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thz_ctr_ramp { Low-charge, low-energy electron bunch exits an ionized gas jet in Cartesian geometry, generating coherent transition radiation (CTR) in the THz range of frequencies -- This simulation

afterB_Li.inp { High-energy electron bunch enters a quiet plasma in cylindrical geometry -- Modeling the SLAC "afterburner" concept of Tom Katsouleas. Tunneling ionization effects are ignored.. Coll

thz_ctr_ramp { Low-charge, low-energy electron bunch exits an ionized gas jet in Cartesian geometry, generating coherent transition radiation (CTR) in the THz range of frequencies -- This simulation

afterB_TI_Li.inp { High-energy electron bunch enters a quiet plasma in cylindrical geometry -- Modeling the SLAC "afterburner" concept of Tom Katsouleas. This input file includes the effects of tunn

CHANGES to XOOPIC XOOPIC 2.5-current -- Requires XGrafix version later than Mar. 29, 2005. o fixing routines converting particles' velocity into their energy and gamma to be correct in both relati

#Mend: Heals someone by caster's intelligence. # # if ! variableisstring param0 #Not specific target chat caster "You focus energy into mending your wounds." inc caster hp * caster intelligence

function [tfr2,OrderedSurfaces]=tfrsurf(tfr,threshold,keep,trace); % [tfr2,OrderedSurfaces]=tfrsurf(tfr,threshold,keep,trace); % extract from a time-frequency representation the biggest energy dots

function [tfr2,OrderedSurfaces]=tfrsurf(tfr,threshold,keep,trace); % [tfr2,OrderedSurfaces]=tfrsurf(tfr,threshold,keep,trace); % extract from a time-frequency representation the biggest energy dots

function l = limpz(b,a,varargin); % LIMPZ Calculate the effective length of the impulse response. % % L = LIMPZ(B,A) % L = LIMPZ(B,A,P) where P is the required ratio of energy to pass % L = LIMPZ(B,

function [margt,margf,E]=margtfr(tfr,t,f) %MARGTFR Marginals and energy of a time-frequency representation. % [MARGT,MARGF,E]=MARGTFR(TFR,T,F) calculates the time and % frequency marginals and the en