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Kinetic Investigation of Collision Induced Excitation Transfer in Kr*(4p 5 5p 1 ) + Kr and Kr*(4p 5 5p 1 ) + He Mixtures Md. Humayun Kabir and Michael.

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Presentation on theme: "Kinetic Investigation of Collision Induced Excitation Transfer in Kr*(4p 5 5p 1 ) + Kr and Kr*(4p 5 5p 1 ) + He Mixtures Md. Humayun Kabir and Michael."— Presentation transcript:

1 Kinetic Investigation of Collision Induced Excitation Transfer in Kr*(4p 5 5p 1 ) + Kr and Kr*(4p 5 5p 1 ) + He Mixtures Md. Humayun Kabir and Michael C. Heaven Department of Chemistry Emory University Atlanta, GA 30322 International Symposium on Molecular Spectroscopy 66 th Meeting: June 20 - 24, 2011

2 Motivation  The development of high-power lasers using diode pumped solid-state and fiber lasers are currently limited by material damage and heat dissipation problem.  Optically pumped alkali (Cs, Rb, and K) vapor lasers have recently been demonstrated with high output power and high efficiency. Krupke et al. Opt. Lett. 23 (2003)

3 Atomic Rare Gas Lasers are attractive: Excellent beam quality at high powers Potentially scaleable to high powers Possibility of operating in the IR range Concept of Optically Pumped Atomic Gas Lasers atomic gas Diode Pump, p  atom

4 Objectives and Goal  Detailed knowledge of collision-induced energy transfer kinetics of Kr + Kr and Kr + He: quantum state populations for laser modeling.  To obtain both accurate and comprehensive state-to-state collisional rate constants for the Kr + Kr and Kr + He collisional systems.  Our interest in using elements other than the alkali metals is to expand the range of pump and lasing wavelength.  Optical pumping scheme can be used to pump the rare gas atoms that are in the metastable electronic states. Siegman et al. J. Appl. Phys. 49 (1978)

5 Stepwise Electron-Photon Excitation-Scheme 3P13P1 3P03P0 3P23P2 1P11P1 4p 5 5s 4p 5 5p 3 D 3 (2p 9 ) 3 S 1 (2p 10 ) 1S01S0 e - impact excitation 1 S 0 (2p 1 ) Coll. transfer 3 D 2 (2p 8 ) 1 D 2 (2p 6 ) 3 D 1 (2p 7 ) 11.5 10.0 E/eV Radiative decay Quenching to other multiplet  E = 13 cm -1

6 Experimental Experimental conditions: p(Kr) =0.5-1 Torr, p(He) = 2-20 Torr Discharge: 500-700 V; R=1 k  ; current = 150-300 mA Discharge Period: 350  s; laser fired within the discharge. pump R Nd:YAG LaserDye Laser HV Rg PMT Digital ‘Scope Monochromator Delay Generator Computer

7 Emission Spectra of Kr Plasma

8 Time Dependent Fluorescence Decay of 2p 6 level

9 Decay Rates vs Discharge Voltage Radiation Trapping: when a resonance photon emitted from an excited atom is absorbed and re-emitted from the other atoms cause a dramatic lengthening of the measured lifetimes of resonance transitions.

10 De-excitation of Metastable States Kr m + e -  Kr * (upper excited levels) + e - Kr m + Kr  Kr* + Kr Kr m + e -  Kr ** (1s 2, 1s 4 levels) + e - Kr m + e -  Kr + + 2e - Excitation by electron collision on upper excited levels Quenching by two-body collision: Penning Ionization: Quenching by electron collision to radiative levels Ionization by electron collision Kr m + Kr m  Kr + + Kr + e -

11 Total Collisional Deactivation Rate Constants

12 Comparison to Deactivation in other Rare Gases

13 Fluorescence Spectra following 2p 6 Excitation

14 Population Evolution following Excitation of 2p 6 level

15 State-to-State Rate Constants

16 S IMULATION Master Equation: models the evolution of individual level populations The rate equations for the collisional energy transfer process in the Kr(4p 5 5p) manifold Excitation of the initial state by the laser pulse Radiative decay loss

17 Comparison between expt. & calc. Spectra

18 Is Optically Pumped Laser Scheme Favorable? 3P13P1 3P03P0 3P23P2 1P11P1 4p 5 5s 3D33D3 3S13S1 3D23D2 11.5 10.0 E/eV  E = 13 cm -1 Pumped State Upper Laser Level Optical Pumping Lasing k( 3 S 1 ) = 6 x 10 -12 cm 3 s -1 (upper bound) k 10  9 = 5 x 10 -12 cm 3 s -1

19 Conclusion  Time-resolved LIF measurements were used to examine Kr(4p 5 5p) + Kr and Kr(4p 5 5p) + He collisional energy transfer within the Kr(4p 5 5p) manifold for the first time.  Largest total and state-to-state rate constants were observed for the for 2p 8 and 2p 9 levels.  For the Kr(4p 5 5p) + He collisional system the upper bound rate constant for lowest 2p 10 level is found to be 6 x 10 -12 cm 3 s -1.  Measured rate constants for the Kr(4p 5 5p) + Kr and Kr(4p 5 5p) + He collisions are found to be fairly similar except the lowest 2p 10 level.


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