PhotonTransferCurveSolveTask¶
- class lsst.cp.pipe.PhotonTransferCurveSolveTask(*, config: PipelineTaskConfig | None = None, log: logging.Logger | LsstLogAdapter | None = None, initInputs: dict[str, Any] | None = None, **kwargs: Any)¶
Bases:
PipelineTask
Task to fit the PTC from flat covariances.
The first task of the PTC measurement pipeline,
PhotonTransferCurveMeasureTask
(and assumed to have been run before this task), produced a list ofPhotonTransferCurveDataset
objects. Each dataset contains the mean signal and covariances of the difference image of the flat-field images taken at the same exposure time. The list also contains dummy datasets (with no measurements), whose purpose is to have the input and output dimensions ofPhotonTransferCurveMeasureTask
match.This task,
PhotonTransferCurveSolveTask
, assembles the list of individual PTC datasets produced byPhotonTransferCurveMeasureTask
into one single final PTC dataset, discarding the dummy datset as appropiate. The task fits the measured (co)variances to one of three models: a polynomial model of a given order, or the models described in equations 16 and 20 of Astier+19. These options are referred to asPOLYNOMIAL
,EXPAPPROXIMATION
, andFULLCOVARIANCE
in the configuration options of the task, respectively). Parameters of interest such as the gain and noise are derived from the fits. TheFULLCOVARIANCE
model is fitted to the full covariance data (as oppossed to the other two models, which are fit to the variance vs mean measurements only).Astier+19: “The Shape of the Photon Transfer Curve of CCD sensors”, arXiv:1905.08677
Attributes Summary
Methods Summary
Empty (clear) the metadata for this Task and all sub-Tasks.
evalCovModel
(mu, aMatrix, cMatrix, ...[, ...])Computes full covariances model (Eq.
fillBadAmp
(dataset, ptcFitType, ampName)Fill the dataset with NaNs if there are not enough good points.
fitDataFullCovariance
(dataset)Fit measured flat covariances to the full model in Astier+19 (Eq.
fitMeasurementsToModel
(dataset)Fit the measured covariances vs mean signal to a polynomial or one of the models in Astier+19 (Eq.
fitPtc
(dataset)Fit the photon transfer curve to a polynomial or to the Astier+19 approximation (Eq.
funcFullCovarianceModel
(params, x)Model to fit covariances from flat fields; Equation 20 of Astier+19.
funcFullCovarianceModelNoB
(params, x)Model to fit covariances from flat fields; Equation 20 of Astier+19, with b=0 (equivalent to c=a*b=0 in this code).
Get metadata for all tasks.
Get the task name as a hierarchical name including parent task names.
getName
()Get the name of the task.
Get a dictionary of all tasks as a shallow copy.
initialFitFullCovariance
(mu, cov, sqrtW)Performs a crude parabolic fit of the data in order to start the full fit close to the solution, setting b=0 (c=0) in Eq.
makeField
(doc)Make a
lsst.pex.config.ConfigurableField
for this task.makeSubtask
(name, **keyArgs)Create a subtask as a new instance as the
name
attribute of this task.run
(inputCovariances[, camera, detId])Fit measured covariances to different models.
runQuantum
(butlerQC, inputRefs, outputRefs)Ensure that the input and output dimensions are passed along.
subtractDistantOffset
(muAtAmpMasked, ...[, ...])Subtract distant offset from the covariance matrices.
timer
(name[, logLevel])Context manager to log performance data for an arbitrary block of code.
Attributes Documentation
Methods Documentation
- evalCovModel(mu, aMatrix, cMatrix, noiseMatrix, gain, setBtoZero=False)¶
Computes full covariances model (Eq. 20 of Astier+19).
