3. Intensity distribution

Import Python libraries Hide code cell content

from __future__ import annotations

import logging
import os
from io import BytesIO
from itertools import product
from urllib.request import urlopen
from zipfile import ZipFile

import jax.numpy as jnp
import matplotlib.pyplot as plt
import numpy as np
import sympy as sp
from ampform.helicity.naming import natural_sorting
from ampform.sympy import perform_cached_doit
from ampform_dpd.decay import Particle
from ampform_dpd.io import perform_cached_lambdify
from IPython.display import Markdown
from matplotlib.image import imread
from matplotlib.patches import Rectangle
from tensorwaves.interface import DataSample
from tqdm.auto import tqdm

from polarimetry.data import (
    create_data_transformer,
    generate_meshgrid_sample,
    generate_phasespace_sample,
    generate_sub_meshgrid_sample,
)
from polarimetry.function import (
    compute_sub_function,
    integrate_intensity,
    interference_intensity,
    sub_intensity,
)
from polarimetry.io import mute_jax_warnings
from polarimetry.lhcb import load_model
from polarimetry.lhcb.particle import load_particles
from polarimetry.plot import add_watermark, get_contour_line, use_mpl_latex_fonts

mute_jax_warnings()
particles = load_particles("../data/particle-definitions.yaml")
model = load_model("../data/model-definitions.yaml", particles, model_id=0)

NO_LOG = "EXECUTE_NB" in os.environ
if NO_LOG:
    logging.disable(logging.CRITICAL)

unfolded_intensity_expr = perform_cached_doit(model.full_expression)

The complete intensity expression contains 43,198 mathematical operations.

3.1. Definition of free parameters

free_parameters = {
    symbol: value
    for symbol, value in model.parameter_defaults.items()
    if isinstance(symbol, sp.Indexed)
    if "production" in str(symbol)
}
fixed_parameters = {
    symbol: value
    for symbol, value in model.parameter_defaults.items()
    if symbol not in free_parameters
}
subs_intensity_expr = unfolded_intensity_expr.xreplace(fixed_parameters)

After substituting the parameters that are not production couplings, the total intensity expression contains 9,516 operations.

3.2. Distribution

intensity_func = perform_cached_lambdify(
    subs_intensity_expr,
    parameters=free_parameters,
    backend="jax",
)

transformer = create_data_transformer(model)
grid_sample = generate_meshgrid_sample(model.decay, resolution=1_000)
grid_sample = transformer(grid_sample)
X = grid_sample["sigma1"]
Y = grid_sample["sigma2"]

Show code cell source Hide code cell source

%config InlineBackend.figure_formats = ['png']
s1_label = R"$\sigma_1=m^2\left(K^-\pi^+\right)$ [GeV$^2$]"
s2_label = R"$\sigma_2=m^2\left(pK^-\right)$ [GeV$^2$]"
s3_label = R"$\sigma_3=m^2\left(p\pi^+\right)$ [GeV$^2$]"

plt.rcdefaults()
use_mpl_latex_fonts()
plt.rc("font", size=21)
fig, ax = plt.subplots(dpi=200, figsize=(8.22, 7), tight_layout=True)
ax.set_xlabel(s1_label)
ax.set_ylabel(s2_label)

INTENSITIES = intensity_func(grid_sample)
INTENSITY_INTEGRAL = jnp.nansum(INTENSITIES)
NORMALIZED_INTENSITIES = INTENSITIES / INTENSITY_INTEGRAL
np.testing.assert_almost_equal(jnp.nansum(NORMALIZED_INTENSITIES), 1.0)
mesh = ax.pcolormesh(X, Y, NORMALIZED_INTENSITIES)
c_bar = fig.colorbar(mesh, ax=ax, pad=0.02)
c_bar.ax.set_ylabel("Normalized intensity")
add_watermark(ax, 0.7, 0.82, fontsize=24)
fig.savefig("_static/images/intensity-distribution.png")
plt.show()

