Understanding and Exploring Models¶
This tutorial covers how to work with PyHS3 models - understanding their structure, exploring their contents, and evaluating them.
What is a Model?¶
A Model is the computational representation of your statistical model created from a workspace. It contains:
Parameters: Symbolic tensor variables representing your model parameters
Distributions: Compiled probability distribution functions
Functions: Compiled mathematical functions
Computational Graph: The dependency structure between all components
Models are created from workspaces and provide the interface for evaluating PDFs, generating samples, and performing statistical analysis.
Creating Models¶
Models are created from workspaces using the .model()
method:
import pyhs3
# Create a workspace (see workspace tutorial)
workspace_data = {
"metadata": {"hs3_version": "0.2"},
"distributions": [
{
"name": "gaussian_model",
"type": "gaussian_dist",
"x": "observable",
"mean": "mu",
"sigma": "sigma",
}
],
"parameter_points": [
{
"name": "default_params",
"parameters": [
{"name": "observable", "value": 0.0},
{"name": "mu", "value": 0.0},
{"name": "sigma", "value": 1.0},
],
}
],
"domains": [
{
"name": "valid_range",
"type": "product_domain",
"axes": [
{"name": "observable", "min": -5.0, "max": 5.0},
{"name": "mu", "min": -2.0, "max": 2.0},
{"name": "sigma", "min": 0.1, "max": 3.0},
],
}
],
}
ws = pyhs3.Workspace(**workspace_data)
# Create model with specific domain and parameter set
model = ws.model(domain="valid_range", parameter_set="default_params")
# Or use defaults (first domain and parameter set)
model = ws.model()
Exploring Model Structure¶
Once you have a model, you can explore its structure:
# Print model overview
print(model) # Shows parameters, distributions, functions count
# Access model components
print("Parameters:")
for name, tensor in model.parameters.items():
print(f" {name}: {tensor}")
print("\\nDistributions:")
for name, tensor in model.distributions.items():
print(f" {name}: {tensor}")
print("\\nFunctions:")
for name, tensor in model.functions.items():
print(f" {name}: {tensor}")
# Get detailed graph information for a specific distribution
summary = model.graph_summary("gaussian_model")
print(f"\\nGraph summary for gaussian_model:\\n{summary}")
Understanding the Computational Graph¶
PyHS3 models are built as computational graphs where:
Parameters are leaf nodes (input variables)
Functions transform parameters into intermediate values
Distributions depend on parameters and/or function outputs
Dependencies define the evaluation order
You can visualize the computational graph:
# Generate a visual graph (requires pydot)
try:
model.visualize_graph("gaussian_model", output_file="model_graph.png")
print("Graph saved to model_graph.png")
except ImportError:
print("Install pydot to visualize graphs: pip install pydot")
Parameter Discovery and Bounds¶
PyHS3 automatically discovers parameters from your distributions and functions. Parameters are created with domain bounds applied:
# Parameters are automatically bounded based on domain constraints
# For example, with domain axes:
# {"name": "sigma", "min": 0.1, "max": 3.0}
# The sigma parameter will be automatically constrained to [0.1, 3.0]
# Parameters not in parameter_points are discovered and use default bounds
minimal_workspace = {
"metadata": {"hs3_version": "0.2"},
"distributions": [
{
"name": "discovered_model",
"type": "gaussian_dist",
"x": "data",
"mean": "discovered_mu",
"sigma": "discovered_sigma",
}
],
"domains": [
{
"name": "constraints",
"type": "product_domain",
"axes": [{"name": "discovered_sigma", "min": 0.5, "max": 2.0}],
}
],
# Note: no parameter_points defined
}
ws_minimal = pyhs3.Workspace(**minimal_workspace)
model_minimal = ws_minimal.model()
print("Discovered parameters:")
for param_name in model_minimal.parameters:
print(f" {param_name}")
Evaluating Models¶
The primary use of models is to evaluate probability density functions:
# Evaluate PDF at specific parameter values
pdf_value = model.pdf("gaussian_model", observable=0.0, mu=0.0, sigma=1.0)
print(f"PDF(0.0) = {pdf_value}")
