EXTREME ULTRAVIOLET AND SOFT X-RAY LASERS

Transcription

1 Chapter 7 EXTREME ULTRAVIOLET AND SOFT X-RAY LASERS Hot dense plasma lasing medium d θ λ λ Visible laser pump Ch07_00VG.ai

2 The Processes of Absorption, Spontaneous Emission, and Stimulated Emission Absorption u Spontaneous emission u Stimulated emission u Ch07_F01VG.ai

3 The Lasing Process Begins with Amplified Spontaneous Emission (ASE) Spontaneous emission Gain medium of inverted population density Amplified spontaneous emission both directions equally likely Ch07_F02VG.ai

4 Equilibrium and Non-Equilibrium Energy Distribution Equilibrium energy distribution Non-equilibrium inverted energy distribution Energy level u g Boltzmann distribution Energy level u g Population density Population density Lasing requires an inverted population density (more atoms in the upper state than in the lower state. Ch07_F03VG.ai

5 Three-level Lasing Between an Upper State u and a Lower State λ u Pump g Long lived state λ Fast radiative decay Ch07_04VG.ai

6 Radiative Decay Involves An Atom Oscillating Between Two Stationary States at the Frequency if = (E i E f ) / Oscillation amplitude Time Probability 1 0 Time Lower state Upper state Ch07_Ch01_F09VG.ai

7 EUV/SXR Lasers are High Gain With Minimal Cavity Optics Visible Light Laser Longitudinal mode selector Transverse mode selector λ vis Mirror Gain medium + flash lamp Mirror TEM OO λ λ ~ 10 6 EUV/Soft X-ray Laser λ IR λ EUV d λ EUV θ Refraction in an electron plasma with n = 1 1 n e 2 n c L λ IR pump λ λ ~ 10 4 Spatial and temporal coherence addressed in chapter 8. Ch07_F06VG.ai

8 Early Successes With Lasing in the 4-46 nm Wavelength Region Recombination lasing in rapidly cooled H-like carbon Collisionally pumped lasing in Ne-like Se Extension to shorter wavelengths with collisionally pumped Ni-like Ta, W,... Saturation of Ni-like Ag, In, Sn, Sm,... with refraction compensated plasmas More recently: Table-top lasing in the EUV with high spatial coherence and mw average power Compact lasing with f sec transient gain techniques Ch07_EarlySuccess.ai

9 Stimulated n = 3 to n = 2 Emission for a Hydrogen-Like Ion n = n = 4 n = 3 (7.1) n = 2 Binding energy n = 1 Ch07_F05VG.ai

10 Transitions in Single Electron, Hydrogen-Like Carbon Ions (Z = 6) (7.1) ω Z 2 τ τ H /Z 4 Ch07_Tb7.1.ai

11 Recombination Lasing With H-like Carbon Ions Expanding carbon plasma of length L Carbon disk target Recombination of C +6 and e cascading down excitation states (n) EUV B EUV Axial spectrum C nm (3 2) 10.6 m laser-heating pulse Magnet coils Co 2 laser: 10.6 µm, W/cm 2, 70 ns Ionization of C +5 = 490 ev Plasma: κt = ev, e/cm 3 O nm C nm Laser-heating pulse Expanding plasma B Carbon blade Carbon disk target Diagnostic window L/r ~ r ~ mm 2 Transverse spectrum O nm O nm C nm C nm Channel (pixel) Courtesy of S. Suckewer et al. (1985) Princeton University Ch07_F08_9VG.ai

12 Laser Produced Plasma for Ne-like Lasing in Selenium (Z = 34) Double-sided irradiation of a thin Se foil 2.4 TW, 2ω, 450 ps, W/cm µm 1.1 cm focal spot About 20% ions Ne-like Ionization of Fl-like Se +23 is 1036 ev (Ne-like is 2540 ev) (λ/ λ ~ 2,000; τ ~ 0.5 ns) Two time-gated spectrometers 77 High power m laser light Alignment mirror Ne-like selenium ions in a laserproduced plasma Time-resolved transmission grating spectrometer (λ/ λ ~ 200; τ ~ 20 ps) Courtesy of D. Matthews et al. (1985) Lawrence Livermore National Laboratory Ch07_F12VG.ai

