Skip to content

Commit 56f3ea7

Browse files
Zach MarshallZach Marshall
authored andcommitted
Adding feedback forms to active notebooks
Adding the feedback form as in !126 to the active notebooks
1 parent 8e48f10 commit 56f3ea7

12 files changed

+90
-11
lines changed

13-TeV-examples/uproot_python/Find_the_Z.ipynb

Lines changed: 6 additions & 1 deletion
Original file line numberDiff line numberDiff line change
@@ -488,7 +488,12 @@
488488
"* **Extract the Z boson width from your fit**.\n",
489489
"* **Extend your graph**. Try a larger range in mass. Can you see the Higgs boson? Why or why not? Can you see any particles with much lower mass (around 5-10 GeV)? Why or why not? Can you figure out what some of those particles might be?\n",
490490
"\n",
491-
"With each change, keep an eye on your graph."
491+
"With each change, keep an eye on your graph.",
492+
"\n",
493+
"\n",
494+
"<div class=\"alert alert-block alert-info\">\n",
495+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
496+
"</div>"
492497
]
493498
},
494499
{

13-TeV-examples/uproot_python/HZZAnalysis.ipynb

Lines changed: 11 additions & 0 deletions
Original file line numberDiff line numberDiff line change
@@ -1486,6 +1486,17 @@
14861486
"signal_significance = N_sig/np.sqrt(N_bg + 0.3 * N_bg**2) # EXPLAIN THE 0.3\n",
14871487
"print(f\"\\nResults:\\n{N_sig = }\\n{N_bg = }\\n{signal_significance = }\\n\")"
14881488
]
1489+
},
1490+
{
1491+
"cell_type": "markdown",
1492+
"metadata": {
1493+
"id": "feedback"
1494+
},
1495+
"source": [
1496+
"<div class=\"alert alert-block alert-info\">\n",
1497+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
1498+
"</div>"
1499+
]
14891500
}
14901501
],
14911502
"metadata": {

13-TeV-examples/uproot_python/HbbAnalysis.ipynb

Lines changed: 6 additions & 1 deletion
Original file line numberDiff line numberDiff line change
@@ -1621,7 +1621,12 @@
16211621
"source": [
16221622
"Great progress! We have significantly improved the signal-to-background ratio with the cuts applied above. However, the $H \\to b\\bar{b}$ signal still remains difficult to distinguish from the substantial background contributions, particularly from processes such as $t\\bar{t}$ and $W/Z$ + jets. As noted earlier in the notebook, although $b\\bar{b}$ is the dominant decay channel of the Higgs boson, the search for $H \\to b\\bar{b}$ presents unique challenges due to the variety of other processes that can also produce $b\\bar{b}$ pairs at the LHC.\n",
16231623
"\n",
1624-
"With the insights gained from this analysis, we encourage you to revisit the limitations outlined at the start of the notebook and explore potential strategies to enhance the results."
1624+
"With the insights gained from this analysis, we encourage you to revisit the limitations outlined at the start of the notebook and explore potential strategies to enhance the results.",
1625+
"\n",
1626+
"\n",
1627+
"<div class=\"alert alert-block alert-info\">\n",
1628+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
1629+
"</div>"
16251630
]
16261631
}
16271632
],

13-TeV-examples/uproot_python/Hmumu.ipynb

Lines changed: 11 additions & 0 deletions
Original file line numberDiff line numberDiff line change
@@ -948,6 +948,17 @@
948948
"source": [
949949
"plot_data(data_all,True)"
950950
]
951+
},
952+
{
953+
"cell_type": "markdown",
954+
"metadata": {
955+
"id": "feedback"
956+
},
957+
"source": [
958+
"<div class=\"alert alert-block alert-info\">\n",
959+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
960+
"</div>"
961+
]
951962
}
952963
],
953964
"metadata": {