# Evaluate at different points
pdf_at_1 = model.pdf("gaussian_model", observable=1.0, mu=0.0, sigma=1.0)
pdf_at_2 = model.pdf("gaussian_model", observable=2.0, mu=0.0, sigma=1.0)
print(f"PDF(1.0) = {pdf_at_1}")
print(f"PDF(2.0) = {pdf_at_2}")
# Vectorized evaluation
import numpy as np
x_values = np.linspace(-3, 3, 100)
pdf_values = [
model.pdf("gaussian_model", observable=x, mu=0.0, sigma=1.0) for x in x_values
]
Model Compilation and Performance¶
Models use PyTensor for fast compilation and evaluation:
# Models support different compilation modes
fast_model = ws.model(mode="FAST_RUN") # Maximum optimization
debug_model = ws.model(mode="FAST_COMPILE") # Faster compilation
# Check compilation status
print(f"Model mode: {model.mode}")
summary = model.graph_summary("gaussian_model")
print("Compiled:" in summary) # Shows if function is compiled
Working with Complex Models¶
For models with multiple distributions and functions:
complex_model = {
"metadata": {"hs3_version": "0.2"},
"distributions": [
{
"name": "signal",
"type": "gaussian_dist",
"x": "mass",
"mean": "signal_mean",
"sigma": "resolution",
},
{
"name": "background",
"type": "generic_dist",
"x": "mass",
"expression": "exp(-mass/slope)",
},
],
"functions": [
{
"name": "total_yield",
"type": "sum",
"summands": ["signal_events", "background_events"],
},
{
"name": "signal_fraction",
"type": "generic_function",
"expression": "signal_events / total_yield",
},
],
"parameter_points": [
{
"name": "physics_point",
"parameters": [
{"name": "signal_mean", "value": 125.0},
{"name": "resolution", "value": 2.5},
{"name": "signal_events", "value": 100.0},
{"name": "background_events", "value": 1000.0},
{"name": "slope", "value": 50.0},
],
}
],
}
complex_ws = pyhs3.Workspace(**complex_model)
complex_model = complex_ws.model()
# Evaluate individual components
signal_pdf = complex_model.pdf("signal", mass=125.0, signal_mean=125.0, resolution=2.5)
background_pdf = complex_model.pdf("background", mass=125.0, slope=50.0)
# Evaluate functions
total = complex_model.pdf("total_yield", signal_events=100.0, background_events=1000.0)
fraction = complex_model.pdf(
"signal_fraction", signal_events=100.0, background_events=1000.0
)
print(f"Signal PDF: {signal_pdf}")
print(f"Background PDF: {background_pdf}")
print(f"Total yield: {total}")
print(f"Signal fraction: {fraction}")
Debugging and Troubleshooting¶
When working with models, you can debug issues using:
# 1. Check model structure
print(model)
# 2. Examine computational graph
summary = model.graph_summary("distribution_name")
print(summary)
# 3. Use debug compilation mode
debug_model = ws.model(mode="DebugMode")
# 4. Visualize dependencies
try:
model.visualize_graph("distribution_name")
except ImportError:
print("Install pydot for graph visualization")
# 5. Check parameter discovery
print("Available parameters:", list(model.parameters.keys()))
print("Available distributions:", list(model.distributions.keys()))
print("Available functions:", list(model.functions.keys()))
Advanced Topics¶
Tensor Types¶
Parameters can have different tensor types based on their intended use:
# In parameter_points, you can specify tensor kinds:
vector_params = {
"name": "vector_params",
"parameters": [
{"name": "scalar_param", "value": 1.0, "kind": "scalar"}, # Default
{"name": "vector_param", "value": [1.0, 2.0], "kind": "vector"},
],
}
Custom Functions¶
You can define custom mathematical expressions:
custom_function = {
"name": "custom_calc",
"type": "generic_function",
"expression": "sqrt(x**2 + y**2)", # Uses SymPy syntax
}
Performance Optimization¶
For better performance:
Use
mode="FAST_RUN"
for production modelsAvoid repeated model creation
Cache compiled functions when possible
Use appropriate tensor types for your data
# Good: reuse model
model = ws.model(mode="FAST_RUN")
results = []
for x in data_points:
result = model.pdf("my_dist", observable=x, mu=0.0, sigma=1.0)
results.append(result)
# Less efficient: recreate model each time
# for x in data_points:
# model = ws.model() # Don't do this
# result = model.pdf("my_dist", observable=x, mu=0.0, sigma=1.0)