- Parameters:
- mu
numpy.array
, (N,) List of mean signals (units: adu)
- aMatrix
numpy.array
, (M, M) “a” parameter per flux in Eq. 20 of Astier+19 (units: 1/electron)
- cMatrix
numpy.array
, (M, M) “c”=”ab” parameter per flux in Eq. 20 of Astier+19 (units: 1/electron^2)
- noiseMatrix
numpy.array
, (M, M) “noise” parameter per flux in Eq. 20 of Astier+19 (units: electron^2)
- gain
float
Amplifier gain (e/adu)
- setBtoZero=False
bool
, optional Set “b” parameter in full model (see Astier+19) to zero.
- mu
- Returns:
- covModel
numpy.array
, (N, M, M) Covariances model.
- covModel
Notes
By default, computes the covModel for the mu’s stored(self.mu). Returns cov[Nmu, M, M]. The variance for the PTC is cov[:, 0, 0]. mu and cov are in adus and adus squared. To use electrons for both, the gain should be set to 1. This routine implements the model in Astier+19 (1905.08677). The parameters of the full model for C_ij(mu) (“C_ij” and “mu” in adu^2 and adu, respectively) in Astier+19 (Eq. 20) are:
“a” coefficients (M by M matrix), units: 1/electron
“b” coefficients (M by M matrix), units: 1/electron
noise matrix (M by M matrix), units: electron^2
gain, units: electron/adu
“b” appears in Eq. 20 only through the “ab” combination, which is defined in this code as “c=ab”.
- fillBadAmp(dataset, ptcFitType, ampName)¶
Fill the dataset with NaNs if there are not enough good points.
- Parameters:
- dataset
lsst.ip.isr.ptcDataset.PhotonTransferCurveDataset
The dataset containing the means, variances and exposure times.
- ptcFitType{‘POLYNOMIAL’, ‘EXPAPPROXIMATION’}
Fit a ‘POLYNOMIAL’ (degree: ‘polynomialFitDegree’) or ‘EXPAPPROXIMATION’ (Eq. 16 of Astier+19) to the PTC.
- ampName
str
Amplifier name.
- dataset
- fitDataFullCovariance(dataset)¶
Fit measured flat covariances to the full model in Astier+19 (Eq. 20).
- Parameters:
- dataset
lsst.ip.isr.ptcDataset.PhotonTransferCurveDataset
The dataset containing information such as the means, (co)variances, and exposure times.
- dataset
- Returns:
- dataset
lsst.ip.isr.ptcDataset.PhotonTransferCurveDataset
This is the same dataset as the input parameter, however, it has been modified to include information such as the fit vectors and the fit parameters. See the class
PhotonTransferCurveDatase
.
- dataset
Notes
The parameters of the full model for C_ij(mu) (“C_ij” and “mu” in adu^2 and adu, respectively) in Astier+19 (Eq. 20) are:
“a” coefficients (r by r matrix), units: 1/electron
“b” coefficients (r by r matrix), units: 1/electron
noise matrix (r by r matrix), units: electron^2
gain, units: electron/adu
“b” appears in Eq. 20 only through the “ab” combination, which is defined in this code as “c=ab”.
Total number of parameters: #entries(a) + #entries(c) + #entries(noise) + 1. This is equivalent to r^2 + r^2 + r^2 + 1, where “r” is the maximum lag considered for the covariances calculation, and the extra “1” is the gain. If “b” is 0, then “c” is 0, and len(pInit) will have r^2 fewer entries.
- fitMeasurementsToModel(dataset)¶
Fit the measured covariances vs mean signal to a polynomial or one of the models in Astier+19 (Eq. 16 or Eq.20).
- Parameters:
- dataset
lsst.ip.isr.ptcDataset.PhotonTransferCurveDataset
The dataset containing information such as the means, (co)variances, and exposure times.
- dataset
- Returns:
- dataset
lsst.ip.isr.ptcDataset.PhotonTransferCurveDataset
This is the same dataset as the input parameter, however, it has been modified to include information such as the fit vectors and the fit parameters. See the class
PhotonTransferCurveDatase
.