High-resolution image can be downloaded here: intensity-distribution.png

Comparison with Figure 2 from the original LHCb study [1]:

Show code cell source Hide code cell source

def download_lhcb_intensity() -> None:
    figure_path = "LHCb-PAPER-2022-002-figures/Fig2.png"
    if os.path.exists(figure_path):
        return
    url = "https://cds.cern.ch/record/2824328/files/LHCb-PAPER-2022-002-figures.zip?version=1"
    http_response = urlopen(url)
    zipfile = ZipFile(BytesIO(http_response.read()))
    zipfile.extract(figure_path)


def plot_horizontal_intensity(ax) -> None:
    ax.set_xlabel("$" + s2_label[10:])
    ax.set_ylabel("$" + s1_label[10:])
    ax.set_xlim(1.79, 4.95)
    ax.set_ylim(0.18, 2.05)
    add_watermark(ax, 0.7, 0.78, fontsize=18)
    mesh = ax.pcolormesh(
        grid_sample["sigma2"],
        grid_sample["sigma1"],
        NORMALIZED_INTENSITIES,
    )
    c_bar = fig.colorbar(mesh, ax=ax, pad=0.02)
    c_bar.ax.set_ylabel("Normalized intensity")


%config InlineBackend.figure_formats = ['png']
download_lhcb_intensity()
plt.rcdefaults()
use_mpl_latex_fonts()
plt.rc("font", size=16)
fig = plt.figure(dpi=200, figsize=(11.5, 4))
ax1 = fig.add_axes((0.1, 0.17, 0.40, 0.78))
ax2 = fig.add_axes((0.5, 0.0, 0.5, 1.0))
ax2.axis("off")
plot_horizontal_intensity(ax1)
image = imread("LHCb-PAPER-2022-002-figures/Fig2.png")
ax2.imshow(image)
fig.savefig("_static/images/intensity-distribution-comparison.png")
plt.show()

Export left part of the intensity comparison Hide code cell content

plt.ioff()
fig, ax = plt.subplots(dpi=200, figsize=(5.8, 4))
plot_horizontal_intensity(ax)
fig.savefig(
    "_static/images/intensity-distribution-comparison-left.png",
    bbox_inches="tight",
)
plt.ion()
plt.close(fig)

Show code cell source Hide code cell source

def set_ylim_to_zero(ax):
    _, y_max = ax.get_ylim()
    ax.set_ylim(0, y_max)


%config InlineBackend.figure_formats = ['svg']
plt.rcdefaults()
use_mpl_latex_fonts()
plt.rc("font", size=18)
fig, (ax1, ax2) = plt.subplots(
    ncols=2,
    figsize=(12, 5),
    tight_layout=True,
    sharey=True,
)
ax1.set_xlabel(s1_label)
ax2.set_xlabel(s2_label)
ax1.set_ylabel("Normalized intensity")

subsystem_identifiers = ["K", "L", "D"]
subsystem_labels = ["K^{**}", R"\Lambda^{**}", R"\Delta^{**}"]
x, y = X[0], Y[:, 0]
ax1.fill(x, jnp.nansum(NORMALIZED_INTENSITIES, axis=0), alpha=0.3)
ax2.fill(y, jnp.nansum(NORMALIZED_INTENSITIES, axis=1), alpha=0.3)

original_parameters = dict(intensity_func.parameters)
for label, identifier in zip(subsystem_labels, subsystem_identifiers):
    label = f"${label}$"
    sub_intensities = compute_sub_function(intensity_func, grid_sample, [identifier])
    sub_intensities /= INTENSITY_INTEGRAL
    ax1.plot(x, jnp.nansum(sub_intensities, axis=0), label=label)
    ax2.plot(y, jnp.nansum(sub_intensities, axis=1), label=label)
    del sub_intensities
    intensity_func.update_parameters(original_parameters)
set_ylim_to_zero(ax1)
set_ylim_to_zero(ax2)
ax2.legend()
plt.savefig("_images/intensity-distributions-1D.svg")
plt.show()

