Angle-Action Estimation by Locally Fitting Stackel Potentials: Difference between revisions
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given in the first six columns of the output file. For details of the other columns see <code>src/xv2aa.cpp</code>. | given in the first six columns of the output file. For details of the other columns see <code>src/xv2aa.cpp</code>. | ||
The required accuracy level may be specified as a third optional command line argument. Users may find that when trying to estimate actions for more extreme orbits the default settings are not adequate. Details of what the accuracy level option alters are given in <code>src/xv2aa.cpp</code> and <code>doc/README.txt</code>. | |||
==Testing== | ==Testing== | ||
There is a test file (<code>MNJR0.001Jz0.001Lz1.0.txt</code>) from which the file <code>TEST_OUT.txt</code> | There is a test file (<code>MNJR0.001Jz0.001Lz1.0.txt</code>) from which the file <code>TEST_OUT.txt</code> |
Latest revision as of 16:50, 6 September 2012
written in C++ by Jason Sanders (jason.sanders@physics.ox.ac.uk).
Function
Given a list of 6D phase-space points this code estimates the corresponding actions and angles in a given general axisymmetric potential. For each phase-space point the code
- Integrates the orbit in the true potential to find the region the orbit probes,
- fits a Stäckel potential to this region,
- estimates the angles and actions in the true potential as those calculated in the fit potential.
For more information see the associated paper or the pdf included in the download
(doc/AnglesActionsInAxisymmetricPotential-JasonSanders.pdf
).
Download
All the relevant files are included in aalfs.tar.gz.
Compiling
The code should simply compile with the makefile in the download. However, you may have to change the compiler used in the makefile.
Use
The code compiles to one executable xv2aa
. This executable takes two command-line arguments -
the first is a list of input 6D phase-space points and the second specifies
an output file. The list of actions and angles is
given in the first six columns of the output file. For details of the other columns see src/xv2aa.cpp
.
The required accuracy level may be specified as a third optional command line argument. Users may find that when trying to estimate actions for more extreme orbits the default settings are not adequate. Details of what the accuracy level option alters are given in src/xv2aa.cpp
and doc/README.txt
.
Testing
There is a test file (MNJR0.001Jz0.001Lz1.0.txt
) from which the file TEST_OUT.txt
should be reproduced by the file OUTPUT.txt
with the command:
./xv2aa MNJR0.001Jz0.001Lz1.0.txt OUTPUT.txt
which takes approx. 2.0s on 2.5GHz Intel Core i5 and results in errors in the actions of 0.1%.
Referencing
If you use this code please reference the paper for which it was developed: arXiv or [ADSReference].
Other
Potentials
This distributed version of the code uses a simple potential (Miyamoto-Nagai) as a test potential
(defined in PotMN.cpp
). The user will probably want to specify their own potential which
they can do by altering the functions in this file. The user must specify the potential and its gradients
as a function of the polar coordinates .
The code is designed to work with a realistic Galactic potential such as those
defined by Dehnen & Binney 1998 or McMillan 2011. To use these potentials you need to use Walter Dehnen's GalPot
code which is available from Walter.
Double Integration
The code involves one double integration. The implementation here is a simple double Gauss Legendre
quadrature (DoubleGaussLegendreQuad
) but for a better routine one can use the cubature
library.
The relevant code to alter is in fitpot.cpp
.