- dataset
- fitPtc(dataset)¶
Fit the photon transfer curve to a polynomial or to the Astier+19 approximation (Eq. 16).
Fit the photon transfer curve with either a polynomial of the order specified in the task config (POLNOMIAL), or using the exponential approximation in Astier+19 (Eq. 16, FULLCOVARIANCE).
Sigma clipping is performed iteratively for the fit, as well as an initial clipping of data points that are more than
config.initialNonLinearityExclusionThreshold
away from lying on a straight line. This other step is necessary because the photon transfer curve turns over catastrophically at very high flux (because saturation drops the variance to ~0) and these far outliers cause the initial fit to fail, meaning the sigma cannot be calculated to perform the sigma-clipping.- Parameters:
- dataset
lsst.ip.isr.ptcDataset.PhotonTransferCurveDataset
The dataset containing the means, variances and exposure times.
- dataset
- Returns:
- dataset
lsst.ip.isr.ptcDataset.PhotonTransferCurveDataset
This is the same dataset as the input parameter, however, it has been modified to include information such as the fit vectors and the fit parameters. See the class
PhotonTransferCurveDatase
.
- dataset
- Raises:
- RuntimeError
Raised if dataset.ptcFitType is None or empty.
- funcFullCovarianceModel(params, x)¶
Model to fit covariances from flat fields; Equation 20 of Astier+19.
- Parameters:
- params
list
Parameters of the model: aMatrix, CMatrix, noiseMatrix, gain (e/adu).
- x
numpy.array
, (N,) Signal
mu
(adu)
- params
- Returns:
- y
numpy.array
, (N,) Covariance matrix.
- y
- funcFullCovarianceModelNoB(params, x)¶
Model to fit covariances from flat fields; Equation 20 of Astier+19, with b=0 (equivalent to c=a*b=0 in this code).
- Parameters:
- params
list
Parameters of the model: aMatrix, noiseMatrix, gain (e/adu).
- x
numpy.array
, (N,) Signal mu (adu)
- params
- Returns:
- y
numpy.array
, (N,) Covariance matrix.
- y
- getFullMetadata() TaskMetadata ¶
Get metadata for all tasks.
- Returns:
- metadata
TaskMetadata
The keys are the full task name. Values are metadata for the top-level task and all subtasks, sub-subtasks, etc.
- metadata
Notes
The returned metadata includes timing information (if
@timer.timeMethod
is used) and any metadata set by the task. The name of each item consists of the full task name with.
replaced by:
, followed by.
and the name of the item, e.g.:topLevelTaskName:subtaskName:subsubtaskName.itemName
using
:
in the full task name disambiguates the rare situation that a task has a subtask and a metadata item with the same name.
- getFullName() str ¶
Get the task name as a hierarchical name including parent task names.
- Returns:
- fullName
str
The full name consists of the name of the parent task and each subtask separated by periods. For example:
The full name of top-level task “top” is simply “top”.
The full name of subtask “sub” of top-level task “top” is “top.sub”.
The full name of subtask “sub2” of subtask “sub” of top-level task “top” is “top.sub.sub2”.
- fullName
- getName() str ¶
Get the name of the task.
- Returns:
- taskName
str
Name of the task.
- taskName
See also
getFullName
Get the full name of the task.
- getTaskDict() dict[str, weakref.ReferenceType[lsst.pipe.base.task.Task]] ¶
Get a dictionary of all tasks as a shallow copy.
- Returns:
- taskDict
dict
Dictionary containing full task name: task object for the top-level task and all subtasks, sub-subtasks, etc.
- taskDict
- initialFitFullCovariance(mu, cov, sqrtW)¶
Performs a crude parabolic fit of the data in order to start the full fit close to the solution, setting b=0 (c=0) in Eq. 20 of Astier+19.
