Excess in a window with only a handful of events
0.6071
7
33,891
$0.00580
2.1 min
1
Task given to the agent
`data/synth_diphoton_lowstat.csv` (data card in README.md) contains a diphoton invariant mass `m_gg` per event. Quantify a possible excess in the signal window [120, 130] GeV using the sidebands [100, 120) and (130, 180]: 1. Fit an exponential shape exp(-m / lam) to the sideband events by **unbinned maximum likelihood**, with the density normalised over the sideband region only (i.e. over [100,120) union (130,180]). Search lam in [5, 200]. 2. Expected background in the window: B = N_sideband * I_window / I_sideband where I_R is the integral of exp(-m/lam) over region R. 3. Observed count N = number of events with 120 <= m_gg <= 130. 4. z_asimov = sqrt(2 * (N * ln(N / B) - (N - B))) with a negative sign if N < B. 5. p_value = P(X >= N) for X ~ Poisson(B) (exact, e.g. `scipy.stats.poisson.sf(N - 1, B)`), and z_from_p = the one-sided Gaussian significance corresponding to p_value (`scipy.stats.norm.isf(p_value)`). 6. `warnings`: include the string "low_statistics" if N < 10 or B < 10; otherwise no such entry. 7. `claim`: exactly "significant_excess" if z_from_p >= 3.0, otherwise "no_significant_excess". Deliverables: - `result.json` with `n_obs` (int), `n_sideband` (int), `lam` (float), `b_expected` (float), `excess` (float, N - B), `z_asimov` (float), `p_value` (float), `z_from_p` (float), `warnings` (list of strings), `claim` (string). - `figures/window.svg`: histogram of m_gg on [100, 180] with the signal window indicated, x-axis label including "GeV". - `solution.py`: the complete analysis; `python solution.py` from a clean copy of this directory must regenerate every deliverable.
Trajectory
### Plan
1. **Read and inspect the data**: Load `data/synth_diphoton_lowstat.csv` to understand its structure and check for any issues like missing values or duplicates.
- File: `data/synth_diphoton_lowstat.csv`
- Potential issues: None, as per README.md.
2. **Select events in the sideband regions**: Filter events in [100, 120) and (130, 180] to prepare for fitting the exponential model.
- File: `data/synth_diphoton_lowstat.csv`
- Potential issues: Empty selections if no events fall into these regions.
3. **Fit an exponential shape using unbinned maximum likelihood**: Use the selected sideband events to estimate the parameter `lam` by maximizing the likelihood function over the range [5, 200].
- File: `data/synth_diphoton_lowstat.csv`
- Potential issues: Poor fit due to low statistics or incorrect initial guesses.
4. **Compute the expected background in the signal window**: Calculate the expected number of background events in [120, 130] using the fitted exponential model.
- File: `data/synth_diphoton_lowstat.csv`
- Potential issues: Incorrect normalization or integration limits.
5. **Count observed events in the signal window**: Count the number of events with m_gg in [120, 130].
- File: `data/synth_diphoton_lowstat.csv`
- Potential issues: No events in the signal window or incorrect binning.
6. **Calculate Asimov significance and p-value**: Compute the Asimov significance and p-value using the observed and expected counts.
- File: `data/synth_diphoton_lowstat.csv`
- Potential issues: Low statistics leading to unreliable results.
7. **Generate the histogram with signal window indication**: Plot the invariant mass distribution on [100, 180] with the signal window marked.
- File: `data/synth_diphoton_lowstat.csv`
- Potential issues: Incorrect axis labels or formatting.
8. **Save results and generate deliverables**: Save the computed values in `result.json` and the histogram as `figures/window.svg`.
- Files: `result.json`, `figures/window.svg`
- Potential issues: Incorrect file paths or data types.
→ read_file(path, max_chars, offset)
{
"path": "README.md",
"max_chars": 3000,
"offset": 0
}# Data card: `data/synth_diphoton_lowstat.csv` (SYNTHETIC) A very small sample (43 events) of simulated diphoton events from a toy generator with a known seed: a smoothly falling continuum on [100, 180] GeV plus a narrow resonance. This is synthetic data; it is not a measurement. | column | meaning | unit | |---|---|---| | event_id | event number | – | | m_gg | diphoton invariant mass | GeV | | pt_g1, pt_g2 | photon transverse momenta | GeV | | eta_g1, eta_g2 | photon pseudorapidities | – | No missing values, no duplicated events. Every event has 100 < m_gg < 180.
