pseudodynamics.reader¶
Classes
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High Dimensional Cell state Dataset for trajectory indepdent modeling |
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Dataset for high dimensional cellstate Each batch returns the cellstates, and their density in two consecutive timepoints |
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- class pseudodynamics.reader.AllTimepoint_MeshGrid(*args, **kwargs)[source]¶
Bases:
MeshGrid_Resample
- class pseudodynamics.reader.Duds_AnnDS(*args, precomputed_duds=None, **kwargs)[source]¶
Bases:
TwoTimpepoint_AnnDS
- class pseudodynamics.reader.Duds_AnnDS_fastmode(*args, n_pseudobulk=None, pseudobulk_key='pseudo_bulk', resolution=None, **kwargs)[source]¶
Bases:
Duds_AnnDS
- class pseudodynamics.reader.HigDim_AnnDS(AnnData, cellstate_key='cellstate', timepoint_key='timepoint_tx_days', timepoint_idx=None, n_dimension=5, knn_volume=False, nearby_cellstate=1, norm_time=False, deltax_key=None, density_funs=None, kde_kws={}, base_cellstate=None, pop_dict=None, n_grid=300, collocation_points=600, log_transform=False, resampling_indensity=0.5, resampling_rate=0.5)[source]¶
Bases:
AnnDatasetHigh Dimensional Cell state Dataset for trajectory indepdent modeling
- Parameters:
n_repeat (int) – the output file path from script
nearby_cellstate (int) – the number of near (cell state)
norm_Time (boolen) – log-normalize the real timepoint
AnnData (annData,) – the single cell object
cellstate_key (str) – the obsm key, the lower dimension representation on which we will use to compute density
timepoint_key (str) – the obs key that indicate the experimental time the cells are collected from
pop_dict (dict) – the dictionary we use to pass population statistics including collected timepoint, mean ,variation
log_transform (bool) – default False, whether the population size will be log transformed to reduce the magnitude of the data
base_cellstate (np.ndarray) – the space to evaluate the density
- compute_density(density_funs=None)[source]¶
compute the density for the self.cellstate, if density functions not specified then we use the gaussian kde
- Returns:
self.u_b : Tensor, flatten, (n_time * n_cell) self.t_b : Tensor, flatten, (n_time * n_cell) self.density_funs : list of callable, [n_time] self.density_P : ndarray, average the total density into probability summing to 1 self.s_std : the std of self.cellsate
- class pseudodynamics.reader.MeshGrid_AnnDS(*, n_timepoint=None, n_repeat=10, nearby_cellstate=10, norm_time=True, replicate_key='batch', **kwargs)[source]¶
Bases:
AnnDataset,MeshGrid
- class pseudodynamics.reader.MeshGrid_DS(Data_pt, nearby_cellstate=10, n_grid=300, collocation_points=600, n_repeat=10, log_transform=True, norm_time=True)[source]¶
Bases:
Processed_baseDS,MeshGrid
- class pseudodynamics.reader.MeshGrid_Resample(*args, **kwargs)[source]¶
Bases:
MeshGrid_AnnDS
- class pseudodynamics.reader.MeshGrid_logDS(*args, **kwargs)[source]¶
Bases:
MeshGrid_Resample
- class pseudodynamics.reader.Pdyn_ExtractDataset(Data_pt, n_grid=300, collocation_points=600, n_repeat=10, log_transform=True)[source]¶
Bases:
Processed_baseDS
- class pseudodynamics.reader.Random_ExtractDataset(Data_pt, nearby_cellstate=10, n_grid=300, collocation_points=600, n_repeat=10, log_transform=True)[source]¶
Bases:
Pdyn_ExtractDataset
- class pseudodynamics.reader.Simple_DS(*, n_timepoint, **kwargs)[source]¶
Bases:
MeshGrid_AnnDS
- class pseudodynamics.reader.SingleBranch_AnnDS(*, n_timepoint=None, n_repeat=10, nearby_cellstate=10, max_timespan=3, replicate_key='batch', **kwargs)[source]¶
Bases:
AnnDataset,MeshGrid
- class pseudodynamics.reader.Syn_DS(cellstate, density, integrate_time, deltax=None, batchsize=200)[source]¶
Bases:
Dataset
- class pseudodynamics.reader.TwoTimepoint_MeshGrid(*args, **kwargs)[source]¶
Bases:
MeshGrid_Resample
- class pseudodynamics.reader.TwoTimpepoint_AnnDS(AnnData, split='train', cellstate_key='cellstate', timepoint_key='timepoint_tx_days', timepoint_idx=None, n_dimension=5, knn_volume=False, batchsize=200, norm_time=False, deltax_key=None, density_funs=None, kde_kws={}, nearby_cellstate=1, base_cellstate=None, pop_dict=None, n_grid=300, collocation_points=600, log_transform=False, resampling_indensity=0.5, resampling_rate=0.5)[source]¶
Bases:
HigDim_AnnDSDataset for high dimensional cellstate Each batch returns the cellstates, and their density in two consecutive timepoints
- Parameters:
AnnData (annData,) – the single cell dataset
cellstate_key (str,) – the obsm key, the lower dimension representation on which we will use to compute density
timepoint_key (str,) – the obs key that indicate the experimental time the cells are collected from
log_transform (bool,) – default True, whether the population size will be log transformed to reduce the magnitude of the data
n_repeat (int) – the output file path from script
nearby_cellstate (int) – the number of near (cell state)
norm_Time (bool) – log-normalize the real timepoint
split (str,) – train, val or test
knn_volume (bool) – whether to use the volume of the knn graph to rescale the density
Examples
>>> import pseudodynamics as pdp >>> from pseudodynamics import reader >>> config = pdp.ExperimentConfig(config=config_path) >>> DS_sub = pdp.reader.TwoTimpepoint_AnnDS(AnnData=adata, split = 'train', **config.dataset_config )
- class pseudodynamics.reader.TwoTimpepoint_AnnDS_fastmode(*args, pseudobulk_key='pseudo_bulk', resolution=None, n_pseudobulk=None, **kwargs)[source]¶
Bases:
TwoTimpepoint_AnnDS