Kinetic energy and mass distributions of ablated species formed during pulsed laser deposition

[1]  Y. Nishikawa,et al.  Ion Energy Distribution of KrF Laser Ablation , 1992 .

[2]  J. Horwitz,et al.  Excimer laser ablation of a YBa2Cu3O7−δ target in a vacuum: characterization of the mass and energy of ejected material , 1991 .

[3]  I. Raaijmakers,et al.  Energy distribution of negative O− and OH− ions emitted from YBaCuO and iron garnet targets by dc and rf magnetron sputtering , 1991 .

[4]  H. Helvajian,et al.  Laser photodecomposition of sintered YBa2Cu3O6+x: Ejected species population distributions and initial kinetic energies for the laser ablation wavelengths 351, 248, and 193 nm , 1991 .

[5]  P. H. Key,et al.  Dynamics of excimer laser ablation of superconductors in an oxygen environment , 1990 .

[6]  R. Kelly.  On the dual role of the Knudsen layer and unsteady, adiabatic expansion in pulse sputtering phenomena , 1990 .

[7]  K. Saenger.  Time‐resolved optical emission during laser ablation of Cu, CuO, and high‐Tc superconductors: Bi1.7Sr1.3Ca2Cu3Ox and Y1Ba1.7Cu2.7Oy , 1989 .

[8]  H. Frankena,et al.  Instrumentation for the study of the kinetic energy distribution and mass composition of particles produced by pulsed laser evaporation of solid materials , 1989 .

[9]  R. D. Greenough,et al.  Spectroscopic and ion probe measurements of KrF laser ablated Y‐Ba‐Cu‐O bulk samples , 1988 .

[10]  Orlando Auciello,et al.  Spectroscopic analysis of electronically excited species in XeCl excimer laser‐induced plasmas from the ablated high‐temperature superconductor YBa2Cu3O7 , 1988 .

[11]  Jay S. Pearlman,et al.  Faraday cups for laser plasmas , 1977 .

[12]  T. S. Green.  Space charge effects in plasma particle analyzers , 1970 .

[13]  William I. Linlor,et al.  ION ENERGIES PRODUCED BY LASER GIANT PULSE , 1963 .