abc1st.h [code] | |
abc1stdisc.h [code] | |
acheron3dlgm.h [code] | |
all_pml.h [code] | |
aqhdBaseTypes.h [code] | |
aqhdFrequencyDB.h [code] | |
aqhdMaterials.h [code] | |
aqhdPhysicoMath.h [code] | |
aqhdReleaseInfo.h [code] | |
aqhdSubstrateDB.h [code] | |
aqhdSysParams.h [code] | |
auxiliary.h [code] | |
basefunt.h [code] | |
cases.h [code] | |
disconst.h [code] | |
dlz.h [code] | |
idiscretization.c | The code in this file assembles the local finite element matrix and inserts it into the global finite element matrices |
idiscretization.h [code] | |
iembc.h [code] | |
iinternalsrc.h [code] | |
itdi.c | This is itdi, the implicit time domain integration scheme for the solution of the electric field vector wave equation, aka curl-curl equation in 3-dimensional space and time domain |
itdi.h [code] | |
ivisuals.h [code] | |
linmaterials.h [code] | |
mat3d.h [code] | |
particleswarm.c | This is the implementation file for the particleswarm electromagnetic source, used for the self-consistent finite element time domain maxwell solver that models propagation of charged particles through accelerators |
particleswarm.h [code] | This is the header file for the particleswarm electromagnetic source, used for the self-consistent finite element time domain maxwell solver that models propagation of charged particles through accelerators |
pml_aux.h [code] | |
pml_const.h [code] | |
pml_linear.h [code] | |
problems.h [code] | |
sconfmp.c | This is sconfmp, the self-consistent finite element time domain maxwell solver for tracking charged particles through accelerator cavities |
sconfmp.h [code] | This is sconfmp, the self-consistent finite element time domain maxwell solver for tracking charged particles through accelerator cavities |
sconfmpdisc.c | The code in this file assembles the local finite element matrix and inserts it into the global finite element matrices |
sconfmpdisc.h [code] | This is sconfmp, the self-consistent finite element time domain maxwell solver for tracking charged particles through accelerator cavities |
sconfmppec.c | This is sconfmp, the self-consistent finite element time domain maxwell solver for tracking charged particles through accelerator cavities |
sconfmppec.h [code] | This is sconfmp, the self-consistent finite element time domain maxwell solver for tracking charged particles through accelerator cavities |
sibc1st.c | This is sibc1st. The numproc solves the electric field vector wave equation in 3-dimensional space which is truncated by a cavity wall of finite thickness, thereby causing ohmic loss in the cavity boundary; the surface impedance is approximated as being constant over frequency, instead of varying as determined by the skin effect |
sibc1st.h [code] | This is sibc1st. The numproc solves the electric field vector wave equation in 3-dimensional space which is truncated by a cavity wall of finite thickness, thereby causing ohmic loss in the cavity boundary; the surface impedance is approximated as being constant over frequency, istead of varying as determined by the skin effect |
sibc1stdisc.h [code] | This is sibc1st. The numproc solves the electric field vector wave equation in 3-dimensional space which is truncated by a cavity wall of finite thickness, thereby causing ohmic loss in the cavity boundary; the surface impedance is approximated as being constant over frequency, instead of varying as determined by the skin effect |
slocf.h [code] | |
tdwaveforms.h [code] | |
vtk.h [code] | |
whitney.h [code] | |