Optical Diagnostics and Kinetics of Discharge-Initiated Oxygen-Iodine Energy Transfer

[1]  J. Tellinghuisen.  Transition strengths in the visible–infrared absorption spectrum of I2 , 1982 .

[2]  J. Tellinghuisen.  Resolution of the visible‐infrared absorption spectrum of I2 into three contributing transitions , 1973 .

[3]  Richard M. Badger,et al.  Absolute Intensities of the Discrete and Continuous Absorption Bands of Oxygen Gas at 1.26 and 1.065 μ and the Radiative Lifetime of the 1Δg State of Oxygen , 1965 .

[4]  K. Tachibana,et al.  Excitation of the O2(a 1Δg) state by low energy electrons , 1981 .

[5]  W. Rawlins,et al.  Dynamics of vibrationally excited ozone formed by three‐body recombination. I. Spectroscopy , 1987 .

[6]  B. McCarroll.  An improved microwave discharge cavity for 2450 MHz (Notes) , 1970 .

[7]  L. G. Piper.  State‐to‐state N2(A 3Σ+u) energy‐pooling reactions. I. The formation of N2(C 3Πu) and the Herman infrared system , 1988 .

[8]  L. G. Piper.  The rate coefficient for quenching N(2D) by O(3P) , 1989 .

[9]  G. T. Fraser,et al.  Rotational Line Strengths and Self-Pressure-Broadening Coefficients for the 1.27-microm, a (1)D(g)-X (3)?(g)(-), v = 0-0 Band of O(2). , 1998, Applied optics.

[10]  L F Rubin,et al.  Measurement of the Raman cross section of O(2)(a(1)D(g)). , 1997, Optics letters.

[11]  Steven J. Davis,et al.  Historical perspective of COIL diagnostics , 2002, SPIE LASE.

[12]  William J. Kessler,et al.  Progress in the development of sensors for COIL devices , 2000, LASE.

[13]  S. Lawton,et al.  Excitation of the b 1Σ+g state of O2 by low energy electrons , 1978 .

[14]  William J. Kessler,et al.  Collisional broadening of absorption lines in water vapor and atomic iodine relevant to COIL diagnostics , 1999, Photonics West.

[15]  J. T. Verdeyen,et al.  Recent work on the development of an electric-discharge oxygen-iodine laser , 2003, International Symposium on High Power Laser Systems and Applications.

[16]  W. T. Rawlins,et al.  Dynamics of vibrationally excited ozone formed by three-body recombination. II. Kinetics and mechanism , 1987 .

[17]  L F Rubin,et al.  Direct Measurement of O(2)(a(1)D) and O(2)(X(3)?) in Chemical Oxygen-Iodine Lasers with use of Spontaneous Raman Imaging. , 1998, Applied optics.

[18]  David A. Newnham,et al.  Integrated absorption intensity and Einstein coefficients for the O2 a1Δg-X3Σg- (0,0) transition: a comparison of cavity ringdown and high resolution Fourier transform spectroscopy with a long-path absorption cell , 1999 .

[19]  Martin G. Mlynczak,et al.  On the utility of the molecular oxygen dayglow emissions as proxies for middle atmospheric ozone , 1995 .

[20]  R. J. Richardson,et al.  The electron spin resonance spectrum of the 2P1/2 state of atomic iodine , 1981 .

[21]  A. V. Phelps,et al.  MOMENTUM TRANSFER CROSS SECTIONS FOR SLOW ELECTRONS IN HE, AR, KR, AND XE FROM TRANSPORT COEFFICIENTS, , 1964 .

[22]  L. G. Piper,et al.  Rate constants for deactivation of N2(A 3Σ+u, v′ = 0,1) by O , 1981 .

[23]  L. G. Piper,et al.  O-Atom Yields from Microwave Discharges in N2O/Ar Mixtures. , 1986 .