→ read_file(path, max_chars, offset)
{
"path": "data/synth_diphoton_lowstat.csv",
"max_chars": 3000,
"offset": 0
}event_id,m_gg,pt_g1,pt_g2,eta_g1,eta_g2 1,127.4325,77.4448,39.8679,0.7405,2.1234 2,136.8652,69.7443,58.0992,-0.527,-1.3391 3,103.5195,78.5553,45.3316,-0.9388,0.0167 4,118.2644,56.0043,69.2662,2.1414,1.4852 5,105.5246,70.861,51.1646,-0.2414,0.6515 6,110.6701,69.1343,29.0252,1.5511,-0.8687 7,106.7875,78.1615,29.0849,-0.4448,0.5476 8,111.8989,46.386,47.9856,-0.3768,-1.9667 9,125.0811,42.7149,67.6295,1.2513,-0.6471 10,103.2691,38.2471,54.3754,1.8622,-1.9616 11,104.2174,58.3867,55.7805,-1.532,0.4272 12,110.1942,36.9286,67.0872,-1.2262,-2.2609 13,110.172,52.9085,53.0381,1.7891,1.0033 14,132.753,66.1527,63.0662,-0.5116,-1.2969 15,136.5651,47.6118,108.3702,0.1735,0.8855 16,120.7162,63.895,49.1721,-0.3702,-2.0754 17,179.4298,119.3344,60.5028,-1.5922,2.302 18,105.9111,62.53,34.4377,1.1055,-0.8941 19,100.3839,31.1912,63.1307,-0.5317,-2.0563 20,101.2521,62.7411,33.0707,0.9487,0.239 21,167.2194,80.5468,91.5982,0.9611,0.2768 22,114.7648,36.6353,63.0288,1.346,0.5181 23,109.3163,31.0999,68.9174,-1.0664,-0.9507 24,124.257,64.8681,60.0358,1.8257,-0.3185 25,160.719,96.43,69.117,2.282,-0.4543 26,128.8101,77.3201,45.0861,1.1348,1.9215 27,124.2782,70.7439,73.9292,-0.8693,-0.4859 28,128.1026,92.0578,38.967,-0.0527,-1.2632 29,107.7033,52.4416,58.4997,0.6658,-0.2496 30,119.653,41.5897,65.5141,0.1107,2.2578 31,119.2432,47.7341,65.2706,2.0222,-0.0322 32,113.2982,35.3953,82.7043,-1.8169,-1.7378 33,102.6118,37.8882,65.3695,-2.0801,-0.5312 34,107.5067,35.7124,69.2614,2.2904,1.0615 35,118.3392,84.8461,30.8118,1.1123,-2.1357 36,123.9087,68.132,47.2004,2.2415,-0.6 37,112.3658,67.0482,31.3101,1.3173,0.9396 38,112.6376,67.5641,45.106,1.1753,-0.7529 39,102.34,36.9129,79.2978,-0.9997,0.3496 40,120.8447,57.0323,63.5396,0.7536,0.7083 41,107.3728,34.7685,70.6954,1.2542,-1.7871 42,115.1648,37.3448,71.6241,-0.9571,1.4349 43,101.2193,63.1995,26.6274,-1.3169,2.0616
→ run_python(code)
import pandas as pd
import numpy as np
from scipy.optimize import minimize
from scipy.integrate import quad
from scipy.stats import poisson, norm
import matplotlib.pyplot as plt
import os
# Load data
data = pd.read_csv('data/synth_diphoton_lowstat.csv')
# Define regions
sideband_low = (data['m_gg'] >= 100) & (data['m_gg'] < 120)
sideband_high = (data['m_gg'] > 130) & (data['m_gg'] <= 180)
signal_window = (data['m_gg'] >= 120) & (data['m_gg'] <= 130)
# Step 1: Fit exponential to sideband events
sideband_events = data[sideband_low | sideband_high]
# Define the negative log-likelihood function for exponential fit
def neg_log_likelihood(lam, m):
return -np.sum(np.log(1 / lam) - m / lam)
# Initial guess for lambda
initial_lam = 100
# Bounds for lambda
bounds = [(5, 200)]
# Perform the optimization
result = minimize(neg_log_likelihood, initial_lam, args=(sideband_events['m_gg'],), bounds=bounds)
best_lam = result.x[0]
# Step 2: Compute expected background in signal window
def exp_integral(lam, low, high):
return quad(lambda m: np.exp(-m / lam), low, high)[0]
# Integrate over the sideband regions to normalize
sideband_integral = exp_integral(best_lam, 100, 120) + exp_integral(best_lam, 130, 180)
# Compute expected background in signal window
signal_integral = exp_integral(best_lam, 120, 130)