3.3. Decay rates

integration_sample = generate_phasespace_sample(model.decay, n_events=100_000, seed=0)
integration_sample = transformer(integration_sample)
I_tot = integrate_intensity(intensity_func(integration_sample))

I_K = sub_intensity(intensity_func, integration_sample, non_zero_couplings=["K"])
I_Λ = sub_intensity(intensity_func, integration_sample, non_zero_couplings=["L"])
I_Δ = sub_intensity(intensity_func, integration_sample, non_zero_couplings=["D"])
I_ΛΔ = interference_intensity(intensity_func, integration_sample, ["L"], ["D"])
I_KΔ = interference_intensity(intensity_func, integration_sample, ["K"], ["D"])
I_KΛ = interference_intensity(intensity_func, integration_sample, ["K"], ["L"])
np.testing.assert_allclose(I_tot, I_K + I_Λ + I_Δ + I_ΛΔ + I_KΔ + I_KΛ)

Functions for computing the decay rate Hide code cell content

def compute_decay_rates(func, integration_sample: DataSample):
    decay_rates = np.zeros(shape=(n_resonances, n_resonances))
    combinations = list(product(enumerate(resonances), enumerate(resonances)))
    progress_bar = tqdm(
        desc="Calculating rate matrix",
        disable=NO_LOG,
        total=(len(combinations) + n_resonances) // 2,
    )
    I_tot = integrate_intensity(intensity_func(integration_sample))
    for (i, resonance1), (j, resonance2) in combinations:
        if j < i:
            continue
        progress_bar.postfix = f"{resonance1.name} × {resonance2.name}"
        res1 = resonance1.latex
        res2 = resonance2.latex
        if res1 == res2:
            I_sub = sub_intensity(func, integration_sample, non_zero_couplings=[res1])
        else:
            I_sub = interference_intensity(func, integration_sample, [res1], [res2])
        decay_rates[i, j] = I_sub / I_tot
        if i != j:
            decay_rates[j, i] = decay_rates[i, j]
        progress_bar.update()
    progress_bar.close()
    return decay_rates


def sort_resonances(resonance: Particle):
    KDL = {"L": 1, "D": 2, "K": 3}
    return KDL[resonance.name[0]], natural_sorting(resonance.name)


resonances = sorted(
    (chain.resonance for chain in model.decay.chains),
    key=sort_resonances,
    reverse=True,
)
n_resonances = len(resonances)

Show code cell source Hide code cell source

def visualize_decay_rates(decay_rates, title=R"Rate matrix for isobars (\%)"):
    vmax = jnp.max(jnp.abs(decay_rates))
    plt.rcdefaults()
    use_mpl_latex_fonts()
    plt.rc("font", size=14)
    plt.rc("axes", titlesize=24)
    plt.rc("xtick", labelsize=16)
    plt.rc("ytick", labelsize=16)
    fig, ax = plt.subplots(figsize=(9, 9))
    ax.set_title(title)
    ax.matshow(jnp.rot90(decay_rates).T, cmap=plt.cm.coolwarm, vmin=-vmax, vmax=+vmax)

    resonance_latex = [f"${p.latex}$" for p in resonances]
    ax.set_xticks(range(n_resonances))
    ax.set_xticklabels(reversed(resonance_latex), rotation=90)
    ax.set_yticks(range(n_resonances))
    ax.set_yticklabels(resonance_latex)
    for i in range(n_resonances):
        for j in range(n_resonances):
            if j < i:
                continue
            rate = decay_rates[i, j]
            ax.text(
                n_resonances - j - 1,
                i,
                f"{100 * rate:.2f}",
                va="center",
                ha="center",
            )
    fig.tight_layout()
    return fig


%config InlineBackend.figure_formats = ['svg']
decay_rates = compute_decay_rates(intensity_func, integration_sample)
fig = visualize_decay_rates(decay_rates)
fig.savefig("_images/rate-matrix.svg")
plt.show()

