DetResponse.h

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/*
*  Copyright (C) 2007 David Chin, Jolien Creighton, Kipp Cannon, Teviet Creighton
*  Copyright (C) 2012 Matthew Pitkin
*
*  This program is free software; you can redistribute it and/or modify
*  it under the terms of the GNU General Public License as published by
*  the Free Software Foundation; either version 2 of the License, or
*  (at your option) any later version.
*
*  This program is distributed in the hope that it will be useful,
*  but WITHOUT ANY WARRANTY; without even the implied warranty of
*  MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
*  GNU General Public License for more details.
*
*  You should have received a copy of the GNU General Public License
*  along with with program; see the file COPYING. If not, write to the
*  Free Software Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston,
*  MA  02110-1301  USA
*/
 
#ifndef _DETRESPONSE_H
#define _DETRESPONSE_H
 
#include <lal/LALStdlib.h>
#include <lal/LALStdio.h>
#include <lal/LALConstants.h>
#include <lal/DetectorSite.h>
#include <lal/SkyCoordinates.h>
#include <lal/Date.h>
 
#ifdef __cplusplus
extern "C"
{
#endif
 
/**
 * \defgroup DetResponse_h Header DetResponse.h
 * \ingroup lal_tools
 * \author David Chin <dwchin@umich.edu>, Kipp Cannon <kipp@gravity.phys.uwm.edu>
 *
 * \brief Provides routines to compute gravitational wave detector response to
 * polarized planar gravitational wave originating from a given source,
 * detected at a given time.
 *
 * ### Synopsis ###
 *
 * \code
 * #include <lal/DetResponse.h>
 * \endcode
 *
 * ### Description ###
 *
 * These routines compute the antenna beam pattern for all supported detector
 * types.  <tt>XLALComputeDetAMResponse()</tt> computes the response at one
 * instance in time, and <tt>XLALComputeDetAMResponseSeries()</tt> computes a
 * vector of response for some length of time.
 *
 * ### Algorithm ###
 *
 * This code is a translation of the algorithm in the Maple worksheet by
 * Anderson, <em>et al.</em> \cite ABCCRW_2001 .  We compute the \f$h\f$-tensors for
 * \f$+\f$- and \f$\times\f$-polarized in the Earth-fixed frame, and then contract
 * them (take the scalar product) with the detector response tensors as
 * described in the \ref LALDetectors_h section of the \c tools package.
 *
 * \ref LALDetectors_h provides predefined
 * \c LALDetector structures representing most current detectors,
 * including LIGO (Hanford and Livingston), and GEO.
 *
 * ### Notes ###
 *
 * For examples of usage, please see the test programs in the \c test directory.
 *
 */
/** @{ */
 
/** \name Error Codes */
/** @{ */
#define DETRESPONSEH_ENULLINPUT  1              /**< Input is NULL */
#define DETRESPONSEH_ENULLOUTPUT 2              /**< Output is NULL */
#define DETRESPONSEH_ESRCNOTEQUATORIAL 3        /**< Source coordinates not in Equatorial system */
/** @} */
 
/** \cond DONT_DOXYGEN */
#define DETRESPONSEH_MSGENULLINPUT "Input is NULL"
#define DETRESPONSEH_MSGENULLOUTPUT "Output is NULL"
#define DETRESPONSEH_MSGESRCNOTEQUATORIAL "Source coordinates not in Equatorial system"
/** \endcond */
 
 
/**
 * This structure contains gravitational wave source position (in Equatorial
 * coördinates), and orientation angle.
 * The orientation is measured counter-clockwise with respect to the "line of ascending nodes",
 * i.e. counter-clockwise with respect to a line perpendicular to the
 * source's meridian and extending westwards.  For a source in the Northern
 * celestial hemisphere, and an observer in the Northern hemisphere standing
 * such that they are facing South, this angle is measured counter-clockwise
 * from a 3 o'clock position (pointing West) at the source.  The polarization
 * convention is chosen such that if the source orientation were zero, the
 * source would be a pure \f$+\f$-polarized source.
 */
typedef struct
tagLALSource
{
  CHAR         name[LALNameLength];  /**< name of source, eg catalog number */
  SkyPosition  equatorialCoords;     /**< equatorial coordinates of source, in decimal RADIANS */
  REAL8        orientation;          /**< Orientation angle (\f$\psi\f$) of source:
                                      * counter-clockwise angle \f$x\f$-axis makes with a line perpendicular to
                                      * meridian of source in Westward direction (i.e. North of West),
                                      * in decimal radians.
                                      */
}
LALSource;
 