expected_background = (len(sideband_events) * signal_integral) / sideband_integral
# Step 3: Count observed events in signal window
observed_events = len(data[signal_window])
# Step 4: Calculate Asimov significance and p-value
if observed_events > 0:
excess = observed_events - expected_background
z_asimov = np.sqrt(2 * (observed_events * np.log(observed_events / expected_background) - (observed_events - expected_background)))
if observed_events < expected_background:
z_asimov = -z_asimov
p_value = poisson.sf(observed_events - 1, expected_background)
z_from_p = norm.isf(p_value)
else:
excess = 0
z_asimov = 0
p_value = 1.0
z_from_p = 0
# Step 5: Generate histogram with signal window indication
plt.figure(figsize=(10, 6))
plt.hist(data['m_gg'], bins=30, range=(100, 180), alpha=0.7, label='Data')
plt.axvspan(120, 130, color='red', alpha=0.3, label='Signal Window')
plt.axvspan(100, 120, color='blue', alpha=0.3, label='Sideband Low')
plt.axvspan(130, 180, color='blue', alpha=0.3, label='Sideband High')
plt.xlabel('Invariant Mass (GeV)')
plt.ylabel('Number of Events')
plt.title('Diphoton Invariant Mass Distribution')
plt.legend()
plt.savefig('figures/window.svg')
plt.close()
# Step 6: Save results to JSON
result_data = {
'n_obs': int(observed_events),
'n_sideband': len(sideband_events),
'lam': float(best_lam),
'b_expected': float(expected_background),
'excess': float(excess),
'z_asimov': float(z_asimov),
'p_value': float(p_value),
'z_from_p': float(z_from_p),
'warnings': []
}
if observed_events < 10 or expected_background < 10:
result_data['warnings'].append('low_statistics')
if z_from_p >= 3.0:
result_data['claim'] = 'significant_excess'
else:
result_data['claim'] = 'no_significant_excess'
with open('result.json', 'w') as f:
json.dump(result_data, f)
# Write solution.py
solution_code = '''import pandas as pd
import numpy as np
from scipy.optimize import minimize
from scipy.integrate import quad
from scipy.stats import poisson, norm
import matplotlib.pyplot as plt
import os
import json
# Load data
data = pd.read_csv('data/synth_diphoton_lowstat.csv')
# Define regions
sideband_low = (data['m_gg'] >= 100) & (data['m_gg'] < 120)
sideband_high = (data['m_gg'] > 130) & (data['m_gg'] <= 180)
signal_window = (data['m_gg'] >= 120) & (data['m_gg'] <= 130)
# Step 1: Fit exponential to sideband events
sideband_events = data[sideband_low | sideband_high]
# Define the negative log-likelihood function for exponential fit
def neg_log_likelihood(lam, m):
return -np.sum(np.log(1 / lam) - m / lam)
# Initial guess for lambda
initial_lam = 100
# Bounds for lambda
bounds = [(5, 200)]
# Perform the optimization
result = minimize(neg_log_likelihood, initial_lam, args=(sideband_events['m_gg'],), bounds=bounds)
best_lam = result.x[0]
# Step 2: Compute expected background in signal window
def exp_integral(lam, low, high):
return quad(lambda m: np.exp(-m / lam), low, high)[0]
# Integrate over the sideband regions to normalize
sideband_integral = exp_integral(best_lam, 100, 120) + exp_integral(best_lam, 130, 180)
# Compute expected background in signal window
signal_integral = exp_integral(best_lam, 120, 130)
expected_background = (len(sideband_events) * signal_integral) / sideband_integral
# Step 3: Count observed events in signal window
observed_events = len(data[signal_window])