13-TeV-examples/uproot_python/HyyAnalysis.ipynb

Lines changed: 7 additions & 2 deletions
Original file line numberDiff line numberDiff line change
@@ -973,7 +973,7 @@
973973
"id": "Hjy3wlBoSh4J"
974974
},
975975
"source": [
976-
"And there it is a clear peak in the invariant mass spectrum around 125 GeV, signaling the presence of the Higgs boson!\n",
976+
"And there it is: a clear peak in the invariant mass spectrum around 125 GeV, signaling the presence of the Higgs boson!\n",
977977
"\n",
978978
"This represents a very close result to the one obtained by ATLAS in [Higgs decay to photons measurement paper](https://journals.aps.org/prd/abstract/10.1103/PhysRevD.98.052005), which can be seen below:\n",
979979
"<CENTER><img src=\"https://github.com/atlas-outreach-data-tools/notebooks-collection-opendata/blob/master/13-TeV-examples/uproot_python/images/ImagesHiggs/HyyPaper.png?raw=1\" style=\"width:50%\"></CENTER>"
@@ -993,7 +993,12 @@
993993
"* Find the width of the fitted Gaussian in '[Plotting](#plotting)'\n",
994994
"* Try different initial guesses for the parameters of the fit in '[Plotting](#plotting)'\n",
995995
"* Try different functions for the fit in '[Plotting](#plotting)'\n",
996-
"* Your idea!"
996+
"* Your idea!",
997+
"\n",
998+
"\n",
999+
"<div class=\"alert alert-block alert-info\">\n",
1000+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
1001+
"</div>"
9971002
]
9981003
}
9991004
],

13-TeV-examples/uproot_python/MetadataTutorial.ipynb

Lines changed: 1 addition & 1 deletion
Original file line numberDiff line numberDiff line change
@@ -244,7 +244,7 @@
244244
"\n",
245245
"\n",
246246
"<div class=\"alert alert-block alert-info\">\n",
247-
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7 \">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
247+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
248248
"</div>"
249249
]
250250
}

13-TeV-examples/uproot_python/WZ3l_Analysis.ipynb

Lines changed: 11 additions & 0 deletions
Original file line numberDiff line numberDiff line change
@@ -1547,6 +1547,17 @@
15471547
" np.hstack(all_data['other']['ee_pair_mass']), np.hstack(all_data['other']['totalWeight'])\n",
15481548
")"
15491549
]
1550+
},
1551+
{
1552+
"cell_type": "markdown",
1553+
"metadata": {
1554+
"id": "feedback"
1555+
},
1556+
"source": [
1557+
"<div class=\"alert alert-block alert-info\">\n",
1558+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
1559+
"</div>"
1560+
]
15501561
}
15511562
],
15521563
"metadata": {