13 Exponential Gain Observed With Increasing Plasma Length Relative intensity mm foil 10.1-mm foil 22.4-mm foil Integrated line intensity, J/Sr Gain in axial direction only Use of on and off-axis time gated spectrometers 3p 3s lasing at nm and nm in Ne-like Se nm nm G = 5/cm Target length, mm Wavelength, nm Courtesy of D. Matthews et al. (LLNL) Ch07_F14VG.ai

14 Population Inversion in Neon-like Selenium Simplified Energy Level Diagram for Se +24 1s 2 2s 2 2p 5 3s (J = 1) Lasing transitions nm (59.10 ev) nm (60.07 ev) 1s 2 2s 2 2p 5 3p (J = 2) Laser produced plasma conditions optimized for dominant Ne-like ionization stage Collisionally pumped to a 3p excited state Fast radiative depopulation of the lower 3s state 3p 3s lasing at nm and nm based on selective depopulation Fast radiative decay 1s 2 2s 2 2p 6 Electron collisional excitation (~1.5 kev) Courtesy of M. Rosen et al. (1985), LLNL. Ch07_F13VG.ai

15 Extension to Nickel-like Ions Permits Lasing at Shorter Wavelengths Without the Need for Higher Electron Temperature Lasing in Ni-like Ta +45 Lasing transition at nm 3d 9 4d (J = 0) nm (276 ev) 3d 9 4p (J = 1) Fast radiative decay Electron collisional excitation (~1.1 kev) Intensity cm Ta foil cm Ta foil Wavelength (nm) d 10 ground state (J = 0) Ni-like Ta (Z = 73, 28 e, +45) 1s 2 2s 2 2p 6 3s 2 3p 6 3d 10 ground state (28 e ) Courtesy of B. MacGowen et al. (1987), LLNL. Ch07_F15_16VG.ai

16 Nickel-like Lasing Across the K-edge of Neutral Carbon 4d 4p lasing W at nm Ta at nm C-K at 4.36 nm Intensity Au W Ta Yb The water window is defined by the K-absorption edges of neutral carbon and oxygen Wavelength (nm) Courtesy of B. MacGowen et al. (1987), LLNL. Ch07_F17VG.ai

17 Refractive Index of a Plasma For ω > ω p there is a real propagating wave with phase velocity (6.113a) The refractive index of the plasma is or equivalently (6.114a) (6.114b) Ch06_RefracIndxPlas.ai

18 Refraction Compensating Double-Targets Used to Achieve Saturation of Lasing at nm in Ni-like Ag Ag +60 ps Ag nm Nd laser: 1.05 µm, W/cm 2, 75 ps Target: Ag stripes, 200 µm 25 mm Plasma: 700 ev, e/cm µm, mr Prepulse allows plasma expansion, decreases transverse electron density gradients and increases plasma volume Double targets permit refraction compensation (opposite turning angles) and double the gain length. Time delay of one target irradiation enhances gain in one direction Saturated 4d 4p lasing at nm in Ni-like Ag +19 (Z = 47, 28e ) Courtesy of J. Zhang et al. (1997) Rutherford Appleton Laboratory Ch07_RefracComp.ai

19 Saturation of Nickel-like Lasing in Ag, In, Sn, and Sm Intensity (arb. units) Refraction compensating double targets Si L-edge Ni-like Ag 4d 4p nm Laser output (arb. units) Ni-like Ag nm Ni-like Sn nm G = 8/cm Ni-like In nm Ni-like Sm nm G = 8.8/cm Wavelength (nm) G = 12.5/cm G = 9.5/cm Courtesy of J. Zhang et al. (1977) Appleton Rutherford Laboratory Note: Wavelengths quoted are calculated by J. Scofield and B. MacGowan Target length (mm) Courtesy of J.Y. Lin et al. (1999) Appleton Rutherford Laboratory Ch07_F19_20VG.ai

20 High Average Power, High Spatial Coherence Table-Top Laser at nm Ar +8 3p 3s (J = 0 to 1) 12 cm EUV Discharge plasma Fast, high current pulse compresses (J B) and heats plasma 70 ev, e/cm µm D 36 cm long (1:1000) Ne-like Ar +8, 3p 3s at nm P = 3.5 mw, spatially coherent Intensity (rel. units) Al-like Ar Ne-like Ar Al-like Ar Ar +8 3p 3s (J = 0 to 1) Mg-like Ar Mg-like Ar 6 cm 3d-3p Ne-like Ar 3 cm 3d-3p Ne-like Ar Wavelength (nm) Courtesy of J. Rocca (1995), Colorado State University Ch07_F21_22VG.ai