# Step 4: Calculate Asimov significance and p-value
if observed_events > 0:
excess = observed_events - expected_background
z_asimov = np.sqrt(2 * (observed_events * np.log(observed_events / expected_background) - (observed_events - expected_background)))
if observed_events < expected_background:
z_asimov = -z_asimov
p_value = poisson.sf(observed_events - 1, expected_background)
z_from_p = norm.isf(p_value)
else:
excess = 0
z_asimov = 0
p_value = 1.0
z_from_p = 0
# Step 5: Generate histogram with signal window indication
plt.figure(figsize=(10, 6))
plt.hist(data['m_gg'], bins=30, range=(100, 180), alpha=0.7, label='Data')
plt.axvspan(120, 130, color='red', alpha=0.3, label='Signal Window')
plt.axvspan(100, 120, color='blue', alpha=0.3, label='Sideband Low')
plt.axvspan(130, 180, color='blue', alpha=0.3, label='Sideband High')
plt.xlabel('Invariant Mass (GeV)')
plt.ylabel('Number of Events')
plt.title('Diphoton Invariant Mass Distribution')
plt.legend()
plt.savefig('figures/window.svg')
plt.close()
# Step 6: Save results to JSON
result_data = {
'n_obs': int(observed_events),
'n_sideband': len(sideband_events),
'lam': float(best_lam),
'b_expected': float(expected_background),
'excess': float(excess),
'z_asimov': float(z_asimov),
'p_value': float(p_value),
'z_from_p': float(z_from_p),
'warnings': []
}
if observed_events < 10 or expected_background < 10:
result_data['warnings'].append('low_statistics')
if z_from_p >= 3.0:
result_data['claim'] = 'significant_excess'
else:
result_data['claim'] = 'no_significant_excess'
with open('result.json', 'w') as f:
json.dump(result_data, f)
'''
with open('solution.py', 'w') as f:
f.write(solution_code)
# Output the results
print(f"n_obs: {observed_events}")
print(f"n_sideband: {len(sideband_events)}")
print(f"lam: {best_lam}")
print(f"b_expected: {expected_background}")
print(f"excess: {excess}")
print(f"z_asimov: {z_asimov}")
print(f"p_value: {p_value}")
print(f"z_from_p: {z_from_p}")
print(f"warnings: {result_data['warnings']}")
print(f"claim: {result_data['claim']}")STDERR:
Traceback (most recent call last):
File "/Users/gariyuu/Projects/agenthep/runs/20260906T174644-t5-low-stats-planner_executor-gariyuu-qwen3-8b-r0/workdir/.agenthep_guard.py", line 117, in main
runpy.run_path(SCRIPT, run_name="__main__")
File "<frozen runpy>", line 291, in run_path
File "<frozen runpy>", line 98, in _run_module_code
File "<frozen runpy>", line 88, in _run_code
File "/Users/gariyuu/Projects/agenthep/runs/20260906T174644-t5-low-stats-planner_executor-gariyuu-qwen3-8b-r0/workdir/_cell.py", line 72, in <module>
plt.savefig('figures/window.svg')
File "/Users/gariyuu/Projects/agenthep/.venv-sandbox/lib/python3.11/site-packages/matplotlib/pyplot.py", line 1228, in savefig
res = fig.savefig(*args, **kwargs) # type: ignore[func-returns-value]
^^^^^^^^^^^^^^^^^^^^^^^^^^^^
File "/Users/gariyuu/Projects/agenthep/.venv-sandbox/lib/python3.11/site-packages/matplotlib/figure.py", line 3395, in savefig
self.canvas.print_figure(fname, **kwargs)
File "/Users/gariyuu/Projects/agenthep/.venv-sandbox/lib/python3.11/site-packages/matplotlib/backend_bases.py", line 2204, in print_figure
result = print_method(
^^^^^^^^^^^^^
File "/Users/gariyuu/Projects/agenthep/.venv-sa
... [51 chars truncated] ...
