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Extreme Ultraviolet Radiation Spectrometer Design and Optimization

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Presentation on theme: "Extreme Ultraviolet Radiation Spectrometer Design and Optimization"— Presentation transcript:

1 Extreme Ultraviolet Radiation Spectrometer Design and Optimization
Shaun Pacheco Mentors: Dr. Guillaume Laurent & Wei Cao

2 Research Project Goal 1: Improve the Resolution
Goal 2: Calibrate the Spectrometer to find wavelengths not intensity profile Summarize talk here.

3 Diagram of Apparatus COLTRIMS Interferometer To XUV Spectrometer
GC DM 0.5m FM M1 M4 M2 BS DS RM AF TM High-Order Harmonic COLTRIMS Gas Jet Magnetic Coils Spectrometer MCP PSD PSD To XUV Spectrometer Interferometer M1~M4: Plane mirror BS: Beam splitter RM: Recombination mirror MCP: Microchannel Plate FM: Focusing mirror GS: Gas cell DS: Delay stage PSD: Positon Sensitive Detector DM: Diverging mirror AF: Al filter TM: Toroidal Mirror

4 Diagram of Apparatus Diffraction Grating Spherical Mirror
Minus first and second order diffraction shown in the image Phosphor Plate MCP

5 High Harmonic Generation
Where n is an odd integer, ω0 is the fundamental laser frequency, "High-order Harmonic Generation." Swineburne4 Aug < >.

6 Energies Allowed in Experiment
Transmission Argon Highest Order cut-off determined by E = 3.2Up + Ip Ip is the ionization potential of the gas Up is the mean kinetic energy of the electron Highest energy seen is 51eV Aluminum Foil Citation needed Photon Energy (eV) Aluminum Foil 200 nm thickness Argon mTorr for 3 cm followed by 5 mTorr for 1 m Tong. High-Order Harmonic Generation. < Gullikson, Eric. "X-Ray Interactions With Matter." Lawrence Berkeley National Laboratory. N.p., n.d. Web. 4 Aug <henke.lbl.gov/optical_constants/>

7 Goal 1: Improving the Resolution
Phosphor Plate New Placement 100s of nanonmeter size hole Old placement "Microchannel Plate Principles of Operation." HRC. Web. 4 Aug <hea- >.

8 Goal 1: Improving the Resolution
Microchannel Plate 4 mm Phosphor plate Old Gap 10 mm 1 kV per mm otherwise u’ll get a spark Phosphor plate was moved from 10 mm away to 4 mm

9 Goal 1: Resolution improved
Show photoelectron spectrum Theoretical limit New Resolution Old Resolution

10 Goal 2: Calibrating the Spectrum
Find distance of each spectral line from zero order Integrate across the spectral lines to get intensities d is the slit spacing m is the diffraction order θi is the incident angle θd is the diffracted angle Supplementary slide how determined thetai and b

11 Calibrated Spectrum Black Curve is the photoelectron spectrum
Blue Curve is the spectrum from the XUV spectrometer Energy resolution is comparable to photoelectron spectrum Count (arb. Units) Photoelectron Energy (eV)

12 Results and Discussion
Blue Shift Can be Observed Blue Curve – Low Intensity, no blue shift Red Curve – Medium Intensity, blue shift Yellow Curve – High Intensity, blue shift Calibrate positions of peak, not intensity Harmonics

13 Conclusion XUV spectrum is now comparable to photoelectron spectrum
Spectrometer good enough to observe small change in the harmonic wavelength Improvements: Calibrate the intensity profile of XUV spectrum

14 Work Cited "High-order Harmonic Generation." Swineburne4 Aug < > "Microchannel Plate Principles of Operation." HRC. 4 Aug <hea- >. Gullikson, Eric. "X-Ray Interactions With Matter." Lawrence Berkeley National Laboratory. Web. 4 Aug <henke.lbl.gov/optical_constants> Tong. High-Order Harmonic Generation. <

15 Questions?


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