13-TeV-examples/uproot_python/detector_acceptance_and_efficiency.ipynb

Lines changed: 8 additions & 3 deletions
Original file line numberDiff line numberDiff line change
@@ -1510,13 +1510,18 @@
15101510
"\n",
15111511
"<CENTER><img src=\"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/SUSY-2023-22/figaux_08c.png\" style=\"width:80%\"></CENTER>\n",
15121512
"\n",
1513-
"The setup here is similar, with each number showing the efficiency for a particular configuration of a new physics model with specific masses for the new particles. Here, notice that the efficiency is over 1 for many of the model points, meaning that the efficiency is over 100%! That seems surprising, and requires some thought to understand. Let's consider a simple analogy. Let's say that typically 10% of the cars on a road are white, and you want to count the number of white cars in the next 100. If you have perfect efficiency, and there are 10 white cars, youll find 10 white cars. Now suppose that you can always correctly identify a white car, but now half the time you see a blue car you accidentally count it as white. Then you could count *more* than 10 white cars, when there are only 10 in reality. That would produce an efficiency over 100%.\n",
1513+
"The setup here is similar, with each number showing the efficiency for a particular configuration of a new physics model with specific masses for the new particles. Here, notice that the efficiency is over 1 for many of the model points, meaning that the efficiency is over 100%! That seems surprising, and requires some thought to understand. Let's consider a simple analogy. Let's say that typically 10% of the cars on a road are white, and you want to count the number of white cars in the next 100. If you have perfect efficiency, and there are 10 white cars, you'll find 10 white cars. Now suppose that you can always correctly identify a white car, but now half the time you see a blue car you accidentally count it as white. Then you could count *more* than 10 white cars, when there are only 10 in reality. That would produce an efficiency over 100%.\n",
15141514
"\n",
1515-
"In a similar way, our detector sometimes makes mistakes that make more signal events than expected turn up in the signal region. In some sense, thats nice to have we have more signal in our signal region, and we have an easier time finding new particles than we would if the detector was perfect. In practice, that usually comes with larger backgrounds (larger numbers of Standard Model events), which make the searches more difficult.\n",
1515+
"In a similar way, our detector sometimes makes mistakes that make more signal events than expected turn up in the signal region. In some sense, that's nice to have: we have more signal in our signal region, and we have an easier time finding new particles than we would if the detector was perfect. In practice, that usually comes with larger backgrounds (larger numbers of Standard Model events), which make the searches more difficult.\n",
15161516
"\n",
15171517
"### Reading results\n",
15181518
"\n",
1519-
"Many of the papers that you might read in high energy particle physics will provide, either directly in the paper or in \"auxilliary material\" released with the paper, the acceptance and efficiency of the analysis. Understanding these numbers can be a big help towards understanding the results, and why they look the way they do. They can help you disentangle what is caused by the choices made in the design of the analysis (the acceptance) and what is caused by the detector itself (the efficiency)."
1519+
"Many of the papers that you might read in high energy particle physics will provide, either directly in the paper or in \"auxilliary material\" released with the paper, the acceptance and efficiency of the analysis. Understanding these numbers can be a big help towards understanding the results, and why they look the way they do. They can help you disentangle what is caused by the choices made in the design of the analysis (the acceptance) and what is caused by the detector itself (the efficiency).",
1520+
"\n",
1521+
"\n",
1522+
"<div class=\"alert alert-block alert-info\">\n",
1523+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
1524+
"</div>"
15201525
]
15211526
}
15221527
],

13-TeV-examples/uproot_python/systematics_notebook.ipynb

Lines changed: 6 additions & 1 deletion
Original file line numberDiff line numberDiff line change
@@ -1311,7 +1311,12 @@
13111311
"\n",
13121312
"You have explored the effects and learned the importance of systematic uncertainties in particle physics analyses!\n",
13131313
"\n",
1314-
"Want to learn more? Check out the [ATLAS Open Data website](https://opendata.atlas.cern) for educational content, and explore our [educational analysis notebooks section](https://opendata.atlas.cern/docs/13TeV25Doc/13tutorial) for more analysis examples!"
1314+
"Want to learn more? Check out the [ATLAS Open Data website](https://opendata.atlas.cern) for educational content, and explore our [educational analysis notebooks section](https://opendata.atlas.cern/docs/13TeV25Doc/13tutorial) for more analysis examples!",
1315+
"\n",
1316+
"\n",
1317+
"<div class=\"alert alert-block alert-info\">\n",
1318+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
1319+
"</div>"
13151320
]
13161321
}
13171322
],

13-TeV-examples/uproot_python/ttbar_analysis.ipynb

Lines changed: 11 additions & 0 deletions
Original file line numberDiff line numberDiff line change
@@ -992,6 +992,17 @@
992992
"# Plot the lepton-neutrino-b-jet mass distribution (m_lvb)\n",
993993
"plot_data(data_all_2,r\"$\\mathrm{m_{lvb}} \\ [GeV]$\")"
994994
]
995+
},
996+
{
997+
"cell_type": "markdown",
998+
"metadata": {
999+
"id": "feedback"
1000+
},
1001+
"source": [
1002+
"<div class=\"alert alert-block alert-info\">\n",
1003+
"We welcome your feedback on this notebook or any of our other materials! Please <a href=\"https://forms.gle/zKBqS1opAHHemv9U7\">fill out this survey</a> to let us know how we're doing, and you can enter a raffle to win some <a href=\"https://atlas-secretariat.web.cern.ch/merchandise\">ATLAS merchandise</a>!\n",
1004+
"</div>"
1005+
]
9951006
}
9961007
],
9971008
"metadata": {

0 commit comments

Comments
 (0)