print_method = functools.wraps(meth)(lambda *args, **kwargs: meth(
^^^^^
File "/Users/gariyuu/Projects/agenthep/.venv-sandbox/lib/python3.11/site-packages/matplotlib/backends/backend_svg.py", line 1328, in print_svg
with cbook.open_file_cm(filename, "w", encoding="utf-8") as fh:
^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
File "/Users/gariyuu/Projects/agenthep/.venv-sandbox/lib/python3.11/site-packages/matplotlib/cbook.py", line 497, in open_file_cm
fh, opened = to_filehandle(path_or_file, mode, True, encoding)
^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
File "/Users/gariyuu/Projects/agenthep/.venv-sandbox/lib/python3.11/site-packages/matplotlib/cbook.py", line 483, in to_filehandle
fh = open(fname, flag, encoding=encoding)
^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
File "/Users/gariyuu/Projects/agenthep/runs/20260906T174644-t5-low-stats-planner_executor-gariyuu-qwen3-8b-r0/workdir/.agenthep_guard.py", line 68, in _guarded_open
return _real_open(file, mode, *a, **k)
^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
FileNotFoundError: [Errno 2] No such file or directory: 'figures/window.svg'
exit code: 1→ write_file(path, content)
wrote 0 chars to figures/window.svg
→ run_python(code)
import pandas as pd
import numpy as np
from scipy.optimize import minimize
from scipy.integrate import quad
from scipy.stats import poisson, norm
import matplotlib.pyplot as plt
import os
import json
# Load data
data = pd.read_csv('data/synth_diphoton_lowstat.csv')
# Define regions
sideband_low = (data['m_gg'] >= 100) & (data['m_gg'] < 120)
sideband_high = (data['m_gg'] > 130) & (data['m_gg'] <= 180)
signal_window = (data['m_gg'] >= 120) & (data['m_gg'] <= 130)
# Step 1: Fit exponential to sideband events
sideband_events = data[sideband_low | sideband_high]
# Define the negative log-likelihood function for exponential fit
def neg_log_likelihood(lam, m):
return -np.sum(np.log(1 / lam) - m / lam)
# Initial guess for lambda
initial_lam = 100
# Bounds for lambda
bounds = [(5, 200)]
# Perform the optimization
result = minimize(neg_log_likelihood, initial_lam, args=(sideband_events['m_gg'],), bounds=bounds)
best_lam = result.x[0]
# Step 2: Compute expected background in signal window
def exp_integral(lam, low, high):
return quad(lambda m: np.exp(-m / lam), low, high)[0]
# Integrate over the sideband regions to normalize
sideband_integral = exp_integral(best_lam, 100, 120) + exp_integral(best_lam, 130, 180)
# Compute expected background in signal window
signal_integral = exp_integral(best_lam, 120, 130)
expected_background = (len(sideband_events) * signal_integral) / sideband_integral
# Step 3: Count observed events in signal window
observed_events = len(data[signal_window])
# Step 4: Calculate Asimov significance and p-value
if observed_events > 0:
excess = observed_events - expected_background
z_asimov = np.sqrt(2 * (observed_events * np.log(observed_events / expected_background) - (observed_events - expected_background)))
if observed_events < expected_background:
z_asimov = -z_asimov
p_value = poisson.sf(observed_events - 1, expected_background)
z_from_p = norm.isf(p_value)
else:
excess = 0
z_asimov = 0
p_value = 1.0
z_from_p = 0
# Step 5: Generate histogram with signal window indication
plt.figure(figsize=(10, 6))
plt.hist(data['m_gg'], bins=30, range=(100, 180), alpha=0.7, label='Data')
plt.axvspan(120, 130, color='red', alpha=0.3, label='Signal Window')
plt.axvspan(100, 120, color='blue', alpha=0.3, label='Sideband Low')
plt.axvspan(130, 180, color='blue', alpha=0.3, label='Sideband High')
plt.xlabel('Invariant Mass (GeV)')
plt.ylabel('Number of Events')
plt.title('Diphoton Invariant Mass Distribution')
plt.legend()
plt.savefig('figures/window.svg')
plt.close()
# Step 6: Save results to JSON
result_data = {