Function for computing the total over all rates Hide code cell content

def compute_sum_over_decay_rates(decay_rate_matrix) -> float:
    decay_rate_sum = 0.0
    for i in range(len(resonances)):
        for j in range(len(resonances)):
            if j < i:
                continue
            decay_rate_sum += decay_rate_matrix[i, j]
    return decay_rate_sum

np.testing.assert_almost_equal(compute_sum_over_decay_rates(decay_rates), 1.0)

3.4. Dominant decays

Show code cell source Hide code cell source

%config InlineBackend.figure_formats = ['svg']
threshold = 0.5
percentage = int(100 * threshold)
I_tot = intensity_func(grid_sample)

plt.rcdefaults()
use_mpl_latex_fonts()
plt.rc("font", size=18)
fig, ax = plt.subplots(figsize=(9.1, 7), sharey=True, tight_layout=True)
ax.set_ylabel(s2_label)
ax.set_xlabel(s1_label)
fig.suptitle(
    Rf"Regions where the resonance has a decay ratio of $\geq {percentage}$\%",
    y=0.95,
)

phsp_region = jnp.select(
    [I_tot > 0, True],
    (1, 0),
)
ax.contour(X, Y, phsp_region, colors=["black"], levels=[0], linewidths=[0.2])

resonances = [c.resonance for c in model.decay.chains]
colors = [plt.cm.rainbow(x) for x in np.linspace(0, 1, len(resonances))]
linestyles = {
    "K": "dotted",
    "L": "dashed",
    "D": "solid",
}
items = list(zip(resonances, colors))  # tqdm requires len
progress_bar = tqdm(
    desc="Computing dominant region contours",
    disable=NO_LOG,
    total=len(items),
)
legend_elements = {}
for resonance, color in items:
    progress_bar.postfix = resonance.name
    I_sub = compute_sub_function(intensity_func, grid_sample, [resonance.latex])
    ratio = I_sub / I_tot
    selection = jnp.select(
        [jnp.isnan(ratio), ratio < threshold, True],
        [0, 0, 1],
    )
    progress_bar.update()
    if jnp.all(selection == 0):
        continue
    contour_set = ax.contour(
        *(X, Y, selection),
        colors=[color],
        levels=[0],
        linestyles=linestyles[resonance.name[0]],
    )
    contour_set.set_clim(vmin=1, vmax=len(model.decay.chains))
    line_collection = get_contour_line(contour_set)
    legend_elements[f"${resonance.latex}$"] = line_collection
progress_bar.close()


sub_region_x_range = (0.68, 0.72)
sub_region_y_range = (2.52, 2.60)
region_indicator = Rectangle(
    xy=(
        sub_region_x_range[0],
        sub_region_y_range[0],
    ),
    width=sub_region_x_range[1] - sub_region_x_range[0],
    height=sub_region_y_range[1] - sub_region_y_range[0],
    edgecolor="black",
    facecolor="none",
    label="Sub-region",
    linewidth=0.5,
    zorder=10,
)
ax.add_patch(region_indicator)
legend_elements[region_indicator.get_label()] = region_indicator

leg = ax.legend(
    handles=legend_elements.values(),
    labels=legend_elements.keys(),
    bbox_to_anchor=(1.38, 1),
    framealpha=1,
    loc="upper right",
)
fig.savefig("_images/sub-regions.svg")
plt.show()

Show code cell source Hide code cell source

%config InlineBackend.figure_formats = ['svg']
sub_sample = generate_sub_meshgrid_sample(
    model.decay,
    resolution=50,
    x_range=sub_region_x_range,
    y_range=sub_region_y_range,
)
sub_sample = transformer(sub_sample)
sub_decay_rates = compute_decay_rates(intensity_func, sub_sample)
fig = visualize_decay_rates(sub_decay_rates, title="Rate matrix over sub-region")
fig.savefig("_images/rate-matrix-sub-region.svg")
plt.show()

np.testing.assert_almost_equal(compute_sum_over_decay_rates(sub_decay_rates), 1.0)