21 Spatial Coherence of nm Laser EUV CCD array Pinhole mask Capillary discharge soft x-ray laser Normalized intensity cm capillary 27 cm capillary 36 cm capillary Courtesy of Y. Liu, UC Berkeley, and J. Rocca, Colorado State University (2001) Ch07_SpatialCoh.ai

22 Scaling to 13 nm Requires Excitation of Ni-Like Cd Ions (Cd + 20) 60 S(60.8) Wavelength (nm) Cl(52.9) Ar(46.9) Kr(33.7) Ca(38.3) Sr(26.6) Ti(32.6) Cr(28.5) Y(24.1) Zr(22) Nb(20.4) Ni-like Ne-like Fe(25.5) Mo(18.8) Pd(14.7) Ni(23.1) Ge(19.6) Ag(13.9) In(12.6) Cd(13.2) Sn(12.0) Ionic charge ScalingNeAndNiLikeLasers.ai

23 Generation of laser radiation at 13 nm requires significantly hotter and denser plasma columns 1E+23 1E+22 Electron Density (cm ) -3 1E+21 1E+20 1E+19 1E+18 1E+17 Plasma waveguides EUV lasers nm EUV lithography sources EUV lasers nm 1E Electron Temperature (ev)

24 Pumping configurations for collisional EUV lasers in laser-created plasmas: Grazing incidence increases energy deposition efficiency* Two pulse sequence at normal incidence 120 ps 8 ps N Critical Pump Beam Ne Absorption Region Gain Region Grazing incidence Absorption Region 8 ps 120 ps! = N N e c Ne Pump Beam * R. Keenan, et al. Phys. Rev. Lett, 94, (2005). B.M. Luther et al. Optics Lett, 30, 165 (2005) Courtesy of J. Rocca Colo. State U.

25 5-10 Hz Pump laser: 1 J Short Pulse Table-top Ti: Sapphire System Courtesy of J. Rocca, Colo. State U.

26 Configuration for 30 µm wide short pulse line focus at 14 to 26 degrees grazing incidence Line Focus Pre-pulse: Short-pulse: 30µm FWHM, 30µm FWHM, Courtesy of J. Rocca, Colo. State U.

27 Simulation predicts high gain at 18.9 nm in Ni-like Mo, g ~100 cm -1 (Mark Berrill, CSU) Pre-pulse: 330 mj, 120 ps Heating pulse: 800 mj, 8 ps heating pulse Courtesy of J. Rocca, Colo. State U.

28 Saturated 18.9 nm Ni-like Molybdenum Laser Long pulse: 340 mj - Short pulse: 1 J 4 mm 3 mm 2.5 mm g o = 65 cm -1 gxl= mm 1.5 mm wavelength (nm) Fit with the expression from Tallents et. al. 8 th Int. Conf. XRL, AIP Vol. 641, Iav GL + 2 = g0l I I av = I 0 s 3/2 [ exp( GL)! 1] [ GL exp( GL) ] 1/2 Courtesy of J. Rocca, Colo. State U.

29 Lasing observed at wavelengths as short as 10.9 nm Gain saturated operation demonstrated Courtesy of J. Rocca Colo. State U.

30 Saturated laser operation at 13.9 nm in Nickel-like Ag 1 J short (8 ps) pulse excitation g 0 =67 cm -1 ; gxl= nj/shot Courtesy of J. Rocca, Colo. State U.

31 Gain-saturated Ni-like 13.2 nm Ni-like Cd laser 1 J short pulse 23 degrees grazing incidence angle CCD channel (x10-2 ) Intensity (a. u.) wavelength (nm) Intensity (arb. Units) g 0 =69 cm -1 G L=17.6 Length (mm) Courtesy of J. Rocca, Colo. State U.

32 A Ni-like Cd at 13.2 nm provides a closer laser wavelength match to Mo/Si lithography mirrors At the wavelength of the Ni-like Cd laser the reflectivity of Mo-Si mirrors centered at λ=13.5 nm is ~ 55% Courtesy of J. Rocca, Colo. State U.

33 The new compact EUV lasers are enabling application testbeds Example: 13.9 nm Table-top EUV microscope with resolution better than 50 nm From 13.9 nm laser Objective zone plate Test pattern CCD Grad. Student Fernando Brizuela Courtesy of J. Rocca, Colo. State U.