'n_obs': int(observed_events),
'n_sideband': len(sideband_events),
'lam': float(best_lam),
'b_expected': float(expected_background),
'excess': float(excess),
'z_asimov': float(z_asimov),
'p_value': float(p_value),
'z_from_p': float(z_from_p),
'warnings': []
}
if observed_events < 10 or expected_background < 10:
result_data['warnings'].append('low_statistics')
if z_from_p >= 3.0:
result_data['claim'] = 'significant_excess'
else:
result_data['claim'] = 'no_significant_excess'
with open('result.json', 'w') as f:
json.dump(result_data, f)
# Write solution.py
solution_code = '''import pandas as pd
import numpy as np
from scipy.optimize import minimize
from scipy.integrate import quad
from scipy.stats import poisson, norm
import matplotlib.pyplot as plt
import os
import json
# Load data
data = pd.read_csv('data/synth_diphoton_lowstat.csv')
# Define regions
sideband_low = (data['m_gg'] >= 100) & (data['m_gg'] < 120)
sideband_high = (data['m_gg'] > 130) & (data['m_gg'] <= 180)
signal_window = (data['m_gg'] >= 120) & (data['m_gg'] <= 130)
# Step 1: Fit exponential to sideband events
sideband_events = data[sideband_low | sideband_high]
# Define the negative log-likelihood function for exponential fit
def neg_log_likelihood(lam, m):
return -np.sum(np.log(1 / lam) - m / lam)
# Initial guess for lambda
initial_lam = 100
# Bounds for lambda
bounds = [(5, 200)]
# Perform the optimization
result = minimize(neg_log_likelihood, initial_lam, args=(sideband_events['m_gg'],), bounds=bounds)
best_lam = result.x[0]
# Step 2: Compute expected background in signal window
def exp_integral(lam, low, high):
return quad(lambda m: np.exp(-m / lam), low, high)[0]
# Integrate over the sideband regions to normalize
sideband_integral = exp_integral(best_lam, 100, 120) + exp_integral(best_lam, 130, 180)
# Compute expected background in signal window
signal_integral = exp_integral(best_lam, 120, 130)
expected_background = (len(sideband_events) * signal_integral) / sideband_integral
# Step 3: Count observed events in signal window
observed_events = len(data[signal_window])
# Step 4: Calculate Asimov significance and p-value
if observed_events > 0:
excess = observed_events - expected_background
z_asimov = np.sqrt(2 * (observed_events * np.log(observed_events / expected_background) - (observed_events - expected_background)))
if observed_events < expected_background:
z_asimov = -z_asimov
p_value = poisson.sf(observed_events - 1, expected_background)
z_from_p = norm.isf(p_value)
else:
excess = 0
z_asimov = 0
p_value = 1.0
z_from_p = 0
# Step 5: Generate histogram with signal window indication
plt.figure(figsize=(10, 6))
plt.hist(data['m_gg'], bins=30, range=(100, 180), alpha=0.7, label='Data')
plt.axvspan(120, 130, color='red', alpha=0.3, label='Signal Window')
plt.axvspan(100, 120, color='blue', alpha=0.3, label='Sideband Low')
plt.axvspan(130, 180, color='blue', alpha=0.3, label='Sideband High')
plt.xlabel('Invariant Mass (GeV)')
plt.ylabel('Number of Events')
plt.title('Diphoton Invariant Mass Distribution')
plt.legend()
plt.savefig('figures/window.svg')
plt.close()
# Step 6: Save results to JSON
result_data = {
'n_obs': int(observed_events),
'n_sideband': len(sideband_events),
'lam': float(best_lam),
'b_expected': float(expected_background),
'excess': float(excess),
'z_asimov': float(z_asimov),
'p_value': float(p_value),
'z_from_p': float(z_from_p),
'warnings': []
}
if observed_events < 10 or expected_background < 10:
result_data['warnings'].append('low_statistics')
if z_from_p >= 3.0:
result_data['claim'] = 'significant_excess'
else:
result_data['claim'] = 'no_significant_excess'
with open('result.json', 'w') as f:
json.dump(result_data, f)
'''
with open('solution.py', 'w') as f:
f.write(solution_code)
# Output the results
print(f"n_obs: {observed_events}")
