulse into three sub-pulses; and
adjusting an optical path of each of the three sub-pulses in such a way that a first pulse and a third pulse of the three sub-pulses have an optical path with a first length and arrive at the intersection in space simultaneously to form the femtosecond plasma grating, and a second pulse of the three sub-pulses has an optical path with a second length being different from the first length and arrives at the intersection in space after a preset time interval;
wherein splitting the femtosecond pulse into three sub-pulses comprises:
splitting the femtosecond pulse into the first pulse and a primary reflection light; and
splitting the primary reflection light into the second pulse and the third pulse.
2. The multipulse-induced spectroscopy method according to claim 1 , wherein the femtosecond plasma grating has a one-dimensional or multi-dimensional grating structure.
3. The multipulse-induced spectroscopy method according to claim 1 , wherein the post-pulse is a pulse combination selected from a picosecond pulse combination and a femtosecond pulse combination, and there is a time interval between two adjacent pulses in the pulse combination.
4. The multipulse-induced spectroscopy method according to claim 1 , wherein the sample is excited in a two-color field formed by coupling a double-frequency light of the post-pulse and the femtosecond plasma grating.
5. The multipulse-induced spectroscopy method according to claim 1 , wherein the angle is a first-order or high-order Bragg angle.
6. The multipulse-induced spectroscopy method according to claim 1 , wherein the sample is excited in a gas atmosphere of argon or neon, and the gas atmosphere has a gas flow rate of 2 to 10 L/min.
7. The multipulse-induced spectroscopy method according to claim 1 , further comprising:
moving the stage to allow different parts of the sample to be excited.
8. The multipulse-induced spectroscopy method according to claim 1 , wherein the femtosecond pulse has a wavelength of 800 nm, a repetition frequency of 1000 Hz, and a pulse width of 50 fs.
9. A multipulse-induced spectroscopy device based on a femtosecond plasma grating, comprising:
a femtosecond laser configured to generate a femtosecond laser pulse;
a beam splitting component configured to split the femtosecond laser pulse into three sub-pulses;
a focusing component configured to focus the three sub-pulses to allow focused sub-pulses to be overlapped at an intersection in space;
a time domain synchronization component configured to adjust an optical path of each of the three sub-pulses in such a way that a first pulse and a third pulse of the three sub-pulses have an optical path with a first length and arrive at the intersection in space simultaneously to form the femtosecond plasma grating, and a second pulse of the three sub-pulses has an optical path with a second length being different from the first length and arrives at the intersection in space after a preset time interval;
a stage for supporting a sample; and
a spectrum collection component configured to collect a spectrum signal emitted by sample excitation,
wherein the beam splitting component comprises:
a first beam splitter configured to split the femtosecond laser pulse into the first pulse and a primary reflection light; and
a second beam splitter configured to split the primary reflection light into the second pulse and the third pulse.
10. The multipulse-induced spectroscopy device according to claim 9 , further comprising:
a polarization adjustment component configured to adjust a polarization direction of each sub-pulse.
11. The multipulse-induced spectroscopy device according to claim 9 , wherein the stage is an electronically controlled displacement stage composed of a stepper motor and a stage body, and is configured to move the sample to allow different regions of the sample to be excited.
12. The multipulse-induced spectroscopy device according to claim 9 , wherein the time domain synchronization component comprises two time delay lines each provided with a stepper motor equipped with at least two reflectors.
13. The multipulse-induced spectroscopy device according to claim 9 , wherein the spectrum collection component comprises:
a lens configured to converge fluorescence emitted from the sample;
an optical fiber probe configured to collect a fluorescence signal; and
a spectrometer configured to receive and analyze the fluorescence signal transmitted from the optical fiber probe.
14. The multipulse-induced spectroscopy device according to claim 13 , wherein the spectrometer is an Echelle grating spectrometer coupled with an intensified charge-coupled device and applied in an integrate-on-chip mode.