- Parameters:
- mu
numpy.array
, (N,) Signal
mu
(adu)- cov
numpy.array
, (N, M, M) Covariance arrays of size
(M, M)
(withM = config.maximumRangeCovariancesAstier
), indexed by mean signalmu
.- sqrtW
numpy.array
, (N,) Covariance weights, defined as 1./sqrt(Variances)
- mu
- Returns:
- a
numpy.array
, (M, M) “a” parameter per flux in Eq. 20 of Astier+19 (units: 1/electron).
- c
numpy.array
, (M, M) “c”=”ab” parameter per flux in Eq. 20 of Astier+19. (units: 1/electron^2).
- noiseMatrix
numpy.array
, (M, M) “noise” parameter per flux in Eq. 20 of Astier+19. (units: electron^2)
- gain
float
Amplifier gain (electron/adu)
- a
- classmethod makeField(doc: str) ConfigurableField ¶
Make a
lsst.pex.config.ConfigurableField
for this task.- Parameters:
- doc
str
Help text for the field.
- doc
- Returns:
- configurableField
lsst.pex.config.ConfigurableField
A
ConfigurableField
for this task.
- configurableField
Examples
Provides a convenient way to specify this task is a subtask of another task.
Here is an example of use:
class OtherTaskConfig(lsst.pex.config.Config): aSubtask = ATaskClass.makeField("brief description of task")
- makeSubtask(name: str, **keyArgs: Any) None ¶
Create a subtask as a new instance as the
name
attribute of this task.- Parameters:
- name
str
Brief name of the subtask.
- **keyArgs
Extra keyword arguments used to construct the task. The following arguments are automatically provided and cannot be overridden:
config
.parentTask
.
- name
Notes
The subtask must be defined by
Task.config.name
, an instance ofConfigurableField
orRegistryField
.
- run(inputCovariances, camera=None, detId=0)¶
Fit measured covariances to different models.
- Parameters:
- inputCovariances
list
[lsst.ip.isr.PhotonTransferCurveDataset
] List of lsst.ip.isr.PhotonTransferCurveDataset datasets.
- camera
lsst.afw.cameraGeom.Camera
, optional Input camera.
- detId
int
Detector ID to locate the detector in the camera and populate the
lsst.ip.isr.PhotonTransferCurveDataset
metadata.- Returns
- ——-
- results
lsst.pipe.base.Struct
The resultins structure contains:
outputPtcDatset
Final PTC dataset, containing information such as the means, variances, and exposure times (
lsst.ip.isr.PhotonTransferCurveDataset
).
- inputCovariances
- runQuantum(butlerQC, inputRefs, outputRefs)¶
Ensure that the input and output dimensions are passed along.
- Parameters:
- butlerQC
QuantumContext
Butler to operate on.
- inputRefs
InputQuantizedConnection
Input data refs to load.
- ouptutRefs
OutputQuantizedConnection
Output data refs to persist.
- butlerQC
- subtractDistantOffset(muAtAmpMasked, covAtAmpMasked, covSqrtWeightsAtAmpMasked, start, degree=1)¶
Subtract distant offset from the covariance matrices.
- Parameters:
- muAtAmpMasked
numpy.array
Masked mean flux array for a particular amplifier.
- covAtAmpMasked
numpy.array
Masked measured covariances for a particular amplifier.
- covSqrtWeightsAtAmpMasked
numpy.array
Masked inverse covariance weights for a particular amplifier.
- startint, optional
The starting index to eliminate the core for the fit.
- degreeint, optional
Degree of the polynomial fit.
- muAtAmpMasked
- Returns:
- covAtAmpMasked
numpy.array
Subtracted measured covariances for a particular amplifier.
- covSqrtWeightsAtAmpMasked
numpy.array
Masked inverse covariance weights for a particular amplifier.
- covAtAmpMasked
Notes
Ported from https://gitlab.in2p3.fr/astier/bfptc by P. Astier.
This function subtracts a distant offset from the covariance matrices using polynomial fitting. The core of the matrices is eliminated for the fit.
The function modifies the internal state of the object, updating the covariance matrices and related attributes.