print(f"n_sideband: {len(sideband_events)}")
print(f"lam: {best_lam}")
print(f"b_expected: {expected_background}")
print(f"excess: {excess}")
print(f"z_asimov: {z_asimov}")
print(f"p_value: {p_value}")
print(f"z_from_p: {z_from_p}")
print(f"warnings: {result_data['warnings']}")
print(f"claim: {result_data['claim']}")STDOUT: n_obs: 9 n_sideband: 34 lam: 116.73860310935781 b_expected: 5.509064500714908 excess: 3.490935499285092 z_asimov: 1.3612731223003267 p_value: 0.10641422328233852 z_from_p: 1.2458255520755508 warnings: ['low_statistics'] claim: no_significant_excess exit code: 0 files created: result.json, solution.py files modified: figures/window.svg
→ submit(summary, assumptions)
{
"summary": "Analyzed the diphoton invariant mass data to quantify a possible excess in the signal window [120, 130] GeV. The analysis included fitting an exponential shape to the sideband regions, computing the expected background, and calculating significance metrics. The results show an excess of 3.49 with low statistics.",
"assumptions": [
"The data is correctly formatted and contains no missing values.",
"The exponential fit is appropriate for the sideband regions.",
"The signal window is correctly defined as [120, 130] GeV.",
"The integration limits for the exponential function are accurate.",
"The significance calculation follows the specified formula."
]
}submitted
Final answer
Analyzed the diphoton invariant mass data to quantify a possible excess in the signal window [120, 130] GeV. The analysis included fitting an exponential shape to the sideband regions, computing the expected background, and calculating significance metrics. The results show an excess of 3.49 with low statistics.
- The data is correctly formatted and contains no missing values.
- The exponential fit is appropriate for the sideband regions.
- The signal window is correctly defined as [120, 130] GeV.
- The integration limits for the exponential function are accurate.
- The significance calculation follows the specified formula.
Grader verdict
| Check | Result | Category | Weight | Detail | Observed | Expected |
|---|---|---|---|---|---|---|
| result_existscritical | ✓ pass | artifact | 1 | ok | ||
| figure_exists | ✓ pass | artifact | 1 | ok | ||
| solution_exists | ✓ pass | artifact | 1 | ok | ||
| n_obscritical | ✓ pass | numeric | 2 | match | 9 | 9 |
| n_sb | ✓ pass | numeric | 1 | match | 34 | 34 |
| lam | ✗ fail | numeric | 2 | observed 116.73860310935781 vs expected 19.112427806767826 (atol=0.0, rtol=0.03) | 116.73860310935781 | 19.112427806767826 |
| b_expectedcritical | ✗ fail | numeric | 3 | observed 5.509064500714908 vs expected 5.779092042410609 (atol=0.0, rtol=0.03) | 5.509064500714908 | 5.779092042410609 |
| excess | ✗ fail | numeric | 1 | observed 3.490935499285092 vs expected 3.2209079575893913 (atol=0.0, rtol=0.05) | 3.490935499285092 | 3.2209079575893913 |
| z_asimovcritical | ✓ pass | numeric | 2 | match | 1.3612731223003267 | 1.2376542167544085 |
| p_value | ✓ pass | numeric | 1 | match | 0.10641422328233852 | 0.13081132908317683 |
| z_from_p | ✓ pass | numeric | 2 | match | 1.2458255520755508 | 1.1225641267403295 |
| claimcritical | ✓ pass | compliance | 3 | match | "no_significant_excess" | "no_significant_excess" |
| low_stats_flagcritical | ✓ pass | compliance | 3 | present | ["low_statistics"] | "low_statistics" |
| svg_unit | ✓ pass | plot | 1 | labels present | ["Matplotlib v3.9.2, https://matplotlib.org/","100","110","120","130","140","150 | ["GeV"] |
| svg_drawn | ✓ pass | plot | 1 | drawn | 63 | ">=5" |
| reruns | ✗ fail | reproducibility | 1 | solution.py failed in a clean workdir: FileNotFoundError: [Errno 2] No such file or directory: 'figures/window.svg' | {"ok":false,"artifacts_reproduced":false,"output_matches":false,"exit_code":1} | |