/**
 * This structure aggregates a pointer to a \c LALDetector and a
 * \c LALSource.  Its sole function is to allow the user to pass
 * detector and source parameters to the functions
 * LALComputeDetAMResponse() and
 * LALComputeDetAMResponseSeries().
 */
#ifdef SWIG /* SWIG interface directives */
SWIGLAL(IMMUTABLE_MEMBERS(tagLALDetAndSource, pDetector));
#endif /* SWIG */
typedef struct
tagLALDetAndSource
{
  const LALDetector  *pDetector;/**< Pointer to \c LALDetector object containing information about the detector */
  LALSource    *pSource;        /**< Pointer to \c LALSource object containing information about the source */
}
LALDetAndSource;
 
/**
 * This structure encapsulates the detector AM (beam pattern) coefficients for
 * one source at one instance in time.
 */
typedef struct
tagLALDetAMResponse
{
  REAL4 plus;   /**< Detector response to \f$+\f$-polarized gravitational radiation  */
  REAL4 cross;  /**< Detector response to \f$\times\f$-polarized gravitational radiation */
  REAL4 scalar; /**< Detector response to scalar gravitational radiation (NB: ignored at present -- scalar response computation not yet implemented) */
}
LALDetAMResponse;
 
/**
 * This structure aggregates together three \c REAL4TimeSeries objects containing
 * time series of detector AM response.
 */
typedef struct
tagLALDetAMResponseSeries
{
  REAL4TimeSeries *pPlus;       /**< timeseries of detector response to \f$+\f$-polarized gravitational radiation */
  REAL4TimeSeries *pCross;      /**< timeseries of detector response to \f$\times\f$-polarized gravitational radiation */
  REAL4TimeSeries *pScalar;     /**< timeseries of detector response to scalar gravitational radiation (NB: not yet implemented.) */
}
LALDetAMResponseSeries;
 
 
/**
 * This structure encapsulates time and sampling information for computing a
 * \c LALDetAMResponseSeries. Its fields correspond to some fields of the
 * TimeSeries structures for easy conversion.
 */
typedef struct
tagLALTimeIntervalAndNSample
{
  LIGOTimeGPS     epoch;        /**< The start time \f$t_0\f$ of the time series */
  REAL8           deltaT;       /**< The sampling interval \f$\Delta t\f$, in seconds */
  UINT4           nSample;      /**< The total number of samples to be computed */
}
LALTimeIntervalAndNSample;
 
/*
 * Function prototypes
 */
 
void
LALComputeDetAMResponse( LALStatus             *status,
                         LALDetAMResponse      *pResponse,
                         const LALDetAndSource *pDetAndSrc,
                         const LIGOTimeGPS     *gps);
 
void XLALComputeDetAMResponse(
        double *fplus,
        double *fcross,
        const REAL4 D[3][3],
        const double ra,
        const double dec,
        const double psi,
        const double gmst
);
 
 
void XLALComputeDetAMResponseExtraModes(
  double *fplus,
  double *fcross,
  double *fb,
  double *fl,
  double *fx,
  double *fy,
  const REAL4 D[3][3],
  const double ra,
  const double dec,
  const double psi,
  const double gmst
);
 
 
COMPLEX16 XLALComputeDetArmTransferFunction(
        double beta,
        double mu
);
 
 
void XLALComputeDetAMResponseParts(
        double *armlen,
        double *xcos,
        double *ycos,
        double *fxplus,
        double *fyplus,
        double *fxcross,
        double *fycross,
        const LALDetector *detector,
        double ra,
        double dec,
        double psi,
        double gmst
);
 
/*
 * Gives a time series of the detector's response to plus and cross
 * polarization
 */
void
LALComputeDetAMResponseSeries( LALStatus                      *status,
                               LALDetAMResponseSeries         *pResponseSeries,
                               const LALDetAndSource          *pDetAndSource,
                               const LALTimeIntervalAndNSample *pTimeInfo);
 
int XLALComputeDetAMResponseSeries(
        REAL4TimeSeries **fplus,
        REAL4TimeSeries **fcross,
        const REAL4 D[3][3],
        const double ra,
        const double dec,
        const double psi,
        const LIGOTimeGPS *start,
        const double deltaT,
        const int n
);
 
int XLALComputeDetAMResponseExtraModesSeries(
  REAL4TimeSeries **fplus,
  REAL4TimeSeries **fcross,
  REAL4TimeSeries **fb,
  REAL4TimeSeries **fl,
  REAL4TimeSeries **fx,
  REAL4TimeSeries **fy,
  const REAL4 D[3][3],
  const double ra,
  const double dec,
  const double psi,
  const LIGOTimeGPS *start,
  const double deltaT,
  const int n  
);
 
/** @} */
 
#ifdef __cplusplus
}
#endif
 
#endif /* !defined _DETRESPONSE_H */