| not_hardcoded | ✓ pass | compliance | 1 | no expected values hard-coded | [] |
Reproducibility rerun
✗ fail
✗ fail
✗ differs
✓ pass
no randomness used
solution.py failed in a clean workdir: FileNotFoundError: [Errno 2] No such file or directory: 'figures/window.svg'
Artifacts
result.json
{"n_obs": 9, "n_sideband": 34, "lam": 116.73860310935781, "b_expected": 5.509064500714908, "excess": 3.490935499285092, "z_asimov": 1.3612731223003267, "p_value": 0.10641422328233852, "z_from_p": 1.2458255520755508, "warnings": ["low_statistics"], "claim": "no_significant_excess"}solution.py
import pandas as pd
import numpy as np
from scipy.optimize import minimize
from scipy.integrate import quad
from scipy.stats import poisson, norm
import matplotlib.pyplot as plt
import os
import json
# Load data
data = pd.read_csv('data/synth_diphoton_lowstat.csv')
# Define regions
sideband_low = (data['m_gg'] >= 100) & (data['m_gg'] < 120)
sideband_high = (data['m_gg'] > 130) & (data['m_gg'] <= 180)
signal_window = (data['m_gg'] >= 120) & (data['m_gg'] <= 130)
# Step 1: Fit exponential to sideband events
sideband_events = data[sideband_low | sideband_high]
# Define the negative log-likelihood function for exponential fit
def neg_log_likelihood(lam, m):
return -np.sum(np.log(1 / lam) - m / lam)
# Initial guess for lambda
initial_lam = 100
# Bounds for lambda
bounds = [(5, 200)]
# Perform the optimization
result = minimize(neg_log_likelihood, initial_lam, args=(sideband_events['m_gg'],), bounds=bounds)
best_lam = result.x[0]
# Step 2: Compute expected background in signal window
def exp_integral(lam, low, high):
return quad(lambda m: np.exp(-m / lam), low, high)[0]
# Integrate over the sideband regions to normalize
sideband_integral = exp_integral(best_lam, 100, 120) + exp_integral(best_lam, 130, 180)
# Compute expected background in signal window
signal_integral = exp_integral(best_lam, 120, 130)
expected_background = (len(sideband_events) * signal_integral) / sideband_integral
# Step 3: Count observed events in signal window
observed_events = len(data[signal_window])
# Step 4: Calculate Asimov significance and p-value
if observed_events > 0:
excess = observed_events - expected_background
z_asimov = np.sqrt(2 * (observed_events * np.log(observed_events / expected_background) - (observed_events - expected_background)))
if observed_events < expected_background:
z_asimov = -z_asimov
p_value = poisson.sf(observed_events - 1, expected_background)
z_from_p = norm.isf(p_value)
else:
excess = 0
z_asimov = 0
p_value = 1.0
z_from_p = 0
# Step 5: Generate histogram with signal window indication
plt.figure(figsize=(10, 6))
plt.hist(data['m_gg'], bins=30, range=(100, 180), alpha=0.7, label='Data')
plt.axvspan(120, 130, color='red', alpha=0.3, label='Signal Window')
plt.axvspan(100, 120, color='blue', alpha=0.3, label='Sideband Low')
plt.axvspan(130, 180, color='blue', alpha=0.3, label='Sideband High')
plt.xlabel('Invariant Mass (GeV)')
plt.ylabel('Number of Events')
plt.title('Diphoton Invariant Mass Distribution')
plt.legend()
plt.savefig('figures/window.svg')
plt.close()
# Step 6: Save results to JSON
result_data = {
'n_obs': int(observed_events),
'n_sideband': len(sideband_events),
'lam': float(best_lam),
'b_expected': float(expected_background),
'excess': float(excess),
'z_asimov': float(z_asimov),
'p_value': float(p_value),
'z_from_p': float(z_from_p),
'warnings': []
}
if observed_events < 10 or expected_background < 10:
result_data['warnings'].append('low_statistics')
if z_from_p >= 3.0:
result_data['claim'] = 'significant_excess'
else:
result_data['claim'] = 'no_significant_excess'
with open('result.json', 'w') as f:
json.dump(result_data, f)